Classical Electrodynamics |
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Page 107
(N(x)(pmos(x))) (4.34) This is of the form of the first equation of (4.20) with the
charge density p' replaced by two terms, the first being the average charge per
unit volume of the molecules and the second being the polarization charge per
unit ...
(N(x)(pmos(x))) (4.34) This is of the form of the first equation of (4.20) with the
charge density p' replaced by two terms, the first being the average charge per
unit volume of the molecules and the second being the polarization charge per
unit ...
Page 190
(ex Hole: (6.81) y y Lót 47t Since the volume V is arbitrary, this can be cast into
the form of a differential continuity equation or conservation law, ;+ v.s-- E (6.82)
The vector S, representing energy flow, is called Poynting's vector. It is given by S
...
(ex Hole: (6.81) y y Lót 47t Since the volume V is arbitrary, this can be cast into
the form of a differential continuity equation or conservation law, ;+ v.s-- E (6.82)
The vector S, representing energy flow, is called Poynting's vector. It is given by S
...
Page 384
The Lorentz force equation can be written as a force per unit volume (
representing the rate of change of mechanical momentum of the sources per unit
volume): f = 2E ++ x B (11.126) C where J and p are the current and charge
densities.
The Lorentz force equation can be written as a force per unit volume (
representing the rate of change of mechanical momentum of the sources per unit
volume): f = 2E ++ x B (11.126) C where J and p are the current and charge
densities.
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Multipoles Electrostatics of Macroscopic Media | 98 |
Copyright | |
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