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Page 412
... parallel to B. The solution for the velocity is easily shown to be v ( t ) = V13 + Wɲа ( € 1 = – ic , ) e i ) e - it ( 12.95 ) where is a unit vector parallel to the field , € , and € 1⁄2 are the other orthogonal unit vectors , v ,, is ...
... parallel to B. The solution for the velocity is easily shown to be v ( t ) = V13 + Wɲа ( € 1 = – ic , ) e i ) e - it ( 12.95 ) where is a unit vector parallel to the field , € , and € 1⁄2 are the other orthogonal unit vectors , v ,, is ...
Page 476
... parallel and perpendicular forces the radiation from the parallel 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 ...
... parallel and perpendicular forces the radiation from the parallel 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 ...
Page 575
... parallel and perpendicular to the plane , but their moments directed oppositely . The dipoles rotate with constant angular velocity w about a parallel axis located halfway between them ( w « c / a ) . ( a ) Calculate the components of ...
... parallel and perpendicular to the plane , but their moments directed oppositely . The dipoles rotate with constant angular velocity w about a parallel axis located halfway between them ( w « c / a ) . ( a ) Calculate the components 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