Show that the second equation in (12.126) can be expressed in terms of the field tensor Fv
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Show that the second equation in (12.126) can be expressed in terms of the field tensor Fμv as follows:
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Answer: -yß cos -yß sin 0 -yB cosp (y cos² + sin² ) (y-1) sino cos 0 -yß sin o 0 (y - 1) sino cos 0 (y sin²+ cos² ) 0 0
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We know that a Gv 0 is equivalent to the two homogeneous Maxwell equations VB 0 and VXE All we have ...View the full answer
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