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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 2 = ▽ x ( v x B ) + V2B Απσ ( 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 : дв at 2 = ▽ x ( v x B ) + V2B Απσ ( 10.10 ) Here it is assumed that σ is constant in space . For a fluid at rest ...
Page 419
... field . Consequently they experience no net drift , at least to first order in 1 / R . This method of eliminating drifts due to spatial variations of the magnetic field is used in the Stellarator type of thermonuclear machine , in which ...
... field . Consequently they experience no net drift , at least to first order in 1 / R . This method of eliminating drifts due to spatial variations of the magnetic field is used in the Stellarator type of thermonuclear machine , in which ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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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 coefficients collisions component conducting conductor consider 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave 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 number wavelength ΦΩ