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12. Show that cp? - ( + ; + ) = cp3. 13. Show that (E - cB) is relativistically invariant. 14. Show that
12. Show that cp? - ( + ; + ) = cp3. 13. Show that (E - cB) is relativistically invariant. 14. Show that (E B) is relativistically invariant. 15. Prove that (E - c*B) is relativistically invariant. Hence show that if E = cB in one inertial frame, then E' = cB' in any other frame.
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Introduction to Electrodynamics
Authors: David J. Griffiths
3rd Edition
978-0138053260, 013805326X, 8120316010, 978-8120316010
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