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Polarization density
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===Time-varying polarization density=== When the polarization density changes with time, the time-dependent bound-charge density creates a ''polarization [[current density]]'' of <math display="block"> \mathbf{J}_p = \frac{\partial \mathbf{P}}{\partial t} </math> so that the total current density that enters Maxwell's equations is given by <math display="block"> \mathbf{J} = \mathbf{J}_f + \nabla\times\mathbf{M} + \frac{\partial\mathbf{P}}{\partial t}</math> where '''J'''<sub>f</sub> is the free-charge current density, and the second term is the [[Magnetization#Magnetization current|magnetization current]] density (also called the ''bound current density''), a contribution from atomic-scale [[Magnet#Two models for magnets: magnetic poles and atomic currents|magnetic dipoles]] (when they are present).
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