The work done to move a charge along an equipotential from A to B (a) cannot be defined as -∫E.dI (from A→B)
The work done to move a charge along an equipotential from A to B
(a) cannot be defined as -∫E.dI (from A→B)
(b) must be defined as -∫E.dI (from A→B)
(c) is zero.
(d) can have a non-zero value.
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