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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 ді = ▽ x ( v x B ) + се гов c2 Απσ ( 10.10 ) Here it is assumed that σ is constant in space . For a fluid at ...
... fields occur . The time dependence of the magnetic field can be written , using ( 10.8 ) to eliminate E , in the form : дв ді = ▽ x ( v x B ) + се гов c2 Απσ ( 10.10 ) Here it is assumed that σ is constant in space . For a fluid at ...
Page 382
John David Jackson. induction in the x2 direction . This magnetic field becomes almost equal to the transverse electric field E1 as B → 1. Even at nonrelativistic velocities where y 1 , this magnetic induction is equivalent to ~ B ~ qvx ...
John David Jackson. induction in the x2 direction . This magnetic field becomes almost equal to the transverse electric field E1 as B → 1. Even at nonrelativistic velocities where y 1 , this magnetic induction is equivalent to ~ B ~ qvx ...
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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