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Laplace's equation

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285: 1749: 5942: 6323: 1340: 6628: 6060: 1077: 1833:, one physical interpretation of this problem is as follows: fix the temperature on the boundary of the domain according to the given specification of the boundary condition. Allow heat to flow until a stationary state is reached in which the temperature at each point on the domain does not change anymore. The temperature distribution in the interior will then be given by the solution to the corresponding Dirichlet problem. 6375: 64: 5784: 1026: 8858: 6318:{\displaystyle \nabla ^{2}f={\frac {1}{r^{2}}}{\frac {\partial }{\partial r}}\left(r^{2}{\frac {\partial f}{\partial r}}\right)+{\frac {1}{r^{2}\sin \theta }}{\frac {\partial }{\partial \theta }}\left(\sin \theta {\frac {\partial f}{\partial \theta }}\right)+{\frac {1}{r^{2}\sin ^{2}\theta }}{\frac {\partial ^{2}f}{\partial \varphi ^{2}}}=0.} 1335:{\displaystyle \nabla ^{2}f={\frac {1}{r^{2}}}{\frac {\partial }{\partial r}}\left(r^{2}{\frac {\partial f}{\partial r}}\right)+{\frac {1}{r^{2}\sin \theta }}{\frac {\partial }{\partial \theta }}\left(\sin \theta {\frac {\partial f}{\partial \theta }}\right)+{\frac {1}{r^{2}\sin ^{2}\theta }}{\frac {\partial ^{2}f}{\partial \varphi ^{2}}}=0.} 6623:{\displaystyle {\frac {1}{R}}{\frac {d}{dr}}\left(r^{2}{\frac {dR}{dr}}\right)=\lambda ,\qquad {\frac {1}{Y}}{\frac {1}{\sin \theta }}{\frac {\partial }{\partial \theta }}\left(\sin \theta {\frac {\partial Y}{\partial \theta }}\right)+{\frac {1}{Y}}{\frac {1}{\sin ^{2}\theta }}{\frac {\partial ^{2}Y}{\partial \varphi ^{2}}}=-\lambda .} 9417: 1715: 1526: 5524: 843: 830: 6861: 8703: 7723: 2014: 9115: 1531: 4341: 1356: 5888: 7341: 1877:
within the domain where the equation is satisfied. If any two functions are solutions to Laplace's equation (or any linear homogeneous differential equation), their sum (or any linear combination) is also a solution. This property, called the
4772: 688: 6742: 5779:{\displaystyle u(P)={\frac {1}{4\pi }}a^{3}\left(1-{\frac {\rho ^{2}}{a^{2}}}\right)\int _{0}^{2\pi }\int _{0}^{\pi }{\frac {g(\theta ',\varphi ')\sin \theta '}{(a^{2}+\rho ^{2}-2a\rho \cos \Theta )^{\frac {3}{2}}}}d\theta '\,d\varphi '} 7849: 5113: 7217: 5510:
denotes the angle with the vertical axis, which is contrary to the usual American mathematical notation, but agrees with standard European and physical practice. Then the solution of the Laplace equation with Dirichlet boundary values
4070: 3678: 7581: 5268: 1021:{\displaystyle \nabla ^{2}f={\frac {1}{r}}{\frac {\partial }{\partial r}}\left(r{\frac {\partial f}{\partial r}}\right)+{\frac {1}{r^{2}}}{\frac {\partial ^{2}f}{\partial \phi ^{2}}}+{\frac {\partial ^{2}f}{\partial z^{2}}}=0.} 8311: 1893: 8121: 6738: 4187: 3192: 9088: 4837: 5926:
at the center of the sphere is the mean value of its values on the sphere. This mean value property immediately implies that a non-constant harmonic function cannot assume its maximum value at an interior point.
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Thus every analytic function corresponds to a steady incompressible, irrotational, inviscid fluid flow in the plane. The real part is the velocity potential, and the imaginary part is the stream function.
2355: 8853:{\displaystyle {\begin{aligned}\mathbf {g} &=-\nabla V,\\\nabla \cdot \mathbf {g} &=\nabla \cdot (-\nabla V)=-\nabla ^{2}V,\\\implies \nabla ^{2}V&=-\nabla \cdot \mathbf {g} .\end{aligned}}} 4414: 2603: 4105:). It is common to take a different sign convention for this equation than one typically does when defining fundamental solutions. This choice of sign is often convenient to work with because −Δ is a 3337: 4168: 460: 8696: 8357: 8216: 7222: 4101:
rather than a function; but it can be thought of as a limit of functions whose integrals over space are unity, and whose support (the region where the function is non-zero) shrinks to a point (see
3854: 3552: 5375: 2896: 8708: 3912: 7519: 9412:{\displaystyle R(r)=(-1)^{l}{\frac {(l!)^{2}r_{s}^{l}}{(2l)!}}P_{l}\left(1-{\frac {2r}{r_{s}}}\right)+(-1)^{l+1}{\frac {2(2l+1)!}{(l)!^{2}r_{s}^{l+1}}}Q_{l}\left(1-{\frac {2r}{r_{s}}}\right).} 1710:{\displaystyle \nabla ^{2}f={\frac {1}{\sqrt {|g|}}}{\frac {\partial }{\partial \xi ^{i}}}\!\left({\sqrt {|g|}}g^{ij}{\frac {\partial f}{\partial \xi ^{j}}}\right)=0,\qquad (g=\det\{g_{ij}\})} 4668: 5789: 3468: 3230:
be the horizontal and vertical components of the velocity field of a steady incompressible, irrotational flow in two dimensions. The continuity condition for an incompressible flow is that
2455: 2216: 1521:{\displaystyle \nabla ^{2}f={\frac {\partial }{\partial \xi ^{j}}}\left({\frac {\partial f}{\partial \xi ^{k}}}g^{kj}\right)+{\frac {\partial f}{\partial \xi ^{j}}}g^{jm}\Gamma _{mn}^{n}=0,} 4542: 2786: 4172:
The Laplace equation is unchanged under a rotation of coordinates, and hence we can expect that a fundamental solution may be obtained among solutions that only depend upon the distance
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The close connection between the Laplace equation and analytic functions implies that any solution of the Laplace equation has derivatives of all orders, and can be expanded in a
2116: 1072: 7121: 3395: 2955: 4181: 5971:(left to right). Zonal, sectoral, and tesseral harmonics are depicted along the left-most column, the main diagonal, and elsewhere, respectively. (The negative order harmonics 8066: 2721: 383: 8976: 8514: 8490: 6004: 3277: 7989: 6045: 3582: 1860:
alone. For the example of the heat equation it amounts to prescribing the heat flux through the boundary. In particular, at an adiabatic boundary, the normal derivative of
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implies that the value of the line integral connecting two points is independent of the path. The resulting pair of solutions of the Laplace equation are called
8647: 8574: 8554: 8466: 8143: 7897: 3938: 9009: 4776: 5154: 2460: 825:{\displaystyle \nabla ^{2}f={\frac {\partial ^{2}f}{\partial x^{2}}}+{\frac {\partial ^{2}f}{\partial y^{2}}}+{\frac {\partial ^{2}f}{\partial z^{2}}}=0.} 6856:{\displaystyle \lambda \sin ^{2}\theta +{\frac {\sin \theta }{\Theta }}{\frac {d}{d\theta }}\left(\sin \theta {\frac {d\Theta }{d\theta }}\right)=m^{2}} 315: 8364: 5392: 2240: 10022: 4348: 2539: 3282: 4118: 8652: 8315: 7718:{\displaystyle f(r,\theta ,\varphi )=\sum _{\ell =0}^{\infty }\sum _{m=-\ell }^{\ell }f_{\ell }^{m}r^{\ell }Y_{\ell }^{m}(\theta ,\varphi ),} 9982: 3797: 3495: 2825: 3859: 3201: 7457: 2009:{\displaystyle {\frac {\partial ^{2}\psi }{\partial x^{2}}}+{\frac {\partial ^{2}\psi }{\partial y^{2}}}\equiv \psi _{xx}+\psi _{yy}=0.} 5331: 4336:{\displaystyle -1=\iiint _{V}\nabla \cdot \nabla u\,dV=\iint _{S}{\frac {du}{dr}}\,dS=\left.4\pi a^{2}{\frac {du}{dr}}\right|_{r=a}.} 3414: 2383: 2148: 9652:. 8th edition / ed., Brooks/Cole, Cengage Learning, 2013. Chapter 12: Boundary-value Problems in Rectangular Coordinates. p. 462. 4489: 2726: 558:
is a twice-differentiable real-valued function. The Laplace operator therefore maps a scalar function to another scalar function.
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A potential that does not satisfy Laplace's equation together with the boundary condition is an invalid electrostatic potential.
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The gravitational field is conservative and can therefore be expressed as the negative gradient of the gravitational potential:
8865: 4854: 3683: 3402: 3213: 638: 308: 1854:. Physically, this corresponds to the construction of a potential for a vector field whose effect is known at the boundary of 420: 9942: 9914: 9747: 9726: 9685: 9657: 9636: 8185: 8148: 3918:. The Laplace equation can be used in three-dimensional problems in electrostatics and fluid flow just as in two dimensions. 3736: 4423: 2620: 5936: 2369:
also satisfies the Laplace equation. Conversely, given a harmonic function, it is the real part of an analytic function,
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then the continuity condition is the integrability condition for this differential: the resulting function is called the
3348: 2901: 2680:. This construction is only valid locally, or provided that the path does not loop around a singularity. For example, if 10008:
Find out how boundary value problems governed by Laplace's equation may be solved numerically by boundary element method
4599: 2691: 671:. In general, Laplace's equation describes situations of equilibrium, or those that do not depend explicitly on time. 351: 9888: 8942: 301: 166: 3233: 4569: 17: 9676: 9627: 6974: 637:, a generalization of Laplace's equation. Laplace's equation and Poisson's equation are the simplest examples of 388: 6661:. Applying separation of variables again to the second equation gives way to the pair of differential equations 605: 7372: 7336:{\displaystyle r^{2}\nabla ^{2}Y_{\ell }^{m}(\theta ,\varphi )=-\ell (\ell +1)Y_{\ell }^{m}(\theta ,\varphi ).} 6996: 31: 2801:, at least inside a circle that does not enclose a singularity. This is in sharp contrast to solutions of the 10042: 9969: 1882:, is very useful. For example, solutions to complex problems can be constructed by summing simple solutions. 341: 7554: 6992: 2142: 171: 161: 133: 9544: 1039: 10032: 9964: 6938: 6052: 5883:{\displaystyle \cos \Theta =\cos \theta \cos \theta '+\sin \theta \sin \theta '\cos(\varphi -\varphi ')} 9541:
The delta symbol, Δ, is also commonly used to represent a finite change in some quantity, for example,
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is the charge density. The first Maxwell equation is the integrability condition for the differential
10037: 6978: 6367: 225: 118: 109: 8495: 8471: 5974: 7962: 6015: 5480: 469: 8590: 8221: 8002: 1879: 1346: 836: 147: 656:, which are important in multiple branches of physics, notably electrostatics, gravitation, and 7906: 7550: 7111: 3564: 1800: 564: 520: 9512: 8916: 8422: 7844:{\displaystyle r<R={\frac {1}{\limsup _{\ell \to \infty }|f_{\ell }^{m}|^{{1}/{\ell }}}}.} 5497: 5108:{\displaystyle \iiint _{V}\left\,dV=\iiint _{V}\nabla \cdot \left\,dV=\iint _{S}\left\,dS.\,} 4911: 1753: 1032: 681: 634: 496: 241: 43: 8125:
Now, the electric field can be expressed as the negative gradient of the electric potential
7856: 7212:{\displaystyle Y_{\ell }^{m}(\theta ,\varphi )=Ne^{im\varphi }P_{\ell }^{m}(\cos {\theta })} 9821: 9523: 9515:
uses the Laplace equation to show that stable static ferromagnetic suspension is impossible
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Chicone, C.; Mashhoon, B. (2011-11-20). "Nonlocal Gravity: Modified Poisson's Equation".
9631:. 7th ed., Brooks/Cole, Cengage Learning, 2012. Chapter 14: Partial Derivatives. p. 908. 9109: 7936: 4585: 4573: 1890:
Laplace's equation in two independent variables in rectangular coordinates has the form
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Plugging this relation into Gauss's law, we obtain Poisson's equation for electricity,
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are chosen instead. In that case, one needs to expand the solution of known regions in
7882: 7748: 7569: 7522: 7115: 4479: 3489: 2673: 642: 289: 196: 9993: 3673:{\displaystyle \nabla \times (u,v,0)=(v_{x}-u_{y}){\hat {\mathbf {k} }}=\mathbf {0} ,} 9990: 9938: 9910: 9884: 9834: 9809: 9794: 9743: 9722: 9681: 9653: 9632: 9507: 8649:
the gravitational constant. Then Gauss's law for gravitation in differential form is
6882: 4553: 4106: 2024: 1874: 1870: 1851: 1806: 1748: 653: 284: 211: 123: 95: 4109:. The definition of the fundamental solution thus implies that, if the Laplacian of 9829: 9782: 9518: 9497: 4767:{\displaystyle \nabla \cdot \nabla G=-\delta (x-x',y-y',z-z')\qquad {\text{in }}V,} 4588:
is a fundamental solution that also satisfies a suitable condition on the boundary
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and Poisson's equation reduces to Laplace's equation for the electric potential.
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The general solution to Laplace's equation in a ball centered at the origin is a
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Physical applications often take the solution that vanishes at infinity, making
8306:{\displaystyle \nabla \cdot \mathbf {E} =\nabla \cdot (-\nabla V)=-\nabla ^{2}V} 2898:
with suitably defined coefficients whose real and imaginary parts are given by
652:. The twice continuously differentiable solutions of Laplace's equation are the 9502: 8069: 7900: 7572:
of the spherical harmonic functions multiplied by the appropriate scale factor
5941: 4565: 4561: 4475: 2809: 657: 246: 181: 176: 71: 9935:
Handbook of Linear Partial Differential Equations for Engineers and Scientists
10016: 9857: 7930: 4102: 2802: 1830: 1729: 668: 206: 201: 90: 8116:{\displaystyle \nabla \cdot \mathbf {E} ={\frac {\rho }{\varepsilon _{0}}}.} 6733:{\displaystyle {\frac {1}{\Phi }}{\frac {d^{2}\Phi }{d\varphi ^{2}}}=-m^{2}} 5322:
from the center of the sphere is reflected along its radial line to a point
3187:{\displaystyle f(z)=\sum _{n=0}^{\infty }\left+i\sum _{n=1}^{\infty }\left,} 2798: 1829:
is equal to some given function. Since the Laplace operator appears in the
665: 9590:. Its use to represent the Laplacian should not be confused with this use. 329: 261: 80: 9606:. This does not affect the angular portion of the spherical harmonics. 8516:
is surrounded by a conducting material with a specified charge density
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for electricity (Maxwell's first equation) in differential form states
7390: 4065:{\displaystyle \Delta u=u_{xx}+u_{yy}+u_{zz}=-\delta (x-x',y-y',z-z'),} 490: 9786: 9083:{\displaystyle \Psi (r,\theta ,\varphi )=R(r)Y_{l}(\theta ,\varphi ),} 4832:{\displaystyle G=0\quad {\text{if}}\quad (x,y,z)\qquad {\text{on }}S.} 4176:
from the source point. If we choose the volume to be a ball of radius
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represent colatitude and longitude, respectively. In particular, the
5263:{\displaystyle u(x',y',z')=\iiint _{V}Gf\,dV+\iint _{S}G_{n}g\,dS.\,} 4557: 4471: 2523:{\displaystyle \psi _{x}=-\varphi _{y},\quad \psi _{y}=\varphi _{x}.} 6370:, two differential equations result by imposing Laplace's equation: 5478:′. A consequence of this expression for the Green's function is the 2794:
is single-valued only in a region that does not enclose the origin.
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Laplace Equation (particular solutions and boundary value problems)
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Using the differential form of Gauss's law of gravitation, we have
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is integrated over any volume that encloses the source point, then
3200:. These trigonometric functions can themselves be expanded, using 2672:
may be defined by a line integral. The integrability condition and
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will be outside the sphere. The Green's function is then given by
648:
The general theory of solutions to Laplace's equation is known as
9810:"The Laplace and poisson equations in Schwarzschild's space-time" 7421: 6937:
of the second equation at the boundary points of the domain is a
5306:, the Green's function may be obtained by means of a reflection ( 4467: 2363:
satisfies the Laplace equation. A similar calculation shows that
333: 9881:
Introduction to Partial Differential Equations with Applications
8410:{\displaystyle \nabla ^{2}V=-{\frac {\rho }{\varepsilon _{0}}}.} 6632:
The second equation can be simplified under the assumption that
5450:{\displaystyle {\frac {1}{4\pi R}}-{\frac {a}{4\pi \rho R'}},\,} 9988: 63: 9721:. 4th ed., Pearson, 2013. Chapter 2: Electrostatics. p. 83-4. 4914:, (a consequence of the divergence theorem) which states that 3579:
in two space dimensions that is independent of time satisfies
2457:
then the Cauchy–Riemann equations will be satisfied if we set
2350:{\displaystyle u_{yy}=(-v_{x})_{y}=-(v_{y})_{x}=-(u_{x})_{x}.} 9742:. 4th ed., Pearson, 2013. Chapter 3: Potentials. p. 119-121. 9472:, a coordinate system under which Laplace's equation becomes 348:, who first studied its properties. This is often written as 9697:
The approach to spherical harmonics taken here is found in (
4556:. Note that, with the opposite sign convention, this is the 4274: 4409:{\displaystyle {\frac {du}{dr}}=-{\frac {1}{4\pi r^{2}}},} 2598:{\displaystyle d\psi =-\varphi _{y}\,dx+\varphi _{x}\,dy.} 7089:
independent solutions of this form, one for each integer
3332:{\displaystyle \nabla \times \mathbf {V} =v_{x}-u_{y}=0.} 2808:
There is an intimate connection between power series and
561:
If the right-hand side is specified as a given function,
5937:
Spherical harmonics § Laplace's spherical harmonics
4163:{\displaystyle \iiint _{V}\nabla \cdot \nabla u\,dV=-1.} 3279:
and the condition that the flow be irrotational is that
674: 455:{\displaystyle \Delta =\nabla \cdot \nabla =\nabla ^{2}} 8691:{\displaystyle \nabla \cdot \mathbf {g} =-4\pi G\rho .} 8352:{\displaystyle \nabla ^{2}V=-\nabla \cdot \mathbf {E} } 8211:{\displaystyle \nabla \times \mathbf {E} =\mathbf {0} } 7052:
Here the solution was assumed to have the special form
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which is Laplace's equation for gravitational fields.
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which is Poisson's equation for gravitational fields.
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Consider the problem of finding solutions of the form
4466:
Note that, with the opposite sign convention (used in
3849:{\displaystyle \varphi _{x}=-u,\quad \varphi _{y}=-v.} 3547:{\displaystyle \varphi _{x}=-u,\quad \varphi _{y}=-v.} 3476:
satisfies the Laplace equation. The harmonic function
1809:
for Laplace's equation consists of finding a solution
9547: 9118: 9012: 8945: 8919: 8868: 8706: 8655: 8635: 8615: 8593: 8562: 8542: 8522: 8498: 8474: 8454: 8425: 8367: 8318: 8248: 8224: 8188: 8151: 8131: 8078: 8047: 8027: 8005: 7965: 7939: 7909: 7885: 7859: 7756: 7584: 7460: 7225: 7124: 6745: 6669: 6378: 6063: 6018: 5977: 5792: 5527: 5395: 5334: 5300:. For the case of the interior of a sphere of radius 5272:
Thus the Green's function describes the influence at
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The second of Maxwell's equations then implies that
3800: 3739: 3686: 3585: 3498: 3417: 3351: 3285: 3236: 2963: 2904: 2891:{\displaystyle f(z)=\sum _{n=0}^{\infty }c_{n}z^{n},} 2828: 2729: 2694: 2623: 2542: 2463: 2386: 2243: 2151: 2047: 1896: 1534: 1359: 1080: 1042: 846: 691: 608: 567: 523: 499: 472: 423: 391: 354: 6902:
is a linear combination of the complex exponentials
9650:
Differential Equations with Boundary-Value Problems
7557:), and so counting dimensions shows that there are 5914:. A simple consequence of this formula is that if 3907:{\displaystyle \varphi _{xx}+\varphi _{yy}=-\rho ,} 641:. Laplace's equation is also a special case of the 9985:using Laplace's equation from exampleproblems.com. 9582: 9443:of the first and second kind, respectively, while 9411: 9082: 8970: 8931: 8902: 8852: 8690: 8641: 8621: 8601: 8568: 8548: 8528: 8508: 8484: 8460: 8437: 8409: 8351: 8305: 8232: 8210: 8174: 8137: 8115: 8060: 8033: 8013: 7983: 7951: 7921: 7891: 7871: 7843: 7717: 7514:{\displaystyle r^{2}\nabla ^{2}Y=-\ell (\ell +1)Y} 7513: 7354:is called a spherical harmonic function of degree 7335: 7211: 7036:; requiring the solution to be regular throughout 6855: 6732: 6622: 6317: 6039: 5998: 5882: 5778: 5449: 5369: 5262: 5107: 4884: 4831: 4766: 4662: 4536: 4486:. A similar argument shows that in two dimensions 4456: 4408: 4335: 4162: 4064: 3906: 3848: 3780: 3719: 3672: 3546: 3462: 3389: 3331: 3271: 3186: 2949: 2890: 2780: 2715: 2658: 2597: 2522: 2449: 2349: 2210: 2110: 2008: 1709: 1520: 1334: 1066: 1020: 824: 623: 594: 550: 505: 481: 454: 409: 377: 9814:Journal of Mathematical Analysis and Applications 4097:. No function has this property: in fact it is a 1595: 365: 10014: 9979:at EqWorld: The World of Mathematical Equations. 9878: 8419:In the particular case of a source-free region, 7776: 7549:is the expression in spherical coordinates of a 5930: 5518: 5370:{\displaystyle \rho '={\frac {a^{2}}{\rho }}.\,} 4420:that is centered on the source point, and hence 4081:denotes a unit source concentrated at the point 1840:for Laplace's equation specify not the function 1682: 32:Theory of tides § Laplace's tidal equations 9762: 3470:and the irrotationality condition implies that 3463:{\displaystyle \psi _{x}=v,\quad \psi _{y}=-u,} 2450:{\displaystyle f(z)=\varphi (x,y)+i\psi (x,y),} 2211:{\displaystyle u_{x}=v_{y},\quad v_{x}=-u_{y}.} 2027:both satisfy the Laplace equation. That is, if 9852: 9698: 8981: 8240:is also known as the electrostatic condition. 7879:, the solid harmonics with negative powers of 9909:. Providence: American Mathematical Society. 9713: 9711: 9709: 9707: 9680:. 4th ed., Pearson, 2013. Inner front cover. 6923:is regular at the poles of the sphere, where 2611:implies that the integrability condition for 309: 9937:. Boca Raton: Chapman & Hall/CRC Press. 7110:. These angular solutions are a product of 6933:. Imposing this regularity in the solution 5474:denotes the distance to the reflected point 4537:{\displaystyle u=-{\frac {\log(r)}{2\pi }}.} 3339:If we define the differential of a function 2818:in a power series inside a circle of radius 2781:{\displaystyle f(z)=\log z=\log r+i\theta .} 1701: 1685: 9879:Zachmanoglou, E. C.; Thoe, Dale W. (1986). 9670: 9668: 9666: 8986:S. Persides solved the Laplace equation in 4847:is any solution of the Poisson equation in 1869:Solutions of Laplace's equation are called 9869: 9732: 9704: 8808: 8804: 5920:is a harmonic function, then the value of 5307: 3492:. The Cauchy–Riemann equations imply that 2723:then a corresponding analytic function is 2023:The real and imaginary parts of a complex 316: 302: 27:Second-order partial differential equation 9923: 9872:Partial Differential Equations in Physics 9862:Methods of Mathematical Physics, Volume I 9833: 9776: 8903:{\displaystyle \nabla ^{2}V=4\pi G\rho ,} 8468:is specified on the boundary of a region 6047:with respect to the positive order ones.) 5764: 5461:denotes the distance to the source point 5446: 5366: 5259: 5249: 5216: 5137:. In view of the conditions satisfied by 5104: 5094: 5035: 4978: 4960: 4941: 4885:{\displaystyle \nabla \cdot \nabla u=-f,} 4262: 4222: 4144: 3768: 3755: 3720:{\displaystyle \nabla \cdot (u,v)=\rho ,} 3377: 3364: 2585: 2565: 9932: 9807: 9663: 8068:be the permittivity of free space. Then 5940: 2805:, which generally have less regularity. 1747: 10023:Elliptic partial differential equations 9983:Example initial-boundary value problems 9484:, a general case of Laplace's equation. 8175:{\displaystyle \mathbf {E} =-\nabla V,} 7565:linearly independent such polynomials. 7118:, and associated Legendre polynomials: 3926: 3781:{\displaystyle d\varphi =-u\,dx-v\,dy,} 2380:(at least locally). If a trial form is 639:elliptic partial differential equations 517:operator (also symbolized "grad"), and 14: 10015: 9648:Zill, Dennis G, and Michael R Cullen. 9460:is an arbitrary non-negative integer. 6995:, whose solution is a multiple of the 6981:. Furthermore, a change of variables 4457:{\displaystyle u={\frac {1}{4\pi r}}.} 3921: 3214:Laplace equation for irrotational flow 2659:{\displaystyle \psi _{xy}=\psi _{yx},} 1743: 9989: 9904: 9628:Calculus : Early Transcendentals 8492:, then it is uniquely determined. If 2018: 1770:) with Dirichlet boundary conditions 675:Forms in different coordinate systems 9758: 9756: 9583:{\displaystyle \Delta x=x_{1}-x_{2}} 8041:be the electric charge density, and 7747:. Such an expansion is valid in the 2111:{\displaystyle f(z)=u(x,y)+iv(x,y),} 1885: 1732:relative to the new coordinates and 1067:{\displaystyle (r,\theta ,\varphi )} 7994: 7534:. In fact, for any such solution, 6962:for some non-negative integer with 6877:is a complex constant, but because 5945:Real (Laplace) spherical harmonics 5890:is the cosine of the angle between 4579: 3390:{\displaystyle d\psi =v\,dx-u\,dy,} 2950:{\displaystyle c_{n}=a_{n}+ib_{n}.} 2227:is the first partial derivative of 30:For Laplace's tidal equations, see 24: 9898: 9548: 9013: 8947: 8870: 8832: 8810: 8785: 8769: 8757: 8739: 8726: 8656: 8501: 8477: 8369: 8338: 8320: 8291: 8275: 8263: 8249: 8189: 8163: 8079: 7916: 7786: 7628: 7472: 7237: 6991:transforms this equation into the 6821: 6781: 6693: 6675: 6592: 6578: 6522: 6514: 6488: 6484: 6293: 6279: 6223: 6215: 6189: 6185: 6138: 6130: 6103: 6099: 6065: 5799: 5732: 5024: 5012: 4998: 4967: 4961: 4948: 4942: 4864: 4858: 4683: 4677: 4482:force, arising in the solution of 4216: 4210: 4138: 4132: 3942: 3687: 3586: 3286: 3099: 2995: 2860: 2118:then the necessary condition that 1952: 1938: 1915: 1901: 1642: 1634: 1579: 1575: 1536: 1492: 1462: 1454: 1414: 1406: 1382: 1378: 1361: 1310: 1296: 1240: 1232: 1206: 1202: 1155: 1147: 1120: 1116: 1082: 996: 982: 959: 945: 907: 899: 879: 875: 848: 800: 786: 763: 749: 726: 712: 693: 609: 500: 493:operator (also symbolized "div"), 473: 443: 436: 430: 424: 392: 356: 25: 10054: 9952: 9753: 7381:is a normalization constant, and 6006:would be shown rotated about the 4663:{\displaystyle G(x,y,z;x',y',z')} 3558: 2530:This relation does not determine 8994:. Using the canonical variables 8839: 8746: 8712: 8663: 8595: 8345: 8256: 8226: 8204: 8196: 8153: 8086: 8061:{\displaystyle \varepsilon _{0}} 8007: 4568:), which is the solution of the 3935:of Laplace's equation satisfies 3663: 3649: 3293: 2716:{\displaystyle \varphi =\log r,} 378:{\displaystyle \nabla ^{2}\!f=0} 283: 62: 9928:. Philadelphia: W. B. Saunders. 9801: 9765:Journal of Mathematical Physics 9740:Introduction to Electrodynamics 9719:Introduction to Electrodynamics 9677:Introduction to Electrodynamics 8971:{\displaystyle \nabla ^{2}V=0,} 8448:If the electrostatic potential 7959:), to match the terms and find 6453: 4817: 4795: 4789: 4752: 3823: 3521: 3437: 2493: 2178: 2141:be differentiable and that the 1672: 10028:Eponymous equations of physics 9926:Partial Differential Equations 9907:Partial Differential Equations 9691: 9642: 9619: 9593: 9535: 9321: 9315: 9307: 9292: 9271: 9261: 9201: 9192: 9166: 9156: 9144: 9134: 9128: 9122: 9074: 9062: 9049: 9043: 9034: 9016: 8805: 8775: 8763: 8582: 8509:{\displaystyle {\mathcal {R}}} 8485:{\displaystyle {\mathcal {R}}} 8281: 8269: 8182:if the field is irrotational, 7813: 7792: 7783: 7734:are constants and the factors 7709: 7697: 7606: 7588: 7505: 7493: 7396:, or polar angle, ranges from 7373:associated Legendre polynomial 7327: 7315: 7297: 7285: 7273: 7261: 7206: 7192: 7152: 7140: 6997:associated Legendre polynomial 6898:is necessarily an integer and 5999:{\displaystyle Y_{\ell }^{-m}} 5877: 5860: 5736: 5688: 5669: 5647: 5537: 5531: 5517:inside the sphere is given by( 5194: 5161: 4814: 4796: 4749: 4698: 4657: 4606: 4517: 4511: 4180:around the source point, then 4056: 4005: 3794:may be constructed to satisfy 3705: 3693: 3653: 3642: 3616: 3610: 3592: 3272:{\displaystyle u_{x}+v_{y}=0,} 3194:which is a Fourier series for 2973: 2967: 2838: 2832: 2739: 2733: 2441: 2429: 2417: 2405: 2396: 2390: 2335: 2321: 2306: 2292: 2277: 2260: 2102: 2090: 2078: 2066: 2057: 2051: 1704: 1673: 1612: 1604: 1566: 1558: 1061: 1043: 664:, the Laplace equation is the 589: 571: 545: 527: 13: 1: 9612: 8990:on hypersurfaces of constant 7984:{\displaystyle f_{\ell }^{m}} 7424:, may assume all values with 7012:. Finally, the equation for 6040:{\displaystyle 90^{\circ }/m} 5931:Laplace's spherical harmonics 5131:denote normal derivatives on 3401:because it is constant along 3207: 1344:More generally, in arbitrary 482:{\displaystyle \nabla \cdot } 342:partial differential equation 9835:10.1016/0022-247X(73)90277-1 8609:be the gravitational field, 8602:{\displaystyle \mathbf {g} } 8233:{\displaystyle \mathbf {E} } 8014:{\displaystyle \mathbf {E} } 6885:whose period evenly divides 5519:Zachmanoglou & Thoe 1986 5149:, this result simplifies to 4900:assumes the boundary values 2678:conjugate harmonic functions 7: 9965:Encyclopedia of Mathematics 9874:. New York: Academic Press. 9463: 9110:spherical harmonic function 8982:In the Schwarzschild metric 7413:at the South Pole, and the 5385:is inside the sphere, then 3405:. The first derivatives of 2536:, but only its increments: 1838:Neumann boundary conditions 410:{\displaystyle \Delta f=0,} 10: 10059: 9846: 9699:Courant & Hilbert 1962 8536:, and if the total charge 7454:of the eigenvalue problem 7018:has solutions of the form 6941:that forces the parameter 5934: 4182:Gauss's divergence theorem 3788:so the electric potential 3211: 2812:. If we expand a function 2688:are polar coordinates and 1880:principle of superposition 1846:itself on the boundary of 1798: 624:{\displaystyle \Delta f=h} 29: 9924:Petrovsky, I. G. (1967). 8218:. The irrotationality of 7922:{\displaystyle r=\infty } 6973:; this is also explained 4560:generated by a pointlike 2605:The Laplace equation for 1752:Laplace's equation on an 226:Geometric function theory 172:Cauchy's integral formula 162:Cauchy's integral theorem 9933:Polyanin, A. D. (2002). 9529: 7114:, here represented as a 7075:. For a given value of 6979:orbital angular momentum 6908:. The solution function 5481:Poisson integral formula 2143:Cauchy–Riemann equations 595:{\displaystyle h(x,y,z)} 551:{\displaystyle f(x,y,z)} 134:Cauchy–Riemann equations 9870:Sommerfeld, A. (1949). 8988:Schwarzschild spacetime 8932:{\displaystyle \rho =0} 8438:{\displaystyle \rho =0} 8021:be the electric field, 7435:. For a fixed integer 7112:trigonometric functions 6939:Sturm–Liouville problem 6368:separation of variables 3202:multiple angle formulae 1347:curvilinear coordinates 837:cylindrical coordinates 682:rectangular coordinates 506:{\displaystyle \nabla } 119:Complex-valued function 9584: 9413: 9084: 8972: 8933: 8904: 8854: 8692: 8643: 8629:the mass density, and 8623: 8603: 8570: 8550: 8530: 8510: 8486: 8462: 8439: 8411: 8353: 8307: 8234: 8212: 8176: 8139: 8117: 8062: 8035: 8015: 7985: 7953: 7923: 7893: 7873: 7872:{\displaystyle r>R} 7845: 7719: 7656: 7632: 7553:that is harmonic (see 7551:homogeneous polynomial 7515: 7400:at the North Pole, to 7337: 7213: 6857: 6734: 6624: 6319: 6051:Laplace's equation in 6048: 6041: 6000: 5884: 5780: 5451: 5371: 5326:that is at a distance 5264: 5109: 4886: 4833: 4768: 4664: 4538: 4458: 4416:on a sphere of radius 4410: 4337: 4164: 4066: 3908: 3850: 3782: 3721: 3674: 3548: 3464: 3391: 3333: 3273: 3188: 3103: 2999: 2951: 2892: 2864: 2782: 2717: 2660: 2599: 2524: 2451: 2351: 2212: 2112: 2010: 1801:Boundary value problem 1796: 1711: 1522: 1336: 1068: 1022: 826: 625: 596: 552: 507: 483: 456: 411: 379: 290:Mathematics portal 9905:Evans, L. C. (1998). 9808:Persides, S. (1973). 9585: 9414: 9085: 8973: 8934: 8905: 8855: 8693: 8644: 8624: 8622:{\displaystyle \rho } 8604: 8571: 8551: 8531: 8529:{\displaystyle \rho } 8511: 8487: 8463: 8440: 8412: 8354: 8308: 8235: 8213: 8177: 8140: 8118: 8063: 8036: 8034:{\displaystyle \rho } 8016: 7986: 7954: 7924: 7894: 7874: 7846: 7720: 7633: 7612: 7516: 7338: 7214: 6858: 6735: 6625: 6320: 6053:spherical coordinates 6042: 6001: 5944: 5885: 5781: 5500:for the source point 5498:spherical coordinates 5452: 5372: 5265: 5110: 4887: 4834: 4769: 4665: 4539: 4459: 4411: 4338: 4165: 4067: 3909: 3851: 3783: 3722: 3675: 3549: 3482:that is conjugate to 3465: 3392: 3334: 3274: 3189: 3083: 2979: 2952: 2893: 2844: 2783: 2718: 2661: 2600: 2525: 2452: 2352: 2213: 2113: 2011: 1751: 1712: 1523: 1337: 1069: 1033:spherical coordinates 1023: 827: 626: 597: 553: 508: 484: 457: 412: 380: 242:Augustin-Louis Cauchy 44:Mathematical analysis 10043:Pierre-Simon Laplace 9994:"Laplace's Equation" 9864:, Wiley-Interscience 9738:Griffiths, David J. 9717:Griffiths, David J. 9674:Griffiths, David J. 9545: 9524:Fundamental solution 9470:6-sphere coordinates 9454:Schwarzschild radius 9116: 9010: 8943: 8917: 8866: 8704: 8653: 8633: 8613: 8591: 8560: 8540: 8520: 8496: 8472: 8452: 8423: 8365: 8316: 8246: 8222: 8186: 8149: 8129: 8076: 8045: 8025: 8003: 7963: 7937: 7907: 7883: 7857: 7754: 7582: 7458: 7223: 7122: 6743: 6667: 6376: 6061: 6016: 5975: 5961:(top to bottom) and 5790: 5525: 5393: 5332: 5310:): the source point 5155: 4920: 4910:, then we may apply 4855: 4777: 4674: 4600: 4490: 4424: 4349: 4188: 4119: 4074:Dirac delta function 3939: 3933:fundamental solution 3927:Fundamental solution 3860: 3798: 3737: 3684: 3583: 3567:, an electric field 3496: 3415: 3349: 3283: 3234: 2961: 2902: 2826: 2727: 2692: 2621: 2540: 2461: 2384: 2241: 2149: 2129:be analytic is that 2045: 1894: 1532: 1357: 1078: 1040: 844: 689: 606: 565: 521: 497: 470: 421: 389: 352: 346:Pierre-Simon Laplace 252:Carl Friedrich Gauss 187:Isolated singularity 129:Holomorphic function 9883:. New York: Dover. 9826:1973JMAA...43..571P 9354: 9189: 7980: 7952:{\displaystyle r=0} 7810: 7696: 7671: 7407:at the Equator, to 7314: 7260: 7191: 7139: 7116:complex exponential 5995: 5640: 5625: 4574:incompressible flow 4572:in two-dimensional 3922:In three dimensions 3565:Maxwell's equations 3218:Let the quantities 2790:However, the angle 2237:. It follows that 1825:on the boundary of 1744:Boundary conditions 1738:Christoffel symbols 1508: 139:Formal power series 101:Unit complex number 10033:Harmonic functions 9991:Weisstein, Eric W. 9960:"Laplace equation" 9580: 9513:Earnshaw's theorem 9493:Quadrature domains 9488:Spherical harmonic 9482:Helmholtz equation 9441:Legendre functions 9409: 9334: 9175: 9080: 8968: 8929: 8900: 8850: 8848: 8688: 8639: 8619: 8599: 8566: 8546: 8526: 8506: 8482: 8458: 8435: 8407: 8349: 8303: 8230: 8208: 8172: 8135: 8113: 8058: 8031: 8011: 7981: 7966: 7949: 7919: 7889: 7869: 7841: 7796: 7790: 7715: 7682: 7657: 7570:linear combination 7523:linear combination 7511: 7333: 7300: 7246: 7209: 7177: 7125: 6947:to be of the form 6853: 6730: 6620: 6315: 6049: 6037: 5996: 5978: 5880: 5776: 5626: 5608: 5447: 5367: 5260: 5105: 4882: 4829: 4764: 4660: 4534: 4480:inverse-square law 4454: 4406: 4333: 4160: 4062: 3904: 3846: 3778: 3717: 3670: 3544: 3490:velocity potential 3460: 3387: 3329: 3269: 3184: 2947: 2888: 2822:, this means that 2778: 2713: 2656: 2595: 2520: 2447: 2347: 2208: 2108: 2019:Analytic functions 2006: 1871:harmonic functions 1797: 1707: 1518: 1491: 1332: 1064: 1018: 822: 660:. In the study of 654:harmonic functions 643:Helmholtz equation 635:Poisson's equation 621: 592: 548: 503: 479: 452: 407: 375: 340:is a second-order 338:Laplace's equation 217:Laplace's equation 197:Argument principle 9944:978-1-58488-299-2 9916:978-0-8218-0772-9 9787:10.1063/1.3702449 9748:978-1-108-42041-9 9727:978-1-108-42041-9 9686:978-1-108-42041-9 9658:978-1-111-82706-9 9637:978-0-538-49790-9 9508:Bateman transform 9399: 9356: 9251: 9208: 8642:{\displaystyle G} 8569:{\displaystyle V} 8549:{\displaystyle Q} 8461:{\displaystyle V} 8402: 8138:{\displaystyle V} 8108: 7892:{\displaystyle r} 7836: 7775: 7439:, every solution 6993:Legendre equation 6883:periodic function 6833: 6799: 6784: 6712: 6678: 6606: 6572: 6547: 6529: 6495: 6480: 6462: 6437: 6402: 6387: 6307: 6273: 6230: 6196: 6181: 6145: 6110: 6095: 5751: 5747: 5601: 5556: 5441: 5412: 5361: 4821: 4793: 4756: 4596:. For instance, 4554:natural logarithm 4529: 4449: 4401: 4370: 4345:It follows that 4311: 4260: 4107:positive operator 3656: 2025:analytic function 1966: 1929: 1886:In two dimensions 1852:normal derivative 1807:Dirichlet problem 1763:and outer radius 1728:is the Euclidean 1656: 1616: 1593: 1571: 1570: 1476: 1428: 1396: 1324: 1290: 1247: 1213: 1198: 1162: 1127: 1112: 1010: 973: 939: 914: 886: 871: 814: 777: 740: 326: 325: 212:Harmonic function 124:Analytic function 110:Complex functions 96:Complex conjugate 16:(Redirected from 10050: 10038:Fourier analysis 10004: 10003: 9973: 9948: 9929: 9920: 9894: 9875: 9865: 9854:Courant, Richard 9840: 9839: 9837: 9805: 9799: 9798: 9780: 9760: 9751: 9736: 9730: 9715: 9702: 9701:, §V.8, §VII.5). 9695: 9689: 9672: 9661: 9646: 9640: 9625:Stewart, James. 9623: 9607: 9605: 9597: 9591: 9589: 9587: 9586: 9581: 9579: 9578: 9566: 9565: 9539: 9519:Vector Laplacian 9498:Potential theory 9459: 9456:. The parameter 9451: 9438: 9429: 9418: 9416: 9415: 9410: 9405: 9401: 9400: 9398: 9397: 9388: 9380: 9367: 9366: 9357: 9355: 9353: 9342: 9333: 9332: 9313: 9287: 9285: 9284: 9257: 9253: 9252: 9250: 9249: 9240: 9232: 9219: 9218: 9209: 9207: 9190: 9188: 9183: 9174: 9173: 9154: 9152: 9151: 9107: 9089: 9087: 9086: 9081: 9061: 9060: 9006:the solution is 9005: 9001: 8997: 8993: 8977: 8975: 8974: 8969: 8955: 8954: 8938: 8936: 8935: 8930: 8913:In empty space, 8909: 8907: 8906: 8901: 8878: 8877: 8859: 8857: 8856: 8851: 8849: 8842: 8818: 8817: 8793: 8792: 8749: 8715: 8697: 8695: 8694: 8689: 8666: 8648: 8646: 8645: 8640: 8628: 8626: 8625: 8620: 8608: 8606: 8605: 8600: 8598: 8576:is also unique. 8575: 8573: 8572: 8567: 8555: 8553: 8552: 8547: 8535: 8533: 8532: 8527: 8515: 8513: 8512: 8507: 8505: 8504: 8491: 8489: 8488: 8483: 8481: 8480: 8467: 8465: 8464: 8459: 8444: 8442: 8441: 8436: 8416: 8414: 8413: 8408: 8403: 8401: 8400: 8388: 8377: 8376: 8358: 8356: 8355: 8350: 8348: 8328: 8327: 8312: 8310: 8309: 8304: 8299: 8298: 8259: 8239: 8237: 8236: 8231: 8229: 8217: 8215: 8214: 8209: 8207: 8199: 8181: 8179: 8178: 8173: 8156: 8144: 8142: 8141: 8136: 8122: 8120: 8119: 8114: 8109: 8107: 8106: 8094: 8089: 8067: 8065: 8064: 8059: 8057: 8056: 8040: 8038: 8037: 8032: 8020: 8018: 8017: 8012: 8010: 7990: 7988: 7987: 7982: 7979: 7974: 7958: 7956: 7955: 7950: 7928: 7926: 7925: 7920: 7898: 7896: 7895: 7890: 7878: 7876: 7875: 7870: 7850: 7848: 7847: 7842: 7837: 7835: 7834: 7833: 7832: 7827: 7822: 7816: 7809: 7804: 7795: 7789: 7770: 7742: 7733: 7724: 7722: 7721: 7716: 7695: 7690: 7681: 7680: 7670: 7665: 7655: 7650: 7631: 7626: 7577: 7564: 7548: 7533: 7520: 7518: 7517: 7512: 7480: 7479: 7470: 7469: 7453: 7438: 7434: 7419: 7412: 7406: 7399: 7395: 7388: 7384: 7380: 7370: 7361: 7357: 7353: 7342: 7340: 7339: 7334: 7313: 7308: 7259: 7254: 7245: 7244: 7235: 7234: 7218: 7216: 7215: 7210: 7205: 7190: 7185: 7176: 7175: 7138: 7133: 7109: 7094: 7088: 7080: 7074: 7048: 7041: 7035: 7017: 7011: 6990: 6977:in terms of the 6972: 6961: 6946: 6936: 6932: 6922: 6907: 6901: 6897: 6891: 6880: 6876: 6870: 6865:for some number 6862: 6860: 6859: 6854: 6852: 6851: 6839: 6835: 6834: 6832: 6824: 6816: 6800: 6798: 6787: 6785: 6780: 6769: 6758: 6757: 6739: 6737: 6736: 6731: 6729: 6728: 6713: 6711: 6710: 6709: 6696: 6692: 6691: 6681: 6679: 6671: 6660: 6637: 6629: 6627: 6626: 6621: 6607: 6605: 6604: 6603: 6590: 6586: 6585: 6575: 6573: 6571: 6564: 6563: 6550: 6548: 6540: 6535: 6531: 6530: 6528: 6520: 6512: 6496: 6494: 6483: 6481: 6479: 6465: 6463: 6455: 6443: 6439: 6438: 6436: 6428: 6420: 6418: 6417: 6403: 6401: 6390: 6388: 6380: 6365: 6324: 6322: 6321: 6316: 6308: 6306: 6305: 6304: 6291: 6287: 6286: 6276: 6274: 6272: 6265: 6264: 6255: 6254: 6241: 6236: 6232: 6231: 6229: 6221: 6213: 6197: 6195: 6184: 6182: 6180: 6170: 6169: 6156: 6151: 6147: 6146: 6144: 6136: 6128: 6126: 6125: 6111: 6109: 6098: 6096: 6094: 6093: 6081: 6073: 6072: 6046: 6044: 6043: 6038: 6033: 6028: 6027: 6011: 6005: 6003: 6002: 5997: 5994: 5986: 5970: 5960: 5953: 5925: 5919: 5913: 5901: 5889: 5887: 5886: 5881: 5876: 5853: 5827: 5785: 5783: 5782: 5777: 5775: 5763: 5752: 5750: 5749: 5748: 5740: 5713: 5712: 5700: 5699: 5686: 5685: 5668: 5657: 5642: 5639: 5634: 5624: 5616: 5607: 5603: 5602: 5600: 5599: 5590: 5589: 5580: 5567: 5566: 5557: 5555: 5544: 5516: 5509: 5505: 5495: 5491: 5487: 5473: 5466: 5460: 5456: 5454: 5453: 5448: 5442: 5440: 5439: 5418: 5413: 5411: 5397: 5384: 5376: 5374: 5373: 5368: 5362: 5357: 5356: 5347: 5342: 5321: 5315: 5305: 5299: 5293: 5287: 5269: 5267: 5266: 5261: 5245: 5244: 5235: 5234: 5209: 5208: 5193: 5182: 5171: 5148: 5142: 5136: 5114: 5112: 5111: 5106: 5093: 5089: 5088: 5087: 5072: 5071: 5054: 5053: 5034: 5030: 4997: 4996: 4977: 4973: 4932: 4931: 4912:Green's identity 4909: 4905: 4899: 4891: 4889: 4888: 4883: 4850: 4846: 4838: 4836: 4835: 4830: 4822: 4819: 4794: 4791: 4773: 4771: 4770: 4765: 4757: 4754: 4748: 4731: 4714: 4669: 4667: 4666: 4661: 4656: 4645: 4634: 4595: 4591: 4586:Green's function 4580:Green's function 4551: 4543: 4541: 4540: 4535: 4530: 4528: 4520: 4503: 4484:Poisson equation 4463: 4461: 4460: 4455: 4450: 4448: 4434: 4419: 4415: 4413: 4412: 4407: 4402: 4400: 4399: 4398: 4379: 4371: 4369: 4361: 4353: 4342: 4340: 4339: 4334: 4329: 4328: 4317: 4313: 4312: 4310: 4302: 4294: 4292: 4291: 4261: 4259: 4251: 4243: 4241: 4240: 4209: 4208: 4179: 4175: 4169: 4167: 4166: 4161: 4131: 4130: 4114: 4096: 4080: 4071: 4069: 4068: 4063: 4055: 4038: 4021: 3995: 3994: 3979: 3978: 3963: 3962: 3916:Poisson equation 3913: 3911: 3910: 3905: 3891: 3890: 3875: 3874: 3855: 3853: 3852: 3847: 3833: 3832: 3810: 3809: 3793: 3787: 3785: 3784: 3779: 3732: 3726: 3724: 3723: 3718: 3679: 3677: 3676: 3671: 3666: 3658: 3657: 3652: 3647: 3641: 3640: 3628: 3627: 3578: 3553: 3551: 3550: 3545: 3531: 3530: 3508: 3507: 3487: 3481: 3475: 3469: 3467: 3466: 3461: 3447: 3446: 3427: 3426: 3410: 3396: 3394: 3393: 3388: 3344: 3338: 3336: 3335: 3330: 3322: 3321: 3309: 3308: 3296: 3278: 3276: 3275: 3270: 3259: 3258: 3246: 3245: 3229: 3223: 3199: 3193: 3191: 3190: 3185: 3180: 3176: 3163: 3162: 3153: 3152: 3128: 3127: 3118: 3117: 3102: 3097: 3076: 3072: 3059: 3058: 3049: 3048: 3024: 3023: 3014: 3013: 2998: 2993: 2956: 2954: 2953: 2948: 2943: 2942: 2927: 2926: 2914: 2913: 2897: 2895: 2894: 2889: 2884: 2883: 2874: 2873: 2863: 2858: 2821: 2817: 2793: 2787: 2785: 2784: 2779: 2722: 2720: 2719: 2714: 2687: 2683: 2671: 2665: 2663: 2662: 2657: 2652: 2651: 2636: 2635: 2616: 2610: 2604: 2602: 2601: 2596: 2584: 2583: 2564: 2563: 2535: 2529: 2527: 2526: 2521: 2516: 2515: 2503: 2502: 2489: 2488: 2473: 2472: 2456: 2454: 2453: 2448: 2379: 2368: 2362: 2356: 2354: 2353: 2348: 2343: 2342: 2333: 2332: 2314: 2313: 2304: 2303: 2285: 2284: 2275: 2274: 2256: 2255: 2236: 2233:with respect to 2232: 2226: 2217: 2215: 2214: 2209: 2204: 2203: 2188: 2187: 2174: 2173: 2161: 2160: 2140: 2134: 2128: 2117: 2115: 2114: 2109: 2040: 2015: 2013: 2012: 2007: 1999: 1998: 1983: 1982: 1967: 1965: 1964: 1963: 1950: 1946: 1945: 1935: 1930: 1928: 1927: 1926: 1913: 1909: 1908: 1898: 1865: 1859: 1849: 1845: 1828: 1824: 1818: 1814: 1795: 1780: 1769: 1762: 1735: 1727: 1716: 1714: 1713: 1708: 1700: 1699: 1662: 1658: 1657: 1655: 1654: 1653: 1640: 1632: 1630: 1629: 1617: 1615: 1607: 1602: 1594: 1592: 1591: 1590: 1574: 1572: 1569: 1561: 1556: 1552: 1544: 1543: 1527: 1525: 1524: 1519: 1507: 1502: 1490: 1489: 1477: 1475: 1474: 1473: 1460: 1452: 1447: 1443: 1442: 1441: 1429: 1427: 1426: 1425: 1412: 1404: 1397: 1395: 1394: 1393: 1377: 1369: 1368: 1352: 1341: 1339: 1338: 1333: 1325: 1323: 1322: 1321: 1308: 1304: 1303: 1293: 1291: 1289: 1282: 1281: 1272: 1271: 1258: 1253: 1249: 1248: 1246: 1238: 1230: 1214: 1212: 1201: 1199: 1197: 1187: 1186: 1173: 1168: 1164: 1163: 1161: 1153: 1145: 1143: 1142: 1128: 1126: 1115: 1113: 1111: 1110: 1098: 1090: 1089: 1073: 1071: 1070: 1065: 1027: 1025: 1024: 1019: 1011: 1009: 1008: 1007: 994: 990: 989: 979: 974: 972: 971: 970: 957: 953: 952: 942: 940: 938: 937: 925: 920: 916: 915: 913: 905: 897: 887: 885: 874: 872: 864: 856: 855: 831: 829: 828: 823: 815: 813: 812: 811: 798: 794: 793: 783: 778: 776: 775: 774: 761: 757: 756: 746: 741: 739: 738: 737: 724: 720: 719: 709: 701: 700: 650:potential theory 630: 628: 627: 622: 601: 599: 598: 593: 557: 555: 554: 549: 512: 510: 509: 504: 488: 486: 485: 480: 464:Laplace operator 461: 459: 458: 453: 451: 450: 416: 414: 413: 408: 384: 382: 381: 376: 364: 363: 318: 311: 304: 288: 287: 272:Karl Weierstrass 267:Bernhard Riemann 257:Jacques Hadamard 86:Imaginary number 66: 56:Complex analysis 50: 48:Complex analysis 39: 38: 21: 18:Laplace equation 10058: 10057: 10053: 10052: 10051: 10049: 10048: 10047: 10013: 10012: 9958: 9955: 9945: 9917: 9901: 9899:Further reading 9891: 9849: 9844: 9843: 9806: 9802: 9761: 9754: 9737: 9733: 9716: 9705: 9696: 9692: 9673: 9664: 9647: 9643: 9624: 9620: 9615: 9610: 9600: 9598: 9594: 9574: 9570: 9561: 9557: 9546: 9543: 9542: 9540: 9536: 9532: 9466: 9457: 9449: 9444: 9436: 9431: 9427: 9422: 9393: 9389: 9381: 9379: 9372: 9368: 9362: 9358: 9343: 9338: 9328: 9324: 9314: 9288: 9286: 9274: 9270: 9245: 9241: 9233: 9231: 9224: 9220: 9214: 9210: 9191: 9184: 9179: 9169: 9165: 9155: 9153: 9147: 9143: 9117: 9114: 9113: 9096: 9091: 9056: 9052: 9011: 9008: 9007: 9003: 8999: 8995: 8991: 8984: 8950: 8946: 8944: 8941: 8940: 8918: 8915: 8914: 8873: 8869: 8867: 8864: 8863: 8847: 8846: 8838: 8822: 8813: 8809: 8801: 8800: 8788: 8784: 8750: 8745: 8736: 8735: 8716: 8711: 8707: 8705: 8702: 8701: 8662: 8654: 8651: 8650: 8634: 8631: 8630: 8614: 8611: 8610: 8594: 8592: 8589: 8588: 8585: 8561: 8558: 8557: 8556:is known, then 8541: 8538: 8537: 8521: 8518: 8517: 8500: 8499: 8497: 8494: 8493: 8476: 8475: 8473: 8470: 8469: 8453: 8450: 8449: 8424: 8421: 8420: 8396: 8392: 8387: 8372: 8368: 8366: 8363: 8362: 8344: 8323: 8319: 8317: 8314: 8313: 8294: 8290: 8255: 8247: 8244: 8243: 8225: 8223: 8220: 8219: 8203: 8195: 8187: 8184: 8183: 8152: 8150: 8147: 8146: 8130: 8127: 8126: 8102: 8098: 8093: 8085: 8077: 8074: 8073: 8052: 8048: 8046: 8043: 8042: 8026: 8023: 8022: 8006: 8004: 8001: 8000: 7997: 7975: 7970: 7964: 7961: 7960: 7938: 7935: 7934: 7908: 7905: 7904: 7884: 7881: 7880: 7858: 7855: 7854: 7828: 7823: 7818: 7817: 7812: 7811: 7805: 7800: 7791: 7779: 7774: 7769: 7755: 7752: 7751: 7745:solid harmonics 7740: 7735: 7731: 7726: 7691: 7686: 7676: 7672: 7666: 7661: 7651: 7637: 7627: 7616: 7583: 7580: 7579: 7573: 7558: 7535: 7531: 7526: 7475: 7471: 7465: 7461: 7459: 7456: 7455: 7440: 7436: 7425: 7417: 7408: 7401: 7397: 7393: 7386: 7382: 7376: 7368: 7363: 7359: 7355: 7351: 7346: 7309: 7304: 7255: 7250: 7240: 7236: 7230: 7226: 7224: 7221: 7220: 7201: 7186: 7181: 7165: 7161: 7134: 7129: 7123: 7120: 7119: 7096: 7090: 7082: 7076: 7053: 7043: 7037: 7019: 7013: 7004: 6999: 6982: 6963: 6948: 6942: 6934: 6924: 6909: 6903: 6899: 6893: 6886: 6878: 6872: 6866: 6847: 6843: 6825: 6817: 6815: 6805: 6801: 6791: 6786: 6770: 6768: 6753: 6749: 6744: 6741: 6740: 6724: 6720: 6705: 6701: 6697: 6687: 6683: 6682: 6680: 6670: 6668: 6665: 6664: 6639: 6633: 6599: 6595: 6591: 6581: 6577: 6576: 6574: 6559: 6555: 6554: 6549: 6539: 6521: 6513: 6511: 6501: 6497: 6487: 6482: 6469: 6464: 6454: 6429: 6421: 6419: 6413: 6409: 6408: 6404: 6394: 6389: 6379: 6377: 6374: 6373: 6328: 6300: 6296: 6292: 6282: 6278: 6277: 6275: 6260: 6256: 6250: 6246: 6245: 6240: 6222: 6214: 6212: 6202: 6198: 6188: 6183: 6165: 6161: 6160: 6155: 6137: 6129: 6127: 6121: 6117: 6116: 6112: 6102: 6097: 6089: 6085: 6080: 6068: 6064: 6062: 6059: 6058: 6029: 6023: 6019: 6017: 6014: 6013: 6007: 5987: 5982: 5976: 5973: 5972: 5962: 5955: 5951: 5946: 5939: 5933: 5921: 5915: 5903: 5891: 5869: 5846: 5820: 5791: 5788: 5787: 5768: 5756: 5739: 5735: 5708: 5704: 5695: 5691: 5687: 5678: 5661: 5650: 5643: 5641: 5635: 5630: 5617: 5612: 5595: 5591: 5585: 5581: 5579: 5572: 5568: 5562: 5558: 5548: 5543: 5526: 5523: 5522: 5512: 5507: 5501: 5493: 5489: 5485: 5468: 5462: 5458: 5432: 5422: 5417: 5401: 5396: 5394: 5391: 5390: 5380: 5352: 5348: 5346: 5335: 5333: 5330: 5329: 5317: 5311: 5308:Sommerfeld 1949 5301: 5295: 5289: 5273: 5240: 5236: 5230: 5226: 5204: 5200: 5186: 5175: 5164: 5156: 5153: 5152: 5144: 5138: 5132: 5129: 5122: 5083: 5079: 5067: 5063: 5059: 5055: 5049: 5045: 5008: 5004: 4992: 4988: 4937: 4933: 4927: 4923: 4921: 4918: 4917: 4907: 4901: 4895: 4856: 4853: 4852: 4848: 4842: 4818: 4790: 4778: 4775: 4774: 4753: 4741: 4724: 4707: 4675: 4672: 4671: 4649: 4638: 4627: 4601: 4598: 4597: 4593: 4589: 4582: 4570:Euler equations 4545: 4521: 4504: 4502: 4491: 4488: 4487: 4474:generated by a 4470:), this is the 4438: 4433: 4425: 4422: 4421: 4417: 4394: 4390: 4383: 4378: 4362: 4354: 4352: 4350: 4347: 4346: 4318: 4303: 4295: 4293: 4287: 4283: 4276: 4273: 4272: 4252: 4244: 4242: 4236: 4232: 4204: 4200: 4189: 4186: 4185: 4177: 4173: 4126: 4122: 4120: 4117: 4116: 4110: 4082: 4076: 4048: 4031: 4014: 3987: 3983: 3971: 3967: 3955: 3951: 3940: 3937: 3936: 3929: 3924: 3883: 3879: 3867: 3863: 3861: 3858: 3857: 3828: 3824: 3805: 3801: 3799: 3796: 3795: 3789: 3738: 3735: 3734: 3728: 3685: 3682: 3681: 3662: 3648: 3646: 3645: 3636: 3632: 3623: 3619: 3584: 3581: 3580: 3568: 3561: 3526: 3522: 3503: 3499: 3497: 3494: 3493: 3483: 3477: 3471: 3442: 3438: 3422: 3418: 3416: 3413: 3412: 3406: 3399:stream function 3350: 3347: 3346: 3340: 3317: 3313: 3304: 3300: 3292: 3284: 3281: 3280: 3254: 3250: 3241: 3237: 3235: 3232: 3231: 3225: 3219: 3216: 3210: 3195: 3158: 3154: 3148: 3144: 3123: 3119: 3113: 3109: 3108: 3104: 3098: 3087: 3054: 3050: 3044: 3040: 3019: 3015: 3009: 3005: 3004: 3000: 2994: 2983: 2962: 2959: 2958: 2938: 2934: 2922: 2918: 2909: 2905: 2903: 2900: 2899: 2879: 2875: 2869: 2865: 2859: 2848: 2827: 2824: 2823: 2819: 2813: 2791: 2728: 2725: 2724: 2693: 2690: 2689: 2685: 2681: 2674:Stokes' theorem 2667: 2644: 2640: 2628: 2624: 2622: 2619: 2618: 2612: 2606: 2579: 2575: 2559: 2555: 2541: 2538: 2537: 2531: 2511: 2507: 2498: 2494: 2484: 2480: 2468: 2464: 2462: 2459: 2458: 2385: 2382: 2381: 2370: 2364: 2358: 2338: 2334: 2328: 2324: 2309: 2305: 2299: 2295: 2280: 2276: 2270: 2266: 2248: 2244: 2242: 2239: 2238: 2234: 2228: 2224: 2219: 2199: 2195: 2183: 2179: 2169: 2165: 2156: 2152: 2150: 2147: 2146: 2136: 2130: 2119: 2046: 2043: 2042: 2028: 2021: 1991: 1987: 1975: 1971: 1959: 1955: 1951: 1941: 1937: 1936: 1934: 1922: 1918: 1914: 1904: 1900: 1899: 1897: 1895: 1892: 1891: 1888: 1873:; they are all 1861: 1855: 1847: 1841: 1826: 1820: 1816: 1815:on some domain 1810: 1803: 1782: 1771: 1764: 1757: 1746: 1733: 1726: 1718: 1692: 1688: 1649: 1645: 1641: 1633: 1631: 1622: 1618: 1611: 1603: 1601: 1600: 1596: 1586: 1582: 1578: 1573: 1565: 1557: 1551: 1539: 1535: 1533: 1530: 1529: 1503: 1495: 1482: 1478: 1469: 1465: 1461: 1453: 1451: 1434: 1430: 1421: 1417: 1413: 1405: 1403: 1402: 1398: 1389: 1385: 1381: 1376: 1364: 1360: 1358: 1355: 1354: 1350: 1317: 1313: 1309: 1299: 1295: 1294: 1292: 1277: 1273: 1267: 1263: 1262: 1257: 1239: 1231: 1229: 1219: 1215: 1205: 1200: 1182: 1178: 1177: 1172: 1154: 1146: 1144: 1138: 1134: 1133: 1129: 1119: 1114: 1106: 1102: 1097: 1085: 1081: 1079: 1076: 1075: 1041: 1038: 1037: 1003: 999: 995: 985: 981: 980: 978: 966: 962: 958: 948: 944: 943: 941: 933: 929: 924: 906: 898: 896: 892: 888: 878: 873: 863: 851: 847: 845: 842: 841: 807: 803: 799: 789: 785: 784: 782: 770: 766: 762: 752: 748: 747: 745: 733: 729: 725: 715: 711: 710: 708: 696: 692: 690: 687: 686: 677: 662:heat conduction 633:This is called 607: 604: 603: 566: 563: 562: 522: 519: 518: 498: 495: 494: 471: 468: 467: 446: 442: 422: 419: 418: 390: 387: 386: 359: 355: 353: 350: 349: 322: 282: 192:Residue theorem 167:Local primitive 157:Zeros and poles 72:Complex numbers 42: 35: 28: 23: 22: 15: 12: 11: 5: 10056: 10046: 10045: 10040: 10035: 10030: 10025: 10011: 10010: 10005: 9986: 9980: 9974: 9954: 9953:External links 9951: 9950: 9949: 9943: 9930: 9921: 9915: 9900: 9897: 9896: 9895: 9889: 9876: 9867: 9858:Hilbert, David 9848: 9845: 9842: 9841: 9820:(3): 571–578. 9800: 9752: 9731: 9703: 9690: 9662: 9641: 9617: 9616: 9614: 9611: 9609: 9608: 9592: 9577: 9573: 9569: 9564: 9560: 9556: 9553: 9550: 9533: 9531: 9528: 9527: 9526: 9521: 9516: 9510: 9505: 9503:Potential flow 9500: 9495: 9490: 9485: 9479: 9465: 9462: 9447: 9434: 9425: 9408: 9404: 9396: 9392: 9387: 9384: 9378: 9375: 9371: 9365: 9361: 9352: 9349: 9346: 9341: 9337: 9331: 9327: 9323: 9320: 9317: 9312: 9309: 9306: 9303: 9300: 9297: 9294: 9291: 9283: 9280: 9277: 9273: 9269: 9266: 9263: 9260: 9256: 9248: 9244: 9239: 9236: 9230: 9227: 9223: 9217: 9213: 9206: 9203: 9200: 9197: 9194: 9187: 9182: 9178: 9172: 9168: 9164: 9161: 9158: 9150: 9146: 9142: 9139: 9136: 9133: 9130: 9127: 9124: 9121: 9094: 9079: 9076: 9073: 9070: 9067: 9064: 9059: 9055: 9051: 9048: 9045: 9042: 9039: 9036: 9033: 9030: 9027: 9024: 9021: 9018: 9015: 8983: 8980: 8967: 8964: 8961: 8958: 8953: 8949: 8928: 8925: 8922: 8899: 8896: 8893: 8890: 8887: 8884: 8881: 8876: 8872: 8845: 8841: 8837: 8834: 8831: 8828: 8825: 8823: 8821: 8816: 8812: 8807: 8803: 8802: 8799: 8796: 8791: 8787: 8783: 8780: 8777: 8774: 8771: 8768: 8765: 8762: 8759: 8756: 8753: 8751: 8748: 8744: 8741: 8738: 8737: 8734: 8731: 8728: 8725: 8722: 8719: 8717: 8714: 8710: 8709: 8687: 8684: 8681: 8678: 8675: 8672: 8669: 8665: 8661: 8658: 8638: 8618: 8597: 8584: 8581: 8565: 8545: 8525: 8503: 8479: 8457: 8434: 8431: 8428: 8406: 8399: 8395: 8391: 8386: 8383: 8380: 8375: 8371: 8347: 8343: 8340: 8337: 8334: 8331: 8326: 8322: 8302: 8297: 8293: 8289: 8286: 8283: 8280: 8277: 8274: 8271: 8268: 8265: 8262: 8258: 8254: 8251: 8228: 8206: 8202: 8198: 8194: 8191: 8171: 8168: 8165: 8162: 8159: 8155: 8134: 8112: 8105: 8101: 8097: 8092: 8088: 8084: 8081: 8055: 8051: 8030: 8009: 7996: 7995:Electrostatics 7993: 7978: 7973: 7969: 7948: 7945: 7942: 7929:), instead of 7918: 7915: 7912: 7901:Laurent series 7888: 7868: 7865: 7862: 7840: 7831: 7826: 7821: 7815: 7808: 7803: 7799: 7794: 7788: 7785: 7782: 7778: 7777:lim sup 7773: 7768: 7765: 7762: 7759: 7738: 7729: 7714: 7711: 7708: 7705: 7702: 7699: 7694: 7689: 7685: 7679: 7675: 7669: 7664: 7660: 7654: 7649: 7646: 7643: 7640: 7636: 7630: 7625: 7622: 7619: 7615: 7611: 7608: 7605: 7602: 7599: 7596: 7593: 7590: 7587: 7529: 7510: 7507: 7504: 7501: 7498: 7495: 7492: 7489: 7486: 7483: 7478: 7474: 7468: 7464: 7366: 7349: 7332: 7329: 7326: 7323: 7320: 7317: 7312: 7307: 7303: 7299: 7296: 7293: 7290: 7287: 7284: 7281: 7278: 7275: 7272: 7269: 7266: 7263: 7258: 7253: 7249: 7243: 7239: 7233: 7229: 7219:which fulfill 7208: 7204: 7200: 7197: 7194: 7189: 7184: 7180: 7174: 7171: 7168: 7164: 7160: 7157: 7154: 7151: 7148: 7145: 7142: 7137: 7132: 7128: 7002: 6850: 6846: 6842: 6838: 6831: 6828: 6823: 6820: 6814: 6811: 6808: 6804: 6797: 6794: 6790: 6783: 6779: 6776: 6773: 6767: 6764: 6761: 6756: 6752: 6748: 6727: 6723: 6719: 6716: 6708: 6704: 6700: 6695: 6690: 6686: 6677: 6674: 6619: 6616: 6613: 6610: 6602: 6598: 6594: 6589: 6584: 6580: 6570: 6567: 6562: 6558: 6553: 6546: 6543: 6538: 6534: 6527: 6524: 6519: 6516: 6510: 6507: 6504: 6500: 6493: 6490: 6486: 6478: 6475: 6472: 6468: 6461: 6458: 6452: 6449: 6446: 6442: 6435: 6432: 6427: 6424: 6416: 6412: 6407: 6400: 6397: 6393: 6386: 6383: 6314: 6311: 6303: 6299: 6295: 6290: 6285: 6281: 6271: 6268: 6263: 6259: 6253: 6249: 6244: 6239: 6235: 6228: 6225: 6220: 6217: 6211: 6208: 6205: 6201: 6194: 6191: 6187: 6179: 6176: 6173: 6168: 6164: 6159: 6154: 6150: 6143: 6140: 6135: 6132: 6124: 6120: 6115: 6108: 6105: 6101: 6092: 6088: 6084: 6079: 6076: 6071: 6067: 6036: 6032: 6026: 6022: 5993: 5990: 5985: 5981: 5949: 5935:Main article: 5932: 5929: 5879: 5875: 5872: 5868: 5865: 5862: 5859: 5856: 5852: 5849: 5845: 5842: 5839: 5836: 5833: 5830: 5826: 5823: 5819: 5816: 5813: 5810: 5807: 5804: 5801: 5798: 5795: 5774: 5771: 5767: 5762: 5759: 5755: 5746: 5743: 5738: 5734: 5731: 5728: 5725: 5722: 5719: 5716: 5711: 5707: 5703: 5698: 5694: 5690: 5684: 5681: 5677: 5674: 5671: 5667: 5664: 5660: 5656: 5653: 5649: 5646: 5638: 5633: 5629: 5623: 5620: 5615: 5611: 5606: 5598: 5594: 5588: 5584: 5578: 5575: 5571: 5565: 5561: 5554: 5551: 5547: 5542: 5539: 5536: 5533: 5530: 5445: 5438: 5435: 5431: 5428: 5425: 5421: 5416: 5410: 5407: 5404: 5400: 5365: 5360: 5355: 5351: 5345: 5341: 5338: 5258: 5255: 5252: 5248: 5243: 5239: 5233: 5229: 5225: 5222: 5219: 5215: 5212: 5207: 5203: 5199: 5196: 5192: 5189: 5185: 5181: 5178: 5174: 5170: 5167: 5163: 5160: 5127: 5120: 5117:The notations 5103: 5100: 5097: 5092: 5086: 5082: 5078: 5075: 5070: 5066: 5062: 5058: 5052: 5048: 5044: 5041: 5038: 5033: 5029: 5026: 5023: 5020: 5017: 5014: 5011: 5007: 5003: 5000: 4995: 4991: 4987: 4984: 4981: 4976: 4972: 4969: 4966: 4963: 4959: 4956: 4953: 4950: 4947: 4944: 4940: 4936: 4930: 4926: 4881: 4878: 4875: 4872: 4869: 4866: 4863: 4860: 4828: 4825: 4816: 4813: 4810: 4807: 4804: 4801: 4798: 4788: 4785: 4782: 4763: 4760: 4751: 4747: 4744: 4740: 4737: 4734: 4730: 4727: 4723: 4720: 4717: 4713: 4710: 4706: 4703: 4700: 4697: 4694: 4691: 4688: 4685: 4682: 4679: 4659: 4655: 4652: 4648: 4644: 4641: 4637: 4633: 4630: 4626: 4623: 4620: 4617: 4614: 4611: 4608: 4605: 4581: 4578: 4566:point particle 4533: 4527: 4524: 4519: 4516: 4513: 4510: 4507: 4501: 4498: 4495: 4476:point particle 4453: 4447: 4444: 4441: 4437: 4432: 4429: 4405: 4397: 4393: 4389: 4386: 4382: 4377: 4374: 4368: 4365: 4360: 4357: 4332: 4327: 4324: 4321: 4316: 4309: 4306: 4301: 4298: 4290: 4286: 4282: 4279: 4275: 4271: 4268: 4265: 4258: 4255: 4250: 4247: 4239: 4235: 4231: 4228: 4225: 4221: 4218: 4215: 4212: 4207: 4203: 4199: 4196: 4193: 4159: 4156: 4153: 4150: 4147: 4143: 4140: 4137: 4134: 4129: 4125: 4061: 4058: 4054: 4051: 4047: 4044: 4041: 4037: 4034: 4030: 4027: 4024: 4020: 4017: 4013: 4010: 4007: 4004: 4001: 3998: 3993: 3990: 3986: 3982: 3977: 3974: 3970: 3966: 3961: 3958: 3954: 3950: 3947: 3944: 3928: 3925: 3923: 3920: 3903: 3900: 3897: 3894: 3889: 3886: 3882: 3878: 3873: 3870: 3866: 3845: 3842: 3839: 3836: 3831: 3827: 3822: 3819: 3816: 3813: 3808: 3804: 3777: 3774: 3771: 3767: 3764: 3761: 3758: 3754: 3751: 3748: 3745: 3742: 3716: 3713: 3710: 3707: 3704: 3701: 3698: 3695: 3692: 3689: 3669: 3665: 3661: 3655: 3651: 3644: 3639: 3635: 3631: 3626: 3622: 3618: 3615: 3612: 3609: 3606: 3603: 3600: 3597: 3594: 3591: 3588: 3560: 3559:Electrostatics 3557: 3543: 3540: 3537: 3534: 3529: 3525: 3520: 3517: 3514: 3511: 3506: 3502: 3488:is called the 3459: 3456: 3453: 3450: 3445: 3441: 3436: 3433: 3430: 3425: 3421: 3386: 3383: 3380: 3376: 3373: 3370: 3367: 3363: 3360: 3357: 3354: 3328: 3325: 3320: 3316: 3312: 3307: 3303: 3299: 3295: 3291: 3288: 3268: 3265: 3262: 3257: 3253: 3249: 3244: 3240: 3212:Main article: 3209: 3206: 3183: 3179: 3175: 3172: 3169: 3166: 3161: 3157: 3151: 3147: 3143: 3140: 3137: 3134: 3131: 3126: 3122: 3116: 3112: 3107: 3101: 3096: 3093: 3090: 3086: 3082: 3079: 3075: 3071: 3068: 3065: 3062: 3057: 3053: 3047: 3043: 3039: 3036: 3033: 3030: 3027: 3022: 3018: 3012: 3008: 3003: 2997: 2992: 2989: 2986: 2982: 2978: 2975: 2972: 2969: 2966: 2946: 2941: 2937: 2933: 2930: 2925: 2921: 2917: 2912: 2908: 2887: 2882: 2878: 2872: 2868: 2862: 2857: 2854: 2851: 2847: 2843: 2840: 2837: 2834: 2831: 2810:Fourier series 2777: 2774: 2771: 2768: 2765: 2762: 2759: 2756: 2753: 2750: 2747: 2744: 2741: 2738: 2735: 2732: 2712: 2709: 2706: 2703: 2700: 2697: 2655: 2650: 2647: 2643: 2639: 2634: 2631: 2627: 2617:is satisfied: 2594: 2591: 2588: 2582: 2578: 2574: 2571: 2568: 2562: 2558: 2554: 2551: 2548: 2545: 2519: 2514: 2510: 2506: 2501: 2497: 2492: 2487: 2483: 2479: 2476: 2471: 2467: 2446: 2443: 2440: 2437: 2434: 2431: 2428: 2425: 2422: 2419: 2416: 2413: 2410: 2407: 2404: 2401: 2398: 2395: 2392: 2389: 2346: 2341: 2337: 2331: 2327: 2323: 2320: 2317: 2312: 2308: 2302: 2298: 2294: 2291: 2288: 2283: 2279: 2273: 2269: 2265: 2262: 2259: 2254: 2251: 2247: 2222: 2207: 2202: 2198: 2194: 2191: 2186: 2182: 2177: 2172: 2168: 2164: 2159: 2155: 2145:be satisfied: 2107: 2104: 2101: 2098: 2095: 2092: 2089: 2086: 2083: 2080: 2077: 2074: 2071: 2068: 2065: 2062: 2059: 2056: 2053: 2050: 2020: 2017: 2005: 2002: 1997: 1994: 1990: 1986: 1981: 1978: 1974: 1970: 1962: 1958: 1954: 1949: 1944: 1940: 1933: 1925: 1921: 1917: 1912: 1907: 1903: 1887: 1884: 1790:=4) = 4 sin(5 1756:(inner radius 1745: 1742: 1722: 1706: 1703: 1698: 1695: 1691: 1687: 1684: 1681: 1678: 1675: 1671: 1668: 1665: 1661: 1652: 1648: 1644: 1639: 1636: 1628: 1625: 1621: 1614: 1610: 1606: 1599: 1589: 1585: 1581: 1577: 1568: 1564: 1560: 1555: 1550: 1547: 1542: 1538: 1517: 1514: 1511: 1506: 1501: 1498: 1494: 1488: 1485: 1481: 1472: 1468: 1464: 1459: 1456: 1450: 1446: 1440: 1437: 1433: 1424: 1420: 1416: 1411: 1408: 1401: 1392: 1388: 1384: 1380: 1375: 1372: 1367: 1363: 1331: 1328: 1320: 1316: 1312: 1307: 1302: 1298: 1288: 1285: 1280: 1276: 1270: 1266: 1261: 1256: 1252: 1245: 1242: 1237: 1234: 1228: 1225: 1222: 1218: 1211: 1208: 1204: 1196: 1193: 1190: 1185: 1181: 1176: 1171: 1167: 1160: 1157: 1152: 1149: 1141: 1137: 1132: 1125: 1122: 1118: 1109: 1105: 1101: 1096: 1093: 1088: 1084: 1063: 1060: 1057: 1054: 1051: 1048: 1045: 1017: 1014: 1006: 1002: 998: 993: 988: 984: 977: 969: 965: 961: 956: 951: 947: 936: 932: 928: 923: 919: 912: 909: 904: 901: 895: 891: 884: 881: 877: 870: 867: 862: 859: 854: 850: 821: 818: 810: 806: 802: 797: 792: 788: 781: 773: 769: 765: 760: 755: 751: 744: 736: 732: 728: 723: 718: 714: 707: 704: 699: 695: 676: 673: 658:fluid dynamics 620: 617: 614: 611: 591: 588: 585: 582: 579: 576: 573: 570: 547: 544: 541: 538: 535: 532: 529: 526: 502: 478: 475: 449: 445: 441: 438: 435: 432: 429: 426: 406: 403: 400: 397: 394: 374: 371: 368: 362: 358: 324: 323: 321: 320: 313: 306: 298: 295: 294: 293: 292: 277: 276: 275: 274: 269: 264: 259: 254: 249: 247:Leonhard Euler 244: 236: 235: 229: 228: 222: 221: 220: 219: 214: 209: 204: 199: 194: 189: 184: 182:Laurent series 179: 177:Winding number 174: 169: 164: 159: 151: 150: 144: 143: 142: 141: 136: 131: 126: 121: 113: 112: 106: 105: 104: 103: 98: 93: 88: 83: 75: 74: 68: 67: 59: 58: 52: 51: 26: 9: 6: 4: 3: 2: 10055: 10044: 10041: 10039: 10036: 10034: 10031: 10029: 10026: 10024: 10021: 10020: 10018: 10009: 10006: 10001: 10000: 9995: 9992: 9987: 9984: 9981: 9978: 9975: 9971: 9967: 9966: 9961: 9957: 9956: 9946: 9940: 9936: 9931: 9927: 9922: 9918: 9912: 9908: 9903: 9902: 9892: 9890:9780486652511 9886: 9882: 9877: 9873: 9868: 9863: 9859: 9855: 9851: 9850: 9836: 9831: 9827: 9823: 9819: 9815: 9811: 9804: 9796: 9792: 9788: 9784: 9779: 9774: 9771:(4): 042501. 9770: 9766: 9759: 9757: 9749: 9745: 9741: 9735: 9728: 9724: 9720: 9714: 9712: 9710: 9708: 9700: 9694: 9687: 9683: 9679: 9678: 9671: 9669: 9667: 9659: 9655: 9651: 9645: 9638: 9634: 9630: 9629: 9622: 9618: 9603: 9596: 9575: 9571: 9567: 9562: 9558: 9554: 9551: 9538: 9534: 9525: 9522: 9520: 9517: 9514: 9511: 9509: 9506: 9504: 9501: 9499: 9496: 9494: 9491: 9489: 9486: 9483: 9480: 9478: 9476: 9471: 9468: 9467: 9461: 9455: 9450: 9442: 9437: 9428: 9419: 9406: 9402: 9394: 9390: 9385: 9382: 9376: 9373: 9369: 9363: 9359: 9350: 9347: 9344: 9339: 9335: 9329: 9325: 9318: 9310: 9304: 9301: 9298: 9295: 9289: 9281: 9278: 9275: 9267: 9264: 9258: 9254: 9246: 9242: 9237: 9234: 9228: 9225: 9221: 9215: 9211: 9204: 9198: 9195: 9185: 9180: 9176: 9170: 9162: 9159: 9148: 9140: 9137: 9131: 9125: 9119: 9111: 9105: 9101: 9097: 9077: 9071: 9068: 9065: 9057: 9053: 9046: 9040: 9037: 9031: 9028: 9025: 9022: 9019: 8989: 8979: 8965: 8962: 8959: 8956: 8951: 8926: 8923: 8920: 8911: 8897: 8894: 8891: 8888: 8885: 8882: 8879: 8874: 8860: 8843: 8835: 8829: 8826: 8824: 8819: 8814: 8797: 8794: 8789: 8781: 8778: 8772: 8766: 8760: 8754: 8752: 8742: 8732: 8729: 8723: 8720: 8718: 8698: 8685: 8682: 8679: 8676: 8673: 8670: 8667: 8659: 8636: 8616: 8580: 8577: 8563: 8543: 8523: 8455: 8446: 8432: 8429: 8426: 8417: 8404: 8397: 8393: 8389: 8384: 8381: 8378: 8373: 8359: 8341: 8335: 8332: 8329: 8324: 8300: 8295: 8287: 8284: 8278: 8272: 8266: 8260: 8252: 8241: 8200: 8192: 8169: 8166: 8160: 8157: 8132: 8123: 8110: 8103: 8099: 8095: 8090: 8082: 8071: 8053: 8049: 8028: 7992: 7976: 7971: 7967: 7946: 7943: 7940: 7932: 7931:Taylor series 7913: 7910: 7902: 7886: 7866: 7863: 7860: 7851: 7838: 7829: 7824: 7819: 7806: 7801: 7797: 7780: 7771: 7766: 7763: 7760: 7757: 7750: 7746: 7743:are known as 7741: 7732: 7712: 7706: 7703: 7700: 7692: 7687: 7683: 7677: 7673: 7667: 7662: 7658: 7652: 7647: 7644: 7641: 7638: 7634: 7623: 7620: 7617: 7613: 7609: 7603: 7600: 7597: 7594: 7591: 7585: 7576: 7571: 7566: 7562: 7556: 7552: 7546: 7542: 7538: 7532: 7524: 7508: 7502: 7499: 7496: 7490: 7487: 7484: 7481: 7476: 7466: 7462: 7451: 7447: 7443: 7433: 7429: 7423: 7416: 7411: 7404: 7392: 7379: 7374: 7369: 7352: 7343: 7330: 7324: 7321: 7318: 7310: 7305: 7301: 7294: 7291: 7288: 7282: 7279: 7276: 7270: 7267: 7264: 7256: 7251: 7247: 7241: 7231: 7227: 7202: 7198: 7195: 7187: 7182: 7178: 7172: 7169: 7166: 7162: 7158: 7155: 7149: 7146: 7143: 7135: 7130: 7126: 7117: 7113: 7108: 7104: 7100: 7093: 7086: 7079: 7072: 7068: 7064: 7060: 7056: 7050: 7046: 7040: 7034: 7030: 7026: 7022: 7016: 7009: 7005: 6998: 6994: 6989: 6985: 6980: 6976: 6970: 6966: 6959: 6955: 6951: 6945: 6940: 6931: 6927: 6920: 6916: 6912: 6906: 6896: 6890: 6884: 6875: 6869: 6863: 6848: 6844: 6840: 6836: 6829: 6826: 6818: 6812: 6809: 6806: 6802: 6795: 6792: 6788: 6777: 6774: 6771: 6765: 6762: 6759: 6754: 6750: 6746: 6725: 6721: 6717: 6714: 6706: 6702: 6698: 6688: 6684: 6672: 6662: 6658: 6654: 6650: 6646: 6642: 6638:has the form 6636: 6630: 6617: 6614: 6611: 6608: 6600: 6596: 6587: 6582: 6568: 6565: 6560: 6556: 6551: 6544: 6541: 6536: 6532: 6525: 6517: 6508: 6505: 6502: 6498: 6491: 6476: 6473: 6470: 6466: 6459: 6456: 6450: 6447: 6444: 6440: 6433: 6430: 6425: 6422: 6414: 6410: 6405: 6398: 6395: 6391: 6384: 6381: 6371: 6369: 6363: 6359: 6355: 6351: 6347: 6343: 6339: 6335: 6331: 6325: 6312: 6309: 6301: 6297: 6288: 6283: 6269: 6266: 6261: 6257: 6251: 6247: 6242: 6237: 6233: 6226: 6218: 6209: 6206: 6203: 6199: 6192: 6177: 6174: 6171: 6166: 6162: 6157: 6152: 6148: 6141: 6133: 6122: 6118: 6113: 6106: 6090: 6086: 6082: 6077: 6074: 6069: 6056: 6054: 6034: 6030: 6024: 6020: 6010: 5991: 5988: 5983: 5979: 5969: 5965: 5958: 5952: 5943: 5938: 5928: 5924: 5918: 5911: 5907: 5899: 5895: 5873: 5870: 5866: 5863: 5857: 5854: 5850: 5847: 5843: 5840: 5837: 5834: 5831: 5828: 5824: 5821: 5817: 5814: 5811: 5808: 5805: 5802: 5796: 5793: 5772: 5769: 5765: 5760: 5757: 5753: 5744: 5741: 5729: 5726: 5723: 5720: 5717: 5714: 5709: 5705: 5701: 5696: 5692: 5682: 5679: 5675: 5672: 5665: 5662: 5658: 5654: 5651: 5644: 5636: 5631: 5627: 5621: 5618: 5613: 5609: 5604: 5596: 5592: 5586: 5582: 5576: 5573: 5569: 5563: 5559: 5552: 5549: 5545: 5540: 5534: 5528: 5520: 5515: 5504: 5499: 5483: 5482: 5477: 5471: 5465: 5443: 5436: 5433: 5429: 5426: 5423: 5419: 5414: 5408: 5405: 5402: 5398: 5388: 5383: 5379:Note that if 5377: 5363: 5358: 5353: 5349: 5343: 5339: 5336: 5327: 5325: 5320: 5314: 5309: 5304: 5298: 5292: 5285: 5281: 5277: 5270: 5256: 5253: 5250: 5246: 5241: 5237: 5231: 5227: 5223: 5220: 5217: 5213: 5210: 5205: 5201: 5197: 5190: 5187: 5183: 5179: 5176: 5172: 5168: 5165: 5158: 5150: 5147: 5141: 5135: 5130: 5123: 5115: 5101: 5098: 5095: 5090: 5084: 5080: 5076: 5073: 5068: 5064: 5060: 5056: 5050: 5046: 5042: 5039: 5036: 5031: 5027: 5021: 5018: 5015: 5009: 5005: 5001: 4993: 4989: 4985: 4982: 4979: 4974: 4970: 4964: 4957: 4954: 4951: 4945: 4938: 4934: 4928: 4924: 4915: 4913: 4904: 4898: 4892: 4879: 4876: 4873: 4870: 4867: 4861: 4845: 4839: 4826: 4823: 4811: 4808: 4805: 4802: 4799: 4786: 4783: 4780: 4761: 4758: 4745: 4742: 4738: 4735: 4732: 4728: 4725: 4721: 4718: 4715: 4711: 4708: 4704: 4701: 4695: 4692: 4689: 4686: 4680: 4653: 4650: 4646: 4642: 4639: 4635: 4631: 4628: 4624: 4621: 4618: 4615: 4612: 4609: 4603: 4587: 4577: 4575: 4571: 4567: 4563: 4559: 4555: 4549: 4531: 4525: 4522: 4514: 4508: 4505: 4499: 4496: 4493: 4485: 4481: 4477: 4473: 4469: 4464: 4451: 4445: 4442: 4439: 4435: 4430: 4427: 4403: 4395: 4391: 4387: 4384: 4380: 4375: 4372: 4366: 4363: 4358: 4355: 4343: 4330: 4325: 4322: 4319: 4314: 4307: 4304: 4299: 4296: 4288: 4284: 4280: 4277: 4269: 4266: 4263: 4256: 4253: 4248: 4245: 4237: 4233: 4229: 4226: 4223: 4219: 4213: 4205: 4201: 4197: 4194: 4191: 4184:implies that 4183: 4170: 4157: 4154: 4151: 4148: 4145: 4141: 4135: 4127: 4123: 4113: 4108: 4104: 4103:weak solution 4100: 4094: 4090: 4086: 4079: 4075: 4059: 4052: 4049: 4045: 4042: 4039: 4035: 4032: 4028: 4025: 4022: 4018: 4015: 4011: 4008: 4002: 3999: 3996: 3991: 3988: 3984: 3980: 3975: 3972: 3968: 3964: 3959: 3956: 3952: 3948: 3945: 3934: 3919: 3917: 3914:which is the 3901: 3898: 3895: 3892: 3887: 3884: 3880: 3876: 3871: 3868: 3864: 3843: 3840: 3837: 3834: 3829: 3825: 3820: 3817: 3814: 3811: 3806: 3802: 3792: 3775: 3772: 3769: 3765: 3762: 3759: 3756: 3752: 3749: 3746: 3743: 3740: 3731: 3714: 3711: 3708: 3702: 3699: 3696: 3690: 3667: 3659: 3637: 3633: 3629: 3624: 3620: 3613: 3607: 3604: 3601: 3598: 3595: 3589: 3576: 3572: 3566: 3563:According to 3556: 3541: 3538: 3535: 3532: 3527: 3523: 3518: 3515: 3512: 3509: 3504: 3500: 3491: 3486: 3480: 3474: 3457: 3454: 3451: 3448: 3443: 3439: 3434: 3431: 3428: 3423: 3419: 3411:are given by 3409: 3404: 3400: 3384: 3381: 3378: 3374: 3371: 3368: 3365: 3361: 3358: 3355: 3352: 3343: 3326: 3323: 3318: 3314: 3310: 3305: 3301: 3297: 3289: 3266: 3263: 3260: 3255: 3251: 3247: 3242: 3238: 3228: 3222: 3215: 3205: 3203: 3198: 3181: 3177: 3173: 3170: 3167: 3164: 3159: 3155: 3149: 3145: 3141: 3138: 3135: 3132: 3129: 3124: 3120: 3114: 3110: 3105: 3094: 3091: 3088: 3084: 3080: 3077: 3073: 3069: 3066: 3063: 3060: 3055: 3051: 3045: 3041: 3037: 3034: 3031: 3028: 3025: 3020: 3016: 3010: 3006: 3001: 2990: 2987: 2984: 2980: 2976: 2970: 2964: 2944: 2939: 2935: 2931: 2928: 2923: 2919: 2915: 2910: 2906: 2885: 2880: 2876: 2870: 2866: 2855: 2852: 2849: 2845: 2841: 2835: 2829: 2816: 2811: 2806: 2804: 2803:wave equation 2800: 2795: 2788: 2775: 2772: 2769: 2766: 2763: 2760: 2757: 2754: 2751: 2748: 2745: 2742: 2736: 2730: 2710: 2707: 2704: 2701: 2698: 2695: 2679: 2675: 2670: 2653: 2648: 2645: 2641: 2637: 2632: 2629: 2625: 2615: 2609: 2592: 2589: 2586: 2580: 2576: 2572: 2569: 2566: 2560: 2556: 2552: 2549: 2546: 2543: 2534: 2517: 2512: 2508: 2504: 2499: 2495: 2490: 2485: 2481: 2477: 2474: 2469: 2465: 2444: 2438: 2435: 2432: 2426: 2423: 2420: 2414: 2411: 2408: 2402: 2399: 2393: 2387: 2377: 2373: 2367: 2361: 2344: 2339: 2329: 2325: 2318: 2315: 2310: 2300: 2296: 2289: 2286: 2281: 2271: 2267: 2263: 2257: 2252: 2249: 2245: 2231: 2225: 2205: 2200: 2196: 2192: 2189: 2184: 2180: 2175: 2170: 2166: 2162: 2157: 2153: 2144: 2139: 2133: 2126: 2122: 2105: 2099: 2096: 2093: 2087: 2084: 2081: 2075: 2072: 2069: 2063: 2060: 2054: 2048: 2039: 2035: 2031: 2026: 2016: 2003: 2000: 1995: 1992: 1988: 1984: 1979: 1976: 1972: 1968: 1960: 1956: 1947: 1942: 1931: 1923: 1919: 1910: 1905: 1883: 1881: 1876: 1872: 1867: 1864: 1858: 1853: 1844: 1839: 1834: 1832: 1831:heat equation 1823: 1813: 1808: 1802: 1793: 1789: 1785: 1778: 1774: 1767: 1760: 1755: 1750: 1741: 1739: 1731: 1730:metric tensor 1725: 1721: 1696: 1693: 1689: 1679: 1676: 1669: 1666: 1663: 1659: 1650: 1646: 1637: 1626: 1623: 1619: 1608: 1597: 1587: 1583: 1562: 1553: 1548: 1545: 1540: 1515: 1512: 1509: 1504: 1499: 1496: 1486: 1483: 1479: 1470: 1466: 1457: 1448: 1444: 1438: 1435: 1431: 1422: 1418: 1409: 1399: 1390: 1386: 1373: 1370: 1365: 1349: 1348: 1342: 1329: 1326: 1318: 1314: 1305: 1300: 1286: 1283: 1278: 1274: 1268: 1264: 1259: 1254: 1250: 1243: 1235: 1226: 1223: 1220: 1216: 1209: 1194: 1191: 1188: 1183: 1179: 1174: 1169: 1165: 1158: 1150: 1139: 1135: 1130: 1123: 1107: 1103: 1099: 1094: 1091: 1086: 1058: 1055: 1052: 1049: 1046: 1035: 1034: 1028: 1015: 1012: 1004: 1000: 991: 986: 975: 967: 963: 954: 949: 934: 930: 926: 921: 917: 910: 902: 893: 889: 882: 868: 865: 860: 857: 852: 839: 838: 832: 819: 816: 808: 804: 795: 790: 779: 771: 767: 758: 753: 742: 734: 730: 721: 716: 705: 702: 697: 685: 683: 672: 670: 669:heat equation 667: 663: 659: 655: 651: 646: 644: 640: 636: 631: 618: 615: 612: 586: 583: 580: 577: 574: 568: 559: 542: 539: 536: 533: 530: 524: 516: 492: 476: 465: 447: 439: 433: 427: 404: 401: 398: 395: 372: 369: 366: 360: 347: 343: 339: 335: 331: 319: 314: 312: 307: 305: 300: 299: 297: 296: 291: 286: 281: 280: 279: 278: 273: 270: 268: 265: 263: 260: 258: 255: 253: 250: 248: 245: 243: 240: 239: 238: 237: 234: 231: 230: 227: 224: 223: 218: 215: 213: 210: 208: 207:Schwarz lemma 205: 203: 202:Conformal map 200: 198: 195: 193: 190: 188: 185: 183: 180: 178: 175: 173: 170: 168: 165: 163: 160: 158: 155: 154: 153: 152: 149: 146: 145: 140: 137: 135: 132: 130: 127: 125: 122: 120: 117: 116: 115: 114: 111: 108: 107: 102: 99: 97: 94: 92: 91:Complex plane 89: 87: 84: 82: 79: 78: 77: 76: 73: 70: 69: 65: 61: 60: 57: 54: 53: 49: 45: 41: 40: 37: 33: 19: 9997: 9963: 9934: 9925: 9906: 9880: 9871: 9861: 9817: 9813: 9803: 9768: 9764: 9739: 9734: 9718: 9693: 9675: 9649: 9644: 9626: 9621: 9601: 9595: 9537: 9474: 9445: 9432: 9423: 9420: 9103: 9099: 9092: 8985: 8939:and we have 8912: 8861: 8699: 8586: 8578: 8447: 8418: 8360: 8242: 8124: 7998: 7852: 7736: 7727: 7574: 7567: 7560: 7544: 7540: 7536: 7527: 7449: 7445: 7441: 7431: 7427: 7409: 7402: 7377: 7364: 7347: 7344: 7106: 7102: 7098: 7091: 7084: 7081:, there are 7077: 7070: 7066: 7062: 7058: 7054: 7051: 7044: 7038: 7032: 7028: 7024: 7020: 7014: 7007: 7000: 6987: 6983: 6968: 6964: 6957: 6953: 6949: 6943: 6929: 6925: 6918: 6914: 6910: 6904: 6894: 6888: 6873: 6871:. A priori, 6867: 6864: 6663: 6656: 6652: 6648: 6644: 6640: 6634: 6631: 6372: 6361: 6357: 6353: 6349: 6345: 6341: 6337: 6333: 6329: 6326: 6057: 6050: 6008: 5967: 5963: 5956: 5947: 5922: 5916: 5909: 5905: 5897: 5893: 5513: 5502: 5479: 5475: 5469: 5463: 5386: 5381: 5378: 5328: 5323: 5318: 5316:at distance 5312: 5302: 5296: 5290: 5288:of the data 5283: 5279: 5275: 5271: 5151: 5145: 5139: 5133: 5125: 5118: 5116: 4916: 4902: 4896: 4893: 4843: 4840: 4670:may satisfy 4592:of a volume 4583: 4552:denotes the 4547: 4465: 4344: 4171: 4111: 4099:distribution 4092: 4088: 4084: 4077: 3930: 3790: 3729: 3574: 3570: 3562: 3484: 3478: 3472: 3407: 3341: 3226: 3220: 3217: 3196: 2814: 2807: 2799:power series 2796: 2789: 2677: 2668: 2613: 2607: 2532: 2375: 2371: 2365: 2359: 2229: 2220: 2137: 2131: 2124: 2120: 2037: 2033: 2029: 2022: 1889: 1868: 1862: 1856: 1842: 1835: 1821: 1811: 1804: 1791: 1787: 1783: 1776: 1772: 1765: 1758: 1736:denotes its 1723: 1719: 1345: 1343: 1074:convention, 1036:, using the 1031: 1029: 835: 833: 680: 678: 666:steady-state 647: 632: 560: 344:named after 337: 327: 216: 148:Basic theory 47: 36: 8583:Gravitation 8070:Gauss's law 5959:= 0, ..., 4 330:mathematics 262:Kiyoshi Oka 81:Real number 10017:Categories 9613:References 9477:-separable 7725:where the 7391:colatitude 7358:and order 6881:must be a 5966:= 0, ..., 5521:, p. 228) 4072:where the 3403:flow lines 3208:Fluid flow 2957:Therefore 2357:Therefore 2041:, and if 1819:such that 1799:See also: 602:, we have 491:divergence 9999:MathWorld 9970:EMS Press 9795:118707082 9778:1111.4702 9568:− 9549:Δ 9377:− 9265:− 9229:− 9138:− 9072:φ 9066:θ 9032:φ 9026:θ 9014:Ψ 8948:∇ 8921:ρ 8895:ρ 8889:π 8871:∇ 8836:⋅ 8833:∇ 8830:− 8811:∇ 8806:⟹ 8786:∇ 8782:− 8770:∇ 8767:− 8761:⋅ 8758:∇ 8743:⋅ 8740:∇ 8727:∇ 8724:− 8683:ρ 8677:π 8671:− 8660:⋅ 8657:∇ 8617:ρ 8524:ρ 8427:ρ 8394:ε 8390:ρ 8385:− 8370:∇ 8342:⋅ 8339:∇ 8336:− 8321:∇ 8292:∇ 8288:− 8276:∇ 8273:− 8267:⋅ 8264:∇ 8253:⋅ 8250:∇ 8193:× 8190:∇ 8164:∇ 8161:− 8100:ε 8096:ρ 8083:⋅ 8080:∇ 8050:ε 8029:ρ 7972:ℓ 7917:∞ 7830:ℓ 7802:ℓ 7787:∞ 7784:→ 7781:ℓ 7707:φ 7701:θ 7688:ℓ 7678:ℓ 7663:ℓ 7653:ℓ 7648:ℓ 7645:− 7635:∑ 7629:∞ 7618:ℓ 7614:∑ 7604:φ 7598:θ 7497:ℓ 7491:ℓ 7488:− 7473:∇ 7415:longitude 7325:φ 7319:θ 7306:ℓ 7289:ℓ 7283:ℓ 7280:− 7271:φ 7265:θ 7252:ℓ 7238:∇ 7203:θ 7199:⁡ 7183:ℓ 7173:φ 7150:φ 7144:θ 7131:ℓ 6830:θ 6822:Θ 6813:θ 6810:⁡ 6796:θ 6782:Θ 6778:θ 6775:⁡ 6763:θ 6760:⁡ 6747:λ 6718:− 6703:φ 6694:Φ 6676:Φ 6615:λ 6612:− 6597:φ 6593:∂ 6579:∂ 6569:θ 6566:⁡ 6526:θ 6523:∂ 6515:∂ 6509:θ 6506:⁡ 6492:θ 6489:∂ 6485:∂ 6477:θ 6474:⁡ 6448:λ 6298:φ 6294:∂ 6280:∂ 6270:θ 6267:⁡ 6227:θ 6224:∂ 6216:∂ 6210:θ 6207:⁡ 6193:θ 6190:∂ 6186:∂ 6178:θ 6175:⁡ 6139:∂ 6131:∂ 6104:∂ 6100:∂ 6066:∇ 6025:∘ 5989:− 5984:ℓ 5871:φ 5867:− 5864:φ 5858:⁡ 5848:θ 5844:⁡ 5838:θ 5835:⁡ 5822:θ 5818:⁡ 5812:θ 5809:⁡ 5800:Θ 5797:⁡ 5770:φ 5758:θ 5733:Θ 5730:⁡ 5724:ρ 5715:− 5706:ρ 5680:θ 5676:⁡ 5663:φ 5652:θ 5637:π 5628:∫ 5622:π 5610:∫ 5583:ρ 5577:− 5553:π 5430:ρ 5427:π 5415:− 5406:π 5359:ρ 5337:ρ 5228:∬ 5202:∭ 5074:− 5047:∬ 5025:∇ 5019:− 5013:∇ 5002:⋅ 4999:∇ 4990:∭ 4968:∇ 4965:⋅ 4962:∇ 4955:− 4949:∇ 4946:⋅ 4943:∇ 4925:∭ 4874:− 4865:∇ 4862:⋅ 4859:∇ 4739:− 4722:− 4705:− 4696:δ 4693:− 4684:∇ 4681:⋅ 4678:∇ 4558:potential 4526:π 4509:⁡ 4500:− 4478:, for an 4472:potential 4443:π 4388:π 4376:− 4281:π 4234:∬ 4217:∇ 4214:⋅ 4211:∇ 4202:∭ 4192:− 4155:− 4139:∇ 4136:⋅ 4133:∇ 4124:∭ 4046:− 4029:− 4012:− 4003:δ 4000:− 3943:Δ 3899:ρ 3896:− 3881:φ 3865:φ 3838:− 3826:φ 3815:− 3803:φ 3763:− 3750:− 3744:φ 3712:ρ 3691:⋅ 3688:∇ 3654:^ 3630:− 3590:× 3587:∇ 3536:− 3524:φ 3513:− 3501:φ 3452:− 3440:ψ 3420:ψ 3372:− 3356:ψ 3311:− 3290:× 3287:∇ 3174:θ 3168:⁡ 3139:θ 3133:⁡ 3100:∞ 3085:∑ 3070:θ 3064:⁡ 3038:− 3035:θ 3029:⁡ 2996:∞ 2981:∑ 2861:∞ 2846:∑ 2773:θ 2761:⁡ 2749:⁡ 2705:⁡ 2696:φ 2666:and thus 2642:ψ 2626:ψ 2577:φ 2557:φ 2553:− 2547:ψ 2509:φ 2496:ψ 2482:φ 2478:− 2466:ψ 2427:ψ 2403:φ 2319:− 2290:− 2264:− 2193:− 1989:ψ 1973:ψ 1969:≡ 1953:∂ 1948:ψ 1939:∂ 1916:∂ 1911:ψ 1902:∂ 1866:is zero. 1647:ξ 1643:∂ 1635:∂ 1584:ξ 1580:∂ 1576:∂ 1537:∇ 1493:Γ 1467:ξ 1463:∂ 1455:∂ 1419:ξ 1415:∂ 1407:∂ 1387:ξ 1383:∂ 1379:∂ 1362:∇ 1315:φ 1311:∂ 1297:∂ 1287:θ 1284:⁡ 1244:θ 1241:∂ 1233:∂ 1227:θ 1224:⁡ 1210:θ 1207:∂ 1203:∂ 1195:θ 1192:⁡ 1156:∂ 1148:∂ 1121:∂ 1117:∂ 1083:∇ 1059:φ 1053:θ 997:∂ 983:∂ 964:ϕ 960:∂ 946:∂ 908:∂ 900:∂ 880:∂ 876:∂ 849:∇ 801:∂ 787:∂ 764:∂ 750:∂ 727:∂ 713:∂ 694:∇ 610:Δ 501:∇ 477:⋅ 474:∇ 444:∇ 437:∇ 434:⋅ 431:∇ 425:Δ 393:Δ 357:∇ 9860:(1962), 9464:See also 6012:axis by 5874:′ 5851:′ 5825:′ 5773:′ 5761:′ 5683:′ 5666:′ 5655:′ 5506:. Here 5437:′ 5387:P′ 5340:′ 5191:′ 5180:′ 5169:′ 4820:on  4755:in  4746:′ 4729:′ 4712:′ 4654:′ 4643:′ 4632:′ 4053:′ 4036:′ 4019:′ 1875:analytic 1850:but its 1351:(ξ) 515:gradient 9972:, 2001 9847:Sources 9822:Bibcode 9452:is the 7933:(about 7903:(about 7422:azimuth 7042:forces 4841:Now if 4468:physics 1779:=2) = 0 1754:annulus 513:is the 489:is the 462:is the 334:physics 9941:  9913:  9887:  9793:  9746:  9725:  9684:  9656:  9635:  9112:, and 9090:where 7430:< 2 7371:is an 7065:) = Θ( 6986:= cos 6651:) = Θ( 6366:. By 5786:where 5492:, and 5484:. Let 5457:where 4544:where 3727:where 2218:where 1734:Γ 1717:where 417:where 233:People 9791:S2CID 9773:arXiv 9530:Notes 9421:Here 9108:is a 7555:below 7521:is a 7420:, or 7345:Here 7095:with 7006:(cos 6975:below 6928:= 0, 4564:(see 9939:ISBN 9911:ISBN 9885:ISBN 9744:ISBN 9723:ISBN 9682:ISBN 9654:ISBN 9633:ISBN 9439:are 9430:and 8587:Let 7999:Let 7864:> 7853:For 7761:< 7749:ball 7426:0 ≤ 7385:and 7069:) Φ( 7027:) = 6960:+ 1) 6655:) Φ( 6344:) = 6055:is: 5954:for 5902:and 5467:and 5294:and 5143:and 5124:and 4894:and 4562:sink 4546:log( 3680:and 3224:and 2684:and 2135:and 1836:The 1805:The 1781:and 1528:or 332:and 9830:doi 9783:doi 9604:= 0 7737:r Y 7563:+ 1 7537:r Y 7525:of 7196:cos 7087:+ 1 7047:= 0 7033:B r 7029:A r 6967:≥ | 6807:sin 6772:sin 6751:sin 6557:sin 6503:sin 6471:sin 6258:sin 6204:sin 6172:sin 5908:′, 5855:cos 5841:sin 5832:sin 5815:cos 5806:cos 5794:cos 5727:cos 5673:sin 5496:be 5282:′, 5278:′, 4906:on 4506:log 4091:′, 4087:′, 3345:by 3165:cos 3130:sin 3061:sin 3026:cos 2758:log 2746:log 2702:log 1768:= 4 1761:= 2 1683:det 1275:sin 1221:sin 1189:sin 1030:In 834:In 679:In 385:or 328:In 10019:: 9996:. 9968:, 9962:, 9856:; 9828:. 9818:43 9816:. 9812:. 9789:. 9781:. 9769:53 9767:. 9755:^ 9706:^ 9665:^ 9102:, 9002:, 8998:, 8145:, 7991:. 7578:, 7543:, 7448:, 7405:/2 7375:, 7362:, 7105:≤ 7101:≤ 7061:, 7049:. 7031:+ 6952:= 6917:, 6892:, 6647:, 6360:, 6352:) 6340:, 6336:, 6313:0. 6021:90 5912:′) 5896:, 5488:, 5324:P' 5286:′) 4851:: 4792:if 4584:A 4576:. 4158:1. 4095:′) 3931:A 3573:, 3327:0. 3204:. 2038:iy 2036:+ 2032:= 2004:0. 1740:. 1724:ij 1353:, 1330:0. 1016:0. 840:, 820:0. 645:. 466:, 336:, 46:→ 10002:. 9947:. 9919:. 9893:. 9866:. 9838:. 9832:: 9824:: 9797:. 9785:: 9775:: 9750:. 9729:. 9688:. 9660:. 9639:. 9602:A 9576:2 9572:x 9563:1 9559:x 9555:= 9552:x 9475:R 9458:l 9448:s 9446:r 9435:l 9433:Q 9426:l 9424:P 9407:. 9403:) 9395:s 9391:r 9386:r 9383:2 9374:1 9370:( 9364:l 9360:Q 9351:1 9348:+ 9345:l 9340:s 9336:r 9330:2 9326:! 9322:) 9319:l 9316:( 9311:! 9308:) 9305:1 9302:+ 9299:l 9296:2 9293:( 9290:2 9282:1 9279:+ 9276:l 9272:) 9268:1 9262:( 9259:+ 9255:) 9247:s 9243:r 9238:r 9235:2 9226:1 9222:( 9216:l 9212:P 9205:! 9202:) 9199:l 9196:2 9193:( 9186:l 9181:s 9177:r 9171:2 9167:) 9163:! 9160:l 9157:( 9149:l 9145:) 9141:1 9135:( 9132:= 9129:) 9126:r 9123:( 9120:R 9106:) 9104:φ 9100:θ 9098:( 9095:l 9093:Y 9078:, 9075:) 9069:, 9063:( 9058:l 9054:Y 9050:) 9047:r 9044:( 9041:R 9038:= 9035:) 9029:, 9023:, 9020:r 9017:( 9004:φ 9000:θ 8996:r 8992:t 8966:, 8963:0 8960:= 8957:V 8952:2 8927:0 8924:= 8898:, 8892:G 8886:4 8883:= 8880:V 8875:2 8844:. 8840:g 8827:= 8820:V 8815:2 8798:, 8795:V 8790:2 8779:= 8776:) 8773:V 8764:( 8755:= 8747:g 8733:, 8730:V 8721:= 8713:g 8686:. 8680:G 8674:4 8668:= 8664:g 8637:G 8596:g 8564:V 8544:Q 8502:R 8478:R 8456:V 8433:0 8430:= 8405:. 8398:0 8382:= 8379:V 8374:2 8346:E 8333:= 8330:V 8325:2 8301:V 8296:2 8285:= 8282:) 8279:V 8270:( 8261:= 8257:E 8227:E 8205:0 8201:= 8197:E 8170:, 8167:V 8158:= 8154:E 8133:V 8111:. 8104:0 8091:= 8087:E 8054:0 8008:E 7977:m 7968:f 7947:0 7944:= 7941:r 7914:= 7911:r 7887:r 7867:R 7861:r 7839:. 7825:/ 7820:1 7814:| 7807:m 7798:f 7793:| 7772:1 7767:= 7764:R 7758:r 7739:ℓ 7730:ℓ 7728:f 7713:, 7710:) 7704:, 7698:( 7693:m 7684:Y 7674:r 7668:m 7659:f 7642:= 7639:m 7624:0 7621:= 7610:= 7607:) 7601:, 7595:, 7592:r 7589:( 7586:f 7575:r 7561:ℓ 7559:2 7547:) 7545:φ 7541:θ 7539:( 7530:ℓ 7528:Y 7509:Y 7506:) 7503:1 7500:+ 7494:( 7485:= 7482:Y 7477:2 7467:2 7463:r 7452:) 7450:φ 7446:θ 7444:( 7442:Y 7437:ℓ 7432:π 7428:φ 7418:φ 7410:π 7403:π 7398:0 7394:θ 7387:φ 7383:θ 7378:N 7367:ℓ 7365:P 7360:m 7356:ℓ 7350:ℓ 7348:Y 7331:. 7328:) 7322:, 7316:( 7311:m 7302:Y 7298:) 7295:1 7292:+ 7286:( 7277:= 7274:) 7268:, 7262:( 7257:m 7248:Y 7242:2 7232:2 7228:r 7207:) 7193:( 7188:m 7179:P 7170:m 7167:i 7163:e 7159:N 7156:= 7153:) 7147:, 7141:( 7136:m 7127:Y 7107:ℓ 7103:m 7099:ℓ 7097:− 7092:m 7085:ℓ 7083:2 7078:ℓ 7073:) 7071:φ 7067:θ 7063:φ 7059:θ 7057:( 7055:Y 7045:B 7039:R 7025:r 7023:( 7021:R 7015:R 7010:) 7008:θ 7003:ℓ 7001:P 6988:θ 6984:t 6971:| 6969:m 6965:ℓ 6958:ℓ 6956:( 6954:ℓ 6950:λ 6944:λ 6935:Θ 6930:π 6926:θ 6921:) 6919:φ 6915:θ 6913:( 6911:Y 6905:e 6900:Φ 6895:m 6889:π 6887:2 6879:Φ 6874:m 6868:m 6849:2 6845:m 6841:= 6837:) 6827:d 6819:d 6803:( 6793:d 6789:d 6766:+ 6755:2 6726:2 6722:m 6715:= 6707:2 6699:d 6689:2 6685:d 6673:1 6659:) 6657:φ 6653:θ 6649:φ 6645:θ 6643:( 6641:Y 6635:Y 6618:. 6609:= 6601:2 6588:Y 6583:2 6561:2 6552:1 6545:Y 6542:1 6537:+ 6533:) 6518:Y 6499:( 6467:1 6460:Y 6457:1 6451:, 6445:= 6441:) 6434:r 6431:d 6426:R 6423:d 6415:2 6411:r 6406:( 6399:r 6396:d 6392:d 6385:R 6382:1 6364:) 6362:φ 6358:θ 6356:( 6354:Y 6350:r 6348:( 6346:R 6342:φ 6338:θ 6334:r 6332:( 6330:f 6310:= 6302:2 6289:f 6284:2 6262:2 6252:2 6248:r 6243:1 6238:+ 6234:) 6219:f 6200:( 6167:2 6163:r 6158:1 6153:+ 6149:) 6142:r 6134:f 6123:2 6119:r 6114:( 6107:r 6091:2 6087:r 6083:1 6078:= 6075:f 6070:2 6035:m 6031:/ 6009:z 5992:m 5980:Y 5968:ℓ 5964:m 5957:ℓ 5950:ℓ 5948:Y 5923:u 5917:u 5910:φ 5906:θ 5904:( 5900:) 5898:φ 5894:θ 5892:( 5878:) 5861:( 5829:+ 5803:= 5766:d 5754:d 5745:2 5742:3 5737:) 5721:a 5718:2 5710:2 5702:+ 5697:2 5693:a 5689:( 5670:) 5659:, 5648:( 5645:g 5632:0 5619:2 5614:0 5605:) 5597:2 5593:a 5587:2 5574:1 5570:( 5564:3 5560:a 5550:4 5546:1 5541:= 5538:) 5535:P 5532:( 5529:u 5514:g 5508:θ 5503:P 5494:φ 5490:θ 5486:ρ 5476:P 5472:′ 5470:R 5464:P 5459:R 5444:, 5434:R 5424:4 5420:a 5409:R 5403:4 5399:1 5382:P 5364:. 5354:2 5350:a 5344:= 5319:ρ 5313:P 5303:a 5297:g 5291:f 5284:z 5280:y 5276:x 5274:( 5257:. 5254:S 5251:d 5247:g 5242:n 5238:G 5232:S 5224:+ 5221:V 5218:d 5214:f 5211:G 5206:V 5198:= 5195:) 5188:z 5184:, 5177:y 5173:, 5166:x 5162:( 5159:u 5146:G 5140:u 5134:S 5128:n 5126:G 5121:n 5119:u 5102:. 5099:S 5096:d 5091:] 5085:n 5081:G 5077:u 5069:n 5065:u 5061:G 5057:[ 5051:S 5043:= 5040:V 5037:d 5032:] 5028:G 5022:u 5016:u 5010:G 5006:[ 4994:V 4986:= 4983:V 4980:d 4975:] 4971:G 4958:u 4952:u 4939:G 4935:[ 4929:V 4908:S 4903:g 4897:u 4880:, 4877:f 4871:= 4868:u 4849:V 4844:u 4827:. 4824:S 4815:) 4812:z 4809:, 4806:y 4803:, 4800:x 4797:( 4787:0 4784:= 4781:G 4762:, 4759:V 4750:) 4743:z 4736:z 4733:, 4726:y 4719:y 4716:, 4709:x 4702:x 4699:( 4690:= 4687:G 4658:) 4651:z 4647:, 4640:y 4636:, 4629:x 4625:; 4622:z 4619:, 4616:y 4613:, 4610:x 4607:( 4604:G 4594:V 4590:S 4550:) 4548:r 4532:. 4523:2 4518:) 4515:r 4512:( 4497:= 4494:u 4452:. 4446:r 4440:4 4436:1 4431:= 4428:u 4418:r 4404:, 4396:2 4392:r 4385:4 4381:1 4373:= 4367:r 4364:d 4359:u 4356:d 4331:. 4326:a 4323:= 4320:r 4315:| 4308:r 4305:d 4300:u 4297:d 4289:2 4285:a 4278:4 4270:= 4267:S 4264:d 4257:r 4254:d 4249:u 4246:d 4238:S 4230:= 4227:V 4224:d 4220:u 4206:V 4198:= 4195:1 4178:a 4174:r 4152:= 4149:V 4146:d 4142:u 4128:V 4112:u 4093:z 4089:y 4085:x 4083:( 4078:δ 4060:, 4057:) 4050:z 4043:z 4040:, 4033:y 4026:y 4023:, 4016:x 4009:x 4006:( 3997:= 3992:z 3989:z 3985:u 3981:+ 3976:y 3973:y 3969:u 3965:+ 3960:x 3957:x 3953:u 3949:= 3946:u 3902:, 3893:= 3888:y 3885:y 3877:+ 3872:x 3869:x 3844:. 3841:v 3835:= 3830:y 3821:, 3818:u 3812:= 3807:x 3791:φ 3776:, 3773:y 3770:d 3766:v 3760:x 3757:d 3753:u 3747:= 3741:d 3730:ρ 3715:, 3709:= 3706:) 3703:v 3700:, 3697:u 3694:( 3668:, 3664:0 3660:= 3650:k 3643:) 3638:y 3634:u 3625:x 3621:v 3617:( 3614:= 3611:) 3608:0 3605:, 3602:v 3599:, 3596:u 3593:( 3577:) 3575:v 3571:u 3569:( 3542:. 3539:v 3533:= 3528:y 3519:, 3516:u 3510:= 3505:x 3485:ψ 3479:φ 3473:ψ 3458:, 3455:u 3449:= 3444:y 3435:, 3432:v 3429:= 3424:x 3408:ψ 3385:, 3382:y 3379:d 3375:u 3369:x 3366:d 3362:v 3359:= 3353:d 3342:ψ 3324:= 3319:y 3315:u 3306:x 3302:v 3298:= 3294:V 3267:, 3264:0 3261:= 3256:y 3252:v 3248:+ 3243:x 3239:u 3227:v 3221:u 3197:f 3182:, 3178:] 3171:n 3160:n 3156:r 3150:n 3146:b 3142:+ 3136:n 3125:n 3121:r 3115:n 3111:a 3106:[ 3095:1 3092:= 3089:n 3081:i 3078:+ 3074:] 3067:n 3056:n 3052:r 3046:n 3042:b 3032:n 3021:n 3017:r 3011:n 3007:a 3002:[ 2991:0 2988:= 2985:n 2977:= 2974:) 2971:z 2968:( 2965:f 2945:. 2940:n 2936:b 2932:i 2929:+ 2924:n 2920:a 2916:= 2911:n 2907:c 2886:, 2881:n 2877:z 2871:n 2867:c 2856:0 2853:= 2850:n 2842:= 2839:) 2836:z 2833:( 2830:f 2820:R 2815:f 2792:θ 2776:. 2770:i 2767:+ 2764:r 2755:= 2752:z 2743:= 2740:) 2737:z 2734:( 2731:f 2711:, 2708:r 2699:= 2686:θ 2682:r 2669:ψ 2654:, 2649:x 2646:y 2638:= 2633:y 2630:x 2614:ψ 2608:φ 2593:. 2590:y 2587:d 2581:x 2573:+ 2570:x 2567:d 2561:y 2550:= 2544:d 2533:ψ 2518:. 2513:x 2505:= 2500:y 2491:, 2486:y 2475:= 2470:x 2445:, 2442:) 2439:y 2436:, 2433:x 2430:( 2424:i 2421:+ 2418:) 2415:y 2412:, 2409:x 2406:( 2400:= 2397:) 2394:z 2391:( 2388:f 2378:) 2376:z 2374:( 2372:f 2366:v 2360:u 2345:. 2340:x 2336:) 2330:x 2326:u 2322:( 2316:= 2311:x 2307:) 2301:y 2297:v 2293:( 2287:= 2282:y 2278:) 2272:x 2268:v 2261:( 2258:= 2253:y 2250:y 2246:u 2235:x 2230:u 2223:x 2221:u 2206:. 2201:y 2197:u 2190:= 2185:x 2181:v 2176:, 2171:y 2167:v 2163:= 2158:x 2154:u 2138:v 2132:u 2127:) 2125:z 2123:( 2121:f 2106:, 2103:) 2100:y 2097:, 2094:x 2091:( 2088:v 2085:i 2082:+ 2079:) 2076:y 2073:, 2070:x 2067:( 2064:u 2061:= 2058:) 2055:z 2052:( 2049:f 2034:x 2030:z 2001:= 1996:y 1993:y 1985:+ 1980:x 1977:x 1961:2 1957:y 1943:2 1932:+ 1924:2 1920:x 1906:2 1863:φ 1857:D 1848:D 1843:φ 1827:D 1822:φ 1817:D 1812:φ 1794:) 1792:θ 1788:R 1786:( 1784:u 1777:r 1775:( 1773:u 1766:R 1759:r 1720:g 1705:) 1702:} 1697:j 1694:i 1690:g 1686:{ 1680:= 1677:g 1674:( 1670:, 1667:0 1664:= 1660:) 1651:j 1638:f 1627:j 1624:i 1620:g 1613:| 1609:g 1605:| 1598:( 1588:i 1567:| 1563:g 1559:| 1554:1 1549:= 1546:f 1541:2 1516:, 1513:0 1510:= 1505:n 1500:n 1497:m 1487:m 1484:j 1480:g 1471:j 1458:f 1449:+ 1445:) 1439:j 1436:k 1432:g 1423:k 1410:f 1400:( 1391:j 1374:= 1371:f 1366:2 1327:= 1319:2 1306:f 1301:2 1279:2 1269:2 1265:r 1260:1 1255:+ 1251:) 1236:f 1217:( 1184:2 1180:r 1175:1 1170:+ 1166:) 1159:r 1151:f 1140:2 1136:r 1131:( 1124:r 1108:2 1104:r 1100:1 1095:= 1092:f 1087:2 1062:) 1056:, 1050:, 1047:r 1044:( 1013:= 1005:2 1001:z 992:f 987:2 976:+ 968:2 955:f 950:2 935:2 931:r 927:1 922:+ 918:) 911:r 903:f 894:r 890:( 883:r 869:r 866:1 861:= 858:f 853:2 817:= 809:2 805:z 796:f 791:2 780:+ 772:2 768:y 759:f 754:2 743:+ 735:2 731:x 722:f 717:2 706:= 703:f 698:2 684:, 619:h 616:= 613:f 590:) 587:z 584:, 581:y 578:, 575:x 572:( 569:h 546:) 543:z 540:, 537:y 534:, 531:x 528:( 525:f 448:2 440:= 428:= 405:, 402:0 399:= 396:f 373:0 370:= 367:f 361:2 317:e 310:t 303:v 34:. 20:)

Index

Laplace equation
Theory of tides § Laplace's tidal equations
Mathematical analysis
Complex analysis

Complex numbers
Real number
Imaginary number
Complex plane
Complex conjugate
Unit complex number
Complex functions
Complex-valued function
Analytic function
Holomorphic function
Cauchy–Riemann equations
Formal power series
Basic theory
Zeros and poles
Cauchy's integral theorem
Local primitive
Cauchy's integral formula
Winding number
Laurent series
Isolated singularity
Residue theorem
Argument principle
Conformal map
Schwarz lemma
Harmonic function

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