Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 84
Page 141
... component of J means that A will have only a component also . But this component A cannot be calculated by merely substituting J into ( 5.32 ) . Equation ( 5.32 ) holds only for rectangular components of A. * Thus we write rectangular ...
... component of J means that A will have only a component also . But this component A cannot be calculated by merely substituting J into ( 5.32 ) . Equation ( 5.32 ) holds only for rectangular components of A. * Thus we write rectangular ...
Page 476
... component is negligible ( of order 1/72 ) compared to that from the perpen- dicular component . Consequently we may neglect the parallel component of acceleration and approximate the radiation intensity by that due to the perpendicular ...
... component is negligible ( of order 1/72 ) compared to that from the perpen- dicular component . Consequently we may neglect the parallel component of acceleration and approximate the radiation intensity by that due to the perpendicular ...
Page 549
... component of angular momen- tum of a single photon is known precisely , the uncertainty principle requires that the other components be uncertain , with mean square values such that ( 16.67 ) holds . On the other hand , for a state of ...
... component of angular momen- tum of a single photon is known precisely , the uncertainty principle requires that the other components be uncertain , with mean square values such that ( 16.67 ) holds . On the other hand , for a state of ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
24 other sections not shown
Other editions - View all
Common terms and phrases
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