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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 ...
Page 615
... dimensions ) I B = 2kqα á ( 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 á ( 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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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ