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 | |
6 other sections not shown
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Common terms and phrases
acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge charged particle classical collisions compared component conducting Consequently consider constant coordinates cross section cylinder defined density dependence derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved light limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative relativistic result satisfy scalar scattering shown in Fig shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written
Bibliographic information
| Title | Classical Electrodynamics |
| Author | John David Jackson |
| Publisher | Wiley, 1963 |
| Length | 641 pages |
| Export Citation | BiBTeX EndNote RefMan |