Classical Electrodynamics |
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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 95
... cylinder . 3.7 For the cylinder in Problem 3.6 the cylindrical surface is made of two equal half - cylinders , one at potential V and the other at potential - V , so that V for - << ᅲ 2 V ( $ , z ) = π Зп - V for $ < 2 2 ᅲ FI2 ( a ) ...
... cylinder . 3.7 For the cylinder in Problem 3.6 the cylindrical surface is made of two equal half - cylinders , one at potential V and the other at potential - V , so that V for - << ᅲ 2 V ( $ , z ) = π Зп - V for $ < 2 2 ᅲ FI2 ( a ) ...
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 = μ1 € 1 w2 ...
... 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 = μ1 € 1 w2 ...
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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