
An insulating material that does not conduct electricity but can be polarized by an electric field.A dielectric is an electrical insulator that can be polarized by an applied electric field. Unlike conductors, dielectrics do not allow free flow of charge, but their constituent molecules or atoms shift slightly, creating bound charges that partially cancel the applied field inside the material. This property is fundamental to capacitors, where dielectrics increase charge storage capacity, and to the behavior of light in transparent materials.
The term 'dielectric' was coined by Michael Faraday in the 1830s during his experiments on induction and insulation.
When an electric field is applied, the positive and negative charges within the dielectric's molecules are displaced in opposite directions, creating tiny dipoles. These dipoles align partially with the field, producing a macroscopic polarization that reduces the net electric field inside the material. The degree of this response is quantified by the dielectric constant (relative permittivity), which determines how much the material can store electrical energy.
Dielectrics are used in capacitors, electrical insulation, and as the active medium in many types of sensors and actuators, as well as in the gate oxides of transistors.
The dielectric strength of air is about 3 million volts per meter, which is why lightning can travel through kilometers of it.



















