Electric potential energy
Electric potential energy:
The electric potential energy of a system of point charges may be defined as the amount of work done in assembling the charges at their location by bringing them in, from infinity.
Expression for the potential energy of a system of two point charges:
Suppose a point charge q1 is at rest at a point p1 in space as shown in fig. it takes no work to bring their first charge q1 because there is no field yet to work against therefore W1 = 0
Electric potential due to charge q1 at appoint P2 at a distance r12 from P1 will be
If charge q2 is moved in from infinity to point P2. The work system (q1 + q2) so
Potential energy of a system of three point charges:
AS shown in fig. now we bring in the charge q3 from infinity to point P3. Work has to be done against the forces exerted by q1 and q2 therefore.
W3 = Potential at point P3 due to q1 and q2 * charge q3
Hence the electrostatic potential energy of the system q1 + q2 + q3 is
U = Total word done to assemble the three charges
= W1 + W2 + W3
Potential energy of a system of N point charges:
The expression for the potential of n point charges can be written as
As double summation counts every pair twice, to avoid this factor ½ has been introduced.
Potential energy of a single charge in an external field:
By definition, V at point is the amount of work done in bringing a unit positive charge from infinity to the point P. Thus the work done is
W = qV
This work done is stored as the potential energy of the charge q. if is the position vector of point P relative to some origin, then
P.E. of a charge in an external field = charge * external electric potential
So we can define electric potential at a given point in an external field is the potential energy of a unit positive charge at that point.
Potential energy of a system of two charges in an external electric field:
Let V1 and V2 be the electric potentials of the field E at the points where q1 and q2 are located. Then potential energy of the two charges in the field E is
U = p.E. due to interaction between q1 and + P.E. due to interaction between q2 and E + P.E. due to interaction between q1 and q2