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7 September 2017 Nature of the electromagnetic force between classical magnetic dipoles
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The Lorentz force law of classical electrodynamics states that the force 𝑭𝑭 exerted by the magnetic induction 𝑩𝑩 on a particle of charge π‘žπ‘ž moving with velocity 𝑽𝑽 is given by 𝑭𝑭 = π‘žπ‘žπ‘½π‘½ × π‘©π‘©. Since this force is orthogonal to the direction of motion, the magnetic field is said to be incapable of performing mechanical work. Yet there is no denying that a permanent magnet can readily perform mechanical work by pushing/pulling on another permanent magnet or by attracting pieces of magnetizable material such as scrap iron or iron filings. We explain this apparent contradiction by examining the magnetic Lorentz force acting on an Amperian current loop, which is the model for a magnetic dipole. We then extend the discussion by analyzing the Einstein-Laub model of magnetic dipoles in the presence of external magnetic fields.
Conference Presentation
© (2017) COPYRIGHT Society of Photo-Optical Instrumentation Engineers (SPIE). Downloading of the abstract is permitted for personal use only.
Masud Mansuripur "Nature of the electromagnetic force between classical magnetic dipoles", Proc. SPIE 10357, Spintronics X, 103570R (7 September 2017);

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