Classical Electrodynamics |
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Page 358
... defined at equal times t . The fact that this is not at equal times in the system K ' is not relevant for the definition of length in the system K. This again illustrates that simultaneity is only a relative concept . Another ...
... defined at equal times t . The fact that this is not at equal times in the system K ' is not relevant for the definition of length in the system K. This again illustrates that simultaneity is only a relative concept . Another ...
Page 612
... defined in both magnitude and dimension through theory and experiment in terms of the basic units . Tradition requires that mass ( m ) , length ( 1 ) , and time ( 1 ) be treated as basic units . But for electrical quantities there is as ...
... defined in both magnitude and dimension through theory and experiment in terms of the basic units . Tradition requires that mass ( m ) , length ( 1 ) , and time ( 1 ) be treated as basic units . But for electrical quantities there is as ...
Page 614
... definition of E , since E is the first derived field quantity to be defined . Only when we define other field quantities may it be convenient to insert dimensional proportionality constants in the definitions in order to adjust the ...
... definition of E , since E is the first derived field quantity to be defined . Only when we define other field quantities may it be convenient to insert dimensional proportionality constants in the definitions in order to adjust the ...
Common terms and phrases
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