Classical Electrodynamics |
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Page 150
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 gradient of a potential energy U, we find U ...
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 gradient of a potential energy U, we find U ...
Page 313
10.3 Magnetic Diffusion, Viscosity, and Pressure The behavior of a fluid in the
presence of electromagnetic fields is , governed to a large ... The time
dependence of the magnetic field can be written, using (10.8) to eliminate E, in
the form: 2 ...
10.3 Magnetic Diffusion, Viscosity, and Pressure The behavior of a fluid in the
presence of electromagnetic fields is , governed to a large ... The time
dependence of the magnetic field can be written, using (10.8) to eliminate E, in
the form: 2 ...
Page 382
This magnetic field becomes almost equal to the transverse electric field El as B
— 1. Even at nonrelativistic velocities where y c 1, this magnetic induction is
equivalent to B ~ 4 V × 5. - (11.119) c ro which is just the Ampère-Biot–Savart ...
This magnetic field becomes almost equal to the transverse electric field El as B
— 1. Even at nonrelativistic velocities where y c 1, this magnetic induction is
equivalent to B ~ 4 V × 5. - (11.119) c ro which is just the Ampère-Biot–Savart ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
BoundaryValue Problems in Electrostatics II | 54 |
Copyright | |
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