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Page 13
... equation for the single function P ( x ) : γ Φ = -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 : V2 = 0 ( 1.29 ) We ...
... equation for the single function P ( x ) : γ Φ = -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 : V2 = 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 598
... equation of motion ( 17.50 ) differs from customary mechanical equations of motion in that the acceleration of the ... equation of motion become Newton's equation , mv ( t ) = F ( t ) . This is accomplished by choosing the upper limit on ...
... equation of motion ( 17.50 ) differs from customary mechanical equations of motion in that the acceleration of the ... equation of motion become Newton's equation , mv ( t ) = F ( t ) . This is accomplished by choosing the upper limit on ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ