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Page 13
... equation for the single function ( x ) : Γ Φ = -4πρ Poisson's Eg . ( 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 ...
... equation for the single function ( x ) : Γ Φ = -4πρ Poisson's Eg . ( 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 ...
Page 337
... equation for the density fluctuations : 1 a2n Ət2 + ( Ame®no ) n - V2n = 0 m m an ( 10.92 ) On the other hand , the time derivative of Ampère's law and the force equation can be combined to give an equation for the fields : J2E + a12 દ ...
... equation for the density fluctuations : 1 a2n Ət2 + ( Ame®no ) n - V2n = 0 m m an ( 10.92 ) On the other hand , the time derivative of Ampère's law and the force equation can be combined to give an equation for the fields : J2E + a12 દ ...
Page 582
... Equation ( 17.9 ) is sometimes called the Abraham - Lorentz equation of motion . It can be considered as an equation which includes in some approximate and time - average way the reactive effects of the emission . of radiation . The ...
... Equation ( 17.9 ) is sometimes called the Abraham - Lorentz equation of motion . It can be considered as an equation which includes in some approximate and time - average way the reactive effects of the emission . of radiation . The ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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 coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ 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