Let V and E denote the gravitational potential and gravitational field at a point, respectively. It is possible to have
A
V=0 and E=0
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B
V=0 and E≠0
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C
V≠0 and E=0
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D
V≠0 and E≠0
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Solution
The correct options are AV=0 and E≠0 BV≠0 and E=0 CV≠0 and E≠0 DV=0 and E=0 We know the relations E=−dVdx and hence V=−∫E.dx.
All the options can satisfy both the equations since the parameters are considered only for a point and we know that dydx can be 0 without y=0 for a given point.