Difficulty: Easy
Correct Answer: True
Explanation:
Introduction / Context:
Macroscopic polarization is a central concept in dielectrics. It describes how bound charges in a material shift slightly under an applied electric field, producing an average dipole moment density. Modeling each differential volume as carrying a dipole helps link microscopic charge displacements to macroscopic field equations (Maxwell’s equations with polarization and bound charge densities).
Given Data / Assumptions:
Concept / Approach:
The polarization vector P is defined as electric dipole moment per unit volume, P = dp/dV. In the continuum viewpoint, any sufficiently small volume element ΔV within a polarized medium possesses a net dipole moment p = P ΔV. This does not require permanent dipoles; even in nonpolar materials, electronic and ionic displacements create induced dipoles proportional to E. This local dipole model leads to bound charge densities ρb = −∇·P and surface bound charge σb = P·n̂ at interfaces, which correctly predict field distributions in composite dielectrics.
Step-by-Step Solution:
Verification / Alternative check:
Microscopic models (electronic/ionic/orientational polarization) average to the same macroscopic P. Measurements of capacitance and displacement current confirm the continuum description.
Why Other Options Are Wrong:
Restriction to ionic crystals or gases is unnecessary; permanent dipoles are not required for induced polarization.
Common Pitfalls:
Confusing permanent molecular dipoles with induced dipoles; both are encompassed by the macroscopic P field.
Final Answer:
True
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