Classical ElectrodynamicsProblems after each chapter |
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Page 39
... distance away from the center for points outside the sphere . By a suitable choice of center of inversion and associated parameters we can obtain the potential due to a point charge q a distance d away from an infinite , grounded ...
... distance away from the center for points outside the sphere . By a suitable choice of center of inversion and associated parameters we can obtain the potential due to a point charge q a distance d away from an infinite , grounded ...
Page 52
... distance d from its center , show that the charge induced on the boss is ― q = -9 1 d2 a2 dvd2 + a2 2.7 2,8 A line charge with linear charge density is placed parallel to , and a distance R away from , the axis of a conducting cylinder ...
... distance d from its center , show that the charge induced on the boss is ― q = -9 1 d2 a2 dvd2 + a2 2.7 2,8 A line charge with linear charge density is placed parallel to , and a distance R away from , the axis of a conducting cylinder ...
Page 225
... distance . This means that an electromagnetic wave entering a conductor is damped to 1 / e = 0.369 of its initial amplitude in a distance : с = β 2πμωσ ( 7.85 ) the last form being the approximation for good conductors . The distance ...
... distance . This means that an electromagnetic wave entering a conductor is damped to 1 / e = 0.369 of its initial amplitude in a distance : с = β 2πμωσ ( 7.85 ) the last form being the approximation for good conductors . The distance ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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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