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Page 612
... dimensional analysis . 2 † The proportionality constant k2 in ( A.4 ) is thereby given the magnitude k2 = 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 k2 = 10 ' 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 ( / ) , mass ( m ) , and time ( t ) 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 ( / ) , mass ( m ) , and time ( t ) as independent , basic units . Furthermore , we will make the commonly accepted definition of current ...
Page 616
... dimensions of the electromagnetic constants for various systems of units = = The dimensions are given after the numerical values . The symbol c stands for the velocity of light in vacuum ( c 2.998 x 1010 cm / sec 2.998 × 108 m / sec ) ...
... dimensions of the electromagnetic constants for various systems of units = = The dimensions are given after the numerical values . The symbol c stands for the velocity of light in vacuum ( c 2.998 x 1010 cm / sec 2.998 × 108 m / sec ) ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ 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 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ