The electric displacement vector in a dielectric material is defined as
where is the vacuum permittivity, is the applied electric field, and is the polarization density - density of the permanent and induced electric dipole moments in the material.
According to the Maxwell's equations, the flux lines of must begin and end on the free charges. Thus, it can be considered as sort of analogue of electric field of free charges in a dielectric material (but only sort of, the exact definition is given by the expression above).
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