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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 : дв at = V x ( v x B ) + V2B Απσ ( 10.10 ) Here it is assumed that o 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 : дв at = V x ( v x B ) + V2B Απσ ( 10.10 ) Here it is assumed that o is constant in space . For a fluid at rest ...
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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 ...
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 ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ