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Page 612
... dimensional analysis . 2 † The proportionality constant k2 in ( A.4 ) is thereby given the magnitude k1 = 10- ' 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 k2 in ( A.4 ) is thereby given the magnitude k1 = 10- ' 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 = 2k2α a ( 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 = 2k2α a ( 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 ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ