Two electric charges attract or repel each other. Therefore, some work has to be done in moving the charges away from each other, or in bringing them closer to each other.
This work gets stored in the form of potential energy in the system of those charges. This is called the electric potential energy of the system.
The electric potential energy of a system of charges is equal to the work that is done to make the system by bringing those charges closer to infinity.
Let a system AB be made up of two charges of coulomb +q_{1} and +q_{2} which are located at a distance of r meter from each other.
To find the electric potential energy of these systems, assume that the charge +q_{2} is not at point B but at infinity. Now the electric potential at point B due to charge +q_{1} :
According to the definition of electric potential, the work done in bringing the charge q_{2} from infinity to point B is
W = q_{2}V
This work itself is the electric potential energy U of the system (q_{1} + q_{2}).
If both the charges are of the same type then they repel each other. Then in bringing them closer to each other, work has to be done against the repulsive force, which increases the electric potential energy of the system.
On the contrary, in moving them away from each other, work is done by the system itself, which decreases the potential energy of the system.
If charges are of opposite type, they attract each other. In this case the potential energy of the system decreases when they are brought closer and increases when they are taken away.
Electric potential energy is a scalar quantity. In the formula, the values of charges q_{1} and q_{2} are kept with sign. If there are two or more charges in a system, then finding the electric potential energy of each pair of charges and adding them by algebraic method.
Example : If three charges q_{1} , q_{2} , +q_{3} are at three corners of a triangle, then the electric potential energy of the system
Potential Gradient and Intensity of Electric Field
Let us consider the electric field E along the Xaxis due to the +q point charge at point O. Let there be two points A and B respectively at x and x + Î”x distances from point O. Let the electric potential at points A and B be V and V – Î”v respectively.
Let a small positive test charge q_{0} be taken from point B to point A in electric field E. A force on charge q_{0} acts in the direction of the F field
where F = q_{0} E
Therefore, in moving the charge q_{0} from point B to A, the external agent will have to do work against the force F. If this work is w then
Î”W = F (Î”x)
where Î”x is the displacement from point B to A.
E Î”x = Î”v
E = – Î”v / Î”x
The amount Î”v / Î”x is the rate of change of the potential with distance and is called the potential gradient.

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The intensity of the electric field in a given direction at any point in the electric field is equal to the negative potential gradient in that direction.
The minus sign indicates that the potential decreases in the direction of the electric field.
dimensions of potential gradient = [MLT^{3}A^{1}]
Trajectory of a charged particle in a uniform electric field :
The motion of a charged particle in a uniform electric field is the same as that of a projectile in a uniform gravitational field.
Suppose two parallel plates of metal are located at some distance from each other and have opposite charge on them.
The electric field is the same in the space between the plates, except in places near the edges. If the upper plate is positively charged and the lower one is negativecharged, then the electric field E will be directed downwards in the plane of the paper.
Let an electron (e) moving along the Xaxis enter the electric field with a velocity v. The electric field is facing down in the negative direction of the Yaxis. Therefore, there is no force on the electron along the Xaxis, but a force F is applied along the Yaxis, whose value is
F = e E
Due to this force, the acceleration produced in the motion of the electron
a = F / m = e E / m
where m is the mass of the electron. force F is directed upwards along the Yaxis. Due to this force the electron gets deflected from its initial path and moves upwards.
Now we will consider the motions of the electron along the Xaxis and Yaxis separately. The electron moves along the xaxis with an initial velocity v because there is no significance in this direction. Hence, the distance traveled along the Xaxis in t Second
x = vt
The initial velocity of the electron along the Yaxis is zero, but the acceleration of the electron in this direction is a. Hence, the velocity of electron increases in +Y direction. The distance traveled in this direction in t second â€“
This equation is of the form y = cx^{2} and represents a parabola. Hence, the path of motion of the electron in the normal electric field is parabolic.
Equipotential Surface
The surface drawn in an electric field on which the potential is equal at all the points is called equipotential surface.
The potential difference between any two points on an equivalent surface is zero. Therefore, no work will have to be done in moving a charge from one point of the equipotential surface to another. But this is possible only when the charge is taken perpendicular to the electric field.
Therefore, the equipotential surface is perpendicular to the direction of the electric field at each point. The force lines at each point of the equipotential surface are perpendicular to the surface.
Force lines running through a point charge +q are drawn. A spherical surface drawn with the point charge as the center will be at the same potential due to being at the same distance from each point charge.