The electric potential energy of a charge in the electric field due to any charge is given by the work done by an external force in bringing a test charge from infinity to that point in the electric field.
Consider two point charges q1 and q2 initially lying at infinity.
Work done in bringing a charge q from infinity to a point where electric potential due to any charge is V is given by
W = qV
Initially when charge q1 is brought from infinity to a particular point, there is no work is done in bringing it because at that point no electric potential is presence due any other charge i.e. V = 0 at that point. Therefore
W1 = q1 V = q1 x 0 = 0
Now when charge q2 is brought from infinity to a point at distance r from the charge q1, the electric potential is present at that point due to charge q1 that is given by
V = 1/4πϵ0 q1/r
Therefore, work done in bringing charge q2 is given by
W2 = q2 x V = q2 x 1/4πϵ0 q1/r
⇒ W2 = 1/4πϵ0 q1q2/r
Net work done in bringing both charges from infinity is given by
W = W1 + W2
⇒ W = 0 + 1/4πϵ0 q1q2/r
⇒ W = 1/4πϵ0 q1q2/r
This work done is stored as electric potential energy (U) of the system of the two charges. Hence
U = 1/4πϵ0 q1q2/r
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Two point charges M and N having charges +q and -q respectively are placed at a distance apart. Force acting between them is F. If 30% of charge of N is transferred to M, then the force between the charges becomes:
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The electrostatic potential is also known as the electric field potential, electric potential, or potential drop is defined as “The amount of work that is done in order to move a unit charge from a reference point to a specific point inside the field without producing an acceleration.”
SI unit of electrostatic potential - volt
Other units - statvolt
Symbol of electrostatic potential - V or φ
Dimensional formula - ML2T3I-1
The electric potential energy of the system is given by the following formula:
U = 1/(4πεº) × [q1q2/d]
Where q1 and q2 are the two charges that are separated by the distance d.