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Invarients from the Faraday tensor |
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| Apr19-10, 04:38 AM | #1 |
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Invarients from the Faraday tensor
Hello,
a full contraction of the faraday tensor with itself can be shown to be [tex]F_{\mu\nu}F^{\nu\mu}=2(E^{2}-c^{2}B^{2})[/tex] I have done this by calculating 16 terms in the sum i.e. F11F11 + F12F21, and get this answer, but this is very tedious. Is there a faster way to show this that I am missing? |
| Apr19-10, 05:03 AM | #2 |
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Yes, by using the fact that the Faraday tensor is antisymmetric. This way you only have to calculate 6 terms.
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| Apr19-10, 05:39 AM | #3 |
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That is a good point. makes it much easier. Thanks
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| Apr19-10, 08:15 AM | #4 |
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Invarients from the Faraday tensor
It also gets easier if you recognize that the first row is just [tex]-{\vec E}[/tex], and the 3X3 space-like part is just [tex]-{\vec B}[/tex], a bit mixed up.
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