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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 √ , 2 + ( μse ...
... 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 √ , 2 + ( μse ...
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 γ = 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 γ = μ1 € 1 ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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