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Page 52
... cylinder axis to the line charge as the x axis ) , including the asymptotic form far from the cylinder ; ( c ) the induced surface - charge density , and plot it as a function of angle for R / b = 2 , 4 in units of 7 / 2πb ; ( d ) the ...
... cylinder axis to the line charge as the x axis ) , including the asymptotic form far from the cylinder ; ( c ) the induced surface - charge density , and plot it as a function of angle for R / b = 2 , 4 in units of 7 / 2πb ; ( d ) the ...
Page 259
... cylinder . The general considerations of Section 8.2 still apply , except that the transverse behavior of the fields is governed by two equations like ( 8.19 ) , one for inside the cylinder and one for outside : INSIDE Vi2 + ( 148 ...
... cylinder . The general considerations of Section 8.2 still apply , except that the transverse behavior of the fields is governed by two equations like ( 8.19 ) , one for inside the cylinder and one for outside : INSIDE Vi2 + ( 148 ...
Page 260
... cylinder in order to satisfy boundary conditions at all points on the surface at all times . In the usual way , inside the dielectric cylinder the transverse Laplacian of the fields must be negative so that the constant @ 2 για = μ1 € 1 ...
... cylinder in order to satisfy boundary conditions at all points on the surface at all times . In the usual way , inside the dielectric cylinder the transverse Laplacian of the fields must be negative so that the constant @ 2 για = μ1 € 1 ...
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