The electric displacement vector "\\mathbf{D}" in a dielectric material is defined as
where "\\varepsilon_{0}" is the vacuum permittivity, "\\mathbf{E}" is the applied electric field, and "\\mathbf{P}" 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 "\\mathbf{D}" 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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