An electric current i enters and leaves a uniform circular wire of radius a through diametrically opposite points. A charged particle q moving along the axis of the circular wire passes through its centre at speed v. The magnetic force acting on the particle when it passes through the centre has a magnitude:
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$\text{qv}\frac{\mu_0\text{i}}{2\text{a}}$
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$\text{qv}\frac{\mu_0\text{i}}{2\pi\text{a}}$
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$\text{qv}\frac{\mu_0\text{i}}{\text{a}}$
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$\text{Zero}$



