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Consider a solid cube made up of insulating material having a uniform volume charge density. Assuming the electrostatic potential to be zero at infinity, the ratio of the potential at a corner of the cube to that at the centre will be
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Charge density of the cube
Potential at the corner of a cube of side
Potential at the centre of a cube of side
Potential at the center of a cube of side
Potential at the corner of a cube of side
By dimensional analysis
But by superposition
Because of the centre of the larger cube lies at a corner of the eight smaller cubes of which it is made
Therefore,
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