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
... 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
... 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 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
17 other sections not shown
Other editions - View all
Common terms and phrases
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