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Cavity magnetron

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920:, where it was shown on 19 September 1940 in Alfred Loomis’ apartment. The American NDRC Microwave Committee was stunned at the power level produced. However Bell Labs' director was upset when it was X-rayed and had eight holes rather than the six holes shown on the GEC plans. After contacting (via the transatlantic cable) Dr Eric Megaw, GEC’s vacuum tube expert Megaw recalled that when he had asked for 12 prototypes he said make 10 with 6 holes, one with 7 and one with 8; there was no time to amend the drawings. And No 12 with 8 holes was chosen for the Tizard Mission. So Bell Labs chose to copy the sample; and while early British magnetrons had six cavities the American ones had eight cavities. 885: 55: 419: 205:, England in 1940. Their first working example produced hundreds of watts at 10 cm wavelength, an unprecedented achievement. Within weeks, engineers at GEC had improved this to well over a kilowatt, and within months 25 kilowatts, over 100 kW by 1941 and pushing towards a megawatt by 1943. The high power pulses were generated from a device the size of a small book and transmitted from an antenna only centimeters long, reducing the size of practical radar systems by orders of magnitude. New radars appeared for 459:
them. The anode is constructed of a highly conductive material, almost always copper, so these differences in voltage cause currents to appear to even them out. Since the current has to flow around the outside of the cavity, this process takes time. During that time additional electrons will avoid the hot spots and be deposited further along the anode, as the additional current flowing around it arrives too. This causes an oscillating current to form as the current tries to equalize one spot, then another.
622: 165:, USA, began development of magnetrons to avoid de Forest's patents, but these were never completely successful. Other experimenters picked up on Hull's work and a key advance, the use of two cathodes, was introduced by Habann in Germany in 1924. Further research was limited until Okabe's 1929 Japanese paper noting the production of centimeter-wavelength signals, which led to worldwide interest. The development of magnetrons with multiple cathodes was proposed by A. L. Samuel of 488: 297:, resulting in considerable research into alternate tube designs that would avoid his patents. One concept used a magnetic field instead of an electrical charge to control current flow, leading to the development of the magnetron tube. In this design, the tube was made with two electrodes, typically with the cathode in the form of a metal rod in the center, and the anode as a cylinder around it. The tube was placed between the poles of a 63: 877: 854: 1082: 1126:. Exceptions to this are higher power magnetrons that operate above approximately 10,000 volts where positive ion bombardment becomes damaging to thorium metal, hence pure tungsten (potassium doped) is used. While thorium is a radioactive metal, the risk of cancer is low as it never gets airborne in normal usage. Only if the filament is taken out of the magnetron, finely crushed, and inhaled can it pose a health hazard. 523:. Spaced around the rim of the chamber are cylindrical cavities. Slots are cut along the length of the cavities that open into the central, common cavity space. As electrons sweep past these slots, they induce a high-frequency radio field in each resonant cavity, which in turn causes the electrons to bunch into groups. A portion of the radio frequency energy is extracted by a short coupling loop that is connected to a 333:, these electrons radiate radio frequency energy. The effect is not very efficient. Eventually the electrons hit one of the electrodes, so the number in the circulating state at any given time is a small percentage of the overall current. It was also noticed that the frequency of the radiation depends on the size of the tube, and even early examples were built that produced signals in the microwave regime. 578: 663:
shift within an individual transmitted pulse. The second factor is that the energy of the transmitted pulse is spread over a relatively wide frequency spectrum, which requires the receiver to have a correspondingly wide bandwidth. This wide bandwidth allows ambient electrical noise to be accepted into the receiver, thus obscuring somewhat the weak radar echoes, thereby reducing overall receiver
685: 46: 771:. He settled on a system consisting of a diode with a cylindrical anode surrounding a rod-shaped cathode, placed in the middle of a magnet. The attempt to measure the electron mass failed because he was unable to achieve a good vacuum in the tube. However, as part of this work, Greinacher developed mathematical models of the motion of the electrons in the crossed magnetic and electric fields. 806:, investigated the magnetron for his doctoral dissertation of 1924. Throughout the 1920s, Hull and other researchers around the world worked to develop the magnetron. Most of these early magnetrons were glass vacuum tubes with multiple anodes. However, the two-pole magnetron, also known as a split-anode magnetron, had relatively low efficiency. 354: 396:
of the device was greatly improved. Unfortunately, the higher field also meant that electrons often circled back to the cathode, depositing their energy on it and causing it to heat up. As this normally causes more electrons to be released, it could sometimes lead to a runaway effect, damaging the device.
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The magnetron is a self-oscillating device requiring no external elements other than a power supply. A well-defined threshold anode voltage must be applied before oscillation will build up; this voltage is a function of the dimensions of the resonant cavity, and the applied magnetic field. In pulsed
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Since all of the electrons in the flow experienced this looping motion, the amount of RF energy being radiated was greatly improved. And as the motion occurred at any field level beyond the critical value, it was no longer necessary to carefully tune the fields and voltages, and the overall stability
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systems became widely available in the late 1930s, the ultra high frequency and microwave bands were well beyond the ability of conventional circuits. The magnetron was one of the few devices able to generate signals in the microwave band and it was the only one that was able to produce high power at
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Centimetric radar, made possible by the cavity magnetron, allowed for the detection of much smaller objects and the use of much smaller antennas. The combination of small-cavity magnetrons, small antennas, and high resolution allowed small, high quality radars to be installed in aircraft. They could
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Several characteristics of the magnetron's output make radar use of the device somewhat problematic. The first of these factors is the magnetron's inherent instability in its transmitter frequency. This instability results not only in frequency shifts from one pulse to the next, but also a frequency
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The oscillating currents flowing around the cavities, and their effect on the electron flow within the tube, cause large amounts of microwave radiofrequency energy to be generated in the cavities. The cavities are open on one end, so the entire mechanism forms a single, larger, microwave oscillator.
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The original magnetron was very difficult to keep operating at the critical value, and even then the number of electrons in the circling state at any time was fairly low. This meant that it produced very low-power signals. Nevertheless, as one of the few devices known to create microwaves, interest
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Hull's magnetron was not originally intended to generate VHF (very-high-frequency) electromagnetic waves. However, in 1924, Czech physicist August Žáček (1886–1961) and German physicist Erich Habann (1892–1968) independently discovered that the magnetron could generate waves of 100 megahertz to 1
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mounted on a recreational vessel, a radar with a magnetron output of 2 to 4 kilowatts is often found mounted very near an area occupied by crew or passengers. In practical use these factors have been overcome, or merely accepted, and there are today thousands of magnetron aviation and marine radar
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At very high magnetic field settings the electrons are forced back onto the cathode, preventing current flow. At the opposite extreme, with no field, the electrons are free to flow straight from the cathode to the anode. There is a point between the two extremes, the critical value or Hull cut-off
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The magnetic field is set to a value well below the critical, so the electrons follow curved paths towards the anode. When they strike the anode, they cause it to become negatively charged in that region. As this process is random, some areas will become more or less charged than the areas around
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At any given instant, the electron will naturally be pushed towards the lower-voltage side of the tube. The electron will then oscillate back and forth as the voltage changes. At the same time, a strong magnetic field is applied, stronger than the critical value in the original design. This would
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The magnetron remains the essential radio tube for shortwave radio signals of all types. It not only changed the course of the war by allowing us to develop airborne radar systems, it remains the key piece of technology that lies at the heart of your microwave oven today. The cavity magnetron's
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Mechanically, the cavity magnetron consists of a large, solid cylinder of metal with a hole drilled through the centre of the circular face. A wire acting as the cathode is run down the center of this hole, and the metal block itself forms the anode. Around this hole, known as the "interaction
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produced a working prototype of a cavity magnetron that produced about 400 W. Within a week this had improved to 1 kW, and within the next few months, with the addition of water cooling and many detail changes, this had improved to 10 and then 25 kW. To deal with its drifting
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The modern magnetron is a fairly efficient device. In a microwave oven, for instance, a 1.1-kilowatt input will generally create about 700 watts of microwave power, an efficiency of around 65%. (The high-voltage and the properties of the cathode determine the power of a magnetron.) Large
704:, the waveguide leads to a radio-frequency-transparent port into the cooking chamber. As the fixed dimensions of the chamber and its physical closeness to the magnetron would normally create standing wave patterns in the chamber, the pattern is randomized by a motorized fan-like 849:
proposed in 1937 a system with "six or eight small holes" drilled in a metal block, differing from the later production designs only in the aspects of vacuum sealing. However, his idea was rejected by the Navy, who said their valve department was far too busy to consider it.
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magnetrons can produce up to 2.5 megawatts peak power with an average power of 3.75 kW. Some large magnetrons are water cooled. The magnetron remains in widespread use in roles which require high power, but where precise control over frequency and phase is unimportant.
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Günter Nagel, "Pionier der Funktechnik. Das Lebenswerk des Wissenschaftlers Erich Habann, der in Hessenwinkel lebte, ist heute fast vergessen" (Pioneer in Radio Technology. The life's work of scientist Erich Habann, who lived in Hessenwinkel, is nearly forgotten today.),
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and other effects, results in a slower and less faithful response to control current than electrostatic control using a control grid in a conventional triode (not to mention greater weight and complexity), so magnetrons saw limited use in conventional electronic designs.
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Where there are an even number of cavities, two concentric rings can connect alternate cavity walls to prevent inefficient modes of oscillation. This is called pi-strapping because the two straps lock the phase difference between adjacent cavities at π radians (180°).
659:. The magnetron is operated with very short pulses of applied voltage, resulting in a short pulse of high-power microwave energy being radiated. As in all primary radar systems, the radiation reflected from a target is analyzed to produce a radar map on a screen. 384:. As the name implies, this design used an anode that was split in two—one at each end of the tube—creating two half-cylinders. When both were charged to the same voltage the system worked like the original model. But by slightly altering the voltage of the two 304:
With no magnetic field present, the tube operates as a diode, with electrons flowing directly from the cathode to the anode. In the presence of the magnetic field, the electrons will experience a force at right angles to their direction of motion (the
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be used by maritime patrol aircraft to detect objects as small as a submarine periscope, which allowed aircraft to attack and destroy submerged submarines which had previously been undetectable from the air. Centimetric contour mapping radars like
262:. The components are normally arranged concentrically, placed within a tubular-shaped container from which all air has been evacuated, so that the electrons can move freely (hence the name "vacuum" tubes, called "valves" in British English). 185:
and others, limited to perhaps 10 W output. By this time the klystron was producing more power and the magnetron was not widely used, although a 300W device was built by Aleksereff and Malearoff in the USSR in 1936 (published in 1940).
786:'s patents on the control of current flow using electric fields via the "grid". Hull intended to use a variable magnetic field, instead of an electrostatic one, to control the flow of the electrons from the cathode to the anode. Working at 126:, which are small, open cavities in a metal block. Electrons pass by the cavities and cause microwaves to oscillate within, similar to the functioning of a whistle producing a tone when excited by an air stream blown past its opening. The 825:, around 10 cm (3 GHz), rather than the 50 to 150 cm (200 MHz) that was available from tube-based generators of the time. It was known that a multi-cavity resonant magnetron had been developed and patented in 1935 by 2140:
Slutzkin, A. A.; Steinberg, D. S. (May 1929). "Die Erzeugung von kurzwelligen ungedämpften Schwingungen bei Anwendung des Magnetfeldes" [The generation of undamped shortwave oscillations by application of a magnetic field].
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in the waveguide (more often in commercial ovens), or by a turntable that rotates the food (most common in consumer ovens). An early example of this application was when British scientists in 1954 used a microwave oven to resurrect
388:, the electrons' trajectory could be modified so that they would naturally travel towards the lower voltage side. The plates were connected to an oscillator that reversed the relative voltage of the two plates at a given frequency. 972:
in September 1940. As the discussion turned to radar, the US Navy representatives began to detail the problems with their short-wavelength systems, complaining that their klystrons could only produce 10 W. With a flourish,
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Magnetron with section removed to exhibit the cavities. The cathode in the center is not visible. The antenna emitting microwaves is at the left. The magnets producing a field parallel to the long axis of the device are not
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As the oscillation takes some time to set up, and is inherently random at the start, subsequent startups will have different output parameters. Phase is almost never preserved, which makes the magnetron difficult to use in
927:, Randall and Boot's discovery was "a massive, massive breakthrough" and "deemed by many, even now , to be the most important invention that came out of the Second World War", while professor of military history at the 519:. The electrons initially move radially outward from the cathode attracted by the electric field of the anode walls. The magnetic field causes the electrons to spiral outward in a circular path, a consequence of the 534:
The size of the cavities determine the resonant frequency, and thereby the frequency of the emitted microwaves. However, the frequency is not precisely controllable. The operating frequency varies with changes in load
269:) is inserted between the cathode and the anode, the flow of electrons between the cathode and anode can be regulated by varying the voltage on this third electrode. This allows the resulting electron tube (called a " 1045:
device to specifically detect it. Centimetric gun-laying radars were likewise far more accurate than the older technology. They made the big-gunned Allied battleships more deadly and, along with the newly developed
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space", are a number of similar holes ("resonators") drilled parallel to the interaction space, connected to the interaction space by a short channel. The resulting block looks something like the cylinder on a
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emerged. A key characteristic of the magnetron is that its output signal changes from pulse to pulse, both in frequency and phase. This renders it less suitable for pulse-to-pulse comparisons for performing
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coupling ("strapping") alternate cavities within the magnetron, which reduced the instability by a factor of 5–6. (For an overview of early magnetron designs, including that of Boot and Randall, see .)
696:, cooled by airflow from a fan. The magnetic field is produced by two powerful ring magnets, the lower of which is just visible. Almost all modern oven magnetrons are of similar layout and appearance. 463:
A "tap", normally a wire formed into a loop, extracts microwave energy from one of the cavities. In some systems the tap wire is replaced by an open hole, which allows the microwaves to flow into a
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9.375 GHz 20 kW (peak) magnetron assembly for an early commercial airport radar in 1947. In addition to the magnetron (right), it contains a TR (transmit/receive) switch tube and the
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Cutaway drawing of a cavity magnetron of 1984. Part of the righthand magnet and copper anode block is cut away to show the cathode and cavities. This older magnetron uses two horseshoe shaped
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because small variations in the electric charge applied to the control grid will result in identical variations in the much larger current of electrons flowing between the cathode and anode.
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applications there is a delay of several cycles before the oscillator achieves full peak power, and the build-up of anode voltage must be coordinated with the build-up of oscillator output.
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frequency, they sampled the output signal and synchronized their receiver to whatever frequency was actually being generated. In 1941, the problem of frequency instability was solved by
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and thus performance. The third factor, depending on application, is the radiation hazard caused by the use of high-power electromagnetic radiation. In some applications, for example, a
794:, Hull built tubes that provided switching through the control of the ratio of the magnetic and electric field strengths. He released several papers and patents on the concept in 1921. 317:
magnetic field (and cut-off voltage), where the electrons just reach the anode. At fields around this point, the device operates similar to a triode. However, magnetic control, due to
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normally cause the electron to circle back to the cathode, but due to the oscillating electrical field, the electron instead follows a looping path that continues toward the anodes.
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spectrum. This occurs because a few of the electrons, instead of reaching the anode, continue to circle in the space between the cathode and the anode. Due to an effect now known as
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to develop various types of radar using the magnetron. By early 1941, portable centimetric airborne radars were being tested in American and British aircraft. In late 1941, the
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Kaiser, W. (1994). "The Development of Electron Tubes and of Radar technology: The Relationship of Science and Technology". In Blumtritt, O.; Petzold, H.; Aspray, W. (eds.).
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held a lead in radar that their counterparts in Germany and Japan were never able to close. By the end of the war, practically every Allied radar was based on the magnetron.
309:). In this case, the electrons follow a curved path between the cathode and anode. The curvature of the path can be controlled by varying either the magnetic field using an 1050:, made anti-aircraft guns much more dangerous to attacking aircraft. The two coupled together and used by anti-aircraft batteries, placed along the flight path of German 415:, which works on entirely different principles. In this design the oscillation is created by the physical shape of the anode, rather than external circuits or fields. 1997:Žáček, A. (1928). "Über eine Methode zur Erzeugung von sehr kurzen elektromagnetischen Wellen" [On a method for generating very short electromagnetic waves]. 1900: 1100:
has no cooling blood flow, it is particularly prone to overheating when exposed to microwave radiation. This heating can in turn lead to a higher incidence of
1986: 2009:Žáček, A., "Spojení pro výrobu elektrických vln" , Czechoslovak patent no. 20,293 (filed: 31 May 1924; issued: 15 February 1926). Available (in Czech) at: 3837: 743:, etc.). Although efficient, these lamps are much more complex than other methods of lighting and therefore not commonly used. More modern variants use 475:
systems. Frequency also drifts from pulse to pulse, a more difficult problem for a wider array of radar systems. Neither of these present a problem for
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at a high (continuous or pulsed) negative potential created by a high-voltage, direct-current power supply. The cathode is placed in the center of an
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instead. But klystrons could not at that time achieve the high power output that magnetrons eventually reached. This was one reason that German
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A similar magnetron with a different section removed. Central cathode is visible; antenna conducting microwaves at the top; magnets are not shown.
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where the receiver can be synchronized with an imprecise magnetron frequency. Where precise frequencies are needed, other devices, such as the
539:, with changes in the supply current, and with the temperature of the tube. This is not a problem in uses such as heating, or in some forms of 2524: 1528: 1397: 802:, published first; however, he published in a journal with a small circulation and thus attracted little attention. Habann, a student at the 2493: 1334: 1234: 833:. However, the German military considered the frequency drift of Hollman's device to be undesirable, and based their radar systems on the 2013: 1463: 672:
units in service. Recent advances in aviation weather-avoidance radar and in marine radar have successfully replaced the magnetron with
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Obsolete 9 GHz magnetron tube and magnets from a Soviet aircraft radar. The tube is embraced between the poles of two horseshoe-shaped
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International Conference on the Origins and Evolution of the Cavity Magnetron (CAVMAG 2010), Bournemouth, England, UK, 19–20 April 2010
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Since then, many millions of cavity magnetrons have been manufactured; while some have been for radar the vast majority have been for
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The magnetron continued to be used in radar in the post-war period but fell from favour in the 1960s as high-power klystrons and
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Brookner, Eli (19–20 April 2010). "From $ 10,000 magee to $ 7 magee and $ 10 transmitter and receiver (T/R) on single chip".
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in microwave radar equipment and is often credited with giving Allied radar a considerable performance advantage over
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in the United Kingdom used the magnetron to develop a revolutionary airborne, ground-mapping radar codenamed H2S. The
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to generate the microwaves, which are substantially less complex and can be adjusted to maximize light output using a
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The use of magnetic fields as a means to control the flow of an electric current was spurred by the invention of the
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The electromagnet used in conjunction with Randall and Boot's original magnetron, in the Science Museum, London.
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Lipman, R. M.; B. J. Tripathi; R. C. Tripathi (1988). "Cataracts induced by microwave and ionizing radiation".
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There is also a considerable electrical hazard around magnetrons, as they require a high voltage power supply.
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at Wembley made 12 prototype cavity magnetrons in August 1940, and No 12 was sent to America with Bowen on the
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should offer the magnetron to the Americans in exchange for their financial and industrial help. An early 10
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of the arrangement is determined by the cavities' physical dimensions. Unlike other vacuum tubes, such as a
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Concise, notably-excellent article about magnetrons; Fig. 13 is representative of a modern radar magnetron.
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Redhead, Paul A., "The Invention of the Cavity Magnetron and its Introduction into Canada and the U.S.A.",
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In 1910 Hans Gerdien (1877–1951) of the Siemens Corporation invented a magnetron. In 1912, Swiss physicist
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Lythall, B. W. (1995). "Basic science and research for naval radar, 1935-1945". In Kingsley, F. A. (ed.).
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which in use is attached to a waveguide conducting the microwaves to the radar antenna. Modern tubes use
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It was noticed that when the magnetron was operating at the critical value, it would emit energy in the
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radars, thus directly influencing the outcome of the war. It was later described by American historian
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for front-line aircraft, were not a match for their British counterparts. Likewise, in the UK,
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for increasing the intensity of an applied microwave signal; the magnetron serves solely as an
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mixer. The waveguide aperture (left) would be connected to a waveguide going to the antenna.
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generating a microwave signal from direct current electricity supplied to the vacuum tube.
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Willshaw, W. E.; L. Rushforth; A. G. Stainsby; R. Latham; A. W. Balls; A. H. King (1946).
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Blind Bombing: How Microwave Radar brought the Allies to D-Day and Victory in World War II
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arranged such that the magnetic field was aligned parallel to the axis of the electrodes.
8: 3484: 3392: 3284: 3120: 3097: 2401:(Baxter was the official historian of the Office of Scientific Research and Development.) 1169: 1159: 1070: 974: 764: 341: 330: 221: 135: 2154: 2082: 1875: 1844: 1767: 1593: 1498: 595:
Please expand the section to include this information. Further details may exist on the
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magnetron. Magnetic lines of force are parallel to the geometric axis of this structure.
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made of solid copper, with the resonant frequency defined entirely by its dimensions.
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Radar Origins Worldwide: History of Its Evolution in 13 Nations Through World War II
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Brittain, James E. (1985). "The magnetron and the beginnings of the microwave age".
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The anode block which is part of the cavity magnetron developed by Randall and Boot
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U.S. patent no. 2,123,728 (filed: 1936 November 27 ; issued: 1938 July 12).
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2010 International Conference on the Origins and Evolution of the Cavity Magnetron
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took the example and quickly began making copies, and before the end of 1940, the
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Habann, Erich (1924). "Eine neue Generatorröhre" [A new generator tube].
2017: 1990: 1904: 1401: 1111: 1051: 638: 630: 626: 528: 385: 326: 230: 210: 2935: 2308:"The high-power pulsed magnetron: development and design for radar applications" 1800: 1370: 1144: 621: 3852: 3752: 3533: 3523: 3289: 3092: 2362: 2327: 1174: 1062: 1047: 1004: 969: 917: 752: 701: 689: 536: 512: 337: 286: 119: 103: 83: 2323: 2240: 1976: 1959: 3831: 3814: 3637: 3553: 3372: 3199: 3167: 2660: Hans Erich Hollmann/Telefunken GmbH: „Magnetron“ filed November 27, 1935 2624: 2312:
Journal of the Institution of Electrical Engineers - Part IIIA: Radiolocation
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Goerth, Joachim (2010). "Early magnetron development especially in Germany".
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J. Brittain (1985). "The Magnetron and the Beginnings of the Microwave Age".
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Okabe, Kinjiro (1929). "On the short-wave limit of magnetron oscillations".
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The magnetron stunned the Americans. Their research was years off the pace.
2305: 1655:] (in German). Berlin, Germany: Springer Verlag. p. 514 footnote. 1617: 1011: 949: 814: 740: 706: 668: 472: 266: 2440: 2277:"M.J.B.Scanlan; Early Centimetric Ground Radars – A Personal Reminiscence" 1775: 443:, not the core, of the conductor, the parallel sides of the slot act as a 3737: 3479: 3428: 3334: 3319: 3102: 3064: 1942:] (in German). New York: Waxmann Publishing Co. p. 251 footnote. 1123: 775: 728: 440: 247: 158: 95: 2777: 1213:. Nebraska: Potomac Books/University of Nebraska Press. pp. 24–26. 353: 3809: 3799: 3732: 3606: 3576: 3543: 3518: 3513: 3490: 3362: 3342: 3220: 3082: 3059: 2945: 2847: 2842: 2837: 1936:
Für und Wider "Hitlers Bombe": Studien zur Atomforschung in Deutschland
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At least one hazard in particular is well known and documented. As the
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For and Against "Hitler's Bomb": Studies on atomic research in Germany
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and Britain had no money to develop the magnetron on a massive scale,
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to the lighting cavity containing the light-emitting substance (e.g.,
3772: 3616: 3611: 3601: 3528: 3408: 3242: 3237: 3162: 3087: 2090: 1853: 1828: 1506: 1097: 1031: 996: 818: 732: 693: 464: 444: 423: 406: 274: 251: 139: 111: 1577: 731:, a magnetron provides the microwave field that is passed through a 62: 3794: 3742: 3722: 3700: 3586: 3581: 3469: 3458: 3387: 3157: 2217:
Okabe, Kinjiro (1930). "On the magnetron oscillation of new type".
1149: 1140: 1119: 1101: 1085: 1066: 953: 834: 716: 544: 448: 435:, with a somewhat larger central hole. Early models were cut using 432: 254:
are emitted from a negatively charged, heated component called the
131: 115: 32: 28: 2410: 2181:
Yagi, Hidetsugu (1928). "Beam transmission of ultra-short waves".
977:
pulled out a magnetron and explained it produced 1000 times that.
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The Development of Radar Equipments for the Royal Navy, 1935–45
1862:(Anon.) (1956). "The 70th birthday of Prof. Dr. August Žáček". 1055: 965: 830: 736: 560: 508: 492: 270: 258:
and are attracted to a positively charged component called the
213:
and even the smallest escort ships, and from that point on the
150: 67: 1641:
Gerdien, H., Deutsches Reichspatent 276,528 (12 January 1910).
692:
with magnet in its mounting box. The horizontal plates form a
3804: 3715: 3474: 3247: 3040: 2902: 2897: 1154: 1019: 810: 684: 652: 540: 439:
pistol jigs. Remembering that in an AC circuit the electrons
259: 99: 45: 2399:. Boston, Massachusetts: Little, Brown, and Co. p. 142. 3747: 3130: 3076: 2977: 2930: 2868: 2773:
Valve oscillator circuits; radio frequency output couplings
2197:
Journal of the Institute of Electrical Engineering of Japan
941: 744: 1962:[New method of generating undamped oscillations]. 1576:
Smith, A. U.; Lovelock, J. E.; Parkes, A. S. (June 1954).
1789:
Journal of the American Institute of Electrical Engineers
373:
in the device and potential improvements was widespread.
273:" because it now has three electrodes) to function as an 2454:
Australian Nuclear Science and Technology Organisation.
1697:[On an apparatus for the determination of e/m]. 1026:
as "he most valuable cargo ever brought to our shores".
2264:. London, England: Macmillan Press Ltd. pp. 68–69. 1699:
Verhandlungen der Deutschen Physikalischen Gesellschaft
2127:
Slutskin, Abram A.; Shteinberg, Dmitry S. (1927). "".
2114:
Slutskin, Abram A.; Shteinberg, Dmitry S. (1926). "".
864:'s original cavity magnetron developed in 1940 at the 503:
All cavity magnetrons consist of a heated cylindrical
2559: 2342: 1648:
Taschenbuch der drahtlosen Telegraphie und Telephonie
285:
The idea of using a grid for control was invented by
2191:
Magnetrons are discussed in Part II of this article.
1253: 1034:
improved the accuracy of Allied bombers used in the
336:
Early conventional tube systems were limited to the
169:
in 1934, leading to designs by Postumus in 1934 and
27:"Magnetron" redirects here. Not to be confused with 1575: 1419:"Electric Valves: Diodes, Triodes, and Transistors" 515:parallel to the axis of the cavity is imposed by a 2126: 2113: 655:set, the magnetron's waveguide is connected to an 193:magnetron was a radical improvement introduced by 2139: 727:In microwave-excited lighting systems, such as a 280: 3829: 2607:Magnetron collection in the Virtual Valve Museum 2514: 1934:Karlsch, Rainer; Petermann, Heiko, eds. (2007). 1933: 1653:Pocket book of wireless telegraphy and telephony 365:Installed for use between the poles of a strong 2621:Videos of plasmoids created in a microwave oven 2363:"How the search for a 'death ray' led to radar" 2219:Proceedings of the Institute of Radio Engineers 2206:Proceedings of the Institute of Radio Engineers 2183:Proceedings of the Institute of Radio Engineers 1918:Biographical information about Erich Habann: 1682:. Piscataway, New Jersey: IEEE. pp. 17–22. 1960:"Nová metoda k vytvorení netlumenych oscilací" 1823:Biographical information about August Žáček: 1556:Electronics Engineer's Reference Book, 4th ed. 931:in British Columbia, David Zimmerman, states: 817:, there arose an urgent need for a high-power 404:The great advance in magnetron design was the 293:in 1905. In the USA it was later patented by 2793: 2693:High frequency resonator and circuit therefor 778:put this work to use in an attempt to bypass 236: 2545:: CS1 maint: multiple names: authors list ( 2116:Журнал Русского Физико-Химического Общества 1695:"Über eine Anordnung zur Bestimmung von e/m" 1010:The cavity magnetron was widely used during 1550: 1548: 1546: 1484: 1320:"How important was Tizard's Box of Tricks?" 1284: 1280: 1278: 1276: 1274: 1272: 1270: 1268: 798:gigahertz. Žáček, a professor at Prague's 241: 138:(TWT), the magnetron cannot function as an 3838:Science and technology during World War II 2800: 2786: 2560:Jr. Raymond C. Watson (25 November 2009). 1692: 1356: 1354: 1110:Most magnetrons contain a small amount of 767:was looking for new ways to calculate the 2807: 2049: 2047: 1975: 1964:Časopis Pro Pěstování Matematiky a Fysiky 1852: 1191: 1189: 993:Telecommunications Research Establishment 2757:Inductance-capacitance resonance circuit 2233: 2068: 2058:. Piscataway, NJ: IEEE. pp. 217–36. 1644: 1543: 1478: 1360: 1317: 1313: 1311: 1265: 1080: 883: 875: 852: 683: 620: 486: 417: 352: 348: 61: 53: 44: 2404: 2360: 2259: 1861: 1351: 1202: 841:radars, which never strayed beyond the 14: 3830: 2566:. Trafford Publishing. pp. 315–. 2394: 2053: 2044: 2031: 1677: 1531:from the original on 11 September 2017 1450: 1448: 1446: 1444: 1297:from the original on November 15, 2007 1186: 1038:, despite the existence of the German 940:Because France had just fallen to the 2781: 2496:from the original on 5 September 2017 2216: 2203: 2194: 1996: 1957: 1826: 1728:from the original on 23 December 2017 1404:." University of London Ph.D. Thesis. 1308: 1237:. Bournemouth University. 1995–2009. 989:Massachusetts Institute of Technology 987:had been set up on the campus of the 114:using the interaction of a stream of 3232:Three-dimensional integrated circuit 2395:Baxter, James Phinney (III) (1946). 2348: 2180: 1782: 1749: 1287:"Briefcase 'that changed the world'" 1259: 1208: 1088:Warning sign: Non-ionizing radiation 647:History of radar (Centimetric radar) 571: 376:The first major improvement was the 173:in 1935. Production was taken up by 163:General Electric Research Laboratory 3013:Programmable unijunction transistor 2527:from the original on 1 October 2006 2515:EPA,OAR,ORIA,RPD, US (2014-07-16). 2486:"EngineerGuy Video: microwave oven" 2373:from the original on 9 October 2017 2274: 2034:Zeitschrift für Hochfrequenztechnik 1999:Zeitschrift für Hochfrequenztechnik 1441: 1429:from the original on 25 August 2017 1406:December 2004. Accessed 2009-08-23. 923:According to Andy Manning from the 674:microwave semiconductor oscillators 399: 24: 2914:Multi-gate field-effect transistor 1783:Hull, Albert W. (September 1921). 1716:Wolff, Dipl.-Ing. (FH) Christian. 1395:3D Computer Modeling of Magnetrons 482: 25: 3879: 3868:World War II American electronics 2892:Insulated-gate bipolar transistor 2590: 2287:from the original on 4 March 2016 2195:Okabe, Kinjiro (March 1928). "". 1984:Czech Digital Mathematics Library 1715: 1466:from the original on 3 March 2016 1416: 1241:from the original on 26 July 2011 1076: 956:version, built in England by the 821:generator that worked at shorter 361:The bare tube, about 11 cm high. 357:Split-anode magnetron (c. 1935). 246:In a conventional electron tube ( 3863:World War II British electronics 3136:Heterostructure barrier varactor 2863:Chemical field-effect transistor 2011:Czech Industrial Property Office 1558:Newnes-Butterworth, London 1976 1285:Angela Hind (February 5, 2007). 576: 122:, while moving past a series of 42:Device for generating microwaves 3184:Mixed-signal integrated circuit 2634:Information and PDF Data Sheets 2553: 2508: 2478: 2447: 2388: 2361:Harford, Tim (9 October 2017). 2354: 2299: 2268: 2253: 2097: 2062: 2025: 1948: 1912: 1864:Czechoslovak Journal of Physics 1817: 1740: 1709: 1686: 1671: 1632: 1569: 1513: 1340:from the original on 2011-06-17 567: 422:A cross-sectional diagram of a 265:If a third electrode (called a 110:. A cavity magnetron generates 1410: 1387: 1227: 447:while the round holes form an 281:Hull or single-anode magnetron 13: 1: 2056:Tracking the History of Radar 1525:hyperphysics.phy-astr.gsu.edu 1180: 382:negative-resistance magnetron 3215:Silicon controlled rectifier 3077:Organic light-emitting diode 2967:Diffused junction transistor 2425:10.1016/0039-6257(88)90088-4 2129:Український фізичний журнал 1460:electriciantraining.tpub.com 1318:Schroter, B. (Spring 2008). 936:invention changed the world. 925:RAF Air Defence Radar Museum 790:'s Research Laboratories in 413:electron-resonance magnetron 108:linear particle accelerators 102:systems and subsequently in 7: 3019:Static induction transistor 2956:Bipolar junction transistor 2908:MOS field-effect transistor 2880:Fin field-effect transistor 2723: Spencer, P.L. (1946). 2638:(Title is somewhat cryptic) 1801:10.1109/JoAIEE.1921.6594005 1371:10.1109/CAVMAG.2010.5565574 1129: 981:Bell Telephone Laboratories 813:was being developed during 749:power semiconductor devices 722: 629:receiver front end, a 2K25 479:, nor for microwave ovens. 167:Bell Telephone Laboratories 86:which are much less bulky. 10: 3884: 3226:Static induction thyristor 2771: Dexter, S.A. (1959). 2739: Carter, P.S. (1948). 2707: Carter, P.S. (1944). 2691: Carter, P.S. (1944). 2673: Buchholz, H. (1943). 1645:Banneitz, F., ed. (1927). 1036:strategic bombing campaign 843:low-UHF band to start with 758: 679: 644: 495:magnets, modern tubes use 237:Construction and operation 26: 3763: 3663: 3630: 3562: 3499: 3427: 3395:(Hexode, Heptode, Octode) 3333: 3265: 3147:Hybrid integrated circuit 3111: 3039: 2990:Light-emitting transistor 2944: 2826: 2815: 2324:10.1049/ji-3a-1.1946.0188 1982:Available (in Czech) at: 1977:10.21136/CPMF.1924.121857 1073:systems for these needs. 999:was in part developed by 960:Research Laboratories in 37:Magneton (disambiguation) 3442:Backward-wave oscillator 3152:Light emitting capacitor 3008:Point-contact transistor 2978:Junction Gate FET (JFET) 2741:Cavity resonator circuit 2709:Cavity resonator circuit 2163:10.1002/andp.19293930504 1750:Hull, Albert W. (1921). 1024:James Phinney Baxter III 958:General Electric Company 894:University of Birmingham 866:University of Birmingham 616: 441:travel along the surface 345:centimeter wavelengths. 242:Conventional tube design 227:moving target indication 203:University of Birmingham 179:General Electric Company 3453:Crossed-field amplifier 2972:Field-effect transistor 2755: Rex, H.B. (1952). 2413:Survey of Ophthalmology 2397:Scientists Against Time 1896:Available on-line at: 1693:Greinacher, H. (1912). 1136:Crossed-field amplifier 291:Nobel Prize for Physics 211:anti-submarine aircraft 3622:Voltage-regulator tube 3189:MOS integrated circuit 3054:Constant-current diode 3030:Unijunction transistor 2517:"Radiation Protection" 2239:Hollmann, Hans Erich, 1958:Žáček, A. (May 1924). 1089: 938: 929:University of Victoria 889: 881: 873: 870:Science Museum, London 868:, England, now in the 697: 642: 587:is missing information 531:in the case of radar. 500: 477:continuous-wave radars 427: 369: 215:Allies of World War II 87: 59: 51: 3691:Electrolytic detector 3464:Inductive output tube 3280:Low-dropout regulator 3195:Organic semiconductor 3126:Printed circuit board 2962:Darlington transistor 2809:Electronic components 2456:"In the home – ANSTO" 2199:(in Japanese): 284ff. 1928:Märkische Oderzeitung 1827:Fürth, R. H. (1962). 1776:10.1103/PhysRev.18.31 1521:"Magnetron Operation" 1209:Fine, Norman (2019). 1197:La Physique au Canada 1084: 933: 887: 879: 856: 792:Schenectady, New York 687: 665:signal-to-noise ratio 624: 490: 421: 378:split-anode magnetron 356: 349:Split-anode magnetron 144:electronic oscillator 65: 57: 48: 3848:Microwave technology 3509:Beam deflection tube 3178:Metal-oxide varistor 3071:Light-emitting diode 2925:Thin-film transistor 2886:Floating-gate MOSFET 2281:www.radarpages.co.uk 1924:Bradenburger Blätter 1829:"Prof. August Žáček" 1722:www.radartutorial.eu 1165:Radiation Laboratory 985:Radiation Laboratory 847:Albert Beaumont Wood 591:Magnetron sputtering 340:bands, and although 222:traveling-wave tubes 82:, electromagnets or 3485:Traveling-wave tube 3285:Switching regulator 3121:Printed electronics 3098:Step recovery diode 2875:Depletion-load NMOS 2490:www.engineerguy.com 2466:on 5 September 2017 2173:Japanese engineers: 2155:1929AnP...393..658S 2083:1985PhT....38g..60B 1926:(supplement of the 1876:1956CzJPh...6..204. 1845:1962Natur.193..625F 1768:1921PhRv...18...31H 1594:1954Natur.173.1136S 1499:1985PhT....38g..60B 1170:Traveling-wave tube 1160:Microwave EMP Rifle 1071:traveling-wave tube 968:, was taken on the 765:Heinrich Greinacher 342:very high frequency 331:cyclotron radiation 289:, who received the 136:traveling-wave tube 3843:English inventions 3790:Crystal oscillator 3650:Variable capacitor 3325:Switched capacitor 3267:Voltage regulators 3141:Integrated circuit 3025:Tetrode transistor 3003:Pentode transistor 2996:Organic LET (OLET) 2983:Organic FET (OFET) 2630:2023-06-19 at the 2612:2011-07-16 at the 2246:2018-01-14 at the 2143:Annalen der Physik 2106:Soviet physicists: 2103:See for example: 2016:2011-07-18 at the 1989:2011-07-18 at the 1903:2012-03-12 at the 1884:10.1007/BF01699894 1566:, pp. 7-71 to 7-77 1400:2008-10-10 at the 1090: 890: 882: 874: 804:University of Jena 800:Charles University 698: 643: 501: 497:rare-earth magnets 428: 380:, also known as a 370: 128:resonant frequency 88: 80:rare-earth magnets 60: 52: 3825: 3824: 3785:Ceramic resonator 3597:Mercury-arc valve 3549:Video camera tube 3501:Cathode-ray tubes 3261: 3260: 2869:Complementary MOS 2573:978-1-4269-2110-0 2367:BBC World Service 2351:, pp. 56–64. 2040:: 115–20, 135–41. 1602:10.1038/1731136a0 1588:(4415): 1136–37. 1554:L.W. Turner,(ed), 1380:978-1-4244-5609-3 1327:Imperial Engineer 1262:, pp. 24–26. 1145:as early as 1939. 946:Winston Churchill 688:Magnetron from a 614: 613: 124:cavity resonators 16:(Redirected from 3875: 3679:electrical power 3564:Gas-filled tubes 3448:Cavity magnetron 3275:Linear regulator 2824: 2823: 2802: 2795: 2788: 2779: 2778: 2770: 2769: 2765: 2754: 2753: 2749: 2738: 2737: 2733: 2725:Magnetron casing 2722: 2721: 2717: 2706: 2705: 2701: 2690: 2689: 2685: 2676:Cavity resonator 2672: 2671: 2667: 2659: 2658: 2654: 2619:MicrowaveCam.com 2585: 2584: 2582: 2580: 2557: 2551: 2550: 2544: 2536: 2534: 2532: 2512: 2506: 2505: 2503: 2501: 2482: 2476: 2475: 2473: 2471: 2462:. Archived from 2460:www.ansto.gov.au 2451: 2445: 2444: 2408: 2402: 2400: 2392: 2386: 2385: 2380: 2378: 2358: 2352: 2346: 2340: 2339: 2337: 2335: 2326:. Archived from 2303: 2297: 2296: 2294: 2292: 2272: 2266: 2265: 2257: 2251: 2237: 2231: 2226: 2213: 2200: 2190: 2166: 2136: 2131:(in Ukrainian). 2123: 2101: 2095: 2094: 2091:10.1063/1.880982 2066: 2060: 2059: 2051: 2042: 2041: 2029: 2023: 2006: 1981: 1979: 1952: 1946: 1943: 1916: 1910: 1895: 1858: 1856: 1854:10.1038/193625b0 1821: 1815: 1812: 1779: 1744: 1738: 1737: 1735: 1733: 1713: 1707: 1706: 1690: 1684: 1683: 1675: 1669: 1666: 1636: 1630: 1629: 1573: 1567: 1552: 1541: 1540: 1538: 1536: 1517: 1511: 1510: 1507:10.1063/1.880982 1482: 1476: 1475: 1473: 1471: 1452: 1439: 1438: 1436: 1434: 1414: 1408: 1391: 1385: 1384: 1365:. pp. 1–2. 1358: 1349: 1348: 1346: 1345: 1339: 1324: 1315: 1306: 1305: 1303: 1302: 1282: 1263: 1257: 1251: 1250: 1248: 1246: 1231: 1225: 1224: 1220:978-1640-12279-6 1206: 1200: 1193: 1054:on their way to 1052:V-1 flying bombs 950:Sir Henry Tizard 892:In 1940, at the 858:Sir John Randall 788:General Electric 780:Western Electric 635:local oscillator 609: 606: 600: 580: 572: 517:permanent magnet 400:Cavity magnetron 367:permanent magnet 299:horseshoe magnet 94:is a high-power 92:cavity magnetron 21: 3883: 3882: 3878: 3877: 3876: 3874: 3873: 3872: 3828: 3827: 3826: 3821: 3759: 3674:audio and video 3659: 3626: 3558: 3495: 3423: 3404:Photomultiplier 3329: 3257: 3205:Quantum circuit 3113: 3107: 3049:Avalanche diode 3035: 2947: 2940: 2829: 2818: 2811: 2806: 2767: 2761: 2751: 2745: 2735: 2729: 2719: 2713: 2703: 2697: 2687: 2681: 2669: 2663: 2656: 2650: 2632:Wayback Machine 2614:Wayback Machine 2593: 2588: 2578: 2576: 2574: 2558: 2554: 2538: 2537: 2530: 2528: 2513: 2509: 2499: 2497: 2484: 2483: 2479: 2469: 2467: 2452: 2448: 2409: 2405: 2393: 2389: 2376: 2374: 2359: 2355: 2347: 2343: 2333: 2331: 2318:(5): 985–1005. 2304: 2300: 2290: 2288: 2275:Barrett, Dick. 2273: 2269: 2258: 2254: 2248:Wayback Machine 2238: 2234: 2102: 2098: 2067: 2063: 2052: 2045: 2030: 2026: 2018:Wayback Machine 1991:Wayback Machine 1953: 1949: 1917: 1913: 1905:Wayback Machine 1822: 1818: 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2148: 2145:(in German). 2144: 2138: 2134: 2130: 2125: 2122:(2): 395–407. 2121: 2117: 2112: 2111: 2110: 2109: 2105: 2104: 2100: 2092: 2088: 2084: 2080: 2076: 2072: 2071:Physics Today 2065: 2057: 2050: 2048: 2039: 2036:(in German). 2035: 2028: 2019: 2015: 2012: 2008: 2004: 2001:(in German). 2000: 1995: 1992: 1988: 1985: 1978: 1973: 1969: 1965: 1961: 1956: 1955: 1951: 1941: 1937: 1932: 1929: 1925: 1920: 1919: 1915: 1906: 1902: 1899: 1898:Metapress.com 1893: 1889: 1885: 1881: 1877: 1873: 1870:(2): 204–05. 1869: 1865: 1860: 1855: 1850: 1846: 1842: 1839:(4816): 625. 1838: 1834: 1830: 1825: 1824: 1820: 1810: 1806: 1802: 1798: 1795:(9): 715–23. 1794: 1790: 1786: 1781: 1777: 1773: 1769: 1765: 1761: 1757: 1753: 1748: 1747: 1743: 1727: 1723: 1719: 1712: 1704: 1701:(in German). 1700: 1696: 1689: 1681: 1674: 1664: 1662:9783642507892 1658: 1654: 1650: 1649: 1643: 1640: 1639: 1635: 1627: 1623: 1619: 1615: 1611: 1607: 1603: 1599: 1595: 1591: 1587: 1583: 1579: 1572: 1565: 1564:9780408001687 1561: 1557: 1551: 1549: 1547: 1530: 1526: 1522: 1516: 1508: 1504: 1500: 1496: 1492: 1488: 1487:Physics Today 1481: 1465: 1461: 1457: 1451: 1449: 1447: 1445: 1428: 1424: 1420: 1413: 1407: 1403: 1399: 1396: 1390: 1382: 1376: 1372: 1368: 1364: 1357: 1355: 1336: 1332: 1328: 1321: 1314: 1312: 1296: 1292: 1288: 1281: 1279: 1277: 1275: 1273: 1271: 1269: 1261: 1256: 1240: 1236: 1230: 1222: 1216: 1212: 1205: 1198: 1192: 1190: 1185: 1176: 1173: 1171: 1168: 1166: 1163: 1161: 1158: 1156: 1153: 1151: 1148: 1146: 1142: 1139: 1137: 1134: 1133: 1127: 1125: 1121: 1117: 1113: 1108: 1105: 1103: 1099: 1095: 1087: 1083: 1074: 1072: 1068: 1064: 1059: 1057: 1053: 1049: 1044: 1043: 1037: 1033: 1027: 1025: 1021: 1017: 1013: 1008: 1006: 1002: 1001:Alan Blumlein 998: 994: 990: 986: 982: 978: 976: 975:"Taffy" Bowen 971: 967: 963: 959: 955: 951: 947: 943: 937: 932: 930: 926: 921: 919: 915: 911: 908: 903: 899: 895: 886: 878: 871: 867: 863: 859: 855: 851: 848: 844: 840: 839:night fighter 836: 832: 828: 827:Hans Hollmann 824: 820: 816: 812: 807: 805: 801: 795: 793: 789: 785: 784:Lee De Forest 781: 777: 772: 770: 769:electron mass 766: 756: 754: 750: 746: 742: 741:metal halides 738: 734: 730: 720: 718: 714: 713:cryogenically 709: 708: 703: 695: 691: 686: 677: 675: 670: 666: 660: 658: 654: 648: 640: 636: 632: 628: 623: 608: 598: 592: 588: 585:This section 583: 579: 574: 573: 565: 562: 556: 552: 548: 546: 542: 538: 532: 530: 526: 522: 521:Lorentz force 518: 514: 510: 506: 498: 494: 489: 480: 478: 474: 468: 466: 460: 456: 454: 450: 446: 442: 438: 434: 425: 420: 416: 414: 410: 408: 397: 393: 389: 387: 383: 379: 374: 368: 364: 360: 355: 346: 343: 339: 334: 332: 328: 323: 320: 314: 312: 311:electromagnet 308: 307:Lorentz force 302: 300: 296: 295:Lee de Forest 292: 288: 278: 276: 272: 268: 263: 261: 257: 253: 249: 234: 232: 228: 223: 218: 216: 212: 208: 204: 200: 196: 192: 187: 184: 180: 176: 172: 171:Hans Hollmann 168: 164: 160: 156: 155:Lee de Forest 152: 147: 145: 141: 137: 133: 129: 125: 121: 117: 113: 109: 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Retrieved 2562: 2555: 2529:. Retrieved 2520: 2510: 2498:. Retrieved 2489: 2480: 2468:. Retrieved 2464:the original 2459: 2449: 2416: 2412: 2406: 2396: 2390: 2382: 2375:. Retrieved 2366: 2356: 2344: 2332:. Retrieved 2328:the original 2315: 2311: 2301: 2289:. Retrieved 2280: 2270: 2261: 2255: 2241:"Magnetron," 2235: 2222: 2218: 2212:(4): 652–59. 2209: 2205: 2196: 2189:(6): 715–41. 2186: 2182: 2146: 2142: 2132: 2128: 2119: 2115: 2099: 2077:(7): 60–67. 2074: 2070: 2064: 2055: 2037: 2033: 2027: 2002: 1998: 1967: 1966:(in Czech). 1963: 1950: 1939: 1935: 1927: 1923: 1914: 1867: 1863: 1836: 1832: 1819: 1792: 1788: 1762:(1): 31–57. 1759: 1755: 1742: 1730:. Retrieved 1721: 1711: 1702: 1698: 1688: 1679: 1673: 1652: 1647: 1634: 1585: 1581: 1571: 1555: 1533:. Retrieved 1524: 1515: 1493:(7): 60–67. 1490: 1486: 1480: 1468:. Retrieved 1459: 1431:. Retrieved 1422: 1412: 1405: 1389: 1362: 1342:. Retrieved 1330: 1326: 1299:. Retrieved 1290: 1255: 1243:. Retrieved 1229: 1210: 1204: 1196: 1109: 1106: 1091: 1060: 1041: 1028: 1012:World War II 1009: 979: 948:agreed that 939: 934: 922: 912: 907:James Sayers 898:John Randall 891: 815:World War II 808: 796: 773: 762: 726: 707:mode stirrer 705: 699: 669:marine radar 661: 650: 602: 586: 568:Applications 557: 553: 549: 533: 502: 473:phased array 469: 461: 457: 429: 412: 405: 403: 394: 390: 381: 377: 375: 371: 362: 358: 335: 324: 315: 303: 284: 267:control grid 264: 245: 219: 195:John Randall 190: 188: 148: 91: 89: 75: 71: 3738:Transformer 3480:Sutton tube 3320:Charge pump 3173:Memory cell 3103:Zener diode 3065:Laser diode 2948:transistors 2830:transistors 2596:Information 2135:(2): 22–27. 1118:mixed with 896:in the UK, 823:wavelengths 776:Albert Hull 774:In the US, 729:sulfur lamp 637:and a 1N21 248:vacuum tube 159:Albert Hull 96:vacuum tube 3832:Categories 3810:reed relay 3800:Parametron 3733:Thermistor 3711:resettable 3670:Connector 3631:Adjustable 3607:Nixie tube 3577:Crossatron 3544:Trochotron 3519:Iconoscope 3514:Charactron 3491:X-ray tube 3363:Compactron 3343:Acorn tube 3300:Buck–boost 3221:Solaristor 3083:Photodiode 3060:Gunn diode 3056:(CLD, CRD) 2838:Transistor 2747:US 2611094 2731:US 2444152 2715:US 2408236 2699:US 2357314 2683:US 2357313 2665:US 2315313 2652:US 2123728 2602:Magnetrons 1970:: 378–80. 1423:zipcon.net 1344:2009-08-23 1301:2007-08-16 1181:References 902:Harry Boot 862:Harry Boot 605:March 2023 547:are used. 453:LC circuit 319:hysteresis 199:Harry Boot 183:Telefunken 112:microwaves 3773:Capacitor 3617:Trigatron 3612:Thyratron 3602:Neon lamp 3529:Monoscope 3409:Phototube 3393:Pentagrid 3358:Barretter 3243:Trancitor 3238:Thyristor 3163:Memristor 3088:PIN diode 2865:(ChemFET) 2763:GB 879677 2377:9 October 2349:Fine 2019 2005:: 172–80. 1892:189766320 1705:: 856–64. 1610:0028-0836 1260:Fine 2019 1245:23 August 1122:in their 1102:cataracts 997:H2S radar 819:microwave 733:waveguide 694:heat sink 597:talk page 537:impedance 525:waveguide 509:evacuated 465:waveguide 445:capacitor 409:magnetron 275:amplifier 252:electrons 157:in 1906. 140:amplifier 116:electrons 18:Magnetron 3795:Inductor 3765:Reactive 3743:Varistor 3723:Resistor 3701:Antifuse 3587:Ignitron 3582:Dekatron 3470:Klystron 3459:Gyrotron 3388:Nuvistor 3305:Split-pi 3191:(MOS IC) 3158:Memistor 2916:(MuGFET) 2910:(MOSFET) 2882:(FinFET) 2628:Archived 2610:Archived 2541:cite web 2525:Archived 2494:Archived 2371:Archived 2285:Archived 2244:Archived 2014:Archived 1987:Archived 1901:Archived 1809:51641488 1726:Archived 1618:13165726 1529:Archived 1464:Archived 1427:Archived 1398:Archived 1393:Ma, L. " 1335:Archived 1295:Archived 1291:BBC News 1239:Archived 1150:Klystron 1141:Yoji Ito 1130:See also 1124:filament 1120:tungsten 1086:ISO 7010 1067:klystron 1040:FuG 350 1020:Japanese 835:klystron 723:Lighting 717:hamsters 545:klystron 449:inductor 433:revolver 132:klystron 70:magnets 33:Metatron 29:Megatron 3696:Ferrite 3664:Passive 3655:Varicap 3643:digital 3592:Krytron 3414:Tetrode 3399:Pentode 3253:Varicap 3234:(3D IC) 3210:RF CMOS 3114:devices 2888:(FGMOS) 2819:devices 2645:Patents 2579:24 June 2441:3068822 2433:6071133 2334:22 June 2151:Bibcode 2079:Bibcode 1872:Bibcode 1841:Bibcode 1764:Bibcode 1626:4242031 1590:Bibcode 1495:Bibcode 1116:thorium 1096:of the 962:Wembley 759:History 715:frozen 680:Heating 657:antenna 529:antenna 505:cathode 363:(right) 256:cathode 231:clutter 201:at the 181:(GEC), 175:Philips 118:with a 106:and in 3728:Switch 3419:Triode 3383:Nonode 3348:Audion 3228:(SITh) 3112:Other 3079:(OLED) 3041:Diodes 2992:(LET) 2974:(FET) 2946:Other 2894:(IGBT) 2871:(CMOS) 2858:BioFET 2853:BiCMOS 2768:  2752:  2736:  2720:  2704:  2688:  2670:  2657:  2570:  2521:US EPA 2439:  2431:  1890:  1833:Nature 1807:  1659:  1624:  1616:  1608:  1582:Nature 1562:  1377:  1333:: 10. 1217:  1114:, and 1056:London 1016:German 966:London 831:Berlin 809:While 737:sulfur 589:about 561:S band 493:alnico 386:plates 359:(left) 271:triode 191:cavity 151:Audion 68:alnico 50:shown. 3853:Radar 3805:Relay 3778:types 3716:eFUSE 3487:(TWT) 3475:Maser 3466:(IOT) 3455:(CFA) 3444:(BWO) 3368:Diode 3315:SEPIC 3295:Boost 3248:TRIAC 3217:(SCR) 3180:(MOV) 3154:(LEC) 3073:(LED) 3032:(UJT) 3021:(SIT) 3015:(PUT) 2958:(BJT) 2927:(TFT) 2903:LDMOS 2898:ISFET 2531:5 May 2500:5 May 2470:5 May 2291:5 May 1954:See: 1938:[ 1888:S2CID 1805:S2CID 1746:See: 1732:5 May 1651:[ 1638:See: 1622:S2CID 1535:5 May 1470:5 May 1433:5 May 1338:(PDF) 1323:(PDF) 1155:Maser 1042:Naxos 942:Nazis 811:radar 745:HEMTs 653:radar 651:In a 633:tube 617:Radar 541:radar 451:: an 260:anode 134:or a 100:radar 76:(top) 35:, or 3748:Wire 3706:Fuse 3290:Buck 3143:(IC) 3131:DIAC 3067:(LD) 2936:UMOS 2931:VMOS 2848:PMOS 2843:NMOS 2828:MOS 2581:2011 2568:ISBN 2547:link 2533:2018 2502:2018 2472:2018 2437:PMID 2429:OSTI 2379:2017 2336:2012 2293:2018 1734:2018 1657:ISBN 1614:PMID 1606:ISSN 1560:ISBN 1537:2018 1472:2018 1435:2018 1375:ISBN 1247:2009 1215:ISBN 1094:lens 1069:and 1018:and 1003:and 900:and 860:and 437:Colt 197:and 189:The 90:The 3310:Ćuk 2421:doi 2320:doi 2159:doi 2147:393 2087:doi 1972:doi 1880:doi 1849:doi 1837:193 1797:doi 1772:doi 1598:doi 1586:173 1503:doi 1367:doi 1098:eye 1032:H2S 914:GEC 829:in 700:In 411:or 250:), 161:of 153:by 3834:: 3684:RF 3433:RF 2543:}} 2539:{{ 2523:. 2519:. 2492:. 2488:. 2458:. 2435:. 2427:. 2417:33 2415:. 2381:. 2369:. 2365:. 2316:93 2314:. 2310:. 2283:. 2279:. 2223:18 2221:. 2210:17 2208:. 2187:16 2185:. 2157:. 2120:58 2085:. 2075:38 2073:. 2046:^ 2038:24 2003:32 1968:53 1886:. 1878:. 1866:. 1847:. 1835:. 1831:. 1803:. 1793:40 1791:. 1787:. 1770:. 1760:18 1758:. 1754:. 1724:. 1720:. 1703:14 1620:. 1612:. 1604:. 1596:. 1584:. 1580:. 1545:^ 1527:. 1523:. 1501:. 1491:38 1489:. 1462:. 1458:. 1443:^ 1425:. 1421:. 1373:. 1353:^ 1329:. 1325:. 1310:^ 1293:. 1289:. 1267:^ 1188:^ 1007:. 964:, 954:kW 755:. 739:, 719:. 499:. 467:. 209:, 177:, 31:, 3435:) 3431:( 2801:e 2794:t 2787:v 2583:. 2549:) 2535:. 2504:. 2474:. 2443:. 2423:: 2338:. 2322:: 2295:. 2165:. 2161:: 2153:: 2133:1 2093:. 2089:: 2081:: 2020:. 1993:. 1980:. 1974:: 1907:. 1894:. 1882:: 1874:: 1868:6 1857:. 1851:: 1843:: 1811:. 1799:: 1778:. 1774:: 1766:: 1736:. 1665:. 1628:. 1600:: 1592:: 1539:. 1509:. 1505:: 1497:: 1474:. 1437:. 1383:. 1369:: 1347:. 1331:8 1304:. 1249:. 1223:. 872:. 607:) 603:( 599:. 593:. 39:. 20:)

Index

Magnetron
Megatron
Metatron
Magneton (disambiguation)



alnico
rare-earth magnets
ferrite magnets
vacuum tube
radar
microwave ovens
linear particle accelerators
microwaves
electrons
magnetic field
cavity resonators
resonant frequency
klystron
traveling-wave tube
amplifier
electronic oscillator
Audion
Lee de Forest
Albert Hull
General Electric Research Laboratory
Bell Telephone Laboratories
Hans Hollmann
Philips

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