Classical ElectrodynamicsProblems after each chapter |
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Page 15
... Laplace's equation ) is expressed in ( 1.36 ) in terms of the potential and its normal derivative only on the surface of the volume . This rather surprising result is not a solution to a boundary - value problem , but only an integral ...
... Laplace's equation ) is expressed in ( 1.36 ) in terms of the potential and its normal derivative only on the surface of the volume . This rather surprising result is not a solution to a boundary - value problem , but only an integral ...
Page 54
... Laplace's equation are represented by expansions in series of the appropriate orthonormal functions . Only an outline is given of the solution of the various ordinary differential equations obtained from Laplace's equation by separation ...
... Laplace's equation are represented by expansions in series of the appropriate orthonormal functions . Only an outline is given of the solution of the various ordinary differential equations obtained from Laplace's equation by separation ...
Page 69
... Laplace's Equation in Cylindrical Coordinates ; Bessel Functions In cylindrical coordinates ( p , p , z ) , as shown in Fig . 3.6 , Laplace's equation takes the form : 228 1 дФ + + 1 220 Φ + = 0 ap2 ρθρ p2 262 Əz2 ( 3.71 ) The ...
... Laplace's Equation in Cylindrical Coordinates ; Bessel Functions In cylindrical coordinates ( p , p , z ) , as shown in Fig . 3.6 , Laplace's equation takes the form : 228 1 дФ + + 1 220 Φ + = 0 ap2 ρθρ p2 262 Əz2 ( 3.71 ) The ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ