Abstract
A dielectric is effectively an insulator, meaning that a priori it does not have free and mobile charges. Nevertheless, different types of charges can be found, as shown in Figure 2.1. They are:
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1.
Dipolar charges, which are attached to a molecule that makes up the dielectric; examples are the dipoles attached to HCl molecules where the center of negative electronic charge is displaced towards the Cl atom, while the H has an excess positive charge, thus giving rise to the dipole H+Cl−. These charges are inseparable, tied to the bonded H and Cl, and are called bound charges.
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2.
Charges due to discontinuities such as interfaces between aggregates. Where the solid dielectrics exhibit defaults, charges can accumulate giving rise to particular electronic phenomena, such as the Maxwell-Wagner-Sillars effect at low frequencies.
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3.
Homocharges, which have the same sign as the electrodes to which they are adjacent.
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4.
Heterocharges, which have the opposite sign to the electrode at which they are near.
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5.
Space charges, which are charges localised within a region of space.
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Free charges, in principle, are little or not present in dielectrics. They can appear, however, when there is a breakdown caused the application of an electric field and a sudden loss in the ability of the material to insulate. When the current is relatively weak it is called a leak current and it can be due to a wide range of causes, such as impurities in the dielectric and so forth.
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© 2007 Springer Science+Business Media, LLC
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(2007). Electrostatics of Dielectric Materials. In: Basic Electromagnetism and Materials. Springer, New York, NY. https://doi.org/10.1007/978-0-387-49368-8_2
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DOI: https://doi.org/10.1007/978-0-387-49368-8_2
Publisher Name: Springer, New York, NY
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