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Page 137
... law implies that the total force on the current distribution is F = - √ J ( x ) × B ( x ) d3x Similarly the total torque is N = x x ( J x B ) d3x ( 5.12 ) ( 5.13 ) These general results will be applied to localized ... Ampère's law, 4.
... law implies that the total force on the current distribution is F = - √ J ( x ) × B ( x ) d3x Similarly the total torque is N = x x ( J x B ) d3x ( 5.12 ) ( 5.13 ) These general results will be applied to localized ... Ampère's law, 4.
Page 177
... law : Ampère's law : Faraday's law : V.D = Απρ VX H : = 4πT J ( 6.22 ) 1 дв ▽ × E + = 0 с ді V.B = 0 Absence of free magnetic poles : These equations are written in macroscopic form and in Gaussian units . Let us recall that all but ...
... law : Ampère's law : Faraday's law : V.D = Απρ VX H : = 4πT J ( 6.22 ) 1 дв ▽ × E + = 0 с ді V.B = 0 Absence of free magnetic poles : These equations are written in macroscopic form and in Gaussian units . Let us recall that all but ...
Page 178
... Ampère's law , as can be seen by taking the diver- gence of both sides : 4π V. · V · J = ▽ • ( V x H ) = 0 ( 6.23 ) ... law ( 6.22 ) . Thus V.J + = ▽ J + др at 1 ƏD = 0 4п ді Then Maxwell replaced J in Ampère's law by its generalization ...
... Ampère's law , as can be seen by taking the diver- gence of both sides : 4π V. · V · J = ▽ • ( V x H ) = 0 ( 6.23 ) ... law ( 6.22 ) . Thus V.J + = ▽ J + др at 1 ƏD = 0 4п ді Then Maxwell replaced J in Ampère's law by its generalization ...
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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