The electric force has the following properties: 1) It is directed along a line joining the two particles and is inversely proportional to the square of the separation distance r, between them. 2) It is proportional to the product of the magnitudes of the charges, q1 and q2, of the two particles. 3) It is attractive if the charges are of opposite sign and repulsive if the charges have the same sign.
An electric property associated with each point in space when charge is present in any form. E = Electric Field Strength or Electric Field Intensity (N/C or V/m), F = Force on a Charged Object (N), q_0 = Test Charge (C), Q = Source Charge (C), d = distance of Test Charge from Source Charge (m), ϵ_0 = Absolute Permittivity (8.854 x 10^-12 F/m or C^2/N∙m^2)
The summation of the normal component of the electric field displacement E(normal) over any closed surface is directly proportional to electric charge within the surface. Electric flux is the total number of field lines passing through a given cross sectional area perpendicular to the direction of Electric field lines.
Charges outside the surface do not give a net electric flux through the surface. 2) The net electric flux is directly proportional to the net amount of charge enclosed within the surface but is otherwise independent of the size of the closed surface. 3) Whether there is a net outward or inward electric flux through a closed surface depends on the sign of the enclosed charge.
The number of field lines that crosses a unit area or the lines of force per unit area. D = Electric Flux Density (C/m^2), Ψ = Gaussian Sum or Electric Flux, A = Area
Materials characterized by their ability to resist the flow of electric current. They serve as insulating mediums between conductive surfaces, such as the plates of a capacitor. When subjected to an electric field, dielectric materials polarize, meaning their electric charges become aligned in a way that reduces the overall electric field within the material. This property allows dielectrics to store electrical energy in the form of electric potential energy, thus increasing the capacitance of a capacitor.