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Page 612
... dimensional analysis . 2 † The proportionality constant k1⁄2 in ( A.4 ) is thereby given the magnitude k = 107 in the mks system . The dimensions of the " absolute " ampere , as distinct from its magni- tude , depend on the dimensions ...
... dimensional analysis . 2 † The proportionality constant k1⁄2 in ( A.4 ) is thereby given the magnitude k = 107 in the mks system . The dimensions of the " absolute " ampere , as distinct from its magni- tude , depend on the dimensions ...
Page 614
... dimensional proportionality constants in the definitions in order to adjust the dimensions and magnitude of these fields relative to the electric field . Consequently , with no significant loss of generality the electric field of a ...
... dimensional proportionality constants in the definitions in order to adjust the dimensions and magnitude of these fields relative to the electric field . Consequently , with no significant loss of generality the electric field of a ...
Page 615
... dimensions ) I B = 2kqα d ( A.6 ) The dimensions of the ratio of electric field to magnetic induction can be found from ( A.1 ) , ( A.3 ) , ( A.5 ) , and ( A.6 ) . The result is that ( E / B ) has the dimensions ( / ta ) . The third and ...
... dimensions ) I B = 2kqα d ( A.6 ) The dimensions of the ratio of electric field to magnetic induction can be found from ( A.1 ) , ( A.3 ) , ( A.5 ) , and ( A.6 ) . The result is that ( E / B ) has the dimensions ( / ta ) . The third and ...
Contents
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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