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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 ( / ) , and time ( t ) 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 ( / ) , and time ( t ) 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 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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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