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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 | |
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