Classical Electrodynamics |
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Page 16
... derivative of the potential ) every- where on the surface ( corresponding to a given surface - charge density ) also defines a unique problem . Specification of the normal derivative is known as the Neumann boundary condition . We now ...
... derivative of the potential ) every- where on the surface ( corresponding to a given surface - charge density ) also defines a unique problem . Specification of the normal derivative is known as the Neumann boundary condition . We now ...
Page 172
... derivative in ( 6.4 ) must take into account this motion . The flux through the circuit may change because ( a ) the flux changes with time at a point , or ( b ) the translation of the circuit changes the location of the boundary . It ...
... derivative in ( 6.4 ) must take into account this motion . The flux through the circuit may change because ( a ) the flux changes with time at a point , or ( b ) the translation of the circuit changes the location of the boundary . It ...
Page 188
... derivatives on the boundary surface S. We thus assume that there are no sources within V and that the initial values of y ... derivative of the delta function can be integrated by parts with respect to the time t ' . Then the Kirchhoff ...
... derivatives on the boundary surface S. We thus assume that there are no sources within V and that the initial values of y ... derivative of the delta function can be integrated by parts with respect to the time t ' . Then the Kirchhoff ...
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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