Classical Electrodynamics |
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Page 192
Note that we have written only E and B in (6.90), and not H or D. The reason is,
as mentioned earlier, that we are imagining all the charges as treated in the
mechanical part of the system and so use the microscopic equations which
involve ...
Note that we have written only E and B in (6.90), and not H or D. The reason is,
as mentioned earlier, that we are imagining all the charges as treated in the
mechanical part of the system and so use the microscopic equations which
involve ...
Page
This correspondence will sometimes be written A, = (A, i.A.) (11.95) Sometimes
the subscript on the 4-vector will be omitted, e.g. f(r) means f(x, t). 4. Scalar
products of 4-vectors will be denoted by (A → B) = A • B – Ao Bo (11.96) where A
• B is ...
This correspondence will sometimes be written A, = (A, i.A.) (11.95) Sometimes
the subscript on the 4-vector will be omitted, e.g. f(r) means f(x, t). 4. Scalar
products of 4-vectors will be denoted by (A → B) = A • B – Ao Bo (11.96) where A
• B is ...
Page
John David Jackson. (11.129), the force density becomes 1 9F - - F w vā J. 4t " or,
The right-hand side of (11.131) can be written as the divergence of a tensor of the
second rank. We define the symmetric tensor T., called the electromagnetic ...
John David Jackson. (11.129), the force density becomes 1 9F - - F w vā J. 4t " or,
The right-hand side of (11.131) can be written as the divergence of a tensor of the
second rank. We define the symmetric tensor T., called the electromagnetic ...
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Contents
Introduction to Electrostatics | 1 |
Nš 3 | 3 |
Greens theorem | 14 |
Copyright | |
30 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 classical collisions compared component conducting conductor Consequently consider constant coordinates cross section cylinder defined density depends 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 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 result satisfy scalar scattering shows side simple 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 |