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Page 269
... dependence ( 9.1 ) , the solution for A becomes eik x - x ' A ( x ) = J ( x ' ) d3x ' -ハード x x ' | ( 9.3 ) where k = w / c is the wave number , and a sinusoidal time dependence is understood . The magnetic induction is given by B = V ...
... dependence ( 9.1 ) , the solution for A becomes eik x - x ' A ( x ) = J ( x ' ) d3x ' -ハード x x ' | ( 9.3 ) where k = w / c is the wave number , and a sinusoidal time dependence is understood . The magnetic induction is given by B = V ...
Page 296
... dependence on wave number . But the scalar result has no azimuthal dependence ( apart from that contained in § ) , whereas the vector expression does . The azimuthal variation comes from the polarization properties of the field , and ...
... dependence on wave number . But the scalar result has no azimuthal dependence ( apart from that contained in § ) , whereas the vector expression does . The azimuthal variation comes from the polarization properties of the field , and ...
Page 553
... dependence can be analyzed into its Fourier components , and we consider only harmonically varying sources , p ( x ) e - it , J ( x ) e - iot , M ( x ) e - iost ( 16.76 ) where it is understood that we take the real part of such complex ...
... dependence can be analyzed into its Fourier components , and we consider only harmonically varying sources , p ( x ) e - it , J ( x ) e - iot , M ( x ) e - iost ( 16.76 ) where it is understood that we take the real part of such complex ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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