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Page 24
... equal to q1 , while the second has q2 . Use symmetry arguments and Gauss's law to prove that ( a ) the surface - charge densities on the adjacent faces are equal and opposite ; ( b ) the surface - charge densities on the outer faces of ...
... equal to q1 , while the second has q2 . Use symmetry arguments and Gauss's law to prove that ( a ) the surface - charge densities on the adjacent faces are equal and opposite ; ( b ) the surface - charge densities on the outer faces of ...
Page 397
... equal and oppositely directed momenta . This frame is called the center of momentum system ( soemtimes , loosely , the center of mass system ) and is denoted by CM system . The scattered particles ( or reaction products in a two - body ...
... equal and oppositely directed momenta . This frame is called the center of momentum system ( soemtimes , loosely , the center of mass system ) and is denoted by CM system . The scattered particles ( or reaction products in a two - body ...
Page 549
... equal to the product of the parities of the final state and the multipole field . To determine the parity of a multipole field we merely examine the behavior of the magnetic induction B , under the parity transformation of inversion ...
... equal to the product of the parities of the final state and the multipole field . To determine the parity of a multipole field we merely examine the behavior of the magnetic induction B , under the parity transformation of inversion ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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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 coefficients collisions component conducting conductor consider 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave 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 number wavelength ΦΩ