11771:, we present alternative views of the transverse Doppler shift scenario where source and receiver are at their closest approach to each other. (a) If we analyze the scenario in the frame of the receiver, we find that the analysis is more complicated than it should be. The apparent position of a celestial object is displaced from its true position (or geometric position) because of the object's motion during the time it takes its light to reach an observer. The source would be time-dilated relative to the receiver, but the redshift implied by this time dilation would be offset by a blueshift due to the longitudinal component of the relative motion between the receiver and the apparent position of the source. (b) It is much easier if, instead, we analyze the scenario from the frame of the source. An observer situated at the source knows, from the problem statement, that the receiver is at its closest point to him. That means that the receiver has no longitudinal component of motion to complicate the analysis. Since the receiver's clocks are time-dilated relative to the source, the light that the receiver receives is therefore blue-shifted by a factor of
3069:. It is possible for a not-faster-than-light-speed signal to travel from the position and time of O to the position and time of D (Fig. 2-4). It is hence possible for event O to have a causal influence on event D. The future light cone contains all the events that could be causally influenced by O. Likewise, it is possible for a not-faster-than-light-speed signal to travel from the position and time of A, to the position and time of O. The past light cone contains all the events that could have a causal influence on O. In contrast, assuming that signals cannot travel faster than the speed of light, any event, like e.g. B or C, in the spacelike region (Elsewhere), cannot either affect event O, nor can they be affected by event O employing such signalling. Under this assumption any causal relationship between event O and any events in the spacelike region of a light cone is excluded.
11756:
S. Thus acceleration and deceleration is not the cause of shorter elapsed time during the outward and inward journey. Instead the use of two different constant, high-velocity inertial frames for outward and inward journey is really the cause of shorter elapsed time total. Granted, if the same twin has to travel outward and inward leg of the journey and safely switch from outward to inward leg of the journey, the acceleration and deceleration is required. If the travelling twin could ride the high-velocity outward inertial frame and instantaneously switch to high-velocity inward inertial frame the example would still work. The point is that real reason should be stated clearly. The asymmetry is because of the comparison of sum of elapsed times in two different inertial frames (O and I) to the elapsed time in a single inertial frame S.
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10030:. In the simplified, one-dimensional scenarios that we have been considering, only one additional constraint is necessary before the outgoing momenta of the particles can be determinedâan energy condition. In the one-dimensional case of a completely elastic collision with no loss of kinetic energy, the outgoing velocities of the rebounding particles in the COM frame will be precisely equal and opposite to their incoming velocities. In the case of a completely inelastic collision with total loss of kinetic energy, the outgoing velocities of the rebounding particles will be zero.
7966:
7202:, with no higher powers involved. The linearity of the transformation reflects a fundamental property of spacetime that was tacitly assumed in the derivation, namely, that the properties of inertial frames of reference are independent of location and time. In the absence of gravity, spacetime looks the same everywhere. All inertial observers will agree on what constitutes accelerating and non-accelerating motion. Any one observer can use her own measurements of space and time, but there is nothing absolute about them. Another observer's conventions will do just as well.
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the gravitational field at least at spatial infinity. The puzzling surprise in 1962 was their discovery of a rich infinite-dimensional group (the so-called BMS group) as the asymptotic symmetry group, instead of the finite-dimensional
PoincarĂŠ group, which is a subgroup of the BMS group. Not only are the Lorentz transformations asymptotic symmetry transformations, there are also additional transformations that are not Lorentz transformations but are asymptotic symmetry transformations. In fact, they found an additional infinity of transformation generators known as
7705:
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528:) relates distances measured in space to distances measured in time. The magnitude of this scale factor (nearly 300,000 kilometres or 190,000 miles in space being equivalent to one second in time), along with the fact that spacetime is a manifold, implies that at ordinary, non-relativistic speeds and at ordinary, human-scale distances, there is little that humans might observe that is noticeably different from what they might observe if the world were Euclidean. It was only with the advent of sensitive scientific measurements in the mid-1800s, such as the
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9877:" (also called the zero-momentum frame, or COM frame). This is the frame in which the space component of the system's total momentum is zero. Fig. 3-11 illustrates the breakup of a high speed particle into two daughter particles. In the lab frame, the daughter particles are preferentially emitted in a direction oriented along the original particle's trajectory. In the COM frame, however, the two daughter particles are emitted in opposite directions, although their masses and the magnitude of their velocities are generally not the same.
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paradigm in that they both represent the same physical phenomena. However, their mathematical formulations are entirely different. Working physicists routinely switch between using curved and flat spacetime techniques depending on the requirements of the problem. The flat spacetime paradigm is convenient when performing approximate calculations in weak fields. Hence, flat spacetime techniques tend be used when solving gravitational wave problems, while curved spacetime techniques tend be used in the analysis of black holes.
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1148:. The situation is even more complicated if the two points are separated in time as well as in space. For example, if one observer sees two events occur at the same place, but at different times, a person moving with respect to the first observer will see the two events occurring at different places, because the moving point of view sees itself as stationary, and the position of the event as receding or approaching. Thus, a different measure must be used to measure the effective "distance" between two events.
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830:(the study of moving bodies without reference to forces) rather than dynamics. His results were mathematically equivalent to those of Lorentz and PoincarĂŠ. He obtained them by recognizing that the entire theory can be built upon two postulates: the principle of relativity and the principle of the constancy of light speed. His work was filled with vivid imagery involving the exchange of light signals between clocks in motion, careful measurements of the lengths of moving rods, and other such examples.
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3584:. Clocks that travel faster take longer (in the observer frame) to tick out the same amount of proper time, and they travel further along the xâaxis within that proper time than they would have without time dilation. The measurement of time dilation by two observers in different inertial reference frames is mutual. If observer O measures the clocks of observer OⲠas running slower in his frame, observer OⲠin turn will measure the clocks of observer O as running slower.
948:(superfluous learnedness). However, in order to complete his search for general relativity that started in 1907, the geometric interpretation of relativity proved to be vital. In 1916, Einstein fully acknowledged his indebtedness to Minkowski, whose interpretation greatly facilitated the transition to general relativity. Since there are other types of spacetime, such as the curved spacetime of general relativity, the spacetime of special relativity is today known as
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moving in non-accelerated (inertial) reference frames. In general relativity, to use
Einstein's own (translated) words, "the laws of physics must be of such a nature that they apply to systems of reference in any kind of motion." This leads to an immediate issue: In accelerated frames, one feels forces that seemingly would enable one to assess one's state of acceleration in an absolute sense. Einstein resolved this problem through the principle of equivalence.
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3766:. Recording again the four readings for the events, defined by "two clocks simultaneously at one place", results in the analogous temporal distances of the two events, now temporally and spatially separated in Sâ˛, and only temporally separated but collocated in S. To keep the spacetime interval invariant, the temporal distance in S must be smaller than in Sâ˛, because of the spatial separation of the events in Sâ˛: now clock W is observed to run slower.
62:
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7936:, and in (d), the light is redshifted. The only seeming complication is that the orbiting objects are in accelerated motion. However, if an inertial observer looks at an accelerating clock, only the clock's instantaneous speed is important when computing time dilation. (The converse, however, is not true.) Most reports of transverse Doppler shift refer to the effect as a redshift and analyze the effect in terms of scenarios (b) or (d).
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11145:(as they are using different coordinate systems). Although their kinematic descriptions will differ, dynamical (physical) laws, such as momentum conservation and the first law of thermodynamics, will still hold. In fact, relativity theory requires more than this in the sense that it stipulates these (and all other physical) laws must take the same form in all coordinate systems. This introduces
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gravity greatly complicates the description of spacetime. In general relativity, spacetime is no longer a static background, but actively interacts with the physical systems that it contains. Spacetime curves in the presence of matter, can propagate waves, bends light, and exhibits a host of other phenomena. A few of these phenomena are described in the later sections of this article.
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4221:, his clock will appear to run fast, so much so that the net result will be that Terence has aged more than Stella when they are back together. The theoretical arguments predicting gravitational time dilation are not exclusive to general relativity. Any theory of gravity will predict gravitational time dilation if it respects the principle of equivalence, including Newton's theory.
14187:...redacted transcript of a course given by the author at Harvard in spring semester 2016. It contains a pedagogical overview of recent developments connecting the subjects of soft theorems, the memory effect and asymptotic symmetries in four-dimensional QED, nonabelian gauge theory and gravity with applications to black holes. To be published Princeton University Press, 158 pages.
819:. He did not pursue the 4-dimensional formalism in subsequent papers, however, stating that this line of research seemed to "entail great pain for limited profit", ultimately concluding "that three-dimensional language seems the best suited to the description of our world". Even as late as 1909, PoincarĂŠ continued to describe the dynamical interpretation of the Lorentz transform.
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accelerations that these particles exhibit with respect to each other do not require forces for their explanation. Rather, Einstein described them in terms of the geometry of spacetime, i.e. the curvature of spacetime. These tidal accelerations are strictly local. It is the cumulative total effect of many local manifestations of curvature that result in the
11563:(GedankenâExperimente) as a fundamental tool for understanding physical issues. For special relativity, he employed moving trains and flashes of lightning for his most penetrating insights. For curved spacetime, he considered a painter falling off a roof, accelerating elevators, blind beetles crawling on curved surfaces and the like. In his great
3600:, like time dilation, is a manifestation of the relativity of simultaneity. Measurement of length requires measurement of the spacetime interval between two events that are simultaneous in one's frame of reference. But events that are simultaneous in one frame of reference are, in general, not simultaneous in other frames of reference.
625:
4208:(i.e. between the bold blue lines in the figure), a shift takes place in the angle of her lines of simultaneity, corresponding to a rapid skip-over of the events in Terence's world line that Stella considers to be simultaneous with her own. Therefore, at the end of her trip, Stella finds that Terence has aged more than she has.
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paradox at all. The proper time measured along the traveling twin's world line from O to C, plus the proper time measured from C to B, is less than the stay-at-home twin's proper time measured from O to A to B. More complex trajectories require integrating the proper time between the respective events along the curve (i.e. the
11798:
that one body may act upon another at a distance thro' a Vacuum, without the
Mediation of any thing else, by and through which their Action and Force may be conveyed from one to another, is to me so great an Absurdity that I believe no Man who has in philosophical Matters a competent Faculty of thinking can ever fall into it."
6273:
10603:. A tractable case might be to consider the symmetries of spacetime as seen by observers located far away from all sources of the gravitational field. The naive expectation for asymptotically flat spacetime symmetries might be simply to extend and reproduce the symmetries of flat spacetime of special relativity,
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3638:Ⲡaxis demonstrates that, even as OB is foreshortened from the point of view of observer O, OA is likewise foreshortened from the point of view of observer Oâ˛. In the same way that each observer measures the other's clocks as running slow, each observer measures the other's rulers as being contracted.
11797:
Newton himself was acutely aware of the inherent difficulties with these assumptions, but as a practical matter, making these assumptions was the only way that he could make progress. In 1692, he wrote to his friend
Richard Bentley: "That Gravity should be innate, inherent and essential to Matter, so
11532:
By stating that simultaneity is a matter of convention, PoincarĂŠ meant that to talk about time at all, one must have synchronized clocks, and the synchronization of clocks must be established by a specified, operational procedure (convention). This stance represented a fundamental philosophical break
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assumptions about the nature of the asymptotic symmetry groupânot even the assumption that such a group exists. Then after designing what they considered to be the most sensible boundary conditions, they investigated the nature of the resulting asymptotic symmetry transformations that leave invariant
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This introductory section has focused on the spacetime of special relativity, since it is the easiest to describe. Minkowski spacetime is flat, takes no account of gravity, is uniform throughout, and serves as nothing more than a static background for the events that take place in it. The presence of
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contradiction. It is not about the abstract ticking of two identical clocks, but about how to measure in one frame the temporal distance of two ticks of a moving clock. It turns out that in mutually observing the duration between ticks of clocks, each moving in the respective frame, different sets of
1648:
is a measure of separation between events A and B that are time separated and in addition space separated either because there are two separate objects undergoing events, or because a single object in space is moving inertially between its events. The separation interval is the difference between the
4552:
Fig. 3-1 illustrates that in Newton's theory, time is universal, not the velocity of light. Consider the following thought experiment: The red arrow illustrates a train that is moving at 0.4 c with respect to the platform. Within the train, a passenger shoots a bullet with a speed of 0.4 c
4135:
Many introductions to special relativity illustrate the differences between
Galilean relativity and special relativity by posing a series of "paradoxes". These paradoxes are, in fact, ill-posed problems, resulting from our unfamiliarity with velocities comparable to the speed of light. The remedy is
11755:
Even with no (de)acceleration i.e. using one inertial frame O for constant, high-velocity outward journey and another inertial frame I for constant, high-velocity inward journey â the sum of the elapsed time in those frames (O and I) is shorter than the elapsed time in the stationary inertial frame
10634:
What they found was that the asymptotic symmetry transformations actually do form a group and the structure of this group does not depend on the particular gravitational field that happens to be present. This means that, as expected, one can separate the kinematics of spacetime from the dynamics of
10422:
The first crucial concept is coordinate independence: The laws of physics cannot depend on what coordinate system one uses. This is a major extension of the principle of relativity from the version used in special relativity, which states that the laws of physics must be the same for every observer
7712:
Suppose that a source and a receiver, both approaching each other in uniform inertial motion along non-intersecting lines, are at their closest approach to each other. It would appear that the classical analysis predicts that the receiver detects no
Doppler shift. Due to subtleties in the analysis,
7279:
The classical
Doppler analysis deals with waves that are propagating in a medium, such as sound waves or water ripples, and which are transmitted between sources and receivers that are moving towards or away from each other. The analysis of such waves depends on whether the source, the receiver, or
3771:
The necessary recordings for the two judgements, with "one moving clock" and "two clocks at rest" in respectively S or Sâ˛, involves two different sets, each with three clocks. Since there are different sets of clocks involved in the measurements, there is no inherent necessity that the measurements
865:
I went to
Cologne, met Minkowski and heard his celebrated lecture 'Space and Time' delivered on 2 September 1908. He told me later that it came to him as a great shock when Einstein published his paper in which the equivalence of the different local times of observers moving relative to each other
557:
In Fig. 1-1, imagine that the frame under consideration is equipped with a dense lattice of clocks, synchronized within this reference frame, that extends indefinitely throughout the three dimensions of space. Any specific location within the lattice is not important. The latticework of clocks
553:
In special relativity, an observer will, in most cases, mean a frame of reference from which a set of objects or events is being measured. This usage differs significantly from the ordinary
English meaning of the term. Reference frames are inherently nonlocal constructs, and according to this usage
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electron volts. A charged pion is a particle of mass 139.57 MeV (approx. 273 times the electron mass). It is unstable, and decays into a muon of mass 105.66 MeV (approx. 207 times the electron mass) and an antineutrino, which has an almost negligible mass. The difference between the pion
7835:
In scenario (b) the illustration shows the receiver being illuminated by light from when the source was closest to the receiver, even though the source has moved on. Because the source's clocks are time dilated as measured in frame S, and since dr/dt was equal to zero at this point, the light from
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since
Einstein's original work in 1905, each with its particular focus. Although Einstein's derivation was based on the invariance of the speed of light, there are other physical principles that may serve as starting points. Ultimately, these alternative starting points can be considered different
5911:
The Galilean transformations and their consequent commonsense law of addition of velocities work well in our ordinary low-speed world of planes, cars and balls. Beginning in the mid-1800s, however, sensitive scientific instrumentation began finding anomalies that did not fit well with the ordinary
4251:
A basic goal is to be able to compare measurements made by observers in relative motion. If there is an observer O in frame S who has measured the time and space coordinates of an event, assigning this event three Cartesian coordinates and the time as measured on his lattice of synchronized clocks
4216:
of general relativity does provide some additional insight into the subject. Stella is not stationary in an inertial frame. Analyzed in Stella's rest frame, she is motionless for the entire trip. When she is coasting her rest frame is inertial, and Terence's clock will appear to run slow. But when
4155:
The impression that a paradox exists stems from a misunderstanding of what special relativity states. Special relativity does not declare all frames of reference to be equivalent, only inertial frames. The traveling twin's frame is not inertial during periods when she is accelerating. Furthermore,
10576:
The flat spacetime paradigm posits that matter creates a gravitational field that causes rulers to shrink when they are turned from circumferential orientation to radial, and that causes the ticking rates of clocks to dilate. The flat spacetime paradigm is fully equivalent to the curved spacetime
9767:
of the resultant vector. The four-momentum is, as expected, a conserved quantity. However, the invariant mass of the fused particle, given by the point where the invariant hyperbola of the total momentum intersects the energy axis, is not equal to the sum of the invariant masses of the individual
7453:
Light, unlike sound or water ripples, does not propagate through a medium, and there is no distinction between a source moving away from the receiver or a receiver moving away from the source. Fig. 3-6 illustrates a relativistic spacetime diagram showing a source separating from the receiver
7266:
is the change in frequency or wavelength of a wave for a receiver and source in relative motion. For simplicity, we consider here two basic scenarios: (1) The motions of the source and/or receiver are exactly along the line connecting them (longitudinal Doppler effect), and (2) the motions are at
565:
In this idealized case, every point in space has a clock associated with it, and thus the clocks register each event instantly, with no time delay between an event and its recording. A real observer, will see a delay between the emission of a signal and its detection due to the speed of light. To
486:
Unlike the analogies used in popular writings to explain events, such as firecrackers or sparks, mathematical events have zero duration and represent a single point in spacetime. Although it is possible to be in motion relative to the popping of a firecracker or a spark, it is not possible for an
10398:
In spacetime terms, the path of a satellite orbiting the Earth is not dictated by the distant influences of the Earth, Moon and Sun. Instead, the satellite moves through space only in response to local conditions. Since spacetime is everywhere locally flat when considered on a sufficiently small
10386:
that extends throughout all space and all time. Gravity is mediated by a mysterious force, acting instantaneously across a distance, whose actions are independent of the intervening space. In contrast, Einstein denied that there is any background Euclidean reference frame that extends throughout
10234:
The relativistic conservation law for energy and momentum replaces the three classical conservation laws for energy, momentum and mass. Mass is no longer conserved independently, because it has been subsumed into the total relativistic energy. This makes the relativistic conservation of energy a
4167:
These distinctions should result in a difference in the twins' ages. The spacetime diagram of Fig. 2-11 presents the simple case of a twin going straight out along the x axis and immediately turning back. From the standpoint of the stay-at-home twin, there is nothing puzzling about the twin
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axis, are timelike curves, which is to say that these hyperbolae represent actual paths that can be traversed by (constantly accelerating) particles in spacetime: Between any two events on one hyperbola a causality relation is possible, because the inverse of the slopeârepresenting the necessary
696:
in 1892, independently proposed that material bodies traveling through the fixed aether were physically affected by their passage, contracting in the direction of motion by an amount that was exactly what was necessary to explain the negative results of the MichelsonâMorley experiment. No length
4147:
involving identical twins, one of whom makes a journey into space in a high-speed rocket, returning home to find that the twin who remained on Earth has aged more. This result appears puzzling because each twin observes the other twin as moving, and so at first glance, it would appear that each
3526:
The (1+2)-dimensional boundary between space- and time-like hyperboloids, established by the events forming a zero spacetime interval to the origin, is made up by degenerating the hyperboloids to the light cone. In (1+1)-dimensions the hyperbolae degenerate to the two grey 45°-lines depicted in
10410:
bodies or two separated particles. In Fig. 5-1, two separated particles, free-falling in the gravitational field of the Earth, exhibit tidal accelerations due to local inhomogeneities in the gravitational field such that each particle follows a different path through spacetime. The tidal
6571:
Calling one set of transformations the normal Lorentz transformations and the other the inverse transformations is misleading, since there is no intrinsic difference between the frames. Different authors call one or the other set of transformations the "inverse" set. The forwards and inverse
3740:. The difference of the two readings of WⲠis the temporal distance of the two events in Sâ˛. In SⲠthese events are only separated in time, they happen at the same place in Sâ˛. Because of the invariance of the spacetime interval spanned by these two events, and the nonzero spatial separation
630:
Figure 1-2. Michelson and Morley expected that motion through the aether would cause a differential phase shift between light traversing the two arms of their apparatus. The most logical explanation of their negative result, aether dragging, was in conflict with the observation of stellar
3866:) as the event, where the respective "moving clock" is collocated with the "first clock at rest" in both comparisons. Obviously, for this event the readings on both clocks in both comparisons are zero. As a consequence, the worldlines of the moving clocks are the slanted to the right
8195:. This statement is not a tautology, since many modern formulations of relativity do not start with constant speed of light as a postulate. Photons therefore propagate along a lightlike world line and, in appropriate units, have equal space and time components for every observer.
347:
Until the turn of the 20th century, the assumption had been that the three-dimensional geometry of the universe (its description in terms of locations, shapes, distances, and directions) was distinct from time (the measurement of when events occur within the universe). However,
10537:
views, the essential criteria according to which one should select a Euclidean versus non-Euclidean geometry would be economy and simplicity. A realist would say that Einstein discovered spacetime to be non-Euclidean. A conventionalist would say that Einstein merely found it
2642:
so that it has the same units (meters) as the horizontal space coordinate. Since photons travel at the speed of light, their world lines have a slope of Âą1. In other words, every meter that a photon travels to the left or right requires approximately 3.3 nanoseconds of time.
9558:
3553:). Different world lines represent clocks moving at different speeds. A clock that is stationary with respect to the observer has a world line that is vertical, and the elapsed time measured by the observer is the same as the proper time. For a clock traveling at 0.3
866:
was pronounced; for he had reached the same conclusions independently but did not publish them because he wished first to work out the mathematical structure in all its splendor. He never made a priority claim and always gave Einstein his full share in the great discovery.
10312:
Fig. 3-12a illustrates the energyâmomentum diagram for this decay reaction in the rest frame of the pion. Because of its negligible mass, a neutrino travels at very nearly the speed of light. The relativistic expression for its energy, like that of the photon, is
8782:, although amply validated every day in particle accelerators around the globe (or indeed in any instrumentation whose use depends on high velocity particles, such as electron microscopes, old-fashioned color television sets, etc.), has nevertheless not proven to be a
8789:
For this reason, as well as for pedagogical concerns, most physicists currently prefer a different terminology when referring to the relationship between mass and energy. "Relativistic mass" is a deprecated term. The term "mass" by itself refers to the rest mass or
2948:
While the rest frame has space and time axes that meet at right angles, the moving frame is drawn with axes that meet at an acute angle. The frames are actually equivalent. The asymmetry is due to unavoidable distortions in how spacetime coordinates can map onto a
6856:, otherwise whether a fast moving 1 m ball could fit through a 1 m circular hole would depend on the observer. The first postulate of relativity states that all inertial frames are equivalent, and transverse expansion/contraction would violate this law.
10198:
so that a calculation demonstrating conservation of momentum in one frame will be invalid in other frames. Einstein was faced with either having to give up conservation of momentum, or to change the definition of momentum. This second option was what he chose.
791:
was the first to combine space and time into spacetime. He argued in 1898 that the simultaneity of two events is a matter of convention. In 1900, he recognized that Lorentz's "local time" is actually what is indicated by moving clocks by applying an explicitly
4204:, are simultaneous with events on her world line. (Terence, in turn, would observe a set of horizontal lines of simultaneity.) Throughout both the outbound and the inbound legs of Stella's journey, she measures Terence's clocks as running slower than her own.
5299:
It is straightforward to obtain quantitative expressions for time dilation and length contraction. Fig. 3-3 is a composite image containing individual frames taken from two previous animations, simplified and relabeled for the purposes of this section.
10514:
To go from the elementary description above of curved spacetime to a complete description of gravitation requires tensor calculus and differential geometry, topics both requiring considerable study. Without these mathematical tools, it is possible to write
845:
in 1907, which declares the equivalence of inertial and gravitational mass. By using the massâenergy equivalence, Einstein showed that the gravitational mass of a body is proportional to its energy content, which was one of the early results in developing
11550:, even though a variant of it was already a widely used procedure by telegraphers in the middle 19th century. Basically, to synchronize two clocks, one flashes a light signal from one to the other, and adjusts for the time that the flash takes to arrive.
8160:, since the red axes are rescaled by gamma. Fig. 3-8b illustrates the situation as it appears in the moving frame. It is apparent that the space and time components of the four-momentum go to infinity as the velocity of the moving frame approaches
6763:
The derivation given here and illustrated in Fig. 3-5 is based on one presented by Bais and makes use of previous results from the Relativistic Composition of Velocities, Time Dilation, and Length Contraction sections. Event P has coordinates
2892:
axis. To determine the angle of this tilt, we recall that the slope of the world line of a light pulse is always Âą1. Fig. 2-3c presents a spacetime diagram from the viewpoint of observer Oâ˛. Event P represents the emission of a light pulse at
11152:
Geodesics are said to be timelike, null, or spacelike if the tangent vector to one point of the geodesic is of this nature. Paths of particles and light beams in spacetime are represented by timelike and null (lightlike) geodesics, respectively.
11073:(representing another observer), the intersection of the charts represents the region of spacetime in which both observers can measure physical quantities and hence compare results. The relation between the two sets of measurements is given by a
11423:
In 2019, James Scargill argued that complex life may be possible with two spatial dimensions. According to Scargill, a purely scalar theory of gravity may enable a local gravitational force, and 2D networks may be sufficient for complex neural
12940:(Only pages 1â21 were published in 1915, the entire article including pp. 39â43 concerning the groups of Laguerre and Lorentz was posthumously published in 1955 in Cartan's collected papers, and was reprinted in the EncyclopĂŠdie in 1991.)
11575:
might be evaded. Finally, in a profound contribution to the literature on quantum mechanics, Einstein considered two particles briefly interacting and then flying apart so that their states are correlated, anticipating the phenomenon known as
1172:, which combines distances in space and in time. All observers who measure the time and distance between any two events will end up computing the same spacetime interval. Suppose an observer measures two events as being separated in time by
490:
The path of a particle through spacetime can be considered to be a sequence of events. The series of events can be linked together to form a curve that represents the particle's progress through spacetime. That path is called the particle's
11597:) was edited by Sommerfeld to remove this term. Sommerfeld also edited the published form of this lecture to revise Minkowski's judgement of Einstein from being a mere clarifier of the principle of relativity, to being its chief expositor.
1156:. The fundamental reason for merging space and time into spacetime is that space and time are separately not invariant, which is to say that, under the proper conditions, different observers will disagree on the length of time between two
4136:
to solve many problems in special relativity and to become familiar with its so-called counter-intuitive predictions. The geometrical approach to studying spacetime is considered one of the best methods for developing a modern intuition.
2622:(i.e. paths in spacetime) of two photons, A and B, originating from the same event and going in opposite directions. In addition, C illustrates the world line of a slower-than-light-speed object. The vertical time coordinate is scaled by
11077:
coordinate transformation on this intersection. The idea of coordinate charts as local observers who can perform measurements in their vicinity also makes good physical sense, as this is how one actually collects physical dataâlocally.
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she fires her rockets for the turnaround, her rest frame is an accelerated frame and she experiences a force which is pushing her as if she were in a gravitational field. Terence will appear to be high up in that field and because of
3678:
Mutual time dilation and length contraction tend to strike beginners as inherently self-contradictory concepts. If an observer in frame S measures a clock, at rest in frame S', as running slower than his', while S' is moving at speed
10446:. Person B is in a box resting on Earth. Provided that the spaceship is sufficiently small so that tidal effects are non-measurable (given the sensitivity of current gravity measurement instrumentation, A and B presumably should be
3129:
Fig. 2-6 illustrates the use of spacetime diagrams in the analysis of the relativity of simultaneity. The events in spacetime are invariant, but the coordinate frames transform as discussed above for Fig. 2-3. The three events
681:
of 1887 (Fig. 1-2) showed no differential influence of Earth's motions through the hypothetical aether on the speed of light, and the most likely explanation, complete aether dragging, was in conflict with the observation of
4185:
A pure SR analysis would be as follows: Analyzed in Stella's rest frame, she is motionless for the entire trip. When she fires her rockets for the turnaround, she experiences a pseudo force which resembles a gravitational force.
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Fig. 2-10 illustrates the previous discussion of mutual time dilation with Minkowski diagrams. The upper picture reflects the measurements as seen from frame S "at rest" with unprimed, rectangular axes, and frame SⲠ"moving with
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axis. The edges of the blue band represent the world lines of the rod's two endpoints. The invariant hyperbola illustrates events separated from the origin by a spacelike interval of 1 m. The endpoints O and B measured when
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Likewise, a timelike spacetime interval gives the same measure of time as would be presented by the cumulative ticking of a clock that moves along a given world line. A timelike spacetime interval hence provides a measure of the
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In four-dimensional spacetime, the analog to distance is the interval. Although time comes in as a fourth dimension, it is treated differently than the spatial dimensions. Minkowski space hence differs in important respects from
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Algebraic analyses of the energetics of this decay reaction are available online, so Fig. 3-12b presents instead a graphing calculator solution. The energy of the neutrino is 29.79 MeV, and the energy of the muon is
1123:
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3619: = 0 are simultaneous events in the SⲠframe. But to an observer in frame S, events O and B are not simultaneous. To measure length, the observer in frame S measures the endpoints of the rod as projected onto the
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In Fig. 2â4, event O is at the origin of a spacetime diagram, and the two diagonal lines represent all events that have zero spacetime interval with respect to the origin event. These two lines form what is called the
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In response to the first question, a number of authors including Deser, Grishchuk, Rosen, Weinberg, etc. have provided various formulations of gravitation as a field in a flat manifold. Those theories are variously called
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For both cases (1) and (2), momentum, mass, and total energy are conserved. However, kinetic energy is not conserved in cases of inelastic collision. A certain fraction of the initial kinetic energy is converted to heat.
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led an advanced seminar attended by notable physicists of the time to study the papers of Lorentz, PoincarĂŠ et al. Minkowski saw Einstein's work as an extension of Lorentz's, and was most directly influenced by PoincarĂŠ.
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10626:. Their first step was to decide on some physically sensible boundary conditions to place on the gravitational field at lightlike infinity to characterize what it means to say a metric is asymptotically flat, making no
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The composition of velocities is quite different in relativistic spacetime. To reduce the complexity of the equations slightly, we introduce a common shorthand for the ratio of the speed of an object relative to light,
8008:
In relativistic mechanics, the momentum vector is extended to four dimensions. Added to the momentum vector is a time component that allows the spacetime momentum vector to transform like the spacetime position vector
7969:
Figure 3â8. Relativistic spacetime momentum vector. The coordinate axes of the rest frame are: momentum, p, and mass * c. For comparison, we have overlaid a spacetime coordinate system with axes: position, and time *
404:
as a universal quantity of measurement that is uniform throughout, is separate from space, and is agreed on by all observers. Classical mechanics assumes that time has a constant rate of passage, independent of the
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simpler concept than in nonrelativistic mechanics, because the total energy is conserved without any qualifications. Kinetic energy converted into heat or internal potential energy shows up as an increase in mass.
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The same events P, Q, R are plotted in Fig. 2-3b in the frame of observer O. The light paths have slopes = 1 and â1, so that âłPQR forms a right triangle with PQ and QR both at 45 degrees to the
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The freedom to choose any frame in which to perform an analysis allows us to pick one which may be particularly convenient. For analysis of momentum and energy problems, the most convenient frame is usually the
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A spacelike spacetime interval gives the same distance that an observer would measure if the events being measured were simultaneous to the observer. A spacelike spacetime interval hence provides a measure of
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from Newton, who conceived of an absolute, true time that was independent of the workings of the inaccurate clocks of his day. This stance also represented a direct attack against the influential philosopher
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Different reporters viewing the scenarios presented in this figure interpret the scenarios differently depending on their knowledge of the situation. (i) A first reporter, at the center of mass of particles
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8045:. In exploring the properties of the spacetime momentum, we start, in Fig. 3-8a, by examining what a particle looks like at rest. In the rest frame, the spatial component of the momentum is zero, i.e.
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position of the two points using different coordinate systems, the distance between the points will be the same for both, assuming that they are measuring using the same units. The distance is "invariant".
708:(the study of forces and torques and their effect on motion), his theory assumed actual physical deformations of the physical constituents of matter. Lorentz's equations predicted a quantity that he called
7694:
3339:
Minkowski spacetime (having one temporal and one spatial dimension), the points at some constant spacetime interval away from the origin (using the Minkowski metric) form curves given by the two equations
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From a different reference frame, the orderings of these non-causally-related events can be reversed. In particular, one notes that if two events are simultaneous in a particular reference frame, they are
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itself. The reason is that unlike distances in Euclidean geometry, intervals in Minkowski spacetime can be negative. Rather than deal with square roots of negative numbers, physicists customarily regard
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Figure 2â3. (a) Galilean diagram of two frames of reference in standard configuration, (b) spacetime diagram of two frames of reference, (c) spacetime diagram showing the path of a reflected light pulse
549:: the position in space, and the time, which can be visualized as the reading of a clock located at each position in space. The 'observer' synchronizes the clocks according to their own reference frame.
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In Euclidean space (having spatial dimensions only), the set of points equidistant (using the Euclidean metric) from some point form a circle (in two dimensions) or a sphere (in three dimensions). In
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in a moving frame. This result can be derived by inspection of Fig. 3-9 or by application of the Lorentz transformations, and is consistent with the analysis of Doppler effect given previously.
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include Minkowski's statement that "Henceforth, space for itself, and time for itself shall completely reduce to a mere shadow, and only some sort of union of the two shall preserve independence."
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which is also the value of the space component of its momentum. To conserve momentum, the muon has the same value of the space component of the neutrino's momentum, but in the opposite direction.
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in the frame of the train. The blue arrow illustrates that a person standing on the train tracks measures the bullet as traveling at 0.8 c. This is in accordance with our naive expectations.
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On 5 November 1907 (a little more than a year before his death), Minkowski introduced his geometric interpretation of spacetime in a lecture to the GĂśttingen Mathematical society with the title,
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666:, demonstrated that the speed of light in flowing water was less than the sum of the speed of light in air plus the speed of the water by an amount dependent on the water's index of refraction.
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This apparent contradiction stems from not correctly taking into account the different settings of the necessary, related measurements. These settings allow for a consistent explanation of the
573:
In many books on special relativity, especially older ones, the word "observer" is used in the more ordinary sense of the word. It is usually clear from context which meaning has been adopted.
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should find the other to have aged less. The twin paradox sidesteps the justification for mutual time dilation presented above by avoiding the requirement for a third clock. Nevertheless, the
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To understand how the Newtonian view of conservation of momentum needs to be modified in a relativistic context, we examine the problem of two colliding bodies limited to a single dimension.
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both are moving relative to the medium. Given the scenario where the receiver is stationary with respect to the medium, and the source is moving directly away from the receiver at a speed of
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to relate Ursula's measurements with her own. Because of the linearity of the transformations and the relativistic composition of velocities, Terence can use the Lorentz transformations with
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that expectation is not necessarily true. Nevertheless, when appropriately defined, transverse Doppler shift is a relativistic effect that has no classical analog. The subtleties are these:
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In Fig. 2-7a, each magenta hyperbola connects all events having some fixed spacelike separation from the origin, while the green hyperbolae connect events of equal timelike separation.
3011:
A light (double) cone divides spacetime into separate regions with respect to its apex. The interior of the future light cone consists of all events that are separated from the apex by more
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concept in physics in the sense that it is not a concept that has served as a basis for other theoretical development. Relativistic mass, for instance, plays no role in general relativity.
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Fig. 3-7a. What is the frequency measurement when the receiver is geometrically at its closest approach to the source? This scenario is most easily analyzed from the frame SⲠof the source.
850:. While it would appear that he did not at first think geometrically about spacetime, in the further development of general relativity, Einstein fully incorporated the spacetime formalism.
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3811: > 0", coordinatized by primed, oblique axes, slanted to the right; the lower picture shows frame SⲠ"at rest" with primed, rectangular coordinates, and frame S "moving with â
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said that it "gets the punch-line back to front: it is the three-dimensionality of space that explains why we see inverse-square force laws in Nature, not vice-versa" (Barrow 2002:204).
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In a Newtonian analysis of interacting particles, transformation between frames is simple because all that is necessary is to apply the Galilean transformation to all velocities. Since
3062:) from O. Because of the invariance of the spacetime interval, all observers will assign the same light cone to any given event, and thus will agree on this division of spacetime.
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Figure 2â9. In this spacetime diagram, the 1 m length of the moving rod, as measured in the primed frame, is the foreshortened distance OC when projected onto the unprimed frame.
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being moved from the past of the observer to the future of the observer, highlighting events residing on it. The gray area is the light cone of the observer, which remains invariant.
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3519:
Minkowski spacetime (one temporal and two spatial dimensions) with the corresponding hyperboloids. The invariant hyperbolae displaced by spacelike intervals from the origin generate
2739:(i.e. conventional 3-space frames) are displayed in relative motion. Frame S belongs to a first observer O, and frame SⲠ(pronounced "S prime") belongs to a second observer Oâ˛.
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separated by a spacelike interval and thus are noncausally related. The observation that simultaneity is not absolute, but depends on the observer's reference frame, is termed the
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of clock synchronization assuming constant light speed. In 1900 and 1904, he suggested the inherent undetectability of the aether by emphasizing the validity of what he called the
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The expression involving the square root symbol appears very frequently in relativity, and one over the expression is called the Lorentz factor, denoted by the Greek letter gamma
2541:. Since spatial distance traversed by any massive object is always less than distance traveled by the light for the same time interval, positive intervals are always timelike. If
11329:
can be expressed in terms of an action only for a four-dimensional manifold. Finally, Tangherlini showed in 1963 that when there are more than three spatial dimensions, electron
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We can obtain the transformed components of this vector in the moving frame by using the Lorentz transformations, or we can read it directly from the figure because we know that
2030:
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Although for brevity, one frequently sees interval expressions expressed without deltas, including in most of the following discussion, it should be understood that in general,
13782:. (iii) A third reporter, trained in general relativity, knows that there are, in fact, no forces at all acting between the three objects. Rather, all three objects move along
11421:. However, a self-gravitating gas cannot be stably bound if the mass sphere is larger than ~10 solar masses, due to the small positivity of the cosmological constant observed.
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would be unstable and could decay into particles having greater mass than themselves. (This is not a problem if the particles have a sufficiently low temperature.) Lastly, if
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In scenario (a), the point of closest approach is frame-independent and represents the moment where there is no change in distance versus time (i.e. dr/dt = 0 where
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1257:
463:, and requires four numbers to be specified: the three-dimensional location in space, plus the position in time (Fig. 1). An event is represented by a set of coordinates
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the difference between the twins is observationally detectable: the traveling twin needs to fire her rockets to be able to return home, while the stay-at-home twin does not.
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In special relativity, however, the distance between two points is no longer the same if measured by two different observers, when one of the observers is moving, because of
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greater than zero, the Lorentz factor will be greater than one, although the shape of the curve is such that for low speeds, the Lorentz factor is extremely close to one.
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2063:. The invariance of the spacetime interval between the same events for all inertial frames of reference is one of the fundamental results of special theory of relativity.
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presented a geometric interpretation of special relativity that fused time and the three spatial dimensions of space into a single four-dimensional continuum now known as
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following an experiment, the time when a signal is received will be corrected to reflect its actual time were it to have been recorded by an idealized lattice of clocks.
10599:, which is a ten-dimensional group of three Lorentz boosts, three rotations, and four spacetime translations. It is logical to ask what symmetries if any might apply in
9970:. If the total momentum of an interacting system of particles is observed to be conserved in one frame, it will likewise be observed to be conserved in any other frame.
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In physics, conservation laws state that certain particular measurable properties of an isolated physical system do not change as the system evolves over time. In 1915,
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For example, two observers, one of whom is on Earth, but the other one who is on a fast rocket to Jupiter, may observe a comet crashing into Jupiter (this is the event
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In the original version of this lecture, Minkowski continued to use such obsolescent terms as the ether, but the posthumous publication in 1915 of this lecture in the
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these hyperbolae are spacelike intervals: No causality is possible between any two points on one of these hyperbolae, because all secants represent speeds larger than
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1979:
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Because of the close relationship between mass and energy, the four-momentum (also called 4-momentum) is also called the energyâmomentum 4-vector. Using an uppercase
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504:, which is to say, it appears locally "flat" near each point in the same way that, at small enough scales, the surface of a globe appears to be flat. A scale factor,
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is the distance between receiver and source) and hence no longitudinal Doppler shift. The source observes the receiver as being illuminated by light of frequency
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as she passes the finish line, and she calculates the distance between the starting and finish lines, as measured in her frame, to be 259.81 light-seconds (about
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Scenarios (c) and (d) can be analyzed by simple time dilation arguments. In (c), the receiver observes light from the source as being blueshifted by a factor of
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4200:-plane) represent sets of events that are simultaneous in the observer frame. In Fig. 2-11, the blue lines connect events on Terence's world line which,
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Stella is not in an inertial frame. Given this fact, it is sometimes incorrectly stated that full resolution of the twin paradox requires general relativity:
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of spatial or temporal coordinate values belonging to two events, and since there is no preferred origin, single coordinate values have no essential meaning.
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Minkowski had been concerned with the state of electrodynamics after Michelson's disruptive experiments at least since the summer of 1905, when Minkowski and
11822:, then 3-dimensional solid objects have surface areas proportional to the square of their size in any selected spatial dimension. In particular, a sphere of
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square of the spatial distance separating event B from event A and the square of the spatial distance traveled by a light signal in that same time interval
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While discussing various hypotheses on Lorentz invariant gravitation, he introduced the innovative concept of a 4-dimensional spacetime by defining various
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Figure 2â8. The invariant hyperbola comprises the points that can be reached from the origin in a fixed proper time by clocks traveling at different speeds
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of the Earth, the relative sizes of land masses near the poles (Greenland and Antarctica) are highly exaggerated relative to land masses near the Equator.
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Consideration of the interrelationships between the various components of the relativistic momentum vector led Einstein to several important conclusions.
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A spacetime diagram is typically drawn with only a single space and a single time coordinate. Fig. 2-1 presents a spacetime diagram illustrating the
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In other words, the spacetime interval between two events on the world line of something moving at the speed of light is zero. Such an interval is termed
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6268:{\displaystyle {\begin{aligned}t&=\gamma \left(t'+{\frac {vx'}{c^{2}}}\right)\\x&=\gamma \left(x'+vt'\right)\\y&=y'\\z&=z'\end{aligned}}}
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becomes vanishingly small, and the overall result becomes indistinguishable from the Galilean formula (Newton's formula) for the addition of velocities:
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By 1904, Lorentz had expanded his theory such that he had arrived at equations formally identical with those that Einstein was to derive later, i.e. the
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differ from 1. The argument is often of an anthropic character and possibly the first of its kind, albeit before the complete concept came into vogue.
6083:{\displaystyle {\begin{aligned}t'&=\gamma \left(t-{\frac {vx}{c^{2}}}\right)\\x'&=\gamma \left(x-vt\right)\\y'&=y\\z'&=z\end{aligned}}}
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be reciprocally "consistent" such that, if one observer measures the moving clock to be slow, the other observer measures the one's clock to be fast.
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can be written in a same form as above. Because of the constancy of speed of light, the light events in all inertial frames belong to zero interval,
11676:, a mathematician may, by a free play of imagination, hit upon the thought that natural phenomena actually possess an invariance, not for the group
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spontaneously decays into two lighter particles, total energy is conserved, but the mass is not. Part of the mass is converted into kinetic energy.
424:, time cannot be separated from the three dimensions of space, because the observed rate at which time passes for an object depends on the object's
14094:
Bondi, H.; Van der Burg, M. G. J.; Metzner, A. (1962). "Gravitational waves in general relativity: VII. Waves from axisymmetric isolated systems".
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scale, the satellite is always following a straight line in its local inertial frame. We say that the satellite always follows along the path of a
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Fig. 2-8 illustrates the invariant hyperbola for all events that can be reached from the origin in a proper time of 5 meters (approximately
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Conversely, for judging in frame SⲠthe temporal distance of two events on a moving clock W (at rest in S), one needs two clocks at rest in Sâ˛.
800:. In 1905/1906 he mathematically perfected Lorentz's theory of electrons in order to bring it into accordance with the postulate of relativity.
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Kastrup, H. A. (2008). "On the advancements of conformal transformations and their associated symmetries in geometry and theoretical physics".
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on the nature of reality (1927 and 1930), he devised multiple imaginary contraptions intended to show, at least in concept, means whereby the
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The above equations are alternate expressions for the t and x equations of the inverse Lorentz transformation, as can be seen by substituting
914:
included the first public presentation of spacetime diagrams (Fig. 1-4), and included a remarkable demonstration that the concept of the
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to use non-Euclidean geometry. The conventionalist would maintain that Einstein's analysis said nothing about what the geometry of spacetime
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From this reference frame, event C is observed to occur after event O, and event B is observed to occur before event O.
536:, that puzzling discrepancies began to be noted between observation versus predictions based on the implicit assumption of Euclidean space.
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9252:(2) The two bodies stick together and continue moving as a single particle. This second case is the case of completely inelastic collision.
9226:, and so on. In this section, we examine the Newtonian views of conservation of mass, momentum and energy from a relativistic perspective.
6598:
Terence and Stella are at an Earth-to-Mars space race. Terence is an official at the starting line, while Stella is a participant. At time
14447:. Also see Ehrenfest, P. (1917) "In what way does it become manifest in the fundamental laws of physics that space has three dimensions?"
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Looking at the events of this scenario in reverse sequence, we see that non-conservation of mass is a common occurrence: when an unstable
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On the other hand, given the scenario where source is stationary, and the receiver is moving directly away from the source at a speed of
3655:(analogous to ordinary angles in Euclidean geometry). Because of this rotation, the projection of a primed meter-stick onto the unprimed
2615:. A photon arriving in our eye from a distant star will not have aged, despite having (from our perspective) spent years in its passage.
4278:). A second observer OⲠin a different frame SⲠmeasures the same event in her coordinate system and her lattice of synchronized clocks
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With care, this allows simplification of the math with no loss of generality in the conclusions that are reached. In Fig. 2-2, two
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Figure 2â1. Spacetime diagram illustrating two photons, A and B, originating at the same event, and a slower-than-light-speed object, C
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implied by this experiment on the index of refraction (which is dependent on wavelength) led to the unpalatable conclusion that aether
190:
10733:. Development of Riemannian geometry resulted in synthesis of diverse results concerning the geometry of surfaces and the behavior of
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584:, after one has factored out signal propagation delays, versus what one visually sees without such corrections. Failing to understand
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11373:, gravitation of any kind becomes problematic, and the universe would probably be too simple to contain observers. For example, when
10573:", the "field-theoretical approach to general relativity", and so forth. Kip Thorne has provided a popular review of these theories.
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The word "measure" is important. In classical physics an observer cannot affect an observed object, but the object's state of motion
2476:
A minor variation is to place the time coordinate last rather than first. Both conventions are widely used within the field of study.
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A result of linearity is that if two Lorentz transformations are applied sequentially, the result is also a Lorentz transformation.
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in S, then the principle of relativity requires that an observer in frame S' likewise measures a clock in frame S, moving at speed â
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922:), along with the empirical observation that the speed of light is finite, allows derivation of the entirety of special relativity.
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discovered that underlying each conservation law is a fundamental symmetry of nature. The fact that physical processes do not care
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9553:{\displaystyle {\boldsymbol {v_{cm}}}=\left(m_{1}{\boldsymbol {v_{1}}}+m_{2}{\boldsymbol {v_{2}}}\right)/\left(m_{1}+m_{2}\right)}
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of one sheet, while the invariant hyperbolae displaced by timelike intervals from the origin generate hyperboloids of two sheets.
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spacetime diagram from the viewpoint of observer O. Since S and SⲠare in standard configuration, their origins coincide at times
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of the observer, i.e. no matter how the observer may be moving. The situation is quite different for spacelike-separated events.
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The second term is just an expression for the kinetic energy of the particle. Mass indeed appears to be another form of energy.
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Einstein, for his part, was initially dismissive of Minkowski's geometric interpretation of special relativity, regarding it as
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658:. The various attempts to establish the properties of this hypothetical medium yielded contradictory results. For example, the
11101:). In general, they will disagree about the exact location and timing of this impact, i.e., they will have different 4-tuples
4310:. With inertial frames, neither observer is under acceleration, and a simple set of equations allows us to relate coordinates
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Weinberg, S. (1964). "Derivation of Gauge Invariance and the Equivalence Principle from Lorentz Invariance of the S-Matrix".
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A reference frame (observer) can be identified with one of these coordinate charts; any such observer can describe any event
13768:, smiles at the first reporter's naivetĂŠ. This second reporter knows that in reality, the apparent forces between particles
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measures transverse blueshift using a MĂśssbauer source setup at the center of a centrifuge rotor and an absorber at the rim.
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In Newtonian mechanics, two extreme cases of this problem may be distinguished yielding mathematics of minimum complexity:
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7755:, but also observes the receiver as having a time-dilated clock. In frame S, the receiver is therefore illuminated by
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Lorentz transformations are used to transform the coordinates of an event from one frame to another in special relativity.
3906:> 0, and thus the worldline (not shown in the pictures) of this clock intersects the worldline of the moving clock (the
3659:-axis is foreshortened, while the projection of an unprimed meter-stick onto the primed xâ˛-axis is likewise foreshortened.
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the given event. The beforeâafter relationship observed for timelike-separated events remains unchanged no matter what the
12821:
Weinstein, Galina (2012). "Max Born, Albert Einstein and Hermann Minkowski's SpaceâTime Formalism of Special Relativity".
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states that in any sufficiently small region of space, the effects of gravitation are the same as those from acceleration.
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9615:
Fig. 3-10 illustrates the inelastic collision of two particles from a relativistic perspective. The time components
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clocks must be involved. In order to measure in frame S the tick duration of a moving clock WⲠ(at rest in Sâ˛), one uses
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284:
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Usually, many overlapping coordinate charts are needed to cover a manifold. Given two coordinate charts, one containing
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Because of the equivalence of mass and energy, elementary particle masses are customarily stated in energy units, where
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to relate Stella's measurements to his own. Stella, in her frame, observes Ursula traveling away from her at 0.250
4178:
Weiss's nomenclature, designating the stay-at-home twin as Terence and the traveling twin as Stella, is hereafter used.
2979:
Figure 2â4. The light cone centered on an event divides the rest of spacetime into the future, the past, and "elsewhere"
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The ease of analyzing a relativistic scenario often depends on the frame in which one chooses to perform the analysis.
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changed, but the transmission velocity of the waves relative to the receiver is decreased, and the observed frequency
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Two events can be defined by the condition "two clocks are simultaneously at one place", i.e., when WⲠpasses each W
12524:
11572:
9565:
8508:
5057:
4362:. Given that the two coordinate systems are in standard configuration, meaning that they are aligned with parallel
17859:
17592:
8116:
2118:
238:
17305:
15758:
15413:
14928:
13862:
11165:
10452:
An alternative expression of the equivalence principle is to note that in Newton's universal law of gravitation,
10400:
7071:
7019:
3728:. For both events the two readings of the collocated clocks are recorded. The difference of the two readings of W
3054:
region of the event O, denoted "Elsewhere" in Fig. 2-4. Events on the light cone itself are said to be
678:
533:
31:
11347:
differs from 1, the behavior of physical systems could not be predicted reliably from knowledge of the relevant
10947:
are used. Moreover, for simplicity's sake, units of measurement are usually chosen such that the speed of light
10442:
In Fig. 5-2, person A is in a spaceship, far from any massive objects, that undergoes a uniform acceleration of
5478:
17408:
16569:
15637:
14962:
10794:
For physical reasons, a spacetime continuum is mathematically defined as a four-dimensional, smooth, connected
8402:
8289:
Photons travel at the speed of light, yet have finite momentum and energy. For this to be so, the mass term in
8179:
5753:, and the edges of the blue band representing the world lines of the endpoints of a rod in motion have slope 1/
5250:
5212:. The velocity of light is the same for all observers regardless their motions relative to the emitting source.
3346:
3294:
2680:
838:
17:
13624:
Byers, Nina (1998). "E. Noether's Discovery of the Deep Connection Between Symmetries and Conservation Laws".
11280:. Ehrenfest also showed that if there are an even number of spatial dimensions, then the different parts of a
10450:), there are no experiments that A and B can perform which will enable them to tell which setting they are in.
10406:
In any analysis of spacetime, evidence of gravitation requires that one observe the relative accelerations of
8064:
7158:. From the inverse transformation, the equations of the forwards transformation can be derived by solving for
6760:, which states that the influence that one particle exerts on another can not be transmitted instantaneously.
3089:
All observers will agree that for any given event, an event within the given event's future light cone occurs
2988:
of the event O, since adding a second spatial dimension (Fig. 2-5) makes the appearance that of two
17945:
17839:
17581:
17486:
17416:
16750:
13800:
The Principle of Relativity: A Collection of Original Memoirs on the Special and General Theory of Relativity
11710:
11348:
8465:
7736:
Fig. 3-7d. If the source is moving in a circle around the receiver, what frequency does the receiver measure?
7733:
Fig. 3-7c. If the receiver is moving in a circle around the source, what frequency does the receiver measure?
6311:
5303:
To reduce the complexity of the equations slightly, there are a variety of different shorthand notations for
3748:
temporal distance between the two events, resulting from the readings of the moving clock Wâ˛, belongs to the
599:
406:
17549:
13149:
17940:
17935:
17403:
15720:
11475:
11254:
10746:
9735:
9702:
8568:
7390:
1287:
10725:" ("On the Hypotheses on which Geometry is Based"). It is a very broad and abstract generalization of the
7725:
the source as being closest to it? This scenario is most easily analyzed from the frame S of the receiver.
3042:
The region exterior to the light cone consists of events that are separated from the event O by more
878:
17444:
17178:
17163:
16705:
16685:
16631:
16516:
16352:
16011:
15057:
12209:
11351:. In such a universe, intelligent life capable of manipulating technology could not emerge. Moreover, if
7974:
In classical mechanics, the state of motion of a particle is characterized by its mass and its velocity.
7955:
7625:
7257:
5145:
The relativistic formula for addition of velocities presented above exhibits several important features:
4218:
3093:
the given event. Likewise, for any given event, an event within the given event's past light cone occurs
2728:
647:
613:
444:
14918:
12321:
12068:
A Most Incomprehensible Thing: Notes Towards a Very Gentle Introduction to the Mathematics of Relativity
8614:
Another way of looking at the relationship between mass and energy is to consider a series expansion of
2835:
17960:
17850:
17731:
17173:
17126:
16372:
16357:
16295:
16274:
15363:
15343:
14912:
12420:
11960:
11837:
dimensions, the strength of the gravitational attraction between two bodies separated by a distance of
11658:, exactly becomes the full group belonging to Newtonian Mechanics. In this state of affairs, and since
11460:
9207:
5246:
4899:
of the bullet relative to the platform, as represented by the blue arrow? Referring to Fig. 3-2b:
3691:
than the other, is an important question that "goes to the heart of understanding special relativity."
3290:
3185:
3123:
2676:
39:
35:
14922:
10387:
space. Nor is there any such thing as a force of gravitation, only the structure of spacetime itself.
9773:
6583:. So inverting the equations simply entails switching the primed and unprimed variables and replacing
6377:
3227:
1224:
17761:
17387:
17068:
16526:
16337:
16074:
15923:
15803:
15353:
15266:
14955:
14597:
11564:
11238:
11074:
10403:. No evidence of gravitation can be discovered following alongside the motions of a single particle.
9219:
7268:
5313:
4780:
689:
14349:
13673:
12737:
8794:, and is equal to the invariant length of the relativistic momentum vector. Expressed as a formula,
4192:
and 2-11 illustrate the concept of lines (planes) of simultaneity: Lines parallel to the observer's
2719:
1984:
17955:
17786:
17336:
17096:
17007:
15773:
14992:
14817:
12842:
Galison, Peter Louis (1979). "Minkowski's spaceâtime: From visual thinking to the absolute world".
11547:
11242:
10758:
10066:, fail to behave properly under Lorentzian transformation. The linear transformation of velocities
9985:
9874:
9381:
9211:
8202:
of electromagnetism is that light carries energy and momentum, and that their ratio is a constant:
7445:
4560:
with respect to frame S, then within frame Sâ˛, observer OⲠmeasures an object moving with velocity
4540:
2736:
1820:
558:
is used to determine the time and position of events taking place within the whole frame. The term
376:
140:
11246:
7523:
6306:
terms approach zero, and the Lorentz transformations approximate to the Galilean transformations.
5186:. The Galilean formula is a special case of the relativistic formula applicable to low velocities.
3589:
1621:
17515:
17437:
17057:
17048:
16786:
16564:
16466:
16382:
16377:
16029:
15680:
15200:
15195:
15175:
14753:
13938:
11384:
cannot cross without intersecting. Hence anthropic and other arguments rule out all cases except
11268:
showed that if there is only a single time dimension and more than three spatial dimensions, the
10789:
10738:
10730:
5239:
3283:
2669:
797:
325:
314:
277:
11276:
about its Sun cannot remain stable. The same is true of a star's orbit around the center of its
11226:
and undetectable to date, can be explained by appealing to the physical consequences of letting
10375:
8610:. Simplified to the case of zero velocity, this is Einstein's equation relating energy and mass.
4933:
The two yellow triangles are similar because they are right triangles that share a common angle
4800:
4152:
is not a true paradox because it is easily understood within the context of special relativity.
2089:
1675:
1262:
986:
861:
recounted a meeting he had made with Minkowski, seeking to be Minkowski's student/collaborator:
17741:
17604:
17510:
17468:
17142:
17106:
15383:
15185:
15180:
15160:
14344:
13317:
13012:
13004:
11742:, ordinary rotation leaves a circle unchanged. In spacetime, hyperbolic rotation preserves the
11104:
10906:
10318:
9980:
both before and after collision. In the Newtonian analysis, conservation of mass dictates that
9223:
5902:
3791:
3780:
2711:
2575:
2126:
The equation above is similar to the Pythagorean theorem, except with a minus sign between the
1198:
1153:
701:
480:
353:
105:
13183:
11237:
The implicit notion that the dimensionality of the universe is special is first attributed to
10631:
the form of the boundary conditions appropriate for asymptotically flat gravitational fields.
8890:
3331:
Figure 2â7. (a) Families of invariant hyperbolae, (b) Hyperboloids of two sheets and one sheet
3327:
2781:
Fig. 2-3a redraws Fig. 2-2 in a different orientation. Fig. 2-3b illustrates a
2129:
1955:
1912:
1652:
1175:
853:
When Einstein published in 1905, another of his competitors, his former mathematics professor
17746:
17351:
17290:
16939:
16212:
15844:
15789:
15743:
15728:
15373:
15190:
15170:
15165:
14421:[How do the fundamental laws of physics make manifest that space has 3 dimensions?].
14175:
Strominger, Andrew (2017). "Lectures on the Infrared Structure of Gravity and Gauge Theory".
13591:
13283:
13102:
12714:
12585:
12579:
11418:
10766:
10754:
10666:
10437:
10221:
10207:
9931:
9659:
9620:
8503:
Likewise, comparing the time component of the relativistic momentum with that of the photon,
7919:
7500:
7457:
6757:
5680:
5555:
4727:
4401:
4213:
4175:
Complications arise if the twin paradox is analyzed from the traveling twin's point of view.
842:
200:
100:
14654:
14198:
11546:
The operational procedure adopted by PoincarĂŠ was essentially identical to what is known as
10558:
Are there any situations where a flat spacetime interpretation of general relativity may be
10382:
Newton's theories assumed that motion takes place against the backdrop of a rigid Euclidean
10071:
9890:
9367:{\displaystyle {\boldsymbol {p}}_{\boldsymbol {2}}=m_{2}{\boldsymbol {v}}_{\boldsymbol {2}}}
9309:{\displaystyle {\boldsymbol {p}}_{\boldsymbol {1}}=m_{1}{\boldsymbol {v}}_{\boldsymbol {1}}}
5659:{\displaystyle \gamma ={\frac {1}{\sqrt {1-v^{2}/c^{2}}}}={\frac {1}{\sqrt {1-\beta ^{2}}}}}
4690:
4212:
Although general relativity is not required to analyze the twin paradox, application of the
2192:
1565:{\displaystyle (\Delta s)^{2}=(\Delta ct)^{2}-(\Delta x)^{2}-(\Delta y)^{2}-(\Delta z)^{2}.}
17651:
17577:
17421:
17023:
16766:
16680:
16506:
16367:
16095:
16064:
15513:
15408:
15259:
14676:
14619:
14555:
14487:
14430:
14283:
14146:
14103:
14040:
14005:
13950:
13903:
13546:
12969:
12749:
12622:
12498:
12232:
11577:
11537:, who argued that time, simultaneity, and duration were matters of intuitive understanding.
10858:
10800:
8245:
8207:
8014:
6556:
etc. Although for brevity the Lorentz transformation equations are written without deltas,
4506:
3914:, where "two clocks are simultaneously at one place". In the lower picture the place for Wâ˛
3537:
3417:
2544:
2513:
2486:
2243:
2165:
834:
705:
13939:"Exact Theory of the (Einstein) Gravitational Field in an Arbitrary Background SpaceâTime"
12915:
12353:"Fresnel's (Dragging) Coefficient as a Challenge to 19th Century Optics of Moving Bodies."
11287:
10038:
9697:
of the resultant vector, meaning that energy is conserved. Likewise, the space components
9159:
5376:
5344:
4474:
4442:
3826:â˛) represents a line of simultaneity. All events on such a line have the same time value (
2035:
8:
17726:
17721:
17711:
17543:
17492:
17310:
17295:
17121:
17052:
17000:
16976:
16771:
16626:
16491:
16443:
15969:
15428:
15388:
15067:
15062:
14832:
14419:"Welche Rolle spielt die Dreidimensionalität des Raumes in den Grundgesetzen der Physik?"
13778:
really represent tidal effects resulting from their differential attraction by mass
12284:
Catchers of the Light: Catching Space: Origins, Lunar, Solar, Solar System and Deep Space
12130:
11450:
11322:
11247:
the one which is at the same time the simplest in hypothesis and the richest in phenomena
10795:
10785:
10670:
10662:
10655:
9822:
8199:
7965:
6834:
There can be no such thing as length expansion/contraction in the transverse directions.
4785:
2954:
1884:
1145:
1009:
960:
930:
926:
713:
655:
433:
397:
17716:
16312:
14882:
14680:
14623:
14559:
14491:
14434:
14362:
14287:
14150:
14107:
14044:
14009:
13954:
13907:
13550:
12973:
12753:
12626:
12502:
12373:
12236:
12202:"Student understanding of time in special relativity: Simultaneity and reference frames"
12201:
9234:
7704:
5455:, and the red line representing the world line of a particle in motion has the equation
4856:. From the primed frame of the train, a passenger shoots a bullet with a speed given by
1578:
1327:
562:
refers to the whole ensemble of clocks associated with one inertial frame of reference.
17930:
17912:
17876:
17791:
17691:
17615:
17473:
17454:
17448:
17399:
17341:
17250:
17168:
17086:
17063:
17031:
16951:
16725:
16649:
16579:
15918:
15896:
15763:
15587:
15558:
15493:
15486:
15241:
15082:
15037:
14941:
14692:
14666:
14635:
14609:
14571:
14545:
14503:
14307:
14273:
14176:
14119:
13966:
13919:
13893:
13831:
13625:
13567:
13558:
13534:
13375:
13030:
12985:
12959:
12859:
12822:
12791:
12648:
12248:
12222:
11808:
11560:
11465:
11197:
11084:
11056:
11036:
11013:
10993:
10973:
10950:
10835:
10762:
10623:
10600:
10592:
10492:
7480:
6743:
5286:
4144:
3597:
3495:
3467:
3441:
some positive real constant. These equations describe two families of hyperbolae in an
3098:
3081:
2731:
compare with each other, it is useful to work with a simplified setup with frames in a
2625:
2222:
2069:
1601:
1165:
1157:
980:
934:
847:
683:
546:
507:
429:
421:
372:
357:
333:
310:
270:
256:
220:
77:
72:
10519:
general relativity, but it is not possible to demonstrate any non-trivial derivations.
8878:
This formula applies to all particles, massless as well as massive. For photons where
7729:
Two other scenarios are commonly examined in discussions of transverse Doppler shift:
1672:. If the event separation is due to a light signal, then this difference vanishes and
925:
The spacetime concept and the Lorentz group are closely connected to certain types of
17871:
17801:
17633:
17625:
17226:
17183:
16799:
16664:
16481:
15999:
15878:
15778:
15631:
15534:
15438:
15077:
14878:
14864:
14838:
14803:
14786:
14767:
14757:
14696:
14688:
14639:
14567:
14507:
14358:
14311:
14299:
14295:
14229:
14123:
14074:
14052:
13970:
13837:
13805:
13798:
13715:
13597:
13572:
13513:
13507:
13483:
13458:
13409:
13382:
13323:
13289:
13218:
13128:
13091:
13064:
13016:
12798:
12683:
12678:
Zahar, Elie (1989) , "PoincarĂŠ's Independent Discovery of the relativity principle",
12652:
12589:
12553:
12514:
12462:
12456:
12363:
12288:
12170:
12138:
12071:
12037:
12003:
11964:
11906:
11784:
Not all experiments characterize the effect in terms of a redshift. For example, the
11743:
11726:
11700:
is definitely finite, and only exceedingly large using the ordinary measuring units."
11440:
11193:
10900:
10288:
9768:
particles that collided. Indeed, it is larger than the sum of the individual masses:
8456:
8294:
854:
774:
659:
529:
436:
can slow the passage of time for an object as seen by an observer outside the field.
364:
329:
195:
17671:
14575:
14530:
13923:
13756:, concludes that a force of repulsion exists between the particles in scenario
12989:
12707:"Breaking in the 4-vectors: the four-dimensional movement in gravitation, 1905â1910"
12643:
12031:
10903:
are used to represent observers in reference frames. Usually, Cartesian coordinates
10596:
8286:
must therefore be equated with the time component of the spacetime momentum vector.
5716:
represent equal spacetime intervals. Length contraction is represented by the ratio
4962:
The ratios of corresponding sides of the two yellow triangles are constant, so that
1704:
When the event considered is infinitesimally close to each other, then we may write
788:
744:
17888:
17706:
17696:
17643:
17620:
17198:
16944:
16690:
16669:
16621:
16584:
16397:
16117:
16105:
15933:
15901:
15733:
15602:
15518:
15508:
15423:
15007:
14684:
14627:
14563:
14495:
14438:
14354:
14291:
14154:
14111:
14048:
14013:
13958:
13911:
13562:
13554:
13113:
Landau, L. D., and Lifshitz, E. M. (2013). The classical theory of fields (Vol. 2).
12977:
12851:
12757:
12638:
12630:
12506:
12252:
12240:
11956:
Gravity from the Ground Up: An Introductory Guide to Gravity and General Relativity
11722:
11326:
10853:
10716:
10570:
9193:
7979:
3652:
2466:
1118:{\displaystyle (\Delta {d})^{2}=(\Delta {x})^{2}+(\Delta {y})^{2}+(\Delta {z})^{2}}
973:
663:
410:
322:
210:
17766:
11413:-dimensional spacetime is the marginal dimensionality. Moreover, it is the unique
10622:
problem in order to investigate the flow of energy at infinity due to propagating
4172:) to calculate the total amount of proper time experienced by the traveling twin.
554:
of the term, it does not make sense to speak of an observer as having a location.
17781:
17756:
17681:
17676:
17559:
17520:
17482:
17426:
17300:
17236:
16675:
16654:
16486:
16458:
16223:
16179:
16044:
16021:
15989:
15941:
15928:
15891:
15873:
15503:
15498:
15052:
14997:
14858:
14854:
14799:
14795:
14778:
14743:
14631:
13709:
13403:
13085:
12282:
12164:
11954:
11871:
11739:
10742:
10690:
10615:
10534:
10383:
7975:
7180:
The Lorentz transformations have a mathematical property called linearity, since
3603:
Fig. 2-9 illustrates the motions of a 1 m rod that is traveling at 0.5
2950:
2715:
Figure 2-2. Galilean diagram of two frames of reference in standard configuration
823:
760:
730:
693:
670:
541:
414:
368:
110:
17564:
14226:
Quantum Field Theory on Curved Spacetimes: Concepts and Mathematical Foundations
11718:
5295:
Figure 3-3. Spacetime diagrams illustrating time dilation and length contraction
2755:
axes of frame S are oriented parallel to the respective primed axes of frame Sâ˛.
2727:
To gain insight in how spacetime coordinates measured by observers in different
937:
and their transformation groups already developed in the 19th century, in which
440:
17864:
17806:
17478:
17462:
17458:
17361:
17331:
17188:
17091:
16971:
16730:
16720:
16659:
16616:
16448:
16438:
16407:
16307:
16279:
16122:
16112:
15911:
15783:
15753:
15738:
15523:
15481:
15476:
15348:
15134:
15119:
14739:
14414:
12738:"On the Electrodynamics of Moving Bodies ( Zur Elektrodynamik bewegter KĂśrper)"
11485:
11414:
11334:
11330:
11265:
11258:
10990:. Another reference frame may be identified by a second coordinate chart about
10830:
10390:
9427:
8791:
7263:
7253:
5418:
represent equal spacetime intervals. Time dilation is represented by the ratio
4246:
4159:
3736:
is the temporal distance of the two events in S, and their spatial distance is
567:
243:
3634:(not illustrated) Drawing a vertical line through A so that it intersects the
545:
Figure 1-1. Each location in spacetime is marked by four numbers defined by a
17950:
17924:
17796:
17776:
17771:
17686:
17554:
17382:
17326:
17158:
17111:
16858:
16809:
16794:
16740:
16511:
16347:
16342:
16258:
16202:
16152:
16100:
16034:
16006:
15994:
15984:
15974:
15856:
15700:
15626:
15575:
15528:
15443:
15403:
15398:
15393:
15326:
15124:
14828:
14442:
14325:
14303:
14158:
12762:
12197:
12092:
11534:
11406:
11250:
11223:
10686:
10682:
10611:
9249:(1) The two bodies rebound from each other in a completely elastic collision.
8168:
8005:
is not affected by external forces, its total linear momentum cannot change.
8002:
7947:
6710:{\displaystyle t^{\prime }=\gamma \left(t-vx/c^{2}\right)=519.62\ {\text{s}}}
5906:
5282:
4834:
Fig. 3-2a illustrates a red train that is moving forward at a speed given by
4169:
4013:
To show the mutual time dilation immediately in the upper picture, the event
3581:
1161:
871:
812:
808:
768:
654:
medium; in the case of light waves, this was considered to be a hypothetical
624:
14884:
The Doom of Spacetime: Why It Must Dissolve Into More Fundamental Structures
12797:. Simon & Schuster. pp. 26â27, 122â127, 145â146, 345â349, 448â460.
12510:
9862:
9838:
3988:, connecting all events with the same spacetime interval from the origin as
906:), to the German Society of Scientists and Physicians. The opening words of
17900:
17816:
17736:
17701:
17231:
17193:
16956:
16843:
16838:
16833:
16820:
16559:
16174:
16168:
15834:
15768:
15690:
15621:
15570:
15471:
15418:
15358:
15144:
15109:
15002:
14931:
14807:
14115:
14017:
13576:
13184:"Being and Becoming in Modern Physics. 3. The Special Theory of Relativity"
12981:
11470:
11318:
11172:
10750:
10702:
10643:
reduce to special relativity in the case of weak fields at long distances.
9199:
5052:
in step 1 to yield Einstein's formula for the addition of velocities:
4140:
3984:-axis. This is done by the invariant hyperbola (see also Fig. 2-8) through
3668:
205:
14137:
Sachs, Rainer K. (1962). "Asymptotic symmetries in gravitational theory".
13760:
while a force of attraction exists between the particles in scenario
11317:
is a positive whole number, then wave impulses become distorted. In 1922,
11010:. Two observers (one in each reference frame) may describe the same event
10555:
Is it possible to represent general relativity in terms of flat spacetime?
9973:
Conservation of momentum in the COM frame amounts to the requirement that
4021:Ⲡ= 0 (the location of clock WⲠin Sâ˛), that is simultaneous to
3928: < 0, and so in this measurement the moving clock W passes Wâ˛
2975:
1618:
units (like seconds) into space units (like meters). The squared interval
754:
17600:
17569:
17116:
16966:
16961:
16606:
16589:
16521:
16501:
16387:
16269:
16184:
16162:
16069:
16054:
15849:
15829:
15819:
15748:
15705:
15685:
15614:
15433:
15335:
15229:
15012:
14526:
11815:
and the proportional relationship of flux density and field strength. If
11340:
10899:
of particles and light beams. About each point (event) on this manifold,
10502:
10447:
7756:
3744:
in S, the temporal distance in SⲠmust be smaller than the one in S: the
3520:
2619:
882:
Figure 1â4. Hand-colored transparency presented by Minkowski in his 1908
804:
185:
30:"space and time" and "time and space" redirect here. For other uses, see
13630:
12881:
12863:
12483:
12227:
11343:
expands on the preceding argument in the following anthropic manner. If
11253:
argued that 3-dimensional space was a consequence of the inverse square
7271:). We are ignoring scenarios where they move along intermediate angles.
6612:, Stella's spaceship accelerates instantaneously to a speed of 0.5
857:, had also arrived at most of the basic elements of special relativity.
738:
646:
were considered to have proven the wave nature of light as opposed to a
17811:
17377:
17221:
17216:
16981:
16934:
16918:
16804:
16710:
16531:
16392:
16362:
16300:
16079:
15979:
15886:
15861:
15664:
15448:
15224:
15104:
14499:
13962:
13915:
13480:
The Classical Theory of Fields, Course of Theoretical Physics, Volume 2
12634:
11568:
11402:
10698:
10511:. The equivalence principle states that these two masses are identical.
7837:
5253: in this section. Unsourced material may be challenged and removed.
5160:
are both very small compared with the speed of light, then the product
3711:
at rest in two arbitrarily fixed points in S with the spatial distance
3297: in this section. Unsourced material may be challenged and removed.
2968:
2683: in this section. Unsourced material may be challenged and removed.
827:
816:
639:
14550:
14388:
14278:
13898:
13858:
13789:
12244:
8695:{\displaystyle E=\gamma mc^{2}={\frac {mc^{2}}{\sqrt {1-\beta ^{2}}}}}
3964:, thus giving the elapsed time between the two events, measured with W
3815: < 0", with unprimed, oblique axes, slanted to the left.
2953:, and should be considered no stranger than the manner in which, on a
724:
650:. Propagation of waves was then assumed to require the existence of a
439:
In ordinary space, a position is specified by three numbers, known as
16878:
16715:
16599:
16574:
16554:
16423:
16417:
16402:
16142:
15695:
15607:
15582:
15563:
15453:
15205:
15114:
14978:
14598:"Gravothermal phase transition, black holes and space dimensionality"
13783:
12855:
12134:
11455:
11333:
around nuclei cannot be stable; electrons would either fall into the
8183:
Figure 3â9. Energy and momentum of light in different inertial frames
8167:
We will use this information shortly to obtain an expression for the
3066:
2267:
as a distinct symbol in itself, rather than the square of something.
638:
By the mid-1800s, various experiments such as the observation of the
61:
14418:
11559:
A hallmark of Einstein's career, in fact, was his use of visualized
8939:
to denote the spatial momentum, the four-momentum may be written as
8397:
approaches 1, so the spatial component of the relativistic momentum
6564:, etc. We are, in general, always concerned with the space and time
5228:
3272:
2909:
from the light source (event Q), and returns to the light source at
2658:
2274:
There are two sign conventions in use in the relativity literature:
17751:
17101:
16913:
16893:
16735:
16641:
16541:
16332:
16327:
15710:
15553:
15463:
15321:
15311:
15129:
15092:
15017:
14671:
14614:
14264:
Tegmark, Max (1 April 1997). "On the dimensionality of spacetime".
14181:
13653:. California State University Affordable Learning Solutions Program
11363:
11149:
into relativity, by which all physical quantities are represented.
10896:
10781:
10734:
10710:
10674:
10427:
10363:. Most of the energy is carried off by the near-zero-mass neutrino.
8775:
The concept of relativistic mass that Einstein introduced in 1905,
7951:
3134:
are simultaneous from the reference frame of an observer moving at
858:
697:
changes occur in directions transverse to the direction of motion.
644:
differential measurements of the speed of light in air versus water
500:
425:
14711:"Life could exist in a 2D universe (according to physics, anyway)"
14521:
14519:
14517:
12964:
12827:
12611:"On the Dynamics of the Electron (Sur la dynamique de l'ĂŠlectron)"
12458:'Subtle is the Lordâ': The Science and the Life of Albert Einstein
12036:(3rd ed.). Mineola, New York: Dover Publications. p. 7.
10693:
from point to point). This gives, in particular, local notions of
10213:
Figure 3-12a. Energyâmomentum diagram for decay of a charged pion.
8278:, and since for photons, the space and time components are equal,
4884:, where the distance is measured along a line parallel to the red
16908:
16898:
16828:
16700:
16611:
16476:
16049:
16039:
15961:
15952:
15937:
15824:
15669:
15592:
15301:
15139:
13680:. Department of Physics and Astronomy, Georgia State University.
13090:(illustrated ed.). Oxford University Press. pp. 26â28.
11480:
11146:
10227:
Figure 3-12b. Graphing calculator analysis of charged pion decay.
5402:
5218:
4903:
From the platform, the composite speed of the bullet is given by
3569:, the elapsed time measured by the observer is 7.00 meters (
3557:, the elapsed time measured by the observer is 5.24 meters (
298:
160:
15839:
14771:
13509:
Introduction to Classical Mechanics: With Problems and Solutions
10639:. This implies the conclusion that General Relativity (GR) does
9049:{\displaystyle P\equiv (E/c,{\vec {p}})=(E/c,p_{x},p_{y},p_{z})}
5884:{\displaystyle OB/OK=\gamma (1-\beta ^{2})={\frac {1}{\gamma }}}
2933:
axes. Since OP = OQ = OR, the angle between
17431:
16903:
16853:
16848:
16147:
15306:
14907:
14514:
14380:
11823:
11359:
11277:
11273:
10706:
8446:, the classical term for momentum. Following this perspective,
7721:
Fig. 3-7b. What is the frequency measurement when the receiver
6572:
transformations are trivially related to each other, since the
2993:
2992:
meeting with their apices at O. One cone extends into the
841:, which was instrumental for his subsequent formulation of the
13796:
Lorentz, H. A.; Einstein, A.; Minkowski, H.; Weyl, H. (1952).
13083:
11721:
of the plane, and is isomorphic to the group of isometries in
8460:
of an object increases with velocity according to the formula
7689:{\displaystyle f={\sqrt {\frac {1-\beta }{1+\beta }}}\,f_{0}.}
6826:(or the other way around) it is easier at first to derive the
6616:. The distance from Earth to Mars is 300 light-seconds (about
3870:â˛-axis (upper pictures, clock Wâ˛) and the slanted to the left
1429:{\displaystyle (\Delta s)^{2}=(\Delta ct)^{2}-(\Delta x)^{2},}
588:
is the source of much confusion among students of relativity.
417:: it assumes that space follows the geometry of common sense.
16992:
16883:
16695:
16594:
16549:
16157:
15906:
15597:
15545:
15096:
14887:(Speech). The 2,384th Meeting Of The Society. Washington, D.C
14812:
The Principle of Relativity: A Collection of Original Memoirs
12713:. Berlin, Germany: Springer. pp. 193â252. Archived from
11381:
11269:
10737:
on them, with techniques that can be applied to the study of
10709:. From those, some other global quantities can be derived by
10694:
7212:
Terence observes Stella speeding away from him at 0.500
6631:. But Stella observes the time on her ship chronometer to be
6624:). Terence observes Stella crossing the finish-line clock at
6576:
frame can only be moving forwards or reverse with respect to
4556:
More generally, assuming that frame SⲠis moving at velocity
3647:
illustrates that the primed and unprimed frames are mutually
3085:
Figure 2â6. Animation illustrating relativity of simultaneity
3003:
677:
flows at different speeds for different colors of light. The
349:
14947:
14318:
13795:
10415:
of a gravitational force acting at a long range from Earth.
9149:{\displaystyle P\equiv (E,{\vec {p}})=(E,p_{x},p_{y},p_{z})}
7449:
Figure 3â6. Spacetime diagram of relativistic Doppler effect
6887:
From previous results using similar triangles, we know that
6492:{\displaystyle \Delta t'=\gamma (\Delta t-v\Delta x/c^{2}),}
3980:, measured with Wâ˛, must be transformed to the scale of the
3662:
3107:
was drawn from the reference frame of an observer moving at
3027:
comprises the interior events of the past light cone. So in
17412:
16888:
16873:
16863:
16317:
16254:
15296:
15282:
14393:
Die philosophischen schriften von Gottfried Wilhelm Leibniz
13884:
Deser, S. (1970). "Self-Interaction and Gauge Invariance".
12920:
EncyclopĂŠdie des Sciences MathĂŠmatiques Pures et AppliquĂŠes
11812:
11281:
10722:
Ueber die Hypothesen, welche der Geometrie zu Grunde liegen
10268:
7477:
so that the separation between source and receiver at time
7175:
5918:
The Lorentz factor appears in the Lorentz transformations:
5781:). Since the tangent line through A and B has the equation
3834:â˛). Likewise, each line drawn parallel to a temporal axis (
3762:
In this comparison the clock W is moving by with velocity â
3687:
in S', as running slower than hers. How two clocks can run
3623:-axis along their world lines. The projection of the rod's
3484:. On the other hand, the green hyperbolae, which cross the
3065:
The light cone has an essential role within the concept of
2997:
2989:
2905:. The pulse is reflected from a mirror situated a distance
1168:). Special relativity provides a new invariant, called the
401:
318:
17895:
16323:
International Earth Rotation and Reference Systems Service
14071:
Black Holes & Time Warps: Einstein's Outrageous Legacy
13703:
13701:
13699:
12875:
12873:
12287:. Paphos, Cyprus: ArtDeCiel Publishing. pp. 202â233.
12002:(2nd ed.). New York: Pergamon Press Ltd. p. 33.
11903:
Mathematics & Common Sense: A Case of Creative Tension
11200:(unidirectional). Let the number of spatial dimensions be
7294:, the wavelength is increased, and the observed frequency
4044:
In the lower picture the frame S is moving with velocity â
586:
the difference between what one measures and what one sees
16868:
13996:
Rosen, N. (1940). "General Relativity and Flat Space I".
13647:"Mechanics and Relativity. Chapter 4.3: Reference Frames"
13217:. Cambridge, UK: Cambridge University Press. p. 26.
13087:
Introducing Einstein's Relativity: A Deeper Understanding
12033:
Introduction to Tensor Calculus, Relativity and Cosmology
11717:
transforming planes into planes, it is isomorphic to the
11436:
Basic introduction to the mathematics of curved spacetime
8868:{\displaystyle E^{2}-p^{2}c^{2}=m_{\text{rest}}^{2}c^{4}}
7982:
quantity, possessing the same direction as the velocity:
4774:
4048:
in the frame SⲠat rest. The worldline of clock W is the
2479:
In the following discussion, we use the first convention.
14093:
13861:. Internet Encyclopedia of Philosophy (ISSN 2161-0002).
13825:
13823:
13821:
13322:(1st ed.). Jones & Bartlett Pub. p. 1047.
13127:. New York: Penguin Random House LLC. pp. 155â156.
11417:
that can afford a "stable" gas sphere with a "positive"
11158:
7960:
6790:
in the red frame that is moving with velocity parameter
5373:
One also sees very frequently the use of the convention
3842:) represents a line of equal spatial coordinate values (
3007:
Figure 2â5. Light cone in 2D space plus a time dimension
2797:Ⲡaxis passes through the events in frame SⲠwhich have
2769:
The origins of frames S and SⲠare coincident when time
1807:{\displaystyle ds^{2}=c^{2}dt^{2}-dx^{2}-dy^{2}-dz^{2}.}
1259:
between the two events that are separated by a distance
15251:
13937:
Grishchuk, L. P.; Petrov, A. N.; Popova, A. D. (1984).
13764:. (ii) A second reporter, aware of the large mass
13696:
12870:
11222:, setting aside the compactified dimensions invoked by
9376:
collide to produce a single particle of conserved mass
8450:
can be interpreted as a relativistic generalization of
6732:
3532:
939:
invariant intervals analogous to the spacetime interval
898:). On 21 September 1908, Minkowski presented his talk,
14852:
13381:. Cambridge, Massachusetts: Harvard University Press.
12584:. New York: W. W. Norton & Company, Inc. pp.
11284:
impulse will travel at different speeds. If there are
10418:
Two central propositions underlie general relativity.
8762:{\displaystyle \approx mc^{2}+{\frac {1}{2}}mv^{2}...}
8297:. Infinity times zero is an ill-defined quantity, but
7978:, the product of a particle's mass and velocity, is a
5481:
4163:
Figure 2â11. Spacetime explanation of the twin paradox
2537:
is positive, the spacetime interval is referred to as
17848:
14478:
dimensions and the dimensionality of space problem".
13936:
13836:. Princeton, New Jersey: Princeton University Press.
13818:
13711:
Spacetime Physics: Introduction to Special Relativity
13596:. Cambridge: Cambridge University Press. p. 60.
13177:
13175:
12166:
Spacetime Physics: Introduction to Special Relativity
11905:. Wellesley, Massachusetts: A.K. Peters. p. 86.
11807:
This is because the law of gravitation (or any other
11709:
For instance, the Lorentz group is a subgroup of the
11290:
11107:
11087:
11059:
11039:
11016:
10996:
10976:
10953:
10909:
10861:
10838:
10803:
10321:
10115:
10074:
10041:
9988:
9934:
9893:
9776:
9738:
9705:
9662:
9623:
9568:
9436:
9384:
9326:
9268:
9162:
9064:
8948:
8893:
8803:
8707:
8629:
8571:
8511:
8468:
8405:
8320:
8248:
8210:
8119:
8067:
8017:
7922:
7906:{\displaystyle f=f'/\gamma =f'{\sqrt {1-\beta ^{2}}}}
7849:
7825:{\displaystyle f=f'\gamma =f'/{\sqrt {1-\beta ^{2}}}}
7768:
7637:
7563:
7526:
7503:
7483:
7460:
7393:
7307:
7074:
7022:
6639:
6549:{\displaystyle \Delta x'=\gamma (\Delta x-v\Delta t)}
6504:
6429:
6380:
6314:
6102:
5927:
5822:
5683:
5581:
5558:
5379:
5347:
5316:
5060:
4803:
4730:
4693:
4509:
4477:
4445:
4404:
3498:
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3420:
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3188:
2838:
2628:
2578:
2547:
2516:
2489:
2376:
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2246:
2225:
2195:
2168:
2132:
2092:
2072:
2038:
1987:
1958:
1915:
1887:
1823:
1713:
1678:
1655:
1624:
1604:
1581:
1448:
1356:
1330:
1290:
1265:
1227:
1201:
1178:
1164:) or the distance between the two events (because of
1021:
989:
510:
13714:(2nd ed.). San Francisco, California: Freeman.
13482:(4th ed.). Amsterdam: Elsevier. pp. 1â24.
12886:
Jahresbericht der Deutschen Mathematiker-Vereinigung
12682:, Chicago, Illinois: Open Court Publishing Company,
12362:. Boston, Massachusetts: Birkhäuser. pp. 1â13.
12169:(2nd ed.). San Francisco, California: Freeman.
10741:
of higher dimensions. It enabled the formulation of
8187:
Light particles, or photons, travel at the speed of
7014:
into the equations in Step 2 immediately yield
5406:
Figure 3â4. Lorentz factor as a function of velocity
3976:. For a comparison, the length of the time interval
3874:-axes (lower pictures, clock W). The worldlines of W
1817:
In a different inertial frame, say with coordinates
919:
833:
Einstein in 1905 superseded previous attempts of an
14474:Tangherlini, F. R. (1963). "Schwarzschild field in
12581:
Einstein's Clocks, PoincarĂŠ's Maps: Empires of Time
11409:under its self-gravity, Wei-Xiang Feng showed that
11257:. While Kant's argument is historically important,
10366:
9880:
8308:By this analysis, if the energy of a photon equals
8191:, the constant that is conventionally known as the
7227:, and she can use the Lorentz transformations with
16253:
13797:
13708:Taylor, Edwin F.; Wheeler, John Archibald (1992).
13374:
13172:
13077:
12913:
12790:
12461:(11th ed.). Oxford: Oxford University Press.
12200:; Shaffer, Peter S.; Vokos, Stamatis (July 2001).
12196:
12163:Taylor, Edwin F.; Wheeler, John Archibald (1992).
11305:
11137:
11093:
11065:
11053:(representing an observer) and another containing
11045:
11022:
11002:
10982:
10959:
10939:
10879:
10844:
10821:
10715:Riemannian geometry originated with the vision of
10346:
10189:{\displaystyle v^{\prime }=(v-u)/(1-{vu}/{c^{2}})}
10188:
10097:
10056:
10020:
9960:
9916:
9808:
9753:
9720:
9683:
9644:
9602:
9552:
9416:
9366:
9308:
9238:Figure 3â10. Relativistic conservation of momentum
9174:
9148:
9048:
8911:
8867:
8761:
8694:
8600:
8553:
8490:
8432:
8357:
8268:
8230:
8150:
8101:
8035:
7928:
7905:
7824:
7688:
7616:
7549:
7512:
7489:
7469:
7434:
7351:
7216:, and he can use the Lorentz transformations with
7111:
7059:
6709:
6548:
6491:
6415:
6367:
6267:
6082:
5883:
5689:
5658:
5564:
5542:
5391:
5362:
5333:
5132:
4823:
4789:Figure 3â2. Relativistic composition of velocities
4756:
4716:
4529:
4494:
4462:
4430:
3504:
3476:
3433:
3403:
3250:
3211:
3156:From the reference frame of an observer moving at
3141:From the reference frame of an observer moving at
3015:(temporal distance) than necessary to cross their
2873:
2634:
2599:
2568:is negative, the spacetime interval is said to be
2560:
2529:
2502:
2453:
2356:
2259:
2231:
2211:
2181:
2154:
2103:
2078:
2055:
2024:
1973:
1944:
1901:
1873:
1806:
1693:
1664:
1640:
1610:
1590:
1564:
1428:
1339:
1316:
1276:
1251:
1213:
1187:
1117:
1000:
954:
669:Among other issues, the dependence of the partial
516:
336:effects, such as how different observers perceive
14170:
14168:
13535:"Optics of high-performance electron microscopes"
13190:. Metaphysics Research Lab, Stanford University.
13156:. Metaphysics Research Lab, Stanford University.
12916:"La thĂŠorie des groupes continus et la gĂŠomĂŠtrie"
11878:. Metaphysics Research Lab, Stanford University.
11631:"With respect to this it is clear that the group
6966:Length contraction and similar triangles give us
5701:is the maximum possible speed in nature. For any
4233:
3488:axis, are spacelike curves because all intervals
2817:axis at any time other than zero. Therefore, the
2454:{\displaystyle s^{2}=-(ct)^{2}+x^{2}+y^{2}+z^{2}}
413:, or anything external. It assumes that space is
17922:
13455:Special Relativity for the Enthusiastic Beginner
13002:
7836:the source, emitted from this closest point, is
7617:{\displaystyle T=w+\beta w=\gamma w'(1+\beta ).}
7352:{\displaystyle f={\frac {1}{1+\beta _{s}}}f_{0}}
6747:Figure 3â5. Derivation of Lorentz Transformation
4052:-axis (slanted to the left), the worldline of Wâ˛
2357:{\displaystyle s^{2}=(ct)^{2}-x^{2}-y^{2}-z^{2}}
14087:
13457:. CreateSpace Independent Publishing Platform.
10562:than the usual curved spacetime interpretation?
8933:to represent the four-momentum and a lowercase
8563:, so that Einstein arrived at the relationship
7708:Figure 3â7. Transverse Doppler effect scenarios
4395:, the coordinate transformation is as follows:
4041:, showing that the "moving" clock runs slower.
3046:than can be crossed at lightspeed in the given
2762:-direction of frame S with a constant velocity
2465:These sign conventions are associated with the
487:observer to be in motion relative to an event.
14216:
14165:
13477:
13319:Physics for Scientists and Engineers, Volume 2
12949:
12709:. In Renn, JĂźrgen; Schemmel, Matthias (eds.).
12573:
12571:
12569:
12550:Albert Einstein's Special Theory of Relativity
10528:
8358:{\displaystyle E^{\prime }=(1-\beta )\gamma E}
7557:Since the slope of the green light ray is â1,
7274:
5697:becomes physically meaningless, implying that
5219:Time dilation and length contraction revisited
3855:One may designate in both pictures the origin
2189:terms. The spacetime interval is the quantity
17008:
16239:
15267:
14963:
14064:
14062:
13930:
13707:
13377:Very Special Relativity: An Illustrated Guide
13054:
13052:
13050:
13048:
13046:
12162:
11166:Anthropic principle § Dimensions of spacetime
9828:
9603:{\displaystyle {\boldsymbol {p=p_{1}+p_{2}}}}
8554:{\displaystyle \gamma mc=m_{\text{rel}}c=E/c}
7241:to relate Ursula's measurements with his own.
6772:) in the black "rest system" and coordinates
5133:{\displaystyle u={v+u' \over 1+(vu'/c^{2})}.}
3074:
2572:. Spacetime intervals are equal to zero when
716:, the Fizeau experiment and other phenomena.
278:
14877:
14738:
14096:Proceedings of the Royal Society of London A
14024:
13539:Science and Technology of Advanced Materials
13501:
13499:
13401:
13116:
12816:
12814:
12782:
12729:
12615:Rendiconti del Circolo Matematico di Palermo
12481:
10720:
8151:{\displaystyle p^{\prime }=-\beta \gamma mc}
7699:
3818:Each line drawn parallel to a spatial axis (
1008:between two points can be defined using the
837:âenergy relation by introducing the general
332:are useful in visualizing and understanding
14473:
14217:Bär, Christian; Fredenhagen, Klaus (2009).
13829:
12844:Historical Studies in the Physical Sciences
12711:The Genesis of General Relativity, Volume 3
12680:Einstein's Revolution: A Study in Heuristic
12566:
12358:. In Kox, A. J.; Eisenstaedt, Jean (eds.).
11872:"Newton's Views on Space, Time, and Motion"
11869:
9214:, the fact that such processes do not care
8370:
7112:{\displaystyle x=\gamma x'+\beta \gamma w'}
7060:{\displaystyle w=\gamma w'+\beta \gamma x'}
5724:. The invariant hyperbola has the equation
5543:{\textstyle OB=OK/{\sqrt {1-v^{2}/c^{2}}}.}
5426:. The invariant hyperbola has the equation
4769:Galilean law for the addition of velocities
4240:
4033:) in Sâ˛. This shows that the time interval
3565:), while for a clock traveling at 0.7
2813:, so that they are not coincident with the
27:Mathematical model combining space and time
17015:
17001:
16246:
16232:
15274:
15260:
14970:
14956:
14929:Encyclopedia of Spaceâtime and gravitation
14925:Historical: Albert Einstein's 1926 article
14212:
14210:
14208:
14206:
14174:
14059:
13638:
13206:
13147:
13063:. Massachusetts: Harcourt/Academic Press.
13043:
13035:: CS1 maint: location missing publisher (
12322:"What is Einstein's Theory of Relativity?"
12023:
10246:mass and the muon mass is 33.91 MeV.
6753:derivations of the Lorentz transformations
6739:Derivations of the Lorentz transformations
5896:
4937:. In the large yellow triangle, the ratio
4100:in the upper pictures) as simultaneous to
3882:are the corresponding vertical time axes (
3166:, the events appear to occur in the order
2888:Ⲡaxis is also tilted with respect to the
1952:. For any other infinitesimal event where
371:. This interpretation proved vital to the
285:
271:
14670:
14613:
14549:
14413:
14395:. Vol. 4. Weidmann. pp. 427â463
14348:
14277:
14180:
14130:
13989:
13897:
13877:
13629:
13589:
13566:
13496:
12963:
12909:
12907:
12879:
12826:
12820:
12811:
12761:
12700:
12698:
12642:
12484:"The Genesis of the theory of relativity"
12226:
12061:
12059:
12057:
12055:
12053:
11999:The Theory of Space, Time and Gravitation
11948:
11946:
11944:
11942:
11725:which is often expressed in terms of the
11713:. The Lorentz group is isomorphic to the
11667:is mathematically more intelligible than
11204:and the number of temporal dimensions be
8433:{\displaystyle \beta \gamma mc=\gamma mv}
7672:
6093:The inverse Lorentz transformations are:
5475:. A bit of algebraic manipulation yields
5269:Learn how and when to remove this message
3663:Mutual time dilation and the twin paradox
3641:In regards to mutual length contraction,
3631:axis yields the foreshortened length OC.
3580:This illustrates the phenomenon known as
3515:Fig. 2-7b reflects the situation in
3404:{\displaystyle (ct)^{2}-x^{2}=\pm s^{2},}
3313:Learn how and when to remove this message
3019:at lightspeed; these events comprise the
2699:Learn how and when to remove this message
16777:International Commission on Stratigraphy
14652:
14030:
13830:Mook, Delo E.; Vargish, Thoma s (1987).
13593:Revolutions in Twentieth-Century Physics
13448:
13446:
13444:
13442:
13440:
13438:
13436:
13434:
13432:
13368:
13366:
13246:
13244:
13242:
13240:
13238:
13236:
13234:
12788:
12735:
12608:
12319:
12219:American Association of Physics Teachers
12158:
12156:
12154:
12120:
12118:
12070:(3rd ed.). Incomprehensible Books.
11989:
11940:
11938:
11936:
11934:
11932:
11930:
11928:
11926:
11924:
11922:
11171:
10614:, M. G. van der Burg, A. W. Metzner and
10580:
10426:
10389:
9233:
8178:
8102:{\displaystyle (mc)^{\prime }=\gamma mc}
7964:
7703:
7444:
7176:Linearity of the Lorentz transformations
6742:
5401:
5290:
4784:
4539:
4158:
4076:. The invariant hyperbola through event
3588:
3536:
3459:The magenta hyperbolae, which cross the
3326:
3152:the events appear to occur in the order
3080:
3002:
2974:
2718:
2710:
2117:
2032:which in turn upon integration leads to
877:
826:analyzed special relativity in terms of
576:Physicists distinguish between what one
540:
14827:
14655:"Existence of life in 2 + 1 dimensions"
14653:Scargill, J. H. C. (26 February 2020).
14525:
14386:
14330:"What makes time different from space?"
14263:
14228:. Dordrecht: Springer. pp. 39â58.
14203:
13478:Landau, L. D.; Lifshitz, E. M. (2006).
13402:Forshaw, Jeffrey; Smith, Gavin (2014).
13395:
13364:
13362:
13360:
13358:
13356:
13354:
13352:
13350:
13348:
13346:
13188:The Stanford Encyclopedia of Philosophy
13122:
12841:
12835:
12577:
12450:
12448:
12446:
12350:
12344:
12065:
11401:On the other hand, in view of creating
11398:, which describes the world around us.
9741:
9708:
9590:
9577:
9570:
9497:
9472:
9446:
9443:
9439:
9354:
9329:
9296:
9271:
9260:In case (2), two masses with momentums
8491:{\displaystyle m_{\text{rel}}=\gamma m}
8293:must be zero, meaning that photons are
7194:are obtained as linear combinations of
6368:{\displaystyle t'=\gamma (t-vx/c^{2}),}
4891:axis rather than parallel to the black
4548:Spacetime and composition of velocities
3673:
662:of 1851, conducted by French physicist
352:and time took on new meanings with the
14:
17923:
14068:
13943:Communications in Mathematical Physics
13408:. John Wiley & Sons. p. 118.
13315:
13288:(1st ed.). Springer. p. 42.
13212:
12904:
12704:
12695:
12547:
12541:
12280:
12262:from the original on 28 September 2018
12124:
12050:
12029:
11952:
11870:Rynasiewicz, Robert (12 August 2004).
10648:
7941:
4775:Relativistic composition of velocities
3262:
3050:. These events comprise the so-called
3039:, making timelike intervals positive.
16996:
16227:
15255:
14951:
14136:
13995:
13977:from the original on 25 February 2021
13883:
13865:from the original on 23 December 2020
13850:
13644:
13623:
13505:
13452:
13429:
13281:
13231:
13084:Ray d'Inverno; James Vickers (2022).
13058:
12677:
12530:from the original on 28 February 2008
12151:
12115:
11919:
11900:
11851:
11159:Privileged character of 3+1 spacetime
9754:{\displaystyle {\boldsymbol {p_{2}}}}
9721:{\displaystyle {\boldsymbol {p_{1}}}}
8601:{\displaystyle E=m_{\text{rel}}c^{2}}
7961:Extending momentum to four dimensions
7435:{\displaystyle f=(1-\beta _{r})f_{0}}
4895:axis. What is the composite velocity
2821:Ⲡaxis is tilted with respect to the
2801:Ⲡ= 0. But the points with
2510:can assume any real number value. If
1317:{\displaystyle \Delta {ct}=c\Delta t}
1128:Although two viewers may measure the
967:
166:Newton's law of universal gravitation
16208:
14749:The Anthropic Cosmological Principle
14595:
14531:"On the dimensionality of spacetime"
14449:Proceedings of the Amsterdam academy
14324:
13532:
13372:
13343:
13215:A first course in general relativity
12770:from the original on 6 November 2018
12454:
12443:
12401:from the original on 17 January 2023
12301:from the original on 17 January 2023
11995:
11977:from the original on 17 January 2023
10719:expressed in his inaugural lecture "
10107:is replaced by the highly nonlinear
9187:
8174:
6733:Deriving the Lorentz transformations
5251:adding citations to reliable sources
5222:
5208:regardless of the starting value of
4008:, the "moving" clock WⲠruns slower.
3895:In the upper picture the place for W
3533:Time dilation and length contraction
3449:spacetime diagram, which are termed
3295:adding citations to reliable sources
3266:
2809:-direction of frame S with velocity
2681:adding citations to reliable sources
2652:
2111:, etc. We are always concerned with
1221:Then the squared spacetime interval
459:. A point in spacetime is called an
17587:TolmanâOppenheimerâVolkoff equation
17540:FriedmannâLemaĂŽtreâRobertsonâWalker
14938:Stanford Encyclopedia of Philosophy
14863:. Internet Archive: W. H. Freeman.
14837:. Oxford: Oxford University Press.
13752:but unaware of the large mass
13154:Stanford Encyclopedia of Philosophy
13009:Foundations of Hyperbolic Manifolds
12090:
11876:Stanford Encyclopedia of Philosophy
11841:would be inversely proportional to
11618:is the Galilean group and the group
11192:There are two kinds of dimensions:
11030:but obtain different descriptions.
10775:
10523:
4017:may be constructed as the event at
3464:speedâfor all secants is less than
3023:of the event O. Likewise, the
2648:
24:
14732:
13886:General Relativity and Gravitation
13859:"Jules Henri PoincarĂŠ (1854â1912)"
13674:"Energetics of Charged Pion Decay"
13263:from the original on 27 April 2017
13194:from the original on 11 March 2017
13181:
12930:from the original on 23 March 2018
12360:The Universe of General Relativity
12332:from the original on 3 August 2022
12320:Williams, Matt (28 January 2022).
12103:from the original on 13 March 2017
11711:conformal group in four dimensions
10361:33.91 MeV â 29.79 MeV = 4.12 MeV
10121:
8326:
8125:
8082:
6645:
6537:
6525:
6505:
6462:
6450:
6430:
5318:
2874:{\displaystyle \tan(\theta )=v/c.}
2805:Ⲡ= 0 are moving in the
2093:
1679:
1656:
1625:
1598:the speed of light, converts time
1543:
1521:
1499:
1474:
1452:
1407:
1382:
1360:
1308:
1291:
1266:
1231:
1202:
1179:
1097:
1073:
1049:
1025:
990:
712:, with which he could explain the
604:History of Lorentz transformations
131:Introduction to general relativity
25:
17972:
17357:HamiltonâJacobiâEinstein equation
16497:Discrete time and continuous time
14900:
14860:Spacetime Physics, Second Edition
13856:
13250:
13150:"Lightcones and Causal Structure"
13125:The Biggest Ideas in the Universe
12892:from the original on 28 July 2017
12659:from the original on 11 July 2017
12431:from the original on 23 June 2017
12421:"The Nobel Prize in Physics 1902"
11882:from the original on 16 July 2012
10761:, and spurred the development of
10727:differential geometry of surfaces
10591:The spacetime symmetry group for
10431:Figure 5â2. Equivalence principle
10033:Newtonian momenta, calculated as
9430:velocity of the original system,
9229:
7247:
6998:Substituting the expressions for
3800:Figure 2-10. Mutual time dilation
3703:additional, synchronized clocks W
3212:{\displaystyle {\sqrt {-s^{2}}}.}
2793:Ⲡ= 0 in frame Sâ˛. The
375:, wherein spacetime is curved by
216:Mathematics of general relativity
136:Mathematics of general relativity
17906:
17894:
17882:
17870:
17858:
17835:
17834:
16422:
16416:
16207:
16198:
16197:
15036:
14906:
14689:10.1103/PhysRevResearch.2.013217
14359:10.1111/j.1468-0068.2007.00645.x
13684:from the original on 21 May 2017
13671:
13160:from the original on 17 May 2019
11833:. More generally, in a space of
11573:Heisenberg uncertainty principle
11164:This section is an excerpt from
10654:This section is an excerpt from
10374:This section is an excerpt from
10367:Introduction to curved spacetime
10220:
10206:
9881:Energy and momentum conservation
9861:
9837:
9809:{\displaystyle m>m_{1}+m_{2}}
9745:
9712:
9594:
9586:
9581:
9573:
9501:
9476:
9359:
9334:
9301:
9276:
8924:
8052:, but the time component equals
6416:{\displaystyle x'=\gamma (x-vt)}
5765:. Event A has coordinates (
5227:
4029:has equal spacetime interval as
3790:
3779:
3271:
3251:{\displaystyle {\sqrt {s^{2}}}.}
2657:
1252:{\displaystyle (\Delta {s})^{2}}
1154:four-dimensional Euclidean space
955:Spacetime in special relativity
767:
753:
737:
723:
623:
612:
251:
250:
237:
60:
14942:Space and Time: Inertial Frames
14703:
14646:
14589:
14467:
14454:
14407:
14257:
14192:
13735:
13665:
13617:
13583:
13526:
13471:
13309:
13275:
13148:Curiel, Erik; Bokulich, Peter.
13141:
13107:
12996:
12943:
12793:Einstein: His Life and Universe
12671:
12602:
12475:
12413:
12383:
12313:
12274:
12190:
11959:(Reprint ed.). Cambridge:
11801:
11791:
11778:
11759:
11749:
11732:
11703:
11600:
11583:
11553:
11540:
11526:
11498:
10376:Curved spacetime § Introduction
7267:right angles to the said line (
6935:Substituting equation (4) into
6751:There have been many dozens of
5334:{\displaystyle \mathrm {T} =ct}
5238:needs additional citations for
5040:Substitute the expressions for
4571:with respect to frame S, since
4273:
4234:Basic mathematics of spacetime
4187:
4130:
4060:â˛-axis, and the worldline of Wâ˛
3642:
3282:needs additional citations for
3102:
2668:needs additional citations for
1439:or for three space dimensions,
566:synchronize the clocks, in the
498:Mathematically, spacetime is a
432:provides an explanation of how
384:
32:Space and Time (disambiguation)
17164:Massâenergy equivalence (E=mc)
17022:
16570:History of timekeeping devices
14073:. W. W. Norton & Company.
13645:Idema, Timon (17 April 2019).
13512:. Cambridge University Press.
13257:The Physics and Relativity FAQ
12914:Cartan, Ă.; Fano, G. (1955) .
12217:(S1). College Park, Maryland:
12084:
11894:
11863:
11811:) follows from the concept of
11446:Einstein's thought experiments
11349:partial differential equations
11132:
11108:
10934:
10910:
10874:
10862:
10816:
10804:
10183:
10149:
10141:
10129:
9143:
9098:
9092:
9086:
9071:
9043:
8990:
8984:
8978:
8955:
8346:
8334:
8078:
8068:
8030:
8018:
7608:
7596:
7419:
7400:
6756:expressions of the underlying
6543:
6522:
6483:
6447:
6410:
6395:
6359:
6329:
5865:
5846:
5121:
5092:
4224:
4064:is the vertical through event
3910:â˛-axis) in the event labelled
3360:
3350:
3170:. The white line represents a
2851:
2845:
2789: = 0 in frame S and
2403:
2393:
2306:
2296:
2143:
2133:
2025:{\displaystyle ds^{2}=ds'^{2}}
1868:
1824:
1550:
1540:
1528:
1518:
1506:
1496:
1484:
1471:
1459:
1449:
1414:
1404:
1392:
1379:
1367:
1357:
1240:
1228:
1106:
1094:
1082:
1070:
1058:
1046:
1034:
1022:
839:equivalence of mass and energy
391:
13:
1:
14977:
14919:Albert Einstein on spaceâtime
14538:Classical and Quantum Gravity
14266:Classical and Quantum Gravity
13533:Rose, H. H. (21 April 2008).
12552:. New York: Springer-Verlag.
11856:
11245:suggested that the world is "
10895:, as well as determining the
10021:{\displaystyle m=m_{1}+m_{2}}
9417:{\displaystyle m=m_{1}+m_{2}}
8454:. Einstein proposed that the
8312:in the rest frame, it equals
6423:etc., most often really mean
2996:(t>0), the other into the
2962:
1874:{\displaystyle (t',x',y',z')}
600:History of special relativity
14822:A Treatise on Time and Space
14781:and Ruth M. Williams (1992)
14632:10.1103/PhysRevD.106.L041501
14596:Feng, W.X. (3 August 2022).
14053:10.1016/0031-9163(64)90396-8
13590:Griffiths, David J. (2013).
13559:10.1088/0031-8949/9/1/014107
13316:Lerner, Lawrence S. (1997).
11607:(In the following, the group
11476:Philosophy of space and time
11255:law of universal gravitation
10887:. The metric determines the
10747:general theory of relativity
10474:and in Newton's second law,
8001:quantity, meaning that if a
7550:{\displaystyle w=\gamma w'.}
7520:. Because of time dilation,
7369:for a velocity parameter of
7287:for a velocity parameter of
5673:is greater than or equal to
4116:corresponds again to above.
1641:{\displaystyle \Delta s^{2}}
373:general theory of relativity
358:special theory of relativity
7:
17179:Relativistic Doppler effect
16517:Gravitational time dilation
16353:Barycentric Coordinate Time
16012:Geological history of Earth
14785:. Oxford University Press.
14783:Flat and curved spaceâtimes
14387:Leibniz, Gottfried (1880).
13213:Schutz, Bernard F. (1985).
12880:Minkowski, Hermann (1909).
12391:"George Francis FitzGerald"
12210:American Journal of Physics
11428:
10529:Is spacetime really curved?
7626:relativistic Doppler effect
7275:Longitudinal Doppler effect
7258:Relativistic Doppler effect
4219:gravitational time dilation
4202:from Stella's point of view
4108: = 0. The result
4096:is constructed (similar to
3886:in the upper pictures, and
3182:, i.e. the true distance =
679:MichelsonâMorley experiment
534:MichelsonâMorley experiment
524:(conventionally called the
445:Cartesian coordinate system
161:Introduction to gravitation
10:
17977:
17650:In computational physics:
17174:Relativity of simultaneity
16373:Geocentric Coordinate Time
16358:Barycentric Dynamical Time
16296:Coordinated Universal Time
15364:Orders of magnitude (time)
14568:10.1088/0264-9381/14/4/002
14389:"Discourse on metaphysics"
14296:10.1088/0264-9381/14/4/002
13282:Mould, Richard A. (1994).
13061:Introduction to Relativity
12884:[Space and Time].
12548:Miller, Arthur I. (1998).
11961:Cambridge University Press
11461:Global spacetime structure
11313:spatial dimensions, where
11163:
10779:
10749:, made profound impact on
10689:at each point that varies
10653:
10584:
10394:Figure 5â1. Tidal effects.
10373:
9829:Choice of reference frames
9208:space translation symmetry
9206:in space they take place (
9191:
9156:using the convention that
8379:In the low speed limit as
7945:
7454:with a velocity parameter
7251:
6920:Because of time dilation,
6736:
6629: = 600.00 s
5900:
5280:
5200:, then the formula yields
4824:{\displaystyle \beta =v/c}
4778:
4767:which is the common-sense
4724: or
4244:
3666:
3124:relativity of simultaneity
3075:Relativity of simultaneity
2966:
2104:{\displaystyle \Delta {x}}
1694:{\displaystyle \Delta s=0}
1277:{\displaystyle \Delta {x}}
1001:{\displaystyle \Delta {d}}
971:
958:
946:ĂźberflĂźssige Gelehrsamkeit
597:
591:
428:relative to the observer.
40:Spacetime (disambiguation)
36:Timespace (disambiguation)
29:
17832:
17664:
17529:
17501:
17487:LenseâThirring precession
17370:
17319:
17281:
17260:
17249:
17207:
17151:
17135:
17077:
17069:Doubly special relativity
17041:
17030:
16927:
16818:
16785:
16759:
16640:
16540:
16527:Time-translation symmetry
16457:
16431:
16414:
16338:International Atomic Time
16288:
16265:
16193:
16135:
16088:
16075:Time translation symmetry
16020:
15960:
15950:
15872:
15799:
15719:
15660:
15544:
15462:
15372:
15334:
15320:
15289:
15238:
15217:
15153:
15091:
15045:
15034:
14985:
13003:Ratcliffe, J. G. (1994).
12789:Isaacson, Walter (2007).
12736:Einstein, Albert (1905).
12705:Walter, Scott A. (2007).
11901:Davis, Philip J. (2006).
11685:, but rather for a group
11358:, Tegmark maintains that
11239:Gottfried Wilhelm Leibniz
11138:{\displaystyle (x,y,z,t)}
10940:{\displaystyle (x,y,z,t)}
10587:BondiâMetznerâSachs group
10347:{\displaystyle E_{v}=pc,}
9220:time translation symmetry
7741:<!âend plainlistâ>
7700:Transverse Doppler effect
7269:transverse Doppler effect
4781:Velocity addition formula
4206:But during the turnaround
4080:scales the time interval
3941:In the upper picture the
3890:Ⲡin the lower pictures).
2737:Galilean reference frames
2600:{\displaystyle x=\pm ct.}
1881:, the spacetime interval
1214:{\displaystyle \Delta x.}
978:In three dimensions, the
690:George Francis FitzGerald
447:, these are often called
317:and the one dimension of
315:three dimensions of space
191:Derivations of relativity
17347:Post-Newtonian formalism
17337:Einstein field equations
17273:Mathematical formulation
17097:Hyperbolic orthogonality
15281:
14659:Physical Review Research
14443:10.1002/andp.19203660503
14159:10.1103/PhysRev.128.2851
12763:10.1002/andp.19053221004
12644:2027/uiug.30112063899089
12609:Poincare, Henri (1906).
11953:Schutz, Bernard (2004).
11548:Einstein synchronization
11492:
11243:Discourse on Metaphysics
10829:. This means the smooth
10739:differentiable manifolds
9875:center-of-momentum frame
9854:Center of Momentum Frame
9212:conservation of momentum
8912:{\displaystyle E=\pm pc}
8885:equals zero, it yields,
8371:Massâenergy relationship
6830:Lorentz transformation.
5912:addition of velocities.
5048:into the expression for
4241:Galilean transformations
4088:, which is shorter than
3992:. This yields the event
2155:{\displaystyle (ct)^{2}}
1974:{\displaystyle ds\neq 0}
1945:{\displaystyle ds=ds'=0}
1665:{\displaystyle \Delta t}
1188:{\displaystyle \Delta t}
892:The Relativity Principle
141:Einstein field equations
17058:Galilean transformation
17049:Principle of relativity
16787:Astronomical chronology
16760:Archaeology and geology
16467:Absolute space and time
16383:IERS Reference Meridian
16378:International Date Line
16289:International standards
16030:Absolute space and time
15681:Astronomical chronology
14923:EncyclopĂŚdia Britannica
14754:Oxford University Press
14462:Space, time, and matter
13405:Dynamics and Relativity
13059:Kogut, John B. (2001).
12888:. B. G. Teubner: 1â14.
12578:Galison, Peter (2003).
12511:10.1007/3-7643-7436-5_1
12281:Hughes, Stefan (2013).
12066:Collier, Peter (2017).
11829:has a surface area of 4
11188:-dimensional spacetimes
10790:Differentiable manifold
10501:should be equal to the
9961:{\displaystyle p'=p-mu}
9684:{\displaystyle E_{2}/c}
9645:{\displaystyle E_{1}/c}
7956:Massâenergy equivalence
7929:{\displaystyle \gamma }
7513:{\displaystyle \beta w}
7470:{\displaystyle \beta ,}
5897:Lorentz transformations
5708:In Fig. 3-3b, segments
5690:{\displaystyle \gamma }
5565:{\displaystyle \gamma }
5410:In Fig. 3-3a, segments
4757:{\displaystyle u=u'+v,}
4431:{\displaystyle x'=x-vt}
2766:as measured in frame S.
2733:standard configuration.
1195:and a spatial distance
896:Das Relativitätsprinzip
798:principle of relativity
106:Lorentz transformations
17143:Lorentz transformation
16080:Time reversal symmetry
15384:Italian six-hour clock
14219:"Lorentzian Manifolds"
14116:10.1098/rspa.1962.0161
14018:10.1103/PhysRev.57.147
13804:. Dover Publications.
13123:Carroll, Sean (2022).
12982:10.1002/andp.200810324
12455:Pais, Abraham (1982).
12395:The Linda Hall Library
12351:Stachel, John (2005).
12125:French, A. P. (1968).
12030:Lawden, D. F. (1982).
11523:), pure air, clear sky
11519:from the Greek Îąáź°Î¸ÎŽĎ (
11307:
11189:
11139:
11095:
11067:
11047:
11024:
11004:
10984:
10961:
10941:
10881:
10846:
10823:
10721:
10607:, the PoincarĂŠ group.
10432:
10395:
10348:
10190:
10099:
10098:{\displaystyle v'=v-u}
10058:
10022:
9962:
9918:
9917:{\displaystyle v'=v-u}
9810:
9755:
9722:
9685:
9646:
9604:
9554:
9418:
9368:
9310:
9239:
9224:conservation of energy
9176:
9150:
9050:
8913:
8869:
8763:
8696:
8602:
8555:
8492:
8434:
8359:
8270:
8232:
8184:
8152:
8103:
8037:
7971:
7930:
7907:
7826:
7709:
7690:
7618:
7551:
7514:
7491:
7471:
7450:
7436:
7353:
7113:
7061:
6748:
6711:
6550:
6493:
6417:
6369:
6269:
6084:
5903:Lorentz transformation
5885:
5691:
5660:
5566:
5544:
5407:
5393:
5364:
5335:
5296:
5134:
4825:
4790:
4758:
4718:
4717:{\displaystyle u'=u-v}
4549:
4531:
4496:
4464:
4432:
4210:
4164:
4123:affect the observer's
4000:-axis, and obviously:
3594:
3542:
3506:
3478:
3435:
3405:
3332:
3252:
3213:
3086:
3035:is greater than Δ
3008:
2980:
2913:Ⲡ= 0,
2875:
2758:Frame SⲠmoves in the
2724:
2716:
2636:
2601:
2562:
2531:
2504:
2455:
2358:
2261:
2233:
2213:
2212:{\displaystyle s^{2},}
2183:
2156:
2123:
2105:
2080:
2057:
2026:
1975:
1946:
1903:
1875:
1808:
1695:
1666:
1642:
1612:
1592:
1566:
1430:
1341:
1318:
1278:
1253:
1215:
1189:
1119:
1002:
887:
868:
794:operational definition
702:Lorentz transformation
550:
518:
354:Lorentz transformation
17611:WeylâLewisâPapapetrou
17352:Raychaudhuri equation
17291:Equivalence principle
16746:Weekday determination
16632:Sundial markup schema
15845:Time and fate deities
15790:The Unreality of Time
15729:A series and B series
14464:. Dover reprint: 284.
13506:Morin, David (2008).
13453:Morin, David (2017).
13373:Bais, Sander (2007).
13011:. New York. pp.
13005:"Hyperbolic geometry"
12482:Darrigol, O. (2005),
11419:cosmological constant
11308:
11175:
11140:
11096:
11068:
11048:
11025:
11005:
10985:
10962:
10942:
10891:geometry of spacetime
10882:
10880:{\displaystyle (3,1)}
10847:
10824:
10822:{\displaystyle (M,g)}
10767:differential topology
10755:representation theory
10713:local contributions.
10667:differential geometry
10581:Asymptotic symmetries
10438:equivalence principle
10430:
10393:
10349:
10191:
10100:
10059:
10023:
9963:
9919:
9811:
9756:
9723:
9686:
9647:
9605:
9560:. The total momentum
9555:
9419:
9369:
9311:
9237:
9177:
9151:
9051:
8914:
8870:
8764:
8697:
8603:
8556:
8493:
8435:
8360:
8271:
8269:{\displaystyle E/c=p}
8233:
8231:{\displaystyle E/p=c}
8182:
8153:
8104:
8038:
8036:{\displaystyle (x,t)}
7968:
7931:
7908:
7827:
7707:
7691:
7619:
7552:
7515:
7492:
7472:
7448:
7437:
7354:
7114:
7062:
6758:principle of locality
6746:
6712:
6551:
6494:
6418:
6370:
6290:is small enough, the
6270:
6085:
5886:
5692:
5677:, the expression for
5661:
5567:
5545:
5405:
5394:
5365:
5336:
5294:
5135:
4826:
4788:
4759:
4719:
4543:
4532:
4530:{\displaystyle t'=t.}
4497:
4465:
4433:
4378:coordinates and that
4214:Equivalence Principle
4183:
4162:
3592:
3540:
3507:
3479:
3436:
3434:{\displaystyle s^{2}}
3406:
3330:
3253:
3214:
3172:plane of simultaneity
3084:
3006:
2978:
2876:
2722:
2714:
2637:
2602:
2563:
2561:{\displaystyle s^{2}}
2532:
2530:{\displaystyle s^{2}}
2505:
2503:{\displaystyle s^{2}}
2456:
2359:
2262:
2260:{\displaystyle s^{2}}
2234:
2214:
2184:
2182:{\displaystyle x^{2}}
2157:
2121:
2106:
2081:
2058:
2027:
1981:, one can prove that
1976:
1947:
1904:
1876:
1809:
1696:
1667:
1643:
1613:
1593:
1567:
1431:
1342:
1319:
1279:
1254:
1216:
1190:
1120:
1003:
959:Further information:
881:
863:
843:equivalence principle
544:
519:
201:Differential geometry
101:Equivalence principle
17946:Theory of relativity
17652:Numerical relativity
17493:pulsar timing arrays
16767:Chronological dating
16507:Theory of relativity
16368:Daylight saving time
16096:Chronological dating
16065:Theory of relativity
15409:Daylight saving time
15154:Dimensions by number
14944:" by Robert DiSalle.
14915:at Wikimedia Commons
14818:Lucas, John Randolph
14715:technologyreview.com
14069:Thorne, Kip (1995).
12099:. Wolfram Research.
11768:In this linked image
11578:quantum entanglement
11306:{\displaystyle 5+2k}
11288:
11196:(bidirectional) and
11105:
11085:
11057:
11037:
11014:
10994:
10974:
10951:
10907:
10859:
10836:
10801:
10671:Riemannian manifolds
10319:
10113:
10072:
10057:{\displaystyle p=mv}
10039:
9986:
9932:
9891:
9774:
9736:
9703:
9660:
9621:
9566:
9434:
9382:
9324:
9266:
9175:{\displaystyle c=1.}
9160:
9062:
8946:
8891:
8801:
8705:
8627:
8569:
8509:
8466:
8403:
8318:
8246:
8208:
8117:
8065:
8015:
7920:
7847:
7766:
7635:
7561:
7524:
7501:
7481:
7458:
7391:
7376:, the wavelength is
7305:
7072:
7020:
6637:
6502:
6427:
6378:
6312:
6100:
5925:
5820:
5681:
5579:
5556:
5479:
5392:{\displaystyle c=1.}
5377:
5363:{\displaystyle w=ct}
5345:
5314:
5247:improve this article
5058:
4801:
4728:
4691:
4611:, can be written as
4507:
4495:{\displaystyle z'=z}
4475:
4463:{\displaystyle y'=y}
4443:
4402:
3674:Mutual time dilation
3496:
3468:
3451:invariant hyperbolae
3418:
3347:
3291:improve this article
3228:
3186:
2990:right circular cones
2836:
2773:= 0 for frame S and
2677:improve this article
2626:
2576:
2545:
2514:
2487:
2374:
2280:
2244:
2223:
2193:
2166:
2130:
2090:
2070:
2056:{\displaystyle s=s'}
2036:
1985:
1956:
1913:
1885:
1821:
1711:
1676:
1653:
1622:
1602:
1579:
1446:
1354:
1328:
1288:
1263:
1225:
1199:
1176:
1019:
987:
950:Minkowski spacetime.
935:conformal geometries
835:electromagnetic mass
508:
479:. Spacetime is thus
434:gravitational fields
307:space-time continuum
179:Relevant mathematics
17941:Theoretical physics
17936:Concepts in physics
17544:Friedmann equations
17438:HulseâTaylor binary
17400:Gravitational waves
17296:Riemannian geometry
17122:Proper acceleration
17107:Maxwell's equations
17053:Galilean relativity
16977:Time value of money
16772:Geologic time scale
16627:History of sundials
16492:Cosmological decade
16444:Greenwich Mean Time
16275:Orders of magnitude
15389:Thai six-hour clock
14881:(1 December 2017).
14834:The Road to Reality
14681:2020PhRvR...2a3217S
14624:2022PhRvD.106d1501F
14560:1997CQGra..14L..69T
14492:1963NCim...27..636T
14435:1920AnP...366..440E
14288:1997CQGra..14L..69T
14151:1962PhRv..128.2851S
14108:1962RSPSA.269...21B
14045:1964PhL.....9..357W
14010:1940PhRv...57..147R
13955:1984CMaPh..94..379G
13908:1970GReGr...1....9D
13551:2008STAdM...9a4107R
12974:2008AnP...520..631K
12754:1905AnP...322..891E
12627:1906RCMP...21..129P
12503:2006eins.book....1D
12237:2001AmJPh..69S..24S
12131:Boca Raton, Florida
11629:the Lorentz group.)
11561:thought experiments
11451:Four-dimensionalism
10796:Lorentzian manifold
10786:Lorentzian manifold
10663:Riemannian geometry
10656:Riemannian geometry
10649:Riemannian geometry
10624:gravitational waves
10620:asymptotic symmetry
9823:elementary particle
8854:
7942:Energy and momentum
7759:light of frequency
3263:Invariant hyperbola
2955:Mercator projection
2777:Ⲡ= 0 for frame Sâ˛.
1902:{\displaystyle ds'}
1146:Lorentz contraction
1010:Pythagorean theorem
961:Minkowski spacetime
714:aberration of light
656:luminiferous aether
398:classical mechanics
48:Part of a series on
17593:ReissnerâNordstrĂśm
17511:BransâDicke theory
17342:Linearized gravity
17169:Length contraction
17087:Frame of reference
17064:Special relativity
16952:Mental chronometry
16580:Marine chronometer
16432:Obsolete standards
15919:Rosy retrospection
15897:Mental chronometry
15721:Philosophy of time
15083:Degrees of freedom
14986:Dimensional spaces
14879:Arkani-Hamed, Nima
14824:. London: Methuen.
14804:Minkowski, Hermann
14500:10.1007/BF02784569
14423:Annalen der Physik
13963:10.1007/BF01224832
13916:10.1007/BF00759198
13651:LibreTexts Physics
13253:"The Twin Paradox"
13103:Extract of page 27
12952:Annalen der Physik
12742:Annalen der Physik
12635:10.1007/bf03013466
12491:SĂŠminaire PoincarĂŠ
12137:. pp. 35â60.
12127:Special Relativity
11852:Additional details
11809:inverse-square law
11595:Annalen der Physik
11466:List of spacetimes
11303:
11230:differ from 3 and
11190:
11135:
11091:
11063:
11043:
11020:
11000:
10980:
10957:
10937:
10877:
10842:
10819:
10601:General Relativity
10593:Special Relativity
10493:gravitational mass
10433:
10396:
10344:
10186:
10095:
10054:
10018:
9958:
9914:
9806:
9751:
9718:
9681:
9642:
9600:
9550:
9414:
9364:
9306:
9240:
9172:
9146:
9046:
8909:
8865:
8840:
8759:
8692:
8598:
8551:
8488:
8430:
8355:
8295:massless particles
8266:
8228:
8185:
8148:
8099:
8033:
7972:
7926:
7903:
7822:
7710:
7686:
7614:
7547:
7510:
7487:
7467:
7451:
7432:
7349:
7239: = 0.666
7232: = 0.250
7221: = 0.500
7109:
7057:
6859:From the drawing,
6749:
6707:
6546:
6489:
6413:
6365:
6265:
6263:
6080:
6078:
5881:
5687:
5656:
5562:
5540:
5408:
5389:
5360:
5331:
5297:
5287:Length contraction
5130:
4821:
4791:
4754:
4714:
4550:
4527:
4492:
4460:
4428:
4165:
4145:thought experiment
3598:Length contraction
3595:
3543:
3502:
3474:
3431:
3401:
3333:
3248:
3209:
3087:
3029:timelike intervals
3009:
2981:
2871:
2725:
2717:
2632:
2597:
2558:
2527:
2500:
2451:
2354:
2257:
2229:
2209:
2179:
2152:
2124:
2101:
2076:
2053:
2022:
1971:
1942:
1899:
1871:
1804:
1691:
1662:
1638:
1608:
1591:{\displaystyle c,}
1588:
1562:
1426:
1340:{\displaystyle ct}
1337:
1314:
1274:
1249:
1211:
1185:
1170:spacetime interval
1166:length contraction
1115:
998:
968:Spacetime interval
916:invariant interval
888:
848:general relativity
684:stellar aberration
648:corpuscular theory
551:
547:frame of reference
514:
430:General relativity
422:special relativity
420:In the context of
330:Spacetime diagrams
311:mathematical model
305:, also called the
244:Physics portal
221:Spacetime topology
196:Spacetime diagrams
124:General relativity
96:Spacetime manifold
89:Spacetime concepts
78:General relativity
73:Special relativity
17961:Conceptual models
17846:
17845:
17660:
17659:
17639:OzsvĂĄthâSchĂźcking
17245:
17244:
17227:Minkowski diagram
17184:Thomas precession
17127:Relativistic mass
16990:
16989:
16800:Nuclear timescale
16482:Continuous signal
16221:
16220:
16131:
16130:
16106:Circadian rhythms
15924:Tenseâaspectâmood
15779:Temporal finitism
15656:
15655:
15632:Grandfather clock
15249:
15248:
15058:Lebesgue covering
15023:Algebraic variety
14911:Media related to
14763:978-0-19-282147-8
14602:Physical Review D
14460:Weyl, H. (1922).
14368:on 24 August 2016
14235:978-3-642-02779-6
14080:978-0-393-31276-8
13833:Inside Relativity
13603:978-1-107-60217-5
13519:978-0-521-87622-3
13489:978-0-7506-2768-9
13464:978-1-5423-2351-2
13415:978-1-118-93329-9
13388:978-0-674-02611-7
13329:978-0-7637-0460-5
13295:978-0-387-95210-9
13097:978-0-19-886202-4
12958:(9â10): 631â690.
12804:978-0-7432-6473-0
12520:978-3-7643-7435-8
12379:on 15 April 2017.
12294:978-1-4675-7992-6
12245:10.1119/1.1371254
12198:Scherr, Rachel E.
12097:Wolfram Mathworld
12077:978-0-9573894-6-5
12043:978-0-486-42540-5
11996:Fock, V. (1966).
11912:978-1-4398-6432-6
11786:KĂźndig experiment
11744:hyperbolic metric
11727:hyperboloid model
11640:in the limit for
11591:Annals of Physics
11441:Complex spacetime
11094:{\displaystyle p}
11066:{\displaystyle q}
11046:{\displaystyle p}
11023:{\displaystyle p}
11003:{\displaystyle p}
10983:{\displaystyle p}
10960:{\displaystyle c}
10901:coordinate charts
10845:{\displaystyle g}
10679:Riemannian metric
10665:is the branch of
10637:supertranslations
10549:Such being said,
9426:traveling at the
9218:they take place (
9188:Conservation laws
9089:
9056:or alternatively,
8981:
8847:
8735:
8690:
8689:
8620:at low velocity:
8585:
8531:
8476:
8457:relativistic mass
8393:approaches zero,
8305:is well-defined.
8198:A consequence of
8175:Momentum of light
7901:
7820:
7670:
7669:
7490:{\displaystyle w}
7337:
7242:
6728:
6705:
6701:
6161:
5981:
5879:
5654:
5653:
5626:
5625:
5535:
5279:
5278:
5271:
5125:
4009:
3956:(the reading of W
3937:
3891:
3767:
3753:
3752:running clock Wâ˛.
3517:(1+2)-dimensional
3505:{\displaystyle c}
3477:{\displaystyle c}
3337:(1+1)-dimensional
3323:
3322:
3315:
3243:
3204:
2897:Ⲡ= 0,
2825:axis by an angle
2709:
2708:
2701:
2635:{\displaystyle c}
2467:metric signatures
2232:{\displaystyle s}
2079:{\displaystyle x}
1611:{\displaystyle t}
855:Hermann Minkowski
775:Hermann Minkowski
704:. As a theory of
660:Fizeau experiment
530:Fizeau experiment
517:{\displaystyle c}
396:Non-relativistic
365:Hermann Minkowski
295:
294:
154:Classical gravity
16:(Redirected from
17968:
17911:
17910:
17909:
17899:
17898:
17887:
17886:
17885:
17875:
17874:
17863:
17862:
17854:
17838:
17837:
17621:van Stockum dust
17393:Two-body problem
17311:Mach's principle
17258:
17257:
17199:Terrell rotation
17039:
17038:
17017:
17010:
17003:
16994:
16993:
16691:Dominical letter
16622:Equation of time
16585:Marine sandglass
16426:
16420:
16398:Terrestrial Time
16255:Time measurement
16248:
16241:
16234:
16225:
16224:
16211:
16210:
16201:
16200:
16118:Glottochronology
15958:
15957:
15874:Human experience
15734:B-theory of time
15332:
15331:
15276:
15269:
15262:
15253:
15252:
15046:Other dimensions
15040:
15008:Projective space
14972:
14965:
14958:
14949:
14948:
14910:
14896:
14894:
14892:
14874:
14855:Wheeler, John A.
14848:
14800:Einstein, Albert
14775:
14752:(1st ed.).
14744:Tipler, Frank J.
14726:
14725:
14723:
14721:
14707:
14701:
14700:
14674:
14650:
14644:
14643:
14617:
14593:
14587:
14586:
14584:
14582:
14553:
14535:
14523:
14512:
14511:
14471:
14465:
14458:
14452:
14446:
14411:
14405:
14404:
14402:
14400:
14384:
14378:
14377:
14375:
14373:
14367:
14361:. Archived from
14352:
14334:
14322:
14316:
14315:
14281:
14261:
14255:
14254:
14252:
14250:
14245:on 15 April 2017
14244:
14238:. Archived from
14223:
14214:
14201:
14196:
14190:
14189:
14184:
14172:
14163:
14162:
14145:(6): 2851â2864.
14134:
14128:
14127:
14091:
14085:
14084:
14066:
14057:
14056:
14028:
14022:
14021:
13993:
13987:
13986:
13984:
13982:
13934:
13928:
13927:
13901:
13881:
13875:
13874:
13872:
13870:
13854:
13848:
13847:
13827:
13816:
13815:
13803:
13793:
13787:
13777:
13751:
13739:
13733:
13732:
13730:
13728:
13705:
13694:
13693:
13691:
13689:
13669:
13663:
13662:
13660:
13658:
13642:
13636:
13635:
13633:
13621:
13615:
13614:
13612:
13610:
13587:
13581:
13580:
13570:
13530:
13524:
13523:
13503:
13494:
13493:
13475:
13469:
13468:
13450:
13427:
13426:
13424:
13422:
13399:
13393:
13392:
13380:
13370:
13341:
13340:
13338:
13336:
13313:
13307:
13306:
13304:
13302:
13285:Basic Relativity
13279:
13273:
13272:
13270:
13268:
13251:Weiss, Michael.
13248:
13229:
13228:
13210:
13204:
13203:
13201:
13199:
13182:Savitt, Steven.
13179:
13170:
13169:
13167:
13165:
13145:
13139:
13138:
13120:
13114:
13111:
13105:
13101:
13081:
13075:
13074:
13056:
13041:
13040:
13034:
13026:
13000:
12994:
12993:
12967:
12947:
12941:
12939:
12937:
12935:
12911:
12902:
12901:
12899:
12897:
12877:
12868:
12867:
12856:10.2307/27757388
12839:
12833:
12832:
12830:
12818:
12809:
12808:
12796:
12786:
12780:
12779:
12777:
12775:
12765:
12733:
12727:
12726:
12724:
12722:
12702:
12693:
12692:
12675:
12669:
12668:
12666:
12664:
12646:
12606:
12600:
12599:
12575:
12564:
12563:
12545:
12539:
12538:
12537:
12535:
12529:
12488:
12479:
12473:
12472:
12452:
12441:
12440:
12438:
12436:
12417:
12411:
12410:
12408:
12406:
12387:
12381:
12380:
12378:
12372:. Archived from
12357:
12348:
12342:
12341:
12339:
12337:
12317:
12311:
12310:
12308:
12306:
12278:
12272:
12271:
12269:
12267:
12261:
12230:
12206:
12194:
12188:
12187:
12185:
12183:
12160:
12149:
12148:
12122:
12113:
12112:
12110:
12108:
12088:
12082:
12081:
12063:
12048:
12047:
12027:
12021:
12020:
12018:
12016:
11993:
11987:
11986:
11984:
11982:
11950:
11917:
11916:
11898:
11892:
11891:
11889:
11887:
11867:
11846:
11821:
11805:
11799:
11795:
11789:
11782:
11776:
11763:
11757:
11753:
11747:
11736:
11730:
11723:hyperbolic space
11707:
11701:
11649:, i.e. as group
11648:
11604:
11598:
11587:
11581:
11557:
11551:
11544:
11538:
11530:
11524:
11502:
11412:
11397:
11390:
11379:
11372:
11357:
11327:electromagnetism
11312:
11310:
11309:
11304:
11221:
11214:
11187:
11144:
11142:
11141:
11136:
11100:
11098:
11097:
11092:
11072:
11070:
11069:
11064:
11052:
11050:
11049:
11044:
11029:
11027:
11026:
11021:
11009:
11007:
11006:
11001:
10989:
10987:
10986:
10981:
10966:
10964:
10963:
10958:
10946:
10944:
10943:
10938:
10893:
10892:
10886:
10884:
10883:
10878:
10851:
10849:
10848:
10843:
10828:
10826:
10825:
10820:
10776:Curved manifolds
10724:
10717:Bernhard Riemann
10699:length of curves
10675:smooth manifolds
10571:bimetric gravity
10524:Technical topics
10486:
10464:
10362:
10355:
10353:
10351:
10350:
10345:
10331:
10330:
10308:
10306:
10305:
10298:
10295:
10294:
10285:
10283:
10282:
10275:
10274:
10265:
10264:
10263:
10256:
10255:
10244:
10224:
10210:
10197:
10195:
10193:
10192:
10187:
10182:
10181:
10180:
10170:
10165:
10148:
10125:
10124:
10106:
10104:
10102:
10101:
10096:
10082:
10065:
10063:
10061:
10060:
10055:
10029:
10027:
10025:
10024:
10019:
10017:
10016:
10004:
10003:
9979:
9969:
9967:
9965:
9964:
9959:
9942:
9925:
9923:
9921:
9920:
9915:
9901:
9865:
9841:
9817:
9815:
9813:
9812:
9807:
9805:
9804:
9792:
9791:
9762:
9760:
9758:
9757:
9752:
9750:
9749:
9748:
9729:
9727:
9725:
9724:
9719:
9717:
9716:
9715:
9693:add up to total
9692:
9690:
9688:
9687:
9682:
9677:
9672:
9671:
9653:
9651:
9649:
9648:
9643:
9638:
9633:
9632:
9611:
9609:
9607:
9606:
9601:
9599:
9598:
9597:
9585:
9584:
9559:
9557:
9556:
9551:
9549:
9545:
9544:
9543:
9531:
9530:
9516:
9511:
9507:
9506:
9505:
9504:
9494:
9493:
9481:
9480:
9479:
9469:
9468:
9451:
9450:
9449:
9425:
9423:
9421:
9420:
9415:
9413:
9412:
9400:
9399:
9375:
9373:
9371:
9370:
9365:
9363:
9362:
9357:
9351:
9350:
9338:
9337:
9332:
9317:
9315:
9313:
9312:
9307:
9305:
9304:
9299:
9293:
9292:
9280:
9279:
9274:
9194:Conservation law
9181:
9179:
9178:
9173:
9155:
9153:
9152:
9147:
9142:
9141:
9129:
9128:
9116:
9115:
9091:
9090:
9082:
9055:
9053:
9052:
9047:
9042:
9041:
9029:
9028:
9016:
9015:
9000:
8983:
8982:
8974:
8965:
8920:
8918:
8916:
8915:
8910:
8874:
8872:
8871:
8866:
8864:
8863:
8853:
8848:
8845:
8836:
8835:
8826:
8825:
8813:
8812:
8768:
8766:
8765:
8760:
8749:
8748:
8736:
8728:
8723:
8722:
8701:
8699:
8698:
8693:
8691:
8688:
8687:
8672:
8671:
8670:
8669:
8656:
8651:
8650:
8619:
8609:
8607:
8605:
8604:
8599:
8597:
8596:
8587:
8586:
8583:
8562:
8560:
8558:
8557:
8552:
8547:
8533:
8532:
8529:
8499:
8497:
8495:
8494:
8489:
8478:
8477:
8474:
8441:
8439:
8437:
8436:
8431:
8396:
8392:
8366:
8364:
8362:
8361:
8356:
8330:
8329:
8277:
8275:
8273:
8272:
8267:
8256:
8239:
8237:
8235:
8234:
8229:
8218:
8200:Maxwell's theory
8159:
8157:
8155:
8154:
8149:
8129:
8128:
8110:
8108:
8106:
8105:
8100:
8086:
8085:
8051:
8044:
8042:
8040:
8039:
8034:
7996:
7935:
7933:
7932:
7927:
7912:
7910:
7909:
7904:
7902:
7900:
7899:
7884:
7882:
7868:
7863:
7831:
7829:
7828:
7823:
7821:
7819:
7818:
7803:
7801:
7796:
7782:
7754:
7695:
7693:
7692:
7687:
7682:
7681:
7671:
7668:
7657:
7646:
7645:
7623:
7621:
7620:
7615:
7595:
7556:
7554:
7553:
7548:
7543:
7519:
7517:
7516:
7511:
7496:
7494:
7493:
7488:
7476:
7474:
7473:
7468:
7441:
7439:
7438:
7433:
7431:
7430:
7418:
7417:
7358:
7356:
7355:
7350:
7348:
7347:
7338:
7336:
7335:
7334:
7315:
7240:
7233:
7222:
7208:
7193:
7186:
7171:
7164:
7145:
7138:
7118:
7116:
7115:
7110:
7108:
7091:
7066:
7064:
7063:
7058:
7056:
7039:
6995:
6993:
6978:
6976:
6962:
6959:
6948:
6932:
6930:
6916:
6884:
6851:
6839:
6817:
6810:
6803:
6789:
6787:
6780:
6726:
6724:
6718:
6716:
6714:
6713:
6708:
6706:
6703:
6699:
6692:
6688:
6687:
6686:
6677:
6649:
6648:
6630:
6623:
6621:
6611:
6609:
6594:
6582:
6568:between events.
6555:
6553:
6552:
6547:
6515:
6498:
6496:
6495:
6490:
6482:
6481:
6472:
6440:
6422:
6420:
6419:
6414:
6388:
6374:
6372:
6371:
6366:
6358:
6357:
6348:
6322:
6274:
6272:
6271:
6266:
6264:
6260:
6238:
6216:
6212:
6211:
6197:
6167:
6163:
6162:
6160:
6159:
6150:
6149:
6137:
6132:
6089:
6087:
6086:
6081:
6079:
6065:
6043:
6031:
6027:
5999:
5987:
5983:
5982:
5980:
5979:
5970:
5962:
5939:
5890:
5888:
5887:
5882:
5880:
5872:
5864:
5863:
5833:
5744:
5743:
5742:
5741:
5696:
5694:
5693:
5688:
5665:
5663:
5662:
5657:
5655:
5652:
5651:
5636:
5632:
5627:
5624:
5623:
5614:
5609:
5608:
5593:
5589:
5571:
5569:
5568:
5563:
5549:
5547:
5546:
5541:
5536:
5534:
5533:
5524:
5519:
5518:
5503:
5501:
5446:
5445:
5444:
5443:
5398:
5396:
5395:
5390:
5369:
5367:
5366:
5361:
5340:
5338:
5337:
5332:
5321:
5274:
5267:
5263:
5260:
5254:
5231:
5223:
5196:is set equal to
5195:
5181:
5166:
5155:
5139:
5137:
5136:
5131:
5126:
5124:
5120:
5119:
5110:
5105:
5084:
5083:
5068:
5036:
5028:
5016:
5008:
4996:
4995:
4979:
4958:
4929:
4890:
4883:
4874:
4863:
4855:
4830:
4828:
4827:
4822:
4817:
4763:
4761:
4760:
4755:
4744:
4723:
4721:
4720:
4715:
4701:
4683:
4682:
4675:
4668:
4661:. This leads to
4660:
4659:
4642:
4627:
4618:
4610:
4609:
4597:
4588:
4580:
4566:
4536:
4534:
4533:
4528:
4517:
4501:
4499:
4498:
4493:
4485:
4469:
4467:
4466:
4461:
4453:
4437:
4435:
4434:
4429:
4412:
4394:
4392:
4384:
4377:
4361:
4359:
4352:
4345:
4338:
4329:
4309:
4307:
4300:
4293:
4286:
4271:
4112: >
4056:is the vertical
4004: <
3940:
3894:
3865:
3854:
3794:
3783:
3761:
3719:
3653:hyperbolic angle
3618:
3576:
3574:
3564:
3562:
3552:
3550:
3527:Fig. 2-7a.
3518:
3511:
3509:
3508:
3503:
3483:
3481:
3480:
3475:
3440:
3438:
3437:
3432:
3430:
3429:
3410:
3408:
3407:
3402:
3397:
3396:
3381:
3380:
3368:
3367:
3338:
3318:
3311:
3307:
3304:
3298:
3275:
3267:
3257:
3255:
3254:
3249:
3244:
3242:
3241:
3232:
3218:
3216:
3215:
3210:
3205:
3203:
3202:
3190:
3169:
3165:
3155:
3151:
3140:
3133:
3113:
3017:spatial distance
2880:
2878:
2877:
2872:
2864:
2729:reference frames
2704:
2697:
2693:
2690:
2684:
2661:
2653:
2649:Reference frames
2641:
2639:
2638:
2633:
2606:
2604:
2603:
2598:
2567:
2565:
2564:
2559:
2557:
2556:
2536:
2534:
2533:
2528:
2526:
2525:
2509:
2507:
2506:
2501:
2499:
2498:
2475:
2471:
2460:
2458:
2457:
2452:
2450:
2449:
2437:
2436:
2424:
2423:
2411:
2410:
2386:
2385:
2363:
2361:
2360:
2355:
2353:
2352:
2340:
2339:
2327:
2326:
2314:
2313:
2292:
2291:
2266:
2264:
2263:
2258:
2256:
2255:
2238:
2236:
2235:
2230:
2218:
2216:
2215:
2210:
2205:
2204:
2188:
2186:
2185:
2180:
2178:
2177:
2161:
2159:
2158:
2153:
2151:
2150:
2110:
2108:
2107:
2102:
2100:
2085:
2083:
2082:
2077:
2062:
2060:
2059:
2054:
2052:
2031:
2029:
2028:
2023:
2021:
2020:
2019:
2000:
1999:
1980:
1978:
1977:
1972:
1951:
1949:
1948:
1943:
1935:
1908:
1906:
1905:
1900:
1898:
1880:
1878:
1877:
1872:
1867:
1856:
1845:
1834:
1813:
1811:
1810:
1805:
1800:
1799:
1784:
1783:
1768:
1767:
1752:
1751:
1739:
1738:
1726:
1725:
1700:
1698:
1697:
1692:
1671:
1669:
1668:
1663:
1647:
1645:
1644:
1639:
1637:
1636:
1617:
1615:
1614:
1609:
1597:
1595:
1594:
1589:
1571:
1569:
1568:
1563:
1558:
1557:
1536:
1535:
1514:
1513:
1492:
1491:
1467:
1466:
1435:
1433:
1432:
1427:
1422:
1421:
1400:
1399:
1375:
1374:
1347:-coordinate is:
1346:
1344:
1343:
1338:
1323:
1321:
1320:
1315:
1301:
1284:in space and by
1283:
1281:
1280:
1275:
1273:
1258:
1256:
1255:
1250:
1248:
1247:
1238:
1220:
1218:
1217:
1212:
1194:
1192:
1191:
1186:
1124:
1122:
1121:
1116:
1114:
1113:
1104:
1090:
1089:
1080:
1066:
1065:
1056:
1042:
1041:
1032:
1007:
1005:
1004:
999:
997:
974:Causal structure
771:
757:
741:
727:
664:Hippolyte Fizeau
627:
616:
523:
521:
520:
515:
481:four-dimensional
323:four-dimensional
287:
280:
273:
259:
254:
253:
246:
242:
241:
211:Curved spacetime
64:
45:
44:
21:
17976:
17975:
17971:
17970:
17969:
17967:
17966:
17965:
17956:Time in physics
17921:
17920:
17917:
17907:
17905:
17893:
17883:
17881:
17869:
17857:
17849:
17847:
17842:
17828:
17656:
17560:BKL singularity
17550:LemaĂŽtreâTolman
17525:
17521:Quantum gravity
17503:
17497:
17483:geodetic effect
17457:(together with
17427:LISA Pathfinder
17366:
17315:
17301:Penrose diagram
17283:
17277:
17252:
17241:
17237:Minkowski space
17203:
17147:
17131:
17079:
17073:
17033:
17026:
17021:
16991:
16986:
16923:
16814:
16781:
16755:
16636:
16536:
16487:Coordinate time
16459:Time in physics
16453:
16427:
16421:
16412:
16284:
16261:
16252:
16222:
16217:
16189:
16180:Time immemorial
16127:
16084:
16045:Coordinate time
16016:
15970:Geological time
15946:
15929:Time management
15892:Generation time
15876:
15868:
15813:
15795:
15715:
15674:
15652:
15540:
15458:
15375:
15368:
15324:
15316:
15285:
15280:
15250:
15245:
15234:
15213:
15149:
15087:
15041:
15032:
14998:Euclidean space
14981:
14976:
14934:Expert articles
14903:
14890:
14888:
14871:
14853:Taylor, E. F.;
14849:Chapters 17â18.
14845:
14779:George F. Ellis
14764:
14740:Barrow, John D.
14735:
14733:Further reading
14730:
14729:
14719:
14717:
14709:
14708:
14704:
14651:
14647:
14594:
14590:
14580:
14578:
14533:
14524:
14515:
14472:
14468:
14459:
14455:
14415:Ehrenfest, Paul
14412:
14408:
14398:
14396:
14385:
14381:
14371:
14369:
14365:
14350:10.1.1.404.7853
14332:
14323:
14319:
14262:
14258:
14248:
14246:
14242:
14236:
14221:
14215:
14204:
14197:
14193:
14173:
14166:
14139:Physical Review
14135:
14131:
14102:(1336): 21â52.
14092:
14088:
14081:
14067:
14060:
14033:Physics Letters
14029:
14025:
13998:Physical Review
13994:
13990:
13980:
13978:
13935:
13931:
13882:
13878:
13868:
13866:
13855:
13851:
13844:
13828:
13819:
13812:
13794:
13790:
13769:
13743:
13740:
13736:
13726:
13724:
13722:
13706:
13697:
13687:
13685:
13670:
13666:
13656:
13654:
13643:
13639:
13631:physics/9807044
13622:
13618:
13608:
13606:
13604:
13588:
13584:
13531:
13527:
13520:
13504:
13497:
13490:
13476:
13472:
13465:
13451:
13430:
13420:
13418:
13416:
13400:
13396:
13389:
13371:
13344:
13334:
13332:
13330:
13314:
13310:
13300:
13298:
13296:
13280:
13276:
13266:
13264:
13249:
13232:
13225:
13211:
13207:
13197:
13195:
13180:
13173:
13163:
13161:
13146:
13142:
13135:
13121:
13117:
13112:
13108:
13098:
13082:
13078:
13071:
13057:
13044:
13028:
13027:
13023:
13001:
12997:
12948:
12944:
12933:
12931:
12912:
12905:
12895:
12893:
12882:"Raum und Zeit"
12878:
12871:
12840:
12836:
12819:
12812:
12805:
12787:
12783:
12773:
12771:
12748:(10): 891â921.
12734:
12730:
12720:
12718:
12703:
12696:
12690:
12676:
12672:
12662:
12660:
12607:
12603:
12596:
12576:
12567:
12560:
12546:
12542:
12533:
12531:
12527:
12521:
12486:
12480:
12476:
12469:
12453:
12444:
12434:
12432:
12419:
12418:
12414:
12404:
12402:
12389:
12388:
12384:
12376:
12370:
12355:
12349:
12345:
12335:
12333:
12318:
12314:
12304:
12302:
12295:
12279:
12275:
12265:
12263:
12259:
12228:physics/0207109
12204:
12195:
12191:
12181:
12179:
12177:
12161:
12152:
12145:
12123:
12116:
12106:
12104:
12091:Rowland, Todd.
12089:
12085:
12078:
12064:
12051:
12044:
12028:
12024:
12014:
12012:
12010:
11994:
11990:
11980:
11978:
11971:
11951:
11920:
11913:
11899:
11895:
11885:
11883:
11868:
11864:
11859:
11854:
11849:
11816:
11806:
11802:
11796:
11792:
11783:
11779:
11764:
11760:
11754:
11750:
11740:Cartesian plane
11737:
11733:
11708:
11704:
11692:
11683:
11674:
11665:
11656:
11641:
11638:
11626:
11615:
11605:
11601:
11588:
11584:
11558:
11554:
11545:
11541:
11531:
11527:
11507:from the Latin
11503:
11499:
11495:
11490:
11431:
11426:
11425:
11410:
11392:
11385:
11374:
11367:
11352:
11289:
11286:
11285:
11216:
11209:
11177:
11169:
11161:
11106:
11103:
11102:
11086:
11083:
11082:
11058:
11055:
11054:
11038:
11035:
11034:
11015:
11012:
11011:
10995:
10992:
10991:
10975:
10972:
10971:
10967:is equal to 1.
10952:
10949:
10948:
10908:
10905:
10904:
10890:
10889:
10860:
10857:
10856:
10837:
10834:
10833:
10802:
10799:
10798:
10792:
10780:Main articles:
10778:
10771:
10770:
10659:
10651:
10618:addressed this
10616:Rainer K. Sachs
10589:
10583:
10560:more convenient
10540:more convenient
10535:conventionalist
10531:
10526:
10521:
10520:
10510:
10500:
10491:reason why the
10481:
10475:
10470:
10459:
10453:
10451:
10441:
10384:reference frame
10379:
10369:
10364:
10360:
10326:
10322:
10320:
10317:
10316:
10314:
10304:
10301:
10300:
10299:
10296:
10293:
10291:
10290:
10289:
10287:
10281:
10279:
10278:
10277:
10273:
10271:
10270:
10269:
10267:
10262:
10260:
10259:
10258:
10254:
10252:
10251:
10250:
10249:
10242:
10232:
10231:
10230:
10229:
10228:
10225:
10216:
10215:
10214:
10211:
10176:
10172:
10171:
10166:
10158:
10144:
10120:
10116:
10114:
10111:
10110:
10108:
10075:
10073:
10070:
10069:
10067:
10040:
10037:
10036:
10034:
10012:
10008:
9999:
9995:
9987:
9984:
9983:
9981:
9974:
9935:
9933:
9930:
9929:
9927:
9926:, the momentum
9894:
9892:
9889:
9888:
9886:
9883:
9870:
9869:
9868:
9867:
9866:
9858:
9857:
9851:
9845:
9842:
9831:
9800:
9796:
9787:
9783:
9775:
9772:
9771:
9769:
9763:add up to form
9744:
9740:
9739:
9737:
9734:
9733:
9731:
9711:
9707:
9706:
9704:
9701:
9700:
9698:
9673:
9667:
9663:
9661:
9658:
9657:
9655:
9634:
9628:
9624:
9622:
9619:
9618:
9616:
9593:
9589:
9580:
9576:
9569:
9567:
9564:
9563:
9561:
9539:
9535:
9526:
9522:
9521:
9517:
9512:
9500:
9496:
9495:
9489:
9485:
9475:
9471:
9470:
9464:
9460:
9459:
9455:
9442:
9438:
9437:
9435:
9432:
9431:
9408:
9404:
9395:
9391:
9383:
9380:
9379:
9377:
9358:
9353:
9352:
9346:
9342:
9333:
9328:
9327:
9325:
9322:
9321:
9319:
9300:
9295:
9294:
9288:
9284:
9275:
9270:
9269:
9267:
9264:
9263:
9261:
9232:
9196:
9190:
9161:
9158:
9157:
9137:
9133:
9124:
9120:
9111:
9107:
9081:
9080:
9063:
9060:
9059:
9037:
9033:
9024:
9020:
9011:
9007:
8996:
8973:
8972:
8961:
8947:
8944:
8943:
8927:
8892:
8889:
8888:
8886:
8884:
8859:
8855:
8849:
8844:
8831:
8827:
8821:
8817:
8808:
8804:
8802:
8799:
8798:
8781:
8744:
8740:
8727:
8718:
8714:
8706:
8703:
8702:
8683:
8679:
8665:
8661:
8657:
8655:
8646:
8642:
8628:
8625:
8624:
8615:
8592:
8588:
8582:
8578:
8570:
8567:
8566:
8564:
8543:
8528:
8524:
8510:
8507:
8506:
8504:
8473:
8469:
8467:
8464:
8463:
8461:
8404:
8401:
8400:
8398:
8394:
8380:
8373:
8325:
8321:
8319:
8316:
8315:
8313:
8252:
8247:
8244:
8243:
8241:
8240:. Rearranging,
8214:
8209:
8206:
8205:
8203:
8177:
8124:
8120:
8118:
8115:
8114:
8112:
8081:
8077:
8066:
8063:
8062:
8060:
8046:
8016:
8013:
8012:
8010:
7983:
7976:Linear momentum
7963:
7958:
7946:Main articles:
7944:
7921:
7918:
7917:
7895:
7891:
7883:
7875:
7864:
7856:
7848:
7845:
7844:
7840:with frequency
7814:
7810:
7802:
7797:
7789:
7775:
7767:
7764:
7763:
7752:
7739:
7702:
7677:
7673:
7658:
7647:
7644:
7636:
7633:
7632:
7588:
7562:
7559:
7558:
7536:
7525:
7522:
7521:
7502:
7499:
7498:
7482:
7479:
7478:
7459:
7456:
7455:
7426:
7422:
7413:
7409:
7392:
7389:
7388:
7374:
7367:
7343:
7339:
7330:
7326:
7319:
7314:
7306:
7303:
7302:
7292:
7285:
7277:
7260:
7252:Main articles:
7250:
7235:
7228:
7217:
7191:
7184:
7178:
7169:
7162:
7143:
7136:
7101:
7084:
7073:
7070:
7069:
7049:
7032:
7021:
7018:
7017:
6991:
6980:
6974:
6967:
6957:
6950:
6936:
6928:
6921:
6888:
6872:
6849:
6837:
6815:
6808:
6804:. To determine
6791:
6785:
6778:
6773:
6741:
6735:
6722:
6720:
6702:
6682:
6678:
6673:
6660:
6656:
6644:
6640:
6638:
6635:
6634:
6632:
6625:
6619:
6617:
6607:
6599:
6580:
6508:
6503:
6500:
6499:
6477:
6473:
6468:
6433:
6428:
6425:
6424:
6381:
6379:
6376:
6375:
6353:
6349:
6344:
6315:
6313:
6310:
6309:
6262:
6261:
6253:
6246:
6240:
6239:
6231:
6224:
6218:
6217:
6204:
6190:
6189:
6185:
6175:
6169:
6168:
6155:
6151:
6142:
6138:
6136:
6125:
6124:
6120:
6110:
6103:
6101:
6098:
6097:
6077:
6076:
6066:
6058:
6055:
6054:
6044:
6036:
6033:
6032:
6014:
6010:
6000:
5992:
5989:
5988:
5975:
5971:
5963:
5961:
5954:
5950:
5940:
5932:
5928:
5926:
5923:
5922:
5909:
5901:Main articles:
5899:
5871:
5859:
5855:
5829:
5821:
5818:
5817:
5773:) = (
5733:
5731:
5726:
5725:
5682:
5679:
5678:
5647:
5643:
5631:
5619:
5615:
5610:
5604:
5600:
5588:
5580:
5577:
5576:
5557:
5554:
5553:
5529:
5525:
5520:
5514:
5510:
5502:
5497:
5480:
5477:
5476:
5435:
5433:
5428:
5427:
5378:
5375:
5374:
5346:
5343:
5342:
5317:
5315:
5312:
5311:
5289:
5281:Main articles:
5275:
5264:
5258:
5255:
5244:
5232:
5221:
5193:
5179:
5164:
5153:
5115:
5111:
5106:
5098:
5085:
5076:
5069:
5067:
5059:
5056:
5055:
5026:
5018:
5006:
4998:
4993:
4981:
4963:
4938:
4904:
4888:
4872:
4861:
4857:
4835:
4813:
4802:
4799:
4798:
4783:
4777:
4737:
4729:
4726:
4725:
4694:
4692:
4689:
4688:
4684:and ultimately
4680:
4673:
4666:
4662:
4657:
4644:
4629:
4616:
4612:
4607:
4599:
4586:
4582:
4572:
4564:
4510:
4508:
4505:
4504:
4478:
4476:
4473:
4472:
4446:
4444:
4441:
4440:
4405:
4403:
4400:
4399:
4390:
4386:
4379:
4363:
4357:
4350:
4343:
4336:
4331:
4311:
4305:
4298:
4291:
4284:
4279:
4253:
4249:
4243:
4236:
4227:
4133:
4127:of the object.
4063:
4055:
4037:is longer than
3971:
3967:
3959:
3950:
3931:
3927:
3918:is taken to be
3917:
3904:
3899:is taken to be
3898:
3881:
3877:
3863:
3804:
3803:
3802:
3801:
3797:
3796:
3795:
3786:
3785:
3784:
3735:
3731:
3727:
3723:
3710:
3706:
3676:
3671:
3665:
3616:
3572:
3570:
3560:
3558:
3548:
3546:
3535:
3516:
3497:
3494:
3493:
3469:
3466:
3465:
3425:
3421:
3419:
3416:
3415:
3392:
3388:
3376:
3372:
3363:
3359:
3348:
3345:
3344:
3336:
3319:
3308:
3302:
3299:
3288:
3276:
3265:
3237:
3233:
3231:
3229:
3226:
3225:
3198:
3194:
3189:
3187:
3184:
3183:
3180:proper distance
3167:
3157:
3153:
3142:
3135:
3131:
3108:
3099:reference frame
3077:
3021:timelike future
2971:
2965:
2951:Cartesian plane
2901:Ⲡ= â
2860:
2837:
2834:
2833:
2705:
2694:
2688:
2685:
2674:
2662:
2651:
2627:
2624:
2623:
2577:
2574:
2573:
2552:
2548:
2546:
2543:
2542:
2521:
2517:
2515:
2512:
2511:
2494:
2490:
2488:
2485:
2484:
2473:
2469:
2445:
2441:
2432:
2428:
2419:
2415:
2406:
2402:
2381:
2377:
2375:
2372:
2371:
2348:
2344:
2335:
2331:
2322:
2318:
2309:
2305:
2287:
2283:
2281:
2278:
2277:
2251:
2247:
2245:
2242:
2241:
2224:
2221:
2220:
2200:
2196:
2194:
2191:
2190:
2173:
2169:
2167:
2164:
2163:
2146:
2142:
2131:
2128:
2127:
2096:
2091:
2088:
2087:
2071:
2068:
2067:
2045:
2037:
2034:
2033:
2015:
2011:
2007:
1995:
1991:
1986:
1983:
1982:
1957:
1954:
1953:
1928:
1914:
1911:
1910:
1891:
1886:
1883:
1882:
1860:
1849:
1838:
1827:
1822:
1819:
1818:
1795:
1791:
1779:
1775:
1763:
1759:
1747:
1743:
1734:
1730:
1721:
1717:
1712:
1709:
1708:
1677:
1674:
1673:
1654:
1651:
1650:
1632:
1628:
1623:
1620:
1619:
1603:
1600:
1599:
1580:
1577:
1576:
1553:
1549:
1531:
1527:
1509:
1505:
1487:
1483:
1462:
1458:
1447:
1444:
1443:
1417:
1413:
1395:
1391:
1370:
1366:
1355:
1352:
1351:
1329:
1326:
1325:
1294:
1289:
1286:
1285:
1269:
1264:
1261:
1260:
1243:
1239:
1234:
1226:
1223:
1222:
1200:
1197:
1196:
1177:
1174:
1173:
1109:
1105:
1100:
1085:
1081:
1076:
1061:
1057:
1052:
1037:
1033:
1028:
1020:
1017:
1016:
993:
988:
985:
984:
976:
970:
963:
957:
920:discussed below
824:Albert Einstein
786:
785:
784:
783:
779:
778:
777:
772:
764:
763:
761:Albert Einstein
758:
749:
748:
747:
742:
734:
733:
731:Hendrik Lorentz
728:
694:Hendrik Lorentz
671:aether-dragging
636:
635:
634:
633:
632:
628:
619:
618:
617:
606:
598:Main articles:
594:
509:
506:
505:
394:
387:
377:mass and energy
369:Minkowski space
313:that fuses the
291:
262:
249:
236:
235:
227:
226:
225:
180:
172:
171:
170:
155:
147:
146:
145:
125:
117:
116:
115:
111:Minkowski space
90:
82:
43:
28:
23:
22:
15:
12:
11:
5:
17974:
17964:
17963:
17958:
17953:
17948:
17943:
17938:
17933:
17916:
17915:
17903:
17891:
17879:
17867:
17844:
17843:
17833:
17830:
17829:
17827:
17826:
17819:
17814:
17809:
17804:
17799:
17794:
17789:
17784:
17779:
17774:
17769:
17764:
17759:
17754:
17749:
17747:Choquet-Bruhat
17744:
17739:
17734:
17729:
17724:
17719:
17714:
17709:
17704:
17699:
17694:
17689:
17684:
17679:
17674:
17668:
17666:
17662:
17661:
17658:
17657:
17655:
17654:
17647:
17646:
17641:
17636:
17629:
17628:
17623:
17618:
17613:
17608:
17599:Axisymmetric:
17596:
17595:
17590:
17584:
17573:
17572:
17567:
17562:
17557:
17552:
17547:
17538:Cosmological:
17535:
17533:
17527:
17526:
17524:
17523:
17518:
17513:
17507:
17505:
17499:
17498:
17496:
17495:
17490:
17479:frame-dragging
17476:
17471:
17466:
17463:Einstein rings
17459:Einstein cross
17452:
17441:
17440:
17435:
17429:
17424:
17419:
17406:
17396:
17395:
17390:
17385:
17380:
17374:
17372:
17368:
17367:
17365:
17364:
17362:Ernst equation
17359:
17354:
17349:
17344:
17339:
17334:
17332:BSSN formalism
17329:
17323:
17321:
17317:
17316:
17314:
17313:
17308:
17303:
17298:
17293:
17287:
17285:
17279:
17278:
17276:
17275:
17270:
17264:
17262:
17255:
17247:
17246:
17243:
17242:
17240:
17239:
17234:
17229:
17224:
17219:
17213:
17211:
17205:
17204:
17202:
17201:
17196:
17191:
17189:Ladder paradox
17186:
17181:
17176:
17171:
17166:
17161:
17155:
17153:
17149:
17148:
17146:
17145:
17139:
17137:
17133:
17132:
17130:
17129:
17124:
17119:
17114:
17109:
17104:
17099:
17094:
17092:Speed of light
17089:
17083:
17081:
17075:
17074:
17072:
17071:
17066:
17061:
17055:
17045:
17043:
17036:
17028:
17027:
17020:
17019:
17012:
17005:
16997:
16988:
16987:
16985:
16984:
16979:
16974:
16972:Time metrology
16969:
16964:
16959:
16954:
16949:
16948:
16947:
16937:
16931:
16929:
16928:Related topics
16925:
16924:
16922:
16921:
16916:
16911:
16906:
16901:
16896:
16891:
16886:
16881:
16876:
16871:
16866:
16861:
16856:
16851:
16846:
16841:
16836:
16831:
16825:
16823:
16816:
16815:
16813:
16812:
16807:
16802:
16797:
16791:
16789:
16783:
16782:
16780:
16779:
16774:
16769:
16763:
16761:
16757:
16756:
16754:
16753:
16748:
16743:
16738:
16733:
16728:
16723:
16718:
16713:
16708:
16703:
16698:
16693:
16688:
16683:
16678:
16673:
16667:
16662:
16657:
16652:
16646:
16644:
16638:
16637:
16635:
16634:
16629:
16624:
16619:
16617:Dialing scales
16614:
16609:
16604:
16603:
16602:
16592:
16587:
16582:
16577:
16572:
16567:
16562:
16557:
16552:
16546:
16544:
16538:
16537:
16535:
16534:
16529:
16524:
16519:
16514:
16509:
16504:
16499:
16494:
16489:
16484:
16479:
16474:
16469:
16463:
16461:
16455:
16454:
16452:
16451:
16449:Prime meridian
16446:
16441:
16439:Ephemeris time
16435:
16433:
16429:
16428:
16415:
16413:
16411:
16410:
16408:180th meridian
16405:
16400:
16395:
16390:
16385:
16380:
16375:
16370:
16365:
16360:
16355:
16350:
16345:
16340:
16335:
16330:
16325:
16320:
16315:
16310:
16305:
16304:
16303:
16292:
16290:
16286:
16285:
16283:
16282:
16277:
16272:
16266:
16263:
16262:
16251:
16250:
16243:
16236:
16228:
16219:
16218:
16216:
16215:
16205:
16194:
16191:
16190:
16188:
16187:
16182:
16177:
16172:
16165:
16160:
16155:
16150:
16145:
16139:
16137:
16133:
16132:
16129:
16128:
16126:
16125:
16123:Time geography
16120:
16115:
16113:Clock reaction
16110:
16109:
16108:
16098:
16092:
16090:
16086:
16085:
16083:
16082:
16077:
16072:
16067:
16062:
16057:
16052:
16047:
16042:
16037:
16032:
16026:
16024:
16018:
16017:
16015:
16014:
16009:
16004:
16003:
16002:
15997:
15992:
15987:
15982:
15977:
15966:
15964:
15955:
15948:
15947:
15945:
15944:
15931:
15926:
15921:
15916:
15915:
15914:
15912:time signature
15909:
15899:
15894:
15889:
15883:
15881:
15870:
15869:
15867:
15866:
15865:
15864:
15854:
15853:
15852:
15842:
15837:
15832:
15827:
15822:
15816:
15814:
15812:
15811:
15806:
15800:
15797:
15796:
15794:
15793:
15786:
15784:Temporal parts
15781:
15776:
15771:
15766:
15761:
15756:
15754:Eternal return
15751:
15746:
15741:
15739:Chronocentrism
15736:
15731:
15725:
15723:
15717:
15716:
15714:
15713:
15708:
15703:
15698:
15693:
15688:
15683:
15677:
15675:
15673:
15672:
15667:
15661:
15658:
15657:
15654:
15653:
15651:
15650:
15649:
15648:
15634:
15629:
15624:
15619:
15618:
15617:
15612:
15611:
15610:
15605:
15595:
15590:
15585:
15580:
15579:
15578:
15568:
15567:
15566:
15550:
15548:
15542:
15541:
15539:
15538:
15531:
15526:
15524:Hindu Panchang
15521:
15516:
15511:
15506:
15501:
15496:
15491:
15490:
15489:
15484:
15479:
15468:
15466:
15460:
15459:
15457:
15456:
15451:
15446:
15441:
15436:
15431:
15426:
15421:
15416:
15411:
15406:
15401:
15396:
15391:
15386:
15380:
15378:
15370:
15369:
15367:
15366:
15361:
15356:
15351:
15346:
15340:
15338:
15329:
15318:
15317:
15315:
15314:
15309:
15304:
15299:
15293:
15291:
15287:
15286:
15279:
15278:
15271:
15264:
15256:
15247:
15246:
15239:
15236:
15235:
15233:
15232:
15227:
15221:
15219:
15215:
15214:
15212:
15211:
15203:
15198:
15193:
15188:
15183:
15178:
15173:
15168:
15163:
15157:
15155:
15151:
15150:
15148:
15147:
15142:
15137:
15135:Cross-polytope
15132:
15127:
15122:
15120:Hyperrectangle
15117:
15112:
15107:
15101:
15099:
15089:
15088:
15086:
15085:
15080:
15075:
15070:
15065:
15060:
15055:
15049:
15047:
15043:
15042:
15035:
15033:
15031:
15030:
15025:
15020:
15015:
15010:
15005:
15000:
14995:
14989:
14987:
14983:
14982:
14975:
14974:
14967:
14960:
14952:
14946:
14945:
14935:
14926:
14916:
14902:
14901:External links
14899:
14898:
14897:
14875:
14869:
14850:
14843:
14829:Penrose, Roger
14825:
14815:
14796:Lorentz, H. A.
14793:
14776:
14762:
14734:
14731:
14728:
14727:
14702:
14645:
14608:(4): L041501.
14588:
14544:(4): L69âL75.
14529:(April 1997).
14513:
14486:(3): 636â651.
14466:
14453:
14429:(5): 440â446.
14406:
14379:
14343:(2): 227â252.
14326:Skow, Bradford
14317:
14272:(4): L69âL75.
14256:
14234:
14202:
14191:
14164:
14129:
14086:
14079:
14058:
14039:(4): 357â359.
14023:
14004:(2): 147â150.
13988:
13949:(3): 379â396.
13929:
13876:
13857:Murzi, Mauro.
13849:
13842:
13817:
13810:
13788:
13734:
13720:
13695:
13664:
13637:
13616:
13602:
13582:
13525:
13518:
13495:
13488:
13470:
13463:
13428:
13414:
13394:
13387:
13342:
13328:
13308:
13294:
13274:
13230:
13223:
13205:
13171:
13140:
13133:
13115:
13106:
13096:
13076:
13069:
13042:
13021:
12995:
12942:
12903:
12869:
12834:
12810:
12803:
12781:
12728:
12717:on 28 May 2024
12694:
12688:
12670:
12601:
12594:
12565:
12558:
12540:
12519:
12474:
12467:
12442:
12425:NobelPrize.org
12412:
12382:
12368:
12343:
12326:Universe Today
12312:
12293:
12273:
12189:
12175:
12150:
12143:
12114:
12083:
12076:
12049:
12042:
12022:
12008:
11988:
11969:
11918:
11911:
11893:
11861:
11860:
11858:
11855:
11853:
11850:
11848:
11847:
11800:
11790:
11777:
11758:
11748:
11731:
11715:Laguerre group
11702:
11690:
11681:
11672:
11663:
11654:
11636:
11624:
11613:
11599:
11582:
11565:Solvay Debates
11552:
11539:
11525:
11496:
11494:
11491:
11489:
11488:
11486:Time geography
11483:
11478:
11473:
11468:
11463:
11458:
11453:
11448:
11443:
11438:
11432:
11430:
11427:
11415:dimensionality
11405:from an ideal
11302:
11299:
11296:
11293:
11266:Paul Ehrenfest
11259:John D. Barrow
11176:Properties of
11170:
11162:
11160:
11157:
11134:
11131:
11128:
11125:
11122:
11119:
11116:
11113:
11110:
11090:
11062:
11042:
11019:
10999:
10979:
10956:
10936:
10933:
10930:
10927:
10924:
10921:
10918:
10915:
10912:
10876:
10873:
10870:
10867:
10864:
10841:
10831:Lorentz metric
10818:
10815:
10812:
10809:
10806:
10777:
10774:
10660:
10652:
10650:
10647:
10597:PoincarĂŠ group
10585:Main article:
10582:
10579:
10566:
10565:
10564:
10563:
10556:
10533:In PoincarĂŠ's
10530:
10527:
10525:
10522:
10513:
10512:
10508:
10498:
10479:
10468:
10457:
10425:
10424:
10380:
10372:
10368:
10365:
10343:
10340:
10337:
10334:
10329:
10325:
10310:
10309:
10302:
10292:
10280:
10272:
10261:
10253:
10237:
10226:
10219:
10218:
10217:
10212:
10205:
10204:
10203:
10202:
10201:
10185:
10179:
10175:
10169:
10164:
10161:
10157:
10154:
10151:
10147:
10143:
10140:
10137:
10134:
10131:
10128:
10123:
10119:
10094:
10091:
10088:
10085:
10081:
10078:
10053:
10050:
10047:
10044:
10015:
10011:
10007:
10002:
9998:
9994:
9991:
9978: = 0
9957:
9954:
9951:
9948:
9945:
9941:
9938:
9913:
9910:
9907:
9904:
9900:
9897:
9882:
9879:
9860:
9859:
9843:
9836:
9835:
9834:
9833:
9832:
9830:
9827:
9803:
9799:
9795:
9790:
9786:
9782:
9779:
9747:
9743:
9714:
9710:
9680:
9676:
9670:
9666:
9641:
9637:
9631:
9627:
9612:is conserved.
9596:
9592:
9588:
9583:
9579:
9575:
9572:
9548:
9542:
9538:
9534:
9529:
9525:
9520:
9515:
9510:
9503:
9499:
9492:
9488:
9484:
9478:
9474:
9467:
9463:
9458:
9454:
9448:
9445:
9441:
9428:center of mass
9411:
9407:
9403:
9398:
9394:
9390:
9387:
9361:
9356:
9349:
9345:
9341:
9336:
9331:
9303:
9298:
9291:
9287:
9283:
9278:
9273:
9254:
9253:
9250:
9231:
9230:Total momentum
9228:
9192:Main article:
9189:
9186:
9183:
9182:
9171:
9168:
9165:
9145:
9140:
9136:
9132:
9127:
9123:
9119:
9114:
9110:
9106:
9103:
9100:
9097:
9094:
9088:
9085:
9079:
9076:
9073:
9070:
9067:
9057:
9045:
9040:
9036:
9032:
9027:
9023:
9019:
9014:
9010:
9006:
9003:
8999:
8995:
8992:
8989:
8986:
8980:
8977:
8971:
8968:
8964:
8960:
8957:
8954:
8951:
8926:
8923:
8908:
8905:
8902:
8899:
8896:
8882:
8876:
8875:
8862:
8858:
8852:
8843:
8839:
8834:
8830:
8824:
8820:
8816:
8811:
8807:
8792:invariant mass
8779:
8770:
8769:
8758:
8755:
8752:
8747:
8743:
8739:
8734:
8731:
8726:
8721:
8717:
8713:
8710:
8686:
8682:
8678:
8675:
8668:
8664:
8660:
8654:
8649:
8645:
8641:
8638:
8635:
8632:
8612:
8611:
8595:
8591:
8581:
8577:
8574:
8550:
8546:
8542:
8539:
8536:
8527:
8523:
8520:
8517:
8514:
8501:
8487:
8484:
8481:
8472:
8429:
8426:
8423:
8420:
8417:
8414:
8411:
8408:
8372:
8369:
8354:
8351:
8348:
8345:
8342:
8339:
8336:
8333:
8328:
8324:
8265:
8262:
8259:
8255:
8251:
8227:
8224:
8221:
8217:
8213:
8193:speed of light
8176:
8173:
8147:
8144:
8141:
8138:
8135:
8132:
8127:
8123:
8098:
8095:
8092:
8089:
8084:
8080:
8076:
8073:
8070:
8050: = 0
8032:
8029:
8026:
8023:
8020:
7962:
7959:
7943:
7940:
7925:
7914:
7913:
7898:
7894:
7890:
7887:
7881:
7878:
7874:
7871:
7867:
7862:
7859:
7855:
7852:
7833:
7832:
7817:
7813:
7809:
7806:
7800:
7795:
7792:
7788:
7785:
7781:
7778:
7774:
7771:
7738:
7737:
7734:
7727:
7726:
7719:
7715:
7701:
7698:
7697:
7696:
7685:
7680:
7676:
7667:
7664:
7661:
7656:
7653:
7650:
7643:
7640:
7613:
7610:
7607:
7604:
7601:
7598:
7594:
7591:
7587:
7584:
7581:
7578:
7575:
7572:
7569:
7566:
7546:
7542:
7539:
7535:
7532:
7529:
7509:
7506:
7486:
7466:
7463:
7443:
7442:
7429:
7425:
7421:
7416:
7412:
7408:
7405:
7402:
7399:
7396:
7372:
7365:
7360:
7359:
7346:
7342:
7333:
7329:
7325:
7322:
7318:
7313:
7310:
7290:
7283:
7276:
7273:
7264:Doppler effect
7254:Doppler effect
7249:
7248:Doppler effect
7246:
7177:
7174:
7122:
7121:
7120:
7119:
7107:
7104:
7100:
7097:
7094:
7090:
7087:
7083:
7080:
7077:
7067:
7055:
7052:
7048:
7045:
7042:
7038:
7035:
7031:
7028:
7025:
6996:
6964:
6933:
6918:
6885:
6857:
6737:Main article:
6734:
6731:
6698:
6695:
6691:
6685:
6681:
6676:
6672:
6669:
6666:
6663:
6659:
6655:
6652:
6647:
6643:
6545:
6542:
6539:
6536:
6533:
6530:
6527:
6524:
6521:
6518:
6514:
6511:
6507:
6488:
6485:
6480:
6476:
6471:
6467:
6464:
6461:
6458:
6455:
6452:
6449:
6446:
6443:
6439:
6436:
6432:
6412:
6409:
6406:
6403:
6400:
6397:
6394:
6391:
6387:
6384:
6364:
6361:
6356:
6352:
6347:
6343:
6340:
6337:
6334:
6331:
6328:
6325:
6321:
6318:
6276:
6275:
6259:
6256:
6252:
6249:
6247:
6245:
6242:
6241:
6237:
6234:
6230:
6227:
6225:
6223:
6220:
6219:
6215:
6210:
6207:
6203:
6200:
6196:
6193:
6188:
6184:
6181:
6178:
6176:
6174:
6171:
6170:
6166:
6158:
6154:
6148:
6145:
6141:
6135:
6131:
6128:
6123:
6119:
6116:
6113:
6111:
6109:
6106:
6105:
6091:
6090:
6075:
6072:
6069:
6067:
6064:
6061:
6057:
6056:
6053:
6050:
6047:
6045:
6042:
6039:
6035:
6034:
6030:
6026:
6023:
6020:
6017:
6013:
6009:
6006:
6003:
6001:
5998:
5995:
5991:
5990:
5986:
5978:
5974:
5969:
5966:
5960:
5957:
5953:
5949:
5946:
5943:
5941:
5938:
5935:
5931:
5930:
5898:
5895:
5892:
5891:
5878:
5875:
5870:
5867:
5862:
5858:
5854:
5851:
5848:
5845:
5842:
5839:
5836:
5832:
5828:
5825:
5801: = (
5785: = (
5686:
5667:
5666:
5650:
5646:
5642:
5639:
5635:
5630:
5622:
5618:
5613:
5607:
5603:
5599:
5596:
5592:
5587:
5584:
5561:
5539:
5532:
5528:
5523:
5517:
5513:
5509:
5506:
5500:
5496:
5493:
5490:
5487:
5484:
5400:
5399:
5388:
5385:
5382:
5371:
5359:
5356:
5353:
5350:
5330:
5327:
5324:
5320:
5277:
5276:
5235:
5233:
5226:
5220:
5217:
5214:
5213:
5187:
5143:
5142:
5141:
5140:
5129:
5123:
5118:
5114:
5109:
5104:
5101:
5097:
5094:
5091:
5088:
5082:
5079:
5075:
5072:
5066:
5063:
5038:
4960:
4931:
4832:
4831:
4820:
4816:
4812:
4809:
4806:
4779:Main article:
4776:
4773:
4765:
4764:
4753:
4750:
4747:
4743:
4740:
4736:
4733:
4713:
4710:
4707:
4704:
4700:
4697:
4538:
4537:
4526:
4523:
4520:
4516:
4513:
4502:
4491:
4488:
4484:
4481:
4470:
4459:
4456:
4452:
4449:
4438:
4427:
4424:
4421:
4418:
4415:
4411:
4408:
4247:Galilean group
4245:Main article:
4242:
4239:
4235:
4232:
4226:
4223:
4189:Figs. 2-6
4132:
4129:
4061:
4053:
4011:
4010:
3969:
3965:
3957:
3948:
3938:
3929:
3922:
3915:
3902:
3896:
3892:
3879:
3875:
3799:
3798:
3789:
3788:
3787:
3778:
3777:
3776:
3775:
3774:
3769:
3768:
3755:
3754:
3733:
3729:
3725:
3721:
3708:
3704:
3675:
3672:
3667:Main article:
3664:
3661:
3534:
3531:
3501:
3473:
3428:
3424:
3412:
3411:
3400:
3395:
3391:
3387:
3384:
3379:
3375:
3371:
3366:
3362:
3358:
3355:
3352:
3321:
3320:
3279:
3277:
3270:
3264:
3261:
3247:
3240:
3236:
3208:
3201:
3197:
3193:
3076:
3073:
3060:null separated
2967:Main article:
2964:
2961:
2917:Ⲡ=
2882:
2881:
2870:
2867:
2863:
2859:
2856:
2853:
2850:
2847:
2844:
2841:
2779:
2778:
2767:
2756:
2707:
2706:
2665:
2663:
2656:
2650:
2647:
2631:
2596:
2593:
2590:
2587:
2584:
2581:
2555:
2551:
2524:
2520:
2497:
2493:
2481:
2480:
2477:
2463:
2462:
2461:
2448:
2444:
2440:
2435:
2431:
2427:
2422:
2418:
2414:
2409:
2405:
2401:
2398:
2395:
2392:
2389:
2384:
2380:
2366:
2365:
2364:
2351:
2347:
2343:
2338:
2334:
2330:
2325:
2321:
2317:
2312:
2308:
2304:
2301:
2298:
2295:
2290:
2286:
2254:
2250:
2228:
2208:
2203:
2199:
2176:
2172:
2149:
2145:
2141:
2138:
2135:
2099:
2095:
2075:
2051:
2048:
2044:
2041:
2018:
2014:
2010:
2006:
2003:
1998:
1994:
1990:
1970:
1967:
1964:
1961:
1941:
1938:
1934:
1931:
1927:
1924:
1921:
1918:
1897:
1894:
1890:
1870:
1866:
1863:
1859:
1855:
1852:
1848:
1844:
1841:
1837:
1833:
1830:
1826:
1815:
1814:
1803:
1798:
1794:
1790:
1787:
1782:
1778:
1774:
1771:
1766:
1762:
1758:
1755:
1750:
1746:
1742:
1737:
1733:
1729:
1724:
1720:
1716:
1690:
1687:
1684:
1681:
1661:
1658:
1635:
1631:
1627:
1607:
1587:
1584:
1573:
1572:
1561:
1556:
1552:
1548:
1545:
1542:
1539:
1534:
1530:
1526:
1523:
1520:
1517:
1512:
1508:
1504:
1501:
1498:
1495:
1490:
1486:
1482:
1479:
1476:
1473:
1470:
1465:
1461:
1457:
1454:
1451:
1437:
1436:
1425:
1420:
1416:
1412:
1409:
1406:
1403:
1398:
1394:
1390:
1387:
1384:
1381:
1378:
1373:
1369:
1365:
1362:
1359:
1336:
1333:
1313:
1310:
1307:
1304:
1300:
1297:
1293:
1272:
1268:
1246:
1242:
1237:
1233:
1230:
1210:
1207:
1204:
1184:
1181:
1126:
1125:
1112:
1108:
1103:
1099:
1096:
1093:
1088:
1084:
1079:
1075:
1072:
1069:
1064:
1060:
1055:
1051:
1048:
1045:
1040:
1036:
1031:
1027:
1024:
996:
992:
969:
966:
956:
953:
912:Space and Time
908:Space and Time
900:Space and Time
789:Henri PoincarĂŠ
781:
780:
773:
766:
765:
759:
752:
751:
750:
745:Henri PoincarĂŠ
743:
736:
735:
729:
722:
721:
720:
719:
718:
675:simultaneously
629:
622:
621:
620:
611:
610:
609:
608:
607:
593:
590:
568:data reduction
526:speed-of-light
513:
393:
390:
386:
383:
344:events occur.
321:into a single
293:
292:
290:
289:
282:
275:
267:
264:
263:
261:
260:
247:
232:
229:
228:
224:
223:
218:
213:
208:
203:
198:
193:
188:
182:
181:
178:
177:
174:
173:
169:
168:
163:
157:
156:
153:
152:
149:
148:
144:
143:
138:
133:
127:
126:
123:
122:
119:
118:
114:
113:
108:
103:
98:
92:
91:
88:
87:
84:
83:
81:
80:
75:
69:
66:
65:
57:
56:
50:
49:
26:
18:Spatiotemporal
9:
6:
4:
3:
2:
17973:
17962:
17959:
17957:
17954:
17952:
17949:
17947:
17944:
17942:
17939:
17937:
17934:
17932:
17929:
17928:
17926:
17919:
17914:
17904:
17902:
17897:
17892:
17890:
17880:
17878:
17873:
17868:
17866:
17861:
17856:
17855:
17852:
17841:
17831:
17825:
17824:
17820:
17818:
17815:
17813:
17810:
17808:
17805:
17803:
17800:
17798:
17795:
17793:
17790:
17788:
17785:
17783:
17780:
17778:
17775:
17773:
17770:
17768:
17765:
17763:
17760:
17758:
17755:
17753:
17750:
17748:
17745:
17743:
17740:
17738:
17735:
17733:
17732:Chandrasekhar
17730:
17728:
17725:
17723:
17720:
17718:
17715:
17713:
17710:
17708:
17705:
17703:
17700:
17698:
17695:
17693:
17692:Schwarzschild
17690:
17688:
17685:
17683:
17680:
17678:
17675:
17673:
17670:
17669:
17667:
17663:
17653:
17649:
17648:
17645:
17642:
17640:
17637:
17635:
17631:
17630:
17627:
17624:
17622:
17619:
17617:
17614:
17612:
17609:
17606:
17602:
17598:
17597:
17594:
17591:
17588:
17585:
17583:
17579:
17578:Schwarzschild
17575:
17574:
17571:
17568:
17566:
17563:
17561:
17558:
17556:
17553:
17551:
17548:
17545:
17541:
17537:
17536:
17534:
17532:
17528:
17522:
17519:
17517:
17514:
17512:
17509:
17508:
17506:
17500:
17494:
17491:
17488:
17484:
17480:
17477:
17475:
17474:Shapiro delay
17472:
17470:
17467:
17464:
17460:
17456:
17453:
17450:
17446:
17443:
17442:
17439:
17436:
17433:
17430:
17428:
17425:
17423:
17420:
17418:
17417:collaboration
17414:
17410:
17407:
17405:
17401:
17398:
17397:
17394:
17391:
17389:
17386:
17384:
17383:Event horizon
17381:
17379:
17376:
17375:
17373:
17369:
17363:
17360:
17358:
17355:
17353:
17350:
17348:
17345:
17343:
17340:
17338:
17335:
17333:
17330:
17328:
17327:ADM formalism
17325:
17324:
17322:
17318:
17312:
17309:
17307:
17304:
17302:
17299:
17297:
17294:
17292:
17289:
17288:
17286:
17280:
17274:
17271:
17269:
17266:
17265:
17263:
17259:
17256:
17254:
17248:
17238:
17235:
17233:
17232:Biquaternions
17230:
17228:
17225:
17223:
17220:
17218:
17215:
17214:
17212:
17210:
17206:
17200:
17197:
17195:
17192:
17190:
17187:
17185:
17182:
17180:
17177:
17175:
17172:
17170:
17167:
17165:
17162:
17160:
17159:Time dilation
17157:
17156:
17154:
17150:
17144:
17141:
17140:
17138:
17134:
17128:
17125:
17123:
17120:
17118:
17115:
17113:
17112:Proper length
17110:
17108:
17105:
17103:
17100:
17098:
17095:
17093:
17090:
17088:
17085:
17084:
17082:
17076:
17070:
17067:
17065:
17062:
17059:
17056:
17054:
17050:
17047:
17046:
17044:
17040:
17037:
17035:
17029:
17025:
17018:
17013:
17011:
17006:
17004:
16999:
16998:
16995:
16983:
16980:
16978:
16975:
16973:
16970:
16968:
16965:
16963:
16960:
16958:
16955:
16953:
16950:
16946:
16943:
16942:
16941:
16938:
16936:
16933:
16932:
16930:
16926:
16920:
16917:
16915:
16912:
16910:
16907:
16905:
16902:
16900:
16897:
16895:
16892:
16890:
16887:
16885:
16882:
16880:
16877:
16875:
16872:
16870:
16867:
16865:
16862:
16860:
16857:
16855:
16852:
16850:
16847:
16845:
16842:
16840:
16837:
16835:
16832:
16830:
16827:
16826:
16824:
16822:
16821:units of time
16817:
16811:
16810:Sidereal time
16808:
16806:
16803:
16801:
16798:
16796:
16795:Galactic year
16793:
16792:
16790:
16788:
16784:
16778:
16775:
16773:
16770:
16768:
16765:
16764:
16762:
16758:
16752:
16751:Weekday names
16749:
16747:
16744:
16742:
16741:Tropical year
16739:
16737:
16734:
16732:
16729:
16727:
16724:
16722:
16719:
16717:
16714:
16712:
16709:
16707:
16706:Intercalation
16704:
16702:
16699:
16697:
16694:
16692:
16689:
16687:
16684:
16682:
16679:
16677:
16674:
16672:(lunar Hijri)
16671:
16668:
16666:
16663:
16661:
16658:
16656:
16653:
16651:
16648:
16647:
16645:
16643:
16639:
16633:
16630:
16628:
16625:
16623:
16620:
16618:
16615:
16613:
16610:
16608:
16605:
16601:
16598:
16597:
16596:
16593:
16591:
16588:
16586:
16583:
16581:
16578:
16576:
16573:
16571:
16568:
16566:
16563:
16561:
16558:
16556:
16553:
16551:
16548:
16547:
16545:
16543:
16539:
16533:
16530:
16528:
16525:
16523:
16520:
16518:
16515:
16513:
16512:Time dilation
16510:
16508:
16505:
16503:
16500:
16498:
16495:
16493:
16490:
16488:
16485:
16483:
16480:
16478:
16475:
16473:
16470:
16468:
16465:
16464:
16462:
16460:
16456:
16450:
16447:
16445:
16442:
16440:
16437:
16436:
16434:
16430:
16425:
16419:
16409:
16406:
16404:
16401:
16399:
16396:
16394:
16391:
16389:
16386:
16384:
16381:
16379:
16376:
16374:
16371:
16369:
16366:
16364:
16361:
16359:
16356:
16354:
16351:
16349:
16348:24-hour clock
16346:
16344:
16343:12-hour clock
16341:
16339:
16336:
16334:
16331:
16329:
16326:
16324:
16321:
16319:
16316:
16314:
16311:
16309:
16306:
16302:
16299:
16298:
16297:
16294:
16293:
16291:
16287:
16281:
16278:
16276:
16273:
16271:
16268:
16267:
16264:
16260:
16256:
16249:
16244:
16242:
16237:
16235:
16230:
16229:
16226:
16214:
16206:
16204:
16196:
16195:
16192:
16186:
16183:
16181:
16178:
16176:
16173:
16171:
16170:
16166:
16164:
16161:
16159:
16156:
16154:
16151:
16149:
16146:
16144:
16141:
16140:
16138:
16134:
16124:
16121:
16119:
16116:
16114:
16111:
16107:
16104:
16103:
16102:
16101:Chronobiology
16099:
16097:
16094:
16093:
16091:
16087:
16081:
16078:
16076:
16073:
16071:
16068:
16066:
16063:
16061:
16058:
16056:
16053:
16051:
16048:
16046:
16043:
16041:
16038:
16036:
16035:Arrow of time
16033:
16031:
16028:
16027:
16025:
16023:
16019:
16013:
16010:
16008:
16007:Geochronology
16005:
16001:
15998:
15996:
15993:
15991:
15988:
15986:
15983:
15981:
15978:
15976:
15973:
15972:
15971:
15968:
15967:
15965:
15963:
15959:
15956:
15954:
15949:
15943:
15939:
15935:
15932:
15930:
15927:
15925:
15922:
15920:
15917:
15913:
15910:
15908:
15905:
15904:
15903:
15900:
15898:
15895:
15893:
15890:
15888:
15885:
15884:
15882:
15880:
15875:
15871:
15863:
15860:
15859:
15858:
15857:Wheel of time
15855:
15851:
15848:
15847:
15846:
15843:
15841:
15838:
15836:
15833:
15831:
15828:
15826:
15823:
15821:
15818:
15817:
15815:
15810:
15807:
15805:
15802:
15801:
15798:
15792:
15791:
15787:
15785:
15782:
15780:
15777:
15775:
15772:
15770:
15767:
15765:
15762:
15760:
15757:
15755:
15752:
15750:
15747:
15745:
15742:
15740:
15737:
15735:
15732:
15730:
15727:
15726:
15724:
15722:
15718:
15712:
15709:
15707:
15704:
15702:
15701:Periodization
15699:
15697:
15694:
15692:
15689:
15687:
15684:
15682:
15679:
15678:
15676:
15671:
15668:
15666:
15663:
15662:
15659:
15647:
15646:
15642:
15641:
15640:
15639:
15635:
15633:
15630:
15628:
15627:Digital clock
15625:
15623:
15620:
15616:
15613:
15609:
15606:
15604:
15601:
15600:
15599:
15596:
15594:
15591:
15589:
15586:
15584:
15581:
15577:
15574:
15573:
15572:
15569:
15565:
15562:
15561:
15560:
15557:
15556:
15555:
15552:
15551:
15549:
15547:
15543:
15537:
15536:
15532:
15530:
15527:
15525:
15522:
15520:
15517:
15515:
15512:
15510:
15507:
15505:
15502:
15500:
15497:
15495:
15492:
15488:
15485:
15483:
15480:
15478:
15475:
15474:
15473:
15470:
15469:
15467:
15465:
15461:
15455:
15452:
15450:
15447:
15445:
15442:
15440:
15437:
15435:
15432:
15430:
15427:
15425:
15422:
15420:
15417:
15415:
15412:
15410:
15407:
15405:
15404:Relative hour
15402:
15400:
15399:24-hour clock
15397:
15395:
15394:12-hour clock
15392:
15390:
15387:
15385:
15382:
15381:
15379:
15377:
15371:
15365:
15362:
15360:
15357:
15355:
15352:
15350:
15347:
15345:
15342:
15341:
15339:
15337:
15333:
15330:
15328:
15323:
15319:
15313:
15310:
15308:
15305:
15303:
15300:
15298:
15295:
15294:
15292:
15288:
15284:
15277:
15272:
15270:
15265:
15263:
15258:
15257:
15254:
15244:
15243:
15237:
15231:
15228:
15226:
15223:
15222:
15220:
15216:
15210:
15208:
15204:
15202:
15199:
15197:
15194:
15192:
15189:
15187:
15184:
15182:
15179:
15177:
15174:
15172:
15169:
15167:
15164:
15162:
15159:
15158:
15156:
15152:
15146:
15143:
15141:
15138:
15136:
15133:
15131:
15128:
15126:
15125:Demihypercube
15123:
15121:
15118:
15116:
15113:
15111:
15108:
15106:
15103:
15102:
15100:
15098:
15094:
15090:
15084:
15081:
15079:
15076:
15074:
15071:
15069:
15066:
15064:
15061:
15059:
15056:
15054:
15051:
15050:
15048:
15044:
15039:
15029:
15026:
15024:
15021:
15019:
15016:
15014:
15011:
15009:
15006:
15004:
15001:
14999:
14996:
14994:
14991:
14990:
14988:
14984:
14980:
14973:
14968:
14966:
14961:
14959:
14954:
14953:
14950:
14943:
14939:
14936:
14933:
14930:
14927:
14924:
14921:13th edition
14920:
14917:
14914:
14909:
14905:
14904:
14886:
14885:
14880:
14876:
14872:
14870:0-7167-2327-1
14866:
14862:
14861:
14856:
14851:
14846:
14844:0-679-45443-8
14840:
14836:
14835:
14830:
14826:
14823:
14819:
14816:
14813:
14809:
14808:Weyl, Hermann
14805:
14801:
14797:
14794:
14792:
14791:0-19-851164-7
14788:
14784:
14780:
14777:
14773:
14769:
14765:
14759:
14755:
14751:
14750:
14745:
14741:
14737:
14736:
14716:
14712:
14706:
14698:
14694:
14690:
14686:
14682:
14678:
14673:
14668:
14665:(1): 013217.
14664:
14660:
14656:
14649:
14641:
14637:
14633:
14629:
14625:
14621:
14616:
14611:
14607:
14603:
14599:
14592:
14577:
14573:
14569:
14565:
14561:
14557:
14552:
14551:gr-qc/9702052
14547:
14543:
14539:
14532:
14528:
14522:
14520:
14518:
14509:
14505:
14501:
14497:
14493:
14489:
14485:
14481:
14480:Nuovo Cimento
14477:
14470:
14463:
14457:
14450:
14444:
14440:
14436:
14432:
14428:
14424:
14420:
14416:
14410:
14394:
14390:
14383:
14364:
14360:
14356:
14351:
14346:
14342:
14338:
14331:
14327:
14321:
14313:
14309:
14305:
14301:
14297:
14293:
14289:
14285:
14280:
14279:gr-qc/9702052
14275:
14271:
14267:
14260:
14241:
14237:
14231:
14227:
14220:
14213:
14211:
14209:
14207:
14200:
14195:
14188:
14183:
14178:
14171:
14169:
14160:
14156:
14152:
14148:
14144:
14140:
14133:
14125:
14121:
14117:
14113:
14109:
14105:
14101:
14097:
14090:
14082:
14076:
14072:
14065:
14063:
14054:
14050:
14046:
14042:
14038:
14034:
14027:
14019:
14015:
14011:
14007:
14003:
13999:
13992:
13976:
13972:
13968:
13964:
13960:
13956:
13952:
13948:
13944:
13940:
13933:
13925:
13921:
13917:
13913:
13909:
13905:
13900:
13899:gr-qc/0411023
13895:
13891:
13887:
13880:
13864:
13860:
13853:
13845:
13843:0-691-08472-6
13839:
13835:
13834:
13826:
13824:
13822:
13813:
13811:0-486-60081-5
13807:
13802:
13801:
13792:
13786:in spacetime.
13785:
13781:
13776:
13772:
13767:
13763:
13759:
13755:
13750:
13746:
13738:
13723:
13721:0-7167-0336-X
13717:
13713:
13712:
13704:
13702:
13700:
13683:
13679:
13675:
13668:
13652:
13648:
13641:
13632:
13627:
13620:
13605:
13599:
13595:
13594:
13586:
13578:
13574:
13569:
13564:
13560:
13556:
13552:
13548:
13545:(1): 014107.
13544:
13540:
13536:
13529:
13521:
13515:
13511:
13510:
13502:
13500:
13491:
13485:
13481:
13474:
13466:
13460:
13456:
13449:
13447:
13445:
13443:
13441:
13439:
13437:
13435:
13433:
13417:
13411:
13407:
13406:
13398:
13390:
13384:
13379:
13378:
13369:
13367:
13365:
13363:
13361:
13359:
13357:
13355:
13353:
13351:
13349:
13347:
13331:
13325:
13321:
13320:
13312:
13297:
13291:
13287:
13286:
13278:
13262:
13258:
13254:
13247:
13245:
13243:
13241:
13239:
13237:
13235:
13226:
13224:0-521-27703-5
13220:
13216:
13209:
13193:
13189:
13185:
13178:
13176:
13159:
13155:
13151:
13144:
13136:
13134:9780593186589
13130:
13126:
13119:
13110:
13104:
13099:
13093:
13089:
13088:
13080:
13072:
13070:0-12-417561-9
13066:
13062:
13055:
13053:
13051:
13049:
13047:
13038:
13032:
13024:
13022:0-387-94348-X
13018:
13014:
13010:
13006:
12999:
12991:
12987:
12983:
12979:
12975:
12971:
12966:
12961:
12957:
12953:
12946:
12929:
12925:
12921:
12917:
12910:
12908:
12891:
12887:
12883:
12876:
12874:
12865:
12861:
12857:
12853:
12849:
12845:
12838:
12829:
12824:
12817:
12815:
12806:
12800:
12795:
12794:
12785:
12769:
12764:
12759:
12755:
12751:
12747:
12743:
12739:
12732:
12716:
12712:
12708:
12701:
12699:
12691:
12689:0-8126-9067-2
12685:
12681:
12674:
12658:
12654:
12650:
12645:
12640:
12636:
12632:
12628:
12624:
12620:
12616:
12612:
12605:
12597:
12595:0-393-02001-0
12591:
12587:
12583:
12582:
12574:
12572:
12570:
12561:
12559:0-387-94870-8
12555:
12551:
12544:
12526:
12522:
12516:
12512:
12508:
12504:
12500:
12496:
12492:
12485:
12478:
12470:
12468:0-19-853907-X
12464:
12460:
12459:
12451:
12449:
12447:
12430:
12426:
12422:
12416:
12400:
12396:
12392:
12386:
12375:
12371:
12369:0-8176-4380-X
12365:
12361:
12354:
12347:
12331:
12327:
12323:
12316:
12300:
12296:
12290:
12286:
12285:
12277:
12258:
12254:
12250:
12246:
12242:
12238:
12234:
12229:
12224:
12220:
12216:
12212:
12211:
12203:
12199:
12193:
12178:
12176:0-7167-0336-X
12172:
12168:
12167:
12159:
12157:
12155:
12146:
12144:0-7487-6422-4
12140:
12136:
12132:
12128:
12121:
12119:
12102:
12098:
12094:
12087:
12079:
12073:
12069:
12062:
12060:
12058:
12056:
12054:
12045:
12039:
12035:
12034:
12026:
12011:
12009:0-08-010061-9
12005:
12001:
12000:
11992:
11976:
11972:
11970:0-521-45506-5
11966:
11962:
11958:
11957:
11949:
11947:
11945:
11943:
11941:
11939:
11937:
11935:
11933:
11931:
11929:
11927:
11925:
11923:
11914:
11908:
11904:
11897:
11881:
11877:
11873:
11866:
11862:
11844:
11840:
11836:
11832:
11828:
11825:
11819:
11814:
11810:
11804:
11794:
11787:
11781:
11774:
11770:
11769:
11762:
11752:
11745:
11741:
11735:
11728:
11724:
11720:
11716:
11712:
11706:
11699:
11698:
11693:
11689:
11684:
11680:
11675:
11671:
11666:
11662:
11657:
11653:
11647:
11645:
11639:
11635:
11630:
11627:
11623:
11619:
11616:
11612:
11608:
11603:
11596:
11592:
11586:
11579:
11574:
11570:
11566:
11562:
11556:
11549:
11543:
11536:
11535:Henri Bergson
11529:
11522:
11518:
11514:
11510:
11506:
11501:
11497:
11487:
11484:
11482:
11479:
11477:
11474:
11472:
11469:
11467:
11464:
11462:
11459:
11457:
11454:
11452:
11449:
11447:
11444:
11442:
11439:
11437:
11434:
11433:
11422:
11420:
11416:
11408:
11407:monatomic gas
11404:
11399:
11395:
11388:
11383:
11377:
11370:
11365:
11361:
11355:
11350:
11346:
11342:
11338:
11337:or disperse.
11336:
11332:
11328:
11325:'s theory of
11324:
11321:claimed that
11320:
11316:
11300:
11297:
11294:
11291:
11283:
11279:
11275:
11271:
11267:
11262:
11260:
11256:
11252:
11251:Immanuel Kant
11248:
11244:
11241:, who in the
11240:
11235:
11233:
11229:
11225:
11224:string theory
11219:
11212:
11207:
11203:
11199:
11195:
11185:
11181:
11174:
11167:
11156:
11154:
11150:
11148:
11129:
11126:
11123:
11120:
11117:
11114:
11111:
11088:
11079:
11076:
11060:
11040:
11031:
11017:
10997:
10977:
10968:
10954:
10931:
10928:
10925:
10922:
10919:
10916:
10913:
10902:
10898:
10894:
10871:
10868:
10865:
10855:
10839:
10832:
10813:
10810:
10807:
10797:
10791:
10787:
10783:
10773:
10768:
10764:
10760:
10757:, as well as
10756:
10752:
10748:
10744:
10740:
10736:
10732:
10728:
10723:
10718:
10714:
10712:
10708:
10704:
10700:
10696:
10692:
10688:
10687:tangent space
10684:
10683:inner product
10680:
10676:
10673:, defined as
10672:
10669:that studies
10668:
10664:
10657:
10646:
10644:
10642:
10638:
10632:
10629:
10625:
10621:
10617:
10613:
10612:Hermann Bondi
10608:
10606:
10602:
10598:
10594:
10588:
10578:
10574:
10572:
10561:
10557:
10554:
10553:
10552:
10551:
10550:
10547:
10545:
10541:
10536:
10518:
10507:
10504:
10503:inertial mass
10497:
10494:
10490:
10489:a priori
10484:
10478:
10473:
10467:
10462:
10456:
10449:
10445:
10439:
10435:
10434:
10429:
10421:
10420:
10419:
10416:
10414:
10409:
10404:
10402:
10392:
10388:
10385:
10377:
10371:
10357:
10341:
10338:
10335:
10332:
10327:
10323:
10307:
10284:
10248:
10247:
10240:
10236:
10223:
10209:
10200:
10177:
10173:
10167:
10162:
10159:
10155:
10152:
10145:
10138:
10135:
10132:
10126:
10117:
10092:
10089:
10086:
10083:
10079:
10076:
10051:
10048:
10045:
10042:
10031:
10013:
10009:
10005:
10000:
9996:
9992:
9989:
9977:
9971:
9955:
9952:
9949:
9946:
9943:
9939:
9936:
9911:
9908:
9905:
9902:
9898:
9895:
9878:
9876:
9864:
9855:
9849:
9844:Figure 3-11.
9840:
9826:
9824:
9819:
9801:
9797:
9793:
9788:
9784:
9780:
9777:
9766:
9696:
9678:
9674:
9668:
9664:
9639:
9635:
9629:
9625:
9613:
9546:
9540:
9536:
9532:
9527:
9523:
9518:
9513:
9508:
9490:
9486:
9482:
9465:
9461:
9456:
9452:
9429:
9409:
9405:
9401:
9396:
9392:
9388:
9385:
9347:
9343:
9339:
9289:
9285:
9281:
9258:
9251:
9248:
9247:
9246:
9243:
9236:
9227:
9225:
9221:
9217:
9213:
9209:
9205:
9201:
9195:
9185:
9169:
9166:
9163:
9138:
9134:
9130:
9125:
9121:
9117:
9112:
9108:
9104:
9101:
9095:
9083:
9077:
9074:
9068:
9065:
9058:
9038:
9034:
9030:
9025:
9021:
9017:
9012:
9008:
9004:
9001:
8997:
8993:
8987:
8975:
8969:
8966:
8962:
8958:
8952:
8949:
8942:
8941:
8940:
8938:
8937:
8932:
8925:Four-momentum
8922:
8906:
8903:
8900:
8897:
8894:
8881:
8860:
8856:
8850:
8841:
8837:
8832:
8828:
8822:
8818:
8814:
8809:
8805:
8797:
8796:
8795:
8793:
8787:
8785:
8778:
8773:
8756:
8753:
8750:
8745:
8741:
8737:
8732:
8729:
8724:
8719:
8715:
8711:
8708:
8684:
8680:
8676:
8673:
8666:
8662:
8658:
8652:
8647:
8643:
8639:
8636:
8633:
8630:
8623:
8622:
8621:
8618:
8593:
8589:
8579:
8575:
8572:
8548:
8544:
8540:
8537:
8534:
8525:
8521:
8518:
8515:
8512:
8502:
8485:
8482:
8479:
8470:
8459:
8458:
8453:
8449:
8445:
8427:
8424:
8421:
8418:
8415:
8412:
8409:
8406:
8391:
8387:
8383:
8378:
8377:
8376:
8368:
8352:
8349:
8343:
8340:
8337:
8331:
8322:
8311:
8306:
8304:
8300:
8296:
8292:
8287:
8285:
8281:
8263:
8260:
8257:
8253:
8249:
8225:
8222:
8219:
8215:
8211:
8201:
8196:
8194:
8190:
8181:
8172:
8170:
8169:four-momentum
8165:
8163:
8145:
8142:
8139:
8136:
8133:
8130:
8121:
8096:
8093:
8090:
8087:
8074:
8071:
8057:
8055:
8049:
8027:
8024:
8021:
8006:
8004:
8003:closed system
8000:
7995:
7994:
7989: =
7988:
7987:
7981:
7977:
7967:
7957:
7953:
7949:
7948:Four-momentum
7939:
7937:
7923:
7896:
7892:
7888:
7885:
7879:
7876:
7872:
7869:
7865:
7860:
7857:
7853:
7850:
7843:
7842:
7841:
7839:
7815:
7811:
7807:
7804:
7798:
7793:
7790:
7786:
7783:
7779:
7776:
7772:
7769:
7762:
7761:
7760:
7758:
7751:
7747:
7742:
7735:
7732:
7731:
7730:
7724:
7720:
7717:
7716:
7714:
7706:
7683:
7678:
7674:
7665:
7662:
7659:
7654:
7651:
7648:
7641:
7638:
7631:
7630:
7629:
7627:
7611:
7605:
7602:
7599:
7592:
7589:
7585:
7582:
7579:
7576:
7573:
7570:
7567:
7564:
7544:
7540:
7537:
7533:
7530:
7527:
7507:
7504:
7484:
7464:
7461:
7447:
7427:
7423:
7414:
7410:
7406:
7403:
7397:
7394:
7387:
7386:
7385:
7383:
7379:
7375:
7368:
7344:
7340:
7331:
7327:
7323:
7320:
7316:
7311:
7308:
7301:
7300:
7299:
7297:
7293:
7286:
7272:
7270:
7265:
7259:
7255:
7245:
7243:
7238:
7231:
7226:
7220:
7215:
7211:
7206:
7203:
7201:
7197:
7190:
7183:
7173:
7168:
7161:
7157:
7153:
7149:
7142:
7135:
7131:
7127:
7105:
7102:
7098:
7095:
7092:
7088:
7085:
7081:
7078:
7075:
7068:
7053:
7050:
7046:
7043:
7040:
7036:
7033:
7029:
7026:
7023:
7016:
7015:
7013:
7009:
7005:
7001:
6997:
6994:
6987:
6984: =
6983:
6977:
6971: =
6970:
6965:
6961:
6954: =
6953:
6947:
6944: =
6943:
6939:
6934:
6931:
6925: =
6924:
6919:
6915:
6912: =
6911:
6907:
6903:
6899:
6896: =
6895:
6891:
6886:
6883:
6880: +
6879:
6876: =
6875:
6870:
6866:
6862:
6858:
6855:
6848:
6844:
6840:
6833:
6832:
6831:
6829:
6825:
6821:
6814:
6807:
6802:
6798:
6795: =
6794:
6784:
6777:
6771:
6767:
6761:
6759:
6754:
6745:
6740:
6730:
6696:
6693:
6689:
6683:
6679:
6674:
6670:
6667:
6664:
6661:
6657:
6653:
6650:
6641:
6628:
6615:
6606:
6602:
6597:
6592:
6590:
6586:
6579:
6575:
6569:
6567:
6563:
6559:
6540:
6534:
6531:
6528:
6519:
6516:
6512:
6509:
6486:
6478:
6474:
6469:
6465:
6459:
6456:
6453:
6444:
6441:
6437:
6434:
6407:
6404:
6401:
6398:
6392:
6389:
6385:
6382:
6362:
6354:
6350:
6345:
6341:
6338:
6335:
6332:
6326:
6323:
6319:
6316:
6307:
6305:
6301:
6297:
6293:
6289:
6285:
6282: âŞ
6281:
6257:
6254:
6250:
6248:
6243:
6235:
6232:
6228:
6226:
6221:
6213:
6208:
6205:
6201:
6198:
6194:
6191:
6186:
6182:
6179:
6177:
6172:
6164:
6156:
6152:
6146:
6143:
6139:
6133:
6129:
6126:
6121:
6117:
6114:
6112:
6107:
6096:
6095:
6094:
6073:
6070:
6068:
6062:
6059:
6051:
6048:
6046:
6040:
6037:
6028:
6024:
6021:
6018:
6015:
6011:
6007:
6004:
6002:
5996:
5993:
5984:
5976:
5972:
5967:
5964:
5958:
5955:
5951:
5947:
5944:
5942:
5936:
5933:
5921:
5920:
5919:
5916:
5913:
5908:
5907:Lorentz group
5904:
5894:
5876:
5873:
5868:
5860:
5856:
5852:
5849:
5843:
5840:
5837:
5834:
5830:
5826:
5823:
5816:
5815:
5814:
5812:
5808:
5805: â
5804:
5800:
5796:
5792:
5789: â
5788:
5784:
5780:
5776:
5772:
5768:
5764:
5760:
5757: =
5756:
5752:
5749: =
5748:
5740:
5736:
5729:
5723:
5719:
5715:
5711:
5706:
5704:
5700:
5684:
5676:
5672:
5648:
5644:
5640:
5637:
5633:
5628:
5620:
5616:
5611:
5605:
5601:
5597:
5594:
5590:
5585:
5582:
5575:
5574:
5573:
5559:
5550:
5537:
5530:
5526:
5521:
5515:
5511:
5507:
5504:
5498:
5494:
5491:
5488:
5485:
5482:
5474:
5470:
5467: =
5466:
5462:
5459: =
5458:
5454:
5451: =
5450:
5442:
5438:
5431:
5425:
5421:
5417:
5413:
5404:
5386:
5383:
5380:
5372:
5357:
5354:
5351:
5348:
5328:
5325:
5322:
5310:
5309:
5308:
5306:
5301:
5293:
5288:
5284:
5283:Time dilation
5273:
5270:
5262:
5252:
5248:
5242:
5241:
5236:This section
5234:
5230:
5225:
5224:
5216:
5211:
5207:
5204: =
5203:
5199:
5192:
5188:
5185:
5182: +
5178:
5175: =
5174:
5170:
5163:
5159:
5152:
5148:
5147:
5146:
5127:
5116:
5112:
5107:
5102:
5099:
5095:
5089:
5086:
5080:
5077:
5073:
5070:
5064:
5061:
5054:
5053:
5051:
5047:
5043:
5039:
5035:
5031:
5025:
5021:
5015:
5011:
5005:
5001:
4992:
4988:
4984:
4978:
4974:
4970:
4966:
4961:
4957:
4953:
4949:
4945:
4941:
4936:
4932:
4927:
4923:
4919:
4915:
4911:
4907:
4902:
4901:
4900:
4898:
4894:
4887:
4882:
4878:
4871:
4867:
4860:
4854:
4850:
4846:
4842:
4838:
4818:
4814:
4810:
4807:
4804:
4797:
4796:
4795:
4787:
4782:
4772:
4770:
4751:
4748:
4745:
4741:
4738:
4734:
4731:
4711:
4708:
4705:
4702:
4698:
4695:
4687:
4686:
4685:
4679:
4672:
4665:
4656:
4652:
4648:
4641:
4637:
4633:
4626:
4622:
4615:
4606:
4602:
4596:
4592:
4585:
4579:
4575:
4570:
4563:
4559:
4554:
4547:
4542:
4524:
4521:
4518:
4514:
4511:
4503:
4489:
4486:
4482:
4479:
4471:
4457:
4454:
4450:
4447:
4439:
4425:
4422:
4419:
4416:
4413:
4409:
4406:
4398:
4397:
4396:
4389:
4382:
4375:
4371:
4367:
4356:
4349:
4342:
4335:
4327:
4323:
4319:
4315:
4304:
4297:
4290:
4283:
4277:
4276:
4275:Fig. 1-1
4269:
4265:
4261:
4257:
4248:
4238:
4231:
4222:
4220:
4215:
4209:
4207:
4203:
4199:
4195:
4191:
4190:
4182:
4179:
4176:
4173:
4171:
4170:path integral
4161:
4157:
4153:
4151:
4146:
4142:
4137:
4128:
4126:
4122:
4117:
4115:
4111:
4107:
4103:
4099:
4095:
4091:
4087:
4083:
4079:
4075:
4072:â˛-coordinate
4071:
4067:
4059:
4051:
4047:
4042:
4040:
4036:
4032:
4028:
4024:
4020:
4016:
4007:
4003:
3999:
3995:
3991:
3987:
3983:
3979:
3975:
3963:
3960:) is labeled
3955:
3952:of the event
3951:
3944:
3939:
3935:
3932:in the event
3925:
3921:
3913:
3909:
3905:
3893:
3889:
3885:
3873:
3869:
3862:
3858:
3853:
3852:
3851:
3849:
3845:
3841:
3837:
3833:
3829:
3825:
3821:
3816:
3814:
3810:
3793:
3782:
3773:
3765:
3760:
3759:
3758:
3751:
3747:
3743:
3739:
3718:
3717:
3716:
3714:
3702:
3697:
3696:only apparent
3692:
3690:
3686:
3682:
3670:
3660:
3658:
3654:
3650:
3646:
3645:
3644:Fig. 2-9
3639:
3637:
3632:
3630:
3626:
3622:
3615:
3610:
3606:
3601:
3599:
3591:
3587:
3585:
3583:
3582:time dilation
3578:
3568:
3556:
3539:
3530:
3528:
3524:
3522:
3513:
3499:
3491:
3487:
3471:
3462:
3457:
3454:
3452:
3448:
3444:
3426:
3422:
3398:
3393:
3389:
3385:
3382:
3377:
3373:
3369:
3364:
3356:
3353:
3343:
3342:
3341:
3329:
3325:
3317:
3314:
3306:
3296:
3292:
3286:
3285:
3280:This section
3278:
3274:
3269:
3268:
3260:
3258:
3245:
3238:
3234:
3223:
3206:
3199:
3195:
3191:
3181:
3175:
3173:
3164:
3160:
3149:
3145:
3138:
3127:
3125:
3121:
3115:
3111:
3106:
3105:
3104:Fig. 2-4
3100:
3096:
3092:
3083:
3079:
3072:
3070:
3068:
3063:
3061:
3057:
3053:
3049:
3045:
3040:
3038:
3034:
3030:
3026:
3025:timelike past
3022:
3018:
3014:
3005:
3001:
2999:
2995:
2991:
2987:
2977:
2973:
2970:
2960:
2958:
2956:
2952:
2946:
2944:
2941:must also be
2940:
2936:
2932:
2928:
2922:
2920:
2916:
2912:
2908:
2904:
2900:
2896:
2891:
2887:
2868:
2865:
2861:
2857:
2854:
2848:
2842:
2839:
2832:
2831:
2830:
2828:
2824:
2820:
2816:
2812:
2808:
2804:
2800:
2796:
2792:
2788:
2784:
2776:
2772:
2768:
2765:
2761:
2757:
2754:
2750:
2746:
2742:
2741:
2740:
2738:
2734:
2730:
2721:
2713:
2703:
2700:
2692:
2682:
2678:
2672:
2671:
2666:This section
2664:
2660:
2655:
2654:
2646:
2644:
2629:
2621:
2616:
2614:
2610:
2594:
2591:
2588:
2585:
2582:
2579:
2571:
2553:
2549:
2540:
2522:
2518:
2495:
2491:
2478:
2468:
2464:
2446:
2442:
2438:
2433:
2429:
2425:
2420:
2416:
2412:
2407:
2399:
2396:
2390:
2387:
2382:
2378:
2370:
2369:
2367:
2349:
2345:
2341:
2336:
2332:
2328:
2323:
2319:
2315:
2310:
2302:
2299:
2293:
2288:
2284:
2276:
2275:
2273:
2270:
2269:
2268:
2252:
2248:
2226:
2206:
2201:
2197:
2174:
2170:
2147:
2139:
2136:
2120:
2116:
2114:
2097:
2073:
2064:
2049:
2046:
2042:
2039:
2016:
2012:
2008:
2004:
2001:
1996:
1992:
1988:
1968:
1965:
1962:
1959:
1939:
1936:
1932:
1929:
1925:
1922:
1919:
1916:
1895:
1892:
1888:
1864:
1861:
1857:
1853:
1850:
1846:
1842:
1839:
1835:
1831:
1828:
1801:
1796:
1792:
1788:
1785:
1780:
1776:
1772:
1769:
1764:
1760:
1756:
1753:
1748:
1744:
1740:
1735:
1731:
1727:
1722:
1718:
1714:
1707:
1706:
1705:
1702:
1688:
1685:
1682:
1659:
1633:
1629:
1605:
1585:
1582:
1575:The constant
1559:
1554:
1546:
1537:
1532:
1524:
1515:
1510:
1502:
1493:
1488:
1480:
1477:
1468:
1463:
1455:
1442:
1441:
1440:
1423:
1418:
1410:
1401:
1396:
1388:
1385:
1376:
1371:
1363:
1350:
1349:
1348:
1334:
1331:
1311:
1305:
1302:
1298:
1295:
1270:
1244:
1235:
1208:
1205:
1182:
1171:
1167:
1163:
1162:time dilation
1159:
1155:
1149:
1147:
1142:
1139:
1135:
1131:
1110:
1101:
1091:
1086:
1077:
1067:
1062:
1053:
1043:
1038:
1029:
1015:
1014:
1013:
1011:
994:
983:
982:
975:
965:
962:
952:
951:
947:
942:
940:
936:
932:
928:
923:
921:
917:
913:
909:
905:
904:Raum und Zeit
901:
897:
893:
885:
884:Raum und Zeit
880:
876:
873:
872:David Hilbert
867:
862:
860:
856:
851:
849:
844:
840:
836:
831:
829:
825:
820:
818:
814:
813:four-velocity
810:
809:four-position
806:
801:
799:
795:
790:
776:
770:
762:
756:
746:
740:
732:
726:
717:
715:
711:
707:
703:
698:
695:
692:in 1889, and
691:
687:
685:
680:
676:
672:
667:
665:
661:
657:
653:
649:
645:
641:
626:
615:
605:
601:
596:
589:
587:
583:
579:
574:
571:
569:
563:
561:
555:
548:
543:
539:
537:
535:
531:
527:
511:
503:
502:
496:
494:
488:
484:
482:
478:
474:
470:
466:
462:
458:
454:
450:
446:
442:
437:
435:
431:
427:
423:
418:
416:
412:
408:
403:
399:
389:
382:
380:
378:
374:
370:
366:
361:
359:
355:
351:
345:
343:
339:
335:
331:
327:
324:
320:
316:
312:
308:
304:
300:
288:
283:
281:
276:
274:
269:
268:
266:
265:
258:
248:
245:
240:
234:
233:
231:
230:
222:
219:
217:
214:
212:
209:
207:
204:
202:
199:
197:
194:
192:
189:
187:
184:
183:
176:
175:
167:
164:
162:
159:
158:
151:
150:
142:
139:
137:
134:
132:
129:
128:
121:
120:
112:
109:
107:
104:
102:
99:
97:
94:
93:
86:
85:
79:
76:
74:
71:
70:
68:
67:
63:
59:
58:
55:
52:
51:
47:
46:
41:
37:
33:
19:
17918:
17822:
17516:KaluzaâKlein
17268:Introduction
17208:
17194:Twin paradox
16957:Decimal time
16686:Astronomical
16565:Complication
16560:Atomic clock
16471:
16175:Time capsule
16169:Tempus fugit
16167:
16089:Other fields
16059:
15788:
15769:Perdurantism
15691:Calendar era
15643:
15636:
15622:Cuckoo clock
15559:astronomical
15533:
15359:Unit of time
15290:Key concepts
15240:
15206:
15145:Hyperpyramid
15110:Hypersurface
15027:
15003:Affine space
14993:Vector space
14932:Scholarpedia
14889:. Retrieved
14883:
14859:
14833:
14821:
14811:
14782:
14747:
14718:. Retrieved
14714:
14705:
14662:
14658:
14648:
14605:
14601:
14591:
14579:. Retrieved
14541:
14537:
14527:Tegmark, Max
14483:
14479:
14475:
14469:
14461:
14456:
14448:
14426:
14422:
14409:
14397:. Retrieved
14392:
14382:
14370:. Retrieved
14363:the original
14340:
14336:
14320:
14269:
14265:
14259:
14247:. Retrieved
14240:the original
14225:
14199:maths.tcd.ie
14194:
14186:
14142:
14138:
14132:
14099:
14095:
14089:
14070:
14036:
14032:
14026:
14001:
13997:
13991:
13979:. Retrieved
13946:
13942:
13932:
13889:
13885:
13879:
13867:. Retrieved
13852:
13832:
13799:
13791:
13779:
13774:
13770:
13765:
13761:
13757:
13753:
13748:
13744:
13737:
13725:. Retrieved
13710:
13686:. Retrieved
13678:Hyperphysics
13677:
13667:
13655:. Retrieved
13650:
13640:
13619:
13607:. Retrieved
13592:
13585:
13542:
13538:
13528:
13508:
13479:
13473:
13454:
13419:. Retrieved
13404:
13397:
13376:
13333:. Retrieved
13318:
13311:
13299:. Retrieved
13284:
13277:
13265:. Retrieved
13256:
13214:
13208:
13196:. Retrieved
13187:
13162:. Retrieved
13153:
13143:
13124:
13118:
13109:
13086:
13079:
13060:
13008:
12998:
12955:
12951:
12945:
12932:. Retrieved
12926:(1): 39â43.
12923:
12919:
12894:. Retrieved
12885:
12847:
12843:
12837:
12792:
12784:
12772:. Retrieved
12745:
12741:
12731:
12719:. Retrieved
12715:the original
12710:
12679:
12673:
12661:. Retrieved
12618:
12614:
12604:
12580:
12549:
12543:
12532:, retrieved
12494:
12490:
12477:
12457:
12433:. Retrieved
12424:
12415:
12403:. Retrieved
12394:
12385:
12374:the original
12359:
12346:
12334:. Retrieved
12325:
12315:
12303:. Retrieved
12283:
12276:
12264:. Retrieved
12214:
12208:
12192:
12180:. Retrieved
12165:
12126:
12105:. Retrieved
12096:
12086:
12067:
12032:
12025:
12013:. Retrieved
11998:
11991:
11979:. Retrieved
11955:
11902:
11896:
11884:. Retrieved
11875:
11865:
11842:
11838:
11834:
11830:
11826:
11817:
11803:
11793:
11780:
11772:
11766:
11761:
11751:
11734:
11719:MĂśbius group
11705:
11696:
11695:
11687:
11686:
11678:
11677:
11669:
11668:
11660:
11659:
11651:
11650:
11643:
11642:
11633:
11632:
11628:
11621:
11620:
11617:
11610:
11609:
11606:
11602:
11594:
11590:
11585:
11555:
11542:
11528:
11520:
11516:
11515:, carrying;
11512:
11508:
11505:luminiferous
11504:
11500:
11471:Metric space
11400:
11393:
11386:
11375:
11368:
11353:
11344:
11339:
11319:Hermann Weyl
11314:
11263:
11236:
11231:
11227:
11217:
11210:
11205:
11201:
11191:
11183:
11179:
11155:
11151:
11080:
11075:non-singular
11032:
10969:
10888:
10793:
10772:
10751:group theory
10703:surface area
10678:
10661:
10645:
10640:
10636:
10633:
10627:
10609:
10604:
10590:
10575:
10567:
10559:
10548:
10543:
10539:
10532:
10516:
10505:
10495:
10488:
10487:there is no
10482:
10476:
10471:
10465:
10460:
10454:
10448:Lilliputians
10443:
10417:
10412:
10407:
10405:
10397:
10381:
10370:
10311:
10238:
10233:
10032:
9975:
9972:
9884:
9871:
9853:
9847:
9820:
9764:
9694:
9614:
9259:
9255:
9244:
9241:
9215:
9203:
9200:Emmy Noether
9197:
9184:
8935:
8934:
8930:
8928:
8879:
8877:
8788:
8783:
8776:
8774:
8771:
8616:
8613:
8455:
8451:
8447:
8443:
8389:
8385:
8381:
8374:
8309:
8307:
8302:
8298:
8290:
8288:
8283:
8279:
8197:
8192:
8188:
8186:
8166:
8161:
8058:
8053:
8047:
8007:
7998:
7992:
7990:
7985:
7984:
7973:
7938:
7915:
7834:
7749:
7745:
7743:
7740:
7728:
7722:
7711:
7628:is given by
7452:
7384:is given by
7381:
7377:
7370:
7363:
7361:
7298:is given by
7295:
7288:
7281:
7278:
7261:
7244:
7236:
7229:
7224:
7218:
7213:
7209:
7207:
7204:
7199:
7195:
7188:
7181:
7179:
7166:
7159:
7155:
7151:
7147:
7140:
7133:
7129:
7125:
7123:
7011:
7007:
7003:
6999:
6989:
6985:
6981:
6972:
6968:
6955:
6951:
6945:
6941:
6937:
6926:
6922:
6913:
6909:
6905:
6901:
6897:
6893:
6889:
6881:
6877:
6873:
6868:
6864:
6860:
6853:
6846:
6842:
6835:
6827:
6823:
6819:
6818:in terms of
6812:
6805:
6800:
6796:
6792:
6782:
6775:
6769:
6765:
6762:
6750:
6626:
6613:
6604:
6600:
6595:
6593:
6588:
6584:
6577:
6573:
6570:
6565:
6561:
6560:means Δ
6557:
6308:
6303:
6299:
6295:
6291:
6287:
6283:
6279:
6277:
6092:
5917:
5914:
5910:
5893:
5810:
5806:
5802:
5798:
5794:
5790:
5786:
5782:
5778:
5774:
5770:
5766:
5762:
5758:
5754:
5750:
5746:
5738:
5734:
5727:
5721:
5717:
5713:
5709:
5707:
5702:
5698:
5674:
5670:
5668:
5551:
5472:
5468:
5464:
5460:
5456:
5452:
5448:
5440:
5436:
5429:
5423:
5419:
5415:
5411:
5409:
5304:
5302:
5298:
5265:
5256:
5245:Please help
5240:verification
5237:
5215:
5209:
5205:
5201:
5197:
5190:
5183:
5176:
5172:
5168:
5161:
5157:
5150:
5144:
5049:
5045:
5041:
5033:
5029:
5023:
5019:
5013:
5009:
5003:
4999:
4990:
4986:
4982:
4976:
4972:
4968:
4964:
4955:
4951:
4947:
4943:
4939:
4934:
4925:
4921:
4917:
4913:
4909:
4905:
4896:
4892:
4885:
4880:
4876:
4869:
4865:
4858:
4852:
4848:
4844:
4840:
4836:
4833:
4792:
4768:
4766:
4677:
4670:
4663:
4654:
4650:
4646:
4639:
4635:
4631:
4624:
4620:
4613:
4604:
4600:
4594:
4590:
4583:
4577:
4573:
4568:
4561:
4557:
4555:
4551:
4545:
4544:Figure 3â1.
4387:
4380:
4373:
4369:
4365:
4354:
4347:
4340:
4333:
4325:
4321:
4317:
4313:
4302:
4295:
4288:
4281:
4274:
4267:
4263:
4259:
4255:
4250:
4237:
4228:
4211:
4205:
4201:
4197:
4193:
4188:
4184:
4180:
4177:
4174:
4166:
4154:
4150:twin paradox
4149:
4141:twin paradox
4138:
4134:
4131:Twin paradox
4125:observations
4124:
4120:
4118:
4113:
4109:
4105:
4101:
4097:
4093:
4089:
4085:
4081:
4077:
4073:
4069:
4065:
4057:
4049:
4045:
4043:
4038:
4034:
4030:
4026:
4022:
4018:
4014:
4012:
4005:
4001:
3997:
3993:
3989:
3985:
3981:
3977:
3973:
3961:
3953:
3946:
3945:-coordinate
3942:
3933:
3923:
3919:
3911:
3907:
3900:
3887:
3883:
3871:
3867:
3860:
3856:
3847:
3843:
3839:
3835:
3831:
3827:
3823:
3819:
3817:
3812:
3808:
3805:
3770:
3763:
3756:
3749:
3745:
3741:
3737:
3712:
3700:
3695:
3693:
3688:
3684:
3680:
3677:
3669:Twin paradox
3656:
3643:
3640:
3635:
3633:
3628:
3624:
3620:
3613:
3608:
3604:
3602:
3596:
3586:
3579:
3566:
3554:
3544:
3529:
3525:
3521:hyperboloids
3514:
3489:
3485:
3460:
3458:
3455:
3450:
3446:
3442:
3413:
3334:
3324:
3309:
3300:
3289:Please help
3284:verification
3281:
3259:
3221:
3179:
3176:
3171:
3162:
3158:
3147:
3143:
3136:
3128:
3119:
3116:
3109:
3103:
3094:
3090:
3088:
3078:
3071:
3064:
3059:
3055:
3051:
3047:
3043:
3041:
3036:
3032:
3028:
3024:
3020:
3016:
3012:
3010:
2985:
2982:
2972:
2959:
2947:
2942:
2938:
2934:
2930:
2926:
2923:
2918:
2914:
2910:
2906:
2902:
2898:
2894:
2889:
2885:
2883:
2826:
2822:
2818:
2814:
2810:
2806:
2802:
2798:
2794:
2790:
2786:
2783:relativistic
2782:
2780:
2774:
2770:
2763:
2759:
2752:
2748:
2744:
2732:
2726:
2695:
2686:
2675:Please help
2670:verification
2667:
2645:
2617:
2612:
2608:
2569:
2538:
2482:
2271:
2125:
2112:
2065:
1816:
1703:
1574:
1438:
1169:
1160:(because of
1150:
1143:
1137:
1133:
1129:
1127:
979:
977:
964:
949:
945:
943:
924:
915:
911:
907:
903:
899:
895:
891:
889:
883:
869:
864:
852:
832:
821:
805:four vectors
802:
793:
787:
709:
699:
688:
674:
668:
651:
637:
595:
581:
577:
575:
572:
564:
559:
556:
552:
538:
525:
499:
497:
492:
489:
485:
476:
472:
468:
464:
460:
456:
452:
448:
438:
419:
395:
388:
385:Fundamentals
381:
362:
346:
341:
337:
334:relativistic
306:
302:
296:
206:Curved space
95:
53:
17913:Outer space
17877:Mathematics
17605:KerrâNewman
17576:Spherical:
17445:Other tests
17388:Singularity
17320:Formulation
17282:Fundamental
17136:Formulation
17117:Proper time
17078:Fundamental
16967:System time
16962:Metric time
16681:Solar Hijri
16607:Water clock
16590:Radio clock
16522:Time domain
16502:Proper time
16388:Leap second
16270:Chronometry
16185:Time travel
16163:System time
16070:Time domain
16055:Proper time
15879:use of time
15850:Father Time
15830:Immortality
15820:Ages of Man
15749:Endurantism
15706:Regnal year
15686:Big History
15615:water-based
15514:Solar Hijri
15424:Hexadecimal
15374:Measurement
15336:Chronometry
15322:Measurement
15230:Codimension
15209:-dimensions
15130:Hypersphere
15013:Free module
14581:16 December
13892:(18): 9â8.
12621:: 129â176.
12221:: S24âS35.
11511:, light, +
11403:black holes
11341:Max Tegmark
10711:integrating
8442:approaches
7757:blueshifted
7624:Hence, the
6852:must equal
6841:must equal
6566:differences
5370:are common.
4567:. Velocity
4225:Gravitation
3689:both slower
3625:world sheet
3222:proper time
3120:necessarily
2921:(event R).
2620:world lines
2483:In general
2113:differences
782:Figure 1-3.
631:aberration.
392:Definitions
186:Four-vector
17925:Categories
17757:Zel'dovich
17665:Scientists
17644:Alcubierre
17451:of Mercury
17449:precession
17378:Black hole
17261:Background
17253:relativity
17222:World line
17217:Light cone
17042:Background
17034:relativity
17024:Relativity
16982:Timekeeper
16935:Chronology
16919:Millennium
16805:Precession
16711:Julian day
16532:T-symmetry
16393:Solar time
16363:Civil time
15887:Chronemics
15862:Kalachakra
15774:Presentism
15759:Eternalism
15665:Chronology
15603:mechanical
15554:Main types
15472:Main types
15225:Hyperspace
15105:Hyperplane
14672:1906.05336
14615:2207.14317
14182:1703.05448
12850:: 85â121.
12093:"Manifold"
12015:14 October
11857:References
10413:appearance
10243:1 MeV = 10
7997:. It is a
7838:redshifted
6725:10 km
6622:10 km
5797:, we have
5259:March 2024
3607:along the
3303:March 2024
3000:(t<0).
2986:light cone
2969:light cone
2963:Light cone
2689:March 2024
972:See also:
941:are used.
931:hyperbolic
828:kinematics
817:four-force
710:local time
640:Arago spot
493:world line
441:dimensions
407:observer's
17931:Spacetime
17889:Astronomy
17727:Robertson
17712:Friedmann
17707:Eddington
17697:de Sitter
17531:Solutions
17409:detectors
17404:astronomy
17371:Phenomena
17306:Geodesics
17209:Spacetime
17152:Phenomena
16879:Fortnight
16726:Lunisolar
16716:Leap year
16650:Gregorian
16600:stopwatch
16575:Hourglass
16555:Astrarium
16472:Spacetime
16403:Time zone
16280:Metrology
16259:standards
16143:Leap year
16060:Spacetime
15934:Yesterday
15835:Dreamtime
15809:Mythology
15696:Deep time
15608:stopwatch
15583:hourglass
15564:astrarium
15494:Gregorian
15487:Lunisolar
15464:Calendars
15454:Time zone
15327:standards
15115:Hypercube
15093:Polytopes
15073:Minkowski
15068:Hausdorff
15063:Inductive
15028:Spacetime
14979:Dimension
14913:Spacetime
14697:211734117
14640:251196731
14508:119683293
14345:CiteSeerX
14312:250904081
14304:0264-9381
14124:120125096
13971:120021772
13784:geodesics
13672:Nave, R.
13031:cite book
12965:0808.2730
12828:1210.6929
12653:120211823
12435:13 August
12405:13 August
12336:13 August
12135:CRC Press
11456:Geography
11424:networks.
11364:electrons
11264:In 1920,
10897:geodesics
10854:signature
10763:algebraic
10735:geodesics
10156:−
10136:−
10122:′
10090:−
9950:−
9909:−
9848:Lab Frame
9222:) yields
9210:) yields
9087:→
9069:≡
8979:→
8953:≡
8901:±
8815:−
8709:≈
8681:β
8677:−
8637:γ
8513:γ
8483:γ
8422:γ
8410:γ
8407:β
8350:γ
8344:β
8341:−
8327:′
8140:γ
8137:β
8134:−
8126:′
8091:γ
8083:′
7999:conserved
7924:γ
7893:β
7889:−
7870:γ
7812:β
7808:−
7784:γ
7666:β
7655:β
7652:−
7606:β
7586:γ
7577:β
7534:γ
7505:β
7462:β
7411:β
7407:−
7328:β
7099:γ
7096:β
7082:γ
7047:γ
7044:β
7030:γ
6665:−
6654:γ
6646:′
6538:Δ
6532:−
6526:Δ
6520:γ
6506:Δ
6463:Δ
6457:−
6451:Δ
6445:γ
6431:Δ
6402:−
6393:γ
6336:−
6327:γ
6183:γ
6118:γ
6019:−
6008:γ
5959:−
5948:γ
5877:γ
5857:β
5853:−
5844:γ
5685:γ
5645:β
5641:−
5598:−
5583:γ
5560:γ
5508:−
4805:β
4709:−
4420:−
4104:in S, at
3627:onto the
3575:10 s
3563:10 s
3551:10 s
3386:±
3370:−
3192:−
3132:(A, B, C)
3067:causality
3056:lightlike
3052:spacelike
2849:θ
2843:
2829:given by
2609:lightlike
2586:±
2570:spacelike
2391:−
2342:−
2329:−
2316:−
2094:Δ
1966:≠
1786:−
1770:−
1754:−
1680:Δ
1657:Δ
1626:Δ
1544:Δ
1538:−
1522:Δ
1516:−
1500:Δ
1494:−
1475:Δ
1453:Δ
1408:Δ
1402:−
1383:Δ
1361:Δ
1309:Δ
1292:Δ
1267:Δ
1232:Δ
1203:Δ
1180:Δ
1098:Δ
1074:Δ
1050:Δ
1026:Δ
991:Δ
822:In 1905,
807:, namely
443:. In the
415:Euclidean
409:state of
363:In 1908,
326:continuum
303:spacetime
54:Spacetime
17840:Category
17717:LemaĂŽtre
17682:Einstein
17672:PoincarĂŠ
17632:Others:
17616:TaubâNUT
17582:interior
17504:theories
17502:Advanced
17469:redshift
17284:concepts
17102:Rapidity
17080:concepts
16940:Duration
16914:Saeculum
16894:Olympiad
16736:Solstice
16665:Holocene
16642:Calendar
16542:Horology
16333:ISO 8601
16328:ISO 31-1
16203:Category
15951:Time in
15942:Tomorrow
15804:Religion
15744:Duration
15711:Timeline
15645:Timeline
15444:Sidereal
15312:Eternity
15242:Category
15218:See also
15018:Manifold
14857:(1992).
14831:(2004).
14814:. Dover.
14772:87028148
14746:(1986).
14576:15694111
14417:(1920).
14399:13 April
14372:13 April
14328:(2007).
14249:14 April
13975:Archived
13924:14295121
13863:Archived
13727:14 April
13682:Archived
13577:27877933
13421:24 April
13335:22 April
13301:22 April
13267:10 April
13261:Archived
13198:26 March
13192:Archived
13164:26 March
13158:Archived
12990:12020510
12928:Archived
12890:Archived
12864:27757388
12768:Archived
12657:Archived
12525:archived
12497:: 1â22,
12429:Archived
12399:Archived
12330:Archived
12299:Archived
12266:11 April
12257:Archived
12182:14 April
12107:24 March
12101:Archived
11975:Archived
11886:24 March
11880:Archived
11694:, where
11429:See also
11331:orbitals
11198:temporal
10782:Manifold
10759:analysis
10743:Einstein
10691:smoothly
10628:a priori
10610:In 1962
10401:geodesic
10239:Example:
10080:′
9940:′
9899:′
9852:(right)
9846:(above)
8784:fruitful
8617:γmc
7952:Momentum
7880:′
7861:′
7794:′
7780:′
7593:′
7541:′
7210:Example:
7106:′
7089:′
7054:′
7037:′
6596:Example:
6513:′
6438:′
6386:′
6320:′
6258:′
6236:′
6209:′
6195:′
6147:′
6130:′
6063:′
6041:′
5997:′
5937:′
5799:γβk
5779:γβk
5745:, where
5103:′
5081:′
4742:′
4699:′
4546:Galilean
4515:′
4483:′
4451:′
4410:′
4092:; also,
3154:C, B, A.
2539:timelike
2162:and the
2050:′
2013:′
1933:′
1896:′
1865:′
1854:′
1843:′
1832:′
981:distance
859:Max Born
706:dynamics
582:observes
578:measures
560:observer
532:and the
501:manifold
426:velocity
257:Category
17865:Physics
17851:Portals
17782:Hawking
17777:Penrose
17762:Novikov
17742:Wheeler
17687:Hilbert
17677:Lorentz
17634:pp-wave
17455:lensing
17251:General
17032:Special
16909:Century
16899:Lustrum
16829:Instant
16701:Equinox
16670:Islamic
16612:Sundial
16477:Chronon
16213:Commons
16136:Related
16050:Instant
16040:Chronon
16022:Physics
15962:Geology
15953:science
15825:Destiny
15670:History
15638:History
15593:sundial
15576:quantum
15519:Chinese
15509:Islamic
15419:Decimal
15414:Chinese
15376:systems
15302:Present
15140:Simplex
15078:Fractal
14891:16 July
14820:(1973)
14810:(1952)
14720:16 June
14677:Bibcode
14620:Bibcode
14556:Bibcode
14488:Bibcode
14451:20:200.
14431:Bibcode
14284:Bibcode
14147:Bibcode
14104:Bibcode
14041:Bibcode
14006:Bibcode
13981:9 April
13951:Bibcode
13904:Bibcode
13869:9 April
13568:5099802
13547:Bibcode
12970:Bibcode
12934:6 April
12896:17 July
12774:7 April
12750:Bibcode
12721:15 July
12663:15 July
12623:Bibcode
12534:17 July
12499:Bibcode
12305:7 April
12253:8146369
12233:Bibcode
11481:Present
11411:(3 + 1)
11360:protons
11335:nucleus
11323:Maxwell
11208:. That
11194:spatial
11147:tensors
10685:on the
10677:with a
10595:is the
10455:F = GMm
10354:
10315:
10196:
10109:
10105:
10068:
10064:
10035:
10028:
9982:
9968:
9928:
9924:
9887:
9816:
9770:
9761:
9732:
9728:
9699:
9691:
9656:
9652:
9617:
9610:
9562:
9424:
9378:
9374:
9320:
9316:
9262:
8919:
8887:
8608:
8565:
8561:
8505:
8498:
8462:
8448:γm
8440:
8399:
8365:
8314:
8276:
8242:
8238:
8204:
8158:
8113:
8109:
8061:
8043:
8011:
6973:γx
6956:γw
6949:yields
6927:γw
6828:inverse
6781:,
6768:,
6717:
6633:
5803:γk
5777:,
5775:γk
5769:,
5732:√
5434:√
4196:-axis (
4068:, with
3996:on the
3746:smaller
3649:rotated
3168:A, B, C
2474:(â+++).
1324:in the
886:lecture
592:History
400:treats
309:, is a
299:physics
17823:others
17812:Thorne
17802:Misner
17787:Taylor
17772:Geroch
17767:Ehlers
17737:Zwicky
17555:Kasner
16904:Decade
16859:Moment
16854:Minute
16849:Second
16819:Other
16676:Julian
16655:Hebrew
16301:offset
16153:Moment
16148:Memory
16000:period
15588:marine
15571:atomic
15546:Clocks
15504:Hebrew
15499:Julian
15434:Metric
15307:Future
15097:shapes
14867:
14841:
14806:, and
14789:
14770:
14760:
14695:
14638:
14574:
14506:
14347:
14310:
14302:
14232:
14122:
14077:
13969:
13922:
13840:
13808:
13718:
13688:27 May
13657:6 July
13609:24 May
13600:
13575:
13565:
13516:
13486:
13461:
13412:
13385:
13326:
13292:
13221:
13131:
13094:
13067:
13019:
13013:56â104
12988:
12862:
12801:
12686:
12651:
12592:
12556:
12517:
12465:
12366:
12291:
12251:
12173:
12141:
12074:
12040:
12006:
11981:24 May
11967:
11909:
11824:radius
11521:aithÄr
11517:aether
11513:ferens
11382:nerves
11378:< 3
11371:< 3
11356:> 1
11278:galaxy
11274:planet
10788:, and
10707:volume
10544:really
10303:μ
10297:ν
10276:μ
10257:π
8395:γ
7980:vector
7954:, and
7146:, and
6700:
6697:519.62
6587:with â
5447:where
4598:, and
3878:and Wâ˛
3750:slower
3161:= â0.5
3095:before
3031:Δ
2994:future
2937:Ⲡand
2470:(+âââ)
2086:means
1158:events
1136:, and
927:sphere
815:, and
652:waving
411:motion
255:
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6680:c
6675:/
6671:x
6668:v
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6517:=
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5835:O
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5634:1
5629:=
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5617:c
5612:/
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5595:1
5591:1
5586:=
5538:.
5531:2
5527:c
5522:/
5516:2
5512:v
5505:1
5499:/
5495:K
5492:O
5489:=
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5483:O
5473:v
5471:/
5465:β
5463:/
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5441:k
5437:x
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5422:/
5384:=
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5261:)
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5210:v
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5020:r
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4952:c
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4851:/
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4839:/
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4364:(
4360:)
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3374:x
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3305:)
3301:(
3287:.
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2324:2
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2307:)
2303:t
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2253:2
2249:s
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2207:,
2202:2
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2175:2
2171:x
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2134:(
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2017:2
2009:s
2005:d
2002:=
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1993:s
1989:d
1969:0
1963:s
1960:d
1940:0
1937:=
1930:s
1926:d
1923:=
1920:s
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1889:d
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1862:z
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1840:x
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1749:2
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1606:t
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1560:.
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1456:s
1450:(
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1415:)
1411:x
1405:(
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918:(
902:(
894:(
512:c
477:t
473:z
469:y
465:x
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286:e
279:t
272:v
42:.
20:)
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