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Page 150
... magnetic induction . The potential energy of a permanent magnetic moment ( or dipole ) in an external magnetic field can be obtained from either the force ( 5.69 ) or the torque ( 5.72 ) . If we interpret the force as the negative ...
... magnetic induction . The potential energy of a permanent magnetic moment ( or dipole ) in an external magnetic field can be obtained from either the force ( 5.69 ) or the torque ( 5.72 ) . If we interpret the force as the negative ...
Page 313
... fields occur . The time dependence of the magnetic field can be written , using ( 10.8 ) to eliminate E , in the form : ав at = ▽ x ( v x B ) + c2 Απσ V2B ( 10.10 ) Here it is assumed that σ is constant in space . For a fluid at rest ...
... fields occur . The time dependence of the magnetic field can be written , using ( 10.8 ) to eliminate E , in the form : ав at = ▽ x ( v x B ) + c2 Απσ V2B ( 10.10 ) Here it is assumed that σ is constant in space . For a fluid at rest ...
Page 382
John David Jackson. induction in the x direction . This magnetic field becomes almost equal to the transverse electric field E1 as ẞ → 1. Even at nonrelativistic velocities where y 1 , this magnetic induction is equivalent to B ~ с qvx ...
John David Jackson. induction in the x direction . This magnetic field becomes almost equal to the transverse electric field E1 as ẞ → 1. Even at nonrelativistic velocities where y 1 , this magnetic induction is equivalent to B ~ с qvx ...
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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