Classical Electrodynamics |
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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 48
... Laplace's equation in rectangular coordinates is 2Ф 220 a2c + + = 0 მე 2 dy2 Əz2 ( 2.54 ) A solution of this partial differential equation can be found in terms of three ordinary differential equations , all of the same form , by the ...
... Laplace's equation in rectangular coordinates is 2Ф 220 a2c + + = 0 მე 2 dy2 Əz2 ( 2.54 ) A solution of this partial differential equation can be found in terms of three ordinary differential equations , all of the same form , by the ...
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 ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss factor force equation frame frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ