Classical Electrodynamics |
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Page 13
... equation for the single function ( x ) : √20 = -Απρ ( 1.28 ) This equation is called Poisson's equation . In regions of space where there is no charge density , the scalar potential satisfies Laplace's equation : V20 = 0 ( 1.29 ) We ...
... equation for the single function ( x ) : √20 = -Απρ ( 1.28 ) This equation is called Poisson's equation . In regions of space where there is no charge density , the scalar potential satisfies Laplace's equation : V20 = 0 ( 1.29 ) We ...
Page 337
... equation in ( 10.91 ) is independent of magnetic field , we suspect that there exist solutions of a purely electrostatic nature , with B = 0. The continuity and force equations can be combined to yield a wave equation for the density ...
... equation in ( 10.91 ) is independent of magnetic field , we suspect that there exist solutions of a purely electrostatic nature , with B = 0. The continuity and force equations can be combined to yield a wave equation for the density ...
Page 405
... equations ( 12.2 ) and and ( 11.129 ) we see that we can write the force equation in the form : 1 dr . - ! SFJ , dz = dt с ν d3x ( 12.62 ) where the volume integral is over the extent of the charge . If the particle's velocity is v and ...
... equations ( 12.2 ) and and ( 11.129 ) we see that we can write the force equation in the form : 1 dr . - ! SFJ , dz = dt с ν d3x ( 12.62 ) where the volume integral is over the extent of the charge . If the particle's velocity is v and ...
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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