Classical Electrodynamics |
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Page 612
... dimensional analysis . † The proportionality constant k2 in ( A.4 ) is thereby given the magnitude ką = 10-7 in the mks system . The dimensions of the “ absolute " ampere , as distinct from its magni- tude , depend on the dimensions ...
... dimensional analysis . † The proportionality constant k2 in ( A.4 ) is thereby given the magnitude ką = 10-7 in the mks system . The dimensions of the “ absolute " ampere , as distinct from its magni- tude , depend on the dimensions ...
Page 613
... dimensions of electromagnetism we will take as our starting point the traditional choice of length ( 1 ) , mass ( m ) , and time ( 1 ) as independent , basic units . Furthermore , we will make the commonly accepted definition of current ...
... dimensions of electromagnetism we will take as our starting point the traditional choice of length ( 1 ) , mass ( m ) , and time ( 1 ) as independent , basic units . Furthermore , we will make the commonly accepted definition of current ...
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 ...
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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