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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 | |
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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