Langevin theory of paramagnetism

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Langevin theory of paramagnetism [länzh·van ¦thē·ə·rē əv ‚par·ə′mag·nə‚tiz·əm]

(electromagnetism)

A theory which treats a substance as a classical (non-quantum-mechanical) collection of permanent magnetic dipoles with no interactions between them, having a Boltzmann distribution with respect to energy of interaction with an applied field.

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