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The dipole moment p can be represented as two charges q and -q separated by a distance d along the z=axis, located at a distance r from the wire as shown in Figure 1. Then
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We already know from 3.22 Eqn 1, that the electric field due to a long wire at a distance r from its axis is given by,
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acting radially outwards.
The force on positive and negative electric charges in the dipole are then respectively given by,
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The net force on the dipole is then given by,
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b)
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Similar to part a, now the charges are located along the x-axis. The force is then given by,
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c)
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Similar to parts a and b, the charges are located along the y-axis. The force is then given by,
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