Classical ElectrodynamicsProblems after each chapter |
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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 [ v ? 7,2 + ( μE ...
... 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 [ v ? 7,2 + ( μE ...
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 2,2 = 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 2,2 = μ1 € 1 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ 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