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Page 24
... magnitude 4πσ , where σ is the charge density per unit area on the surface . 1.2 Two infinite , conducting , plane sheets of uniform thicknesses f1 and f2 , respectively , are placed parallel to one another with their adjacent faces ...
... magnitude 4πσ , where σ is the charge density per unit area on the surface . 1.2 Two infinite , conducting , plane sheets of uniform thicknesses f1 and f2 , respectively , are placed parallel to one another with their adjacent faces ...
Page 475
... magnitude of applied force . For circular motion , the magnitude of the rate of change of momentum ( which is equal to the applied force ) is ymv . Consequently , ( 14.46 ) can be written Peircular ( t ' ) = 2 e2 22 3 m2c3 dp dt ( 14.47 ) ...
... magnitude of applied force . For circular motion , the magnitude of the rate of change of momentum ( which is equal to the applied force ) is ymv . Consequently , ( 14.46 ) can be written Peircular ( t ' ) = 2 e2 22 3 m2c3 dp dt ( 14.47 ) ...
Page 614
... magnitude of the two mechanical forces ( A.2 ) and ( A.4 ) for known charges and currents , the magnitude of the ratio k1 / k , in free space can be found . The numerical value is closely given by the square of the velocity of light in ...
... magnitude of the two mechanical forces ( A.2 ) and ( A.4 ) for known charges and currents , the magnitude of the ratio k1 / k , in free space can be found . The numerical value is closely given by the square of the velocity of light in ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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