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Page 13
... equation for the single function ( x ) : V20 = -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 ) : V20 = -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 203
... equation ( 7.2 ) . Equation ( 7.8 ) represents waves traveling to the right and to the left with velocities of propagation equal to v , which is called the phase velocity of the wave . If v is a function of k , the situation is not as ...
... equation ( 7.2 ) . Equation ( 7.8 ) represents waves traveling to the right and to the left with velocities of propagation equal to v , which is called the phase velocity of the wave . If v is a function of k , the situation is not as ...
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 angle angular distribution antenna approximation atomic axis B₁ 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 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ