Dielectrics are materials that are very poor conductors of electric current. These are materials in which the outer electrons are firmly bound to their respective nuclei. These electrons cannot leave the nucleus, even if they can be pulled towards a particular side of the nucleus. They are insulators and contain no free electrons. In stark contrast to insulators are conductors, in which the electrons are free to move from atom to atom. Here, we shall focus on dielectrics and see why they are materials that are very poor conductors of electric current.
Dielectrics are non-conducting materials that are very poor conductors of electric current. Moreover, they have a negligible number of charge carriers. Fundamentally, they are insulators and contain no free electrons.
When there is an external electric field, the creation of dipole moments can take place in dielectrics. This is by the stretching and re-orienting of its molecules. The collective dipole moment can be defined as the net charge on the dielectric’s surface. Also, it opposes and reduces the external field. This is why they are materials that are very poor conductors of electric current.
Examples of dielectric materials are as follows:
Suppose there is an external electric field in which the atoms or molecules of a dielectric are placed. In such a case, there is pushing of nuclei within the field. This causes a high positive charge on a particular side while there is pulling of the electron clouds against it. Consequently, an increased negative charge is formed on the other side. This is a simple explanation of the process called polarisation.
In such a state, the dielectric material becomes polarised. This is why dielectrics can be easily polarised, and this can take place by two main methods:
Below are the various types of polarisation.
Dielectrics are materials that are very poor conductors of electric current. Here, the outer electrons are strongly attached to their nuclei. We can term these materials as insulators that contain no free electrons. Dielectrics can be easily polarised, and this can happen with two methods: stretching and rotation. There are four types of polarisation: electronic polarisation, ionic polarisation, dipole (or orientation) polarisation, and space charge (or interfacial) polarisation.
The measure of temperature is the microscopic kinetic energy of molecules and atoms that is able to transfer to neighbouring molecules and atoms in a process known as heat conduction. The rate of heat conduction varies for different objects and materials. We define a heat conduction equation as one that describes the heat flow for a body of material of known dimension and placed under a temperature difference. The coefficient of thermal conductivity is a constant that appears in this equation. Its value describes how easily heat transfer can take place for different materials. Furthermore, we discussed the applications of thermal conductivities in describing thermal conductors and insulators.