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Larmor's theorem

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Larmor's theorem [′lär·mȯrz ‚thir·əm]
(electromagnetism)
The theorem that for a system of charged particles, all having the same ratio of charge to mass, moving in a central field of force, the motion in a uniform magnetic inductionBis, to first order inB, the same as a possible motion in the absence ofBexcept for the superposition of a common precession of angular frequency equal to the Larmor frequency.


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