The work done to move a charge along an equipotential from A to B
The work done to move a unit charge from any point A and B is defined as
Since, A and B have the same potential, the above integral can be written as
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The work done to move a charge along an equipotential from A to B
The work done to move a unit charge from any point A and B is defined as
Since, A and B have the same potential, the above integral can be written as