A thin rod is bent in the shape of a small circle of radius $'r'$. If the charge per unit length of the rod is $'\sigma ',$ and if the circle is rotated about its axis at the rate of $'n'$ rotation per second, the magnetic induction at a point on the axis at a large distance $'y'$ from the centre is
  • A$\frac{{{\mu _0}\pi {r^3}n\sigma }}{{{y^3}}}$
  • B$\frac{{2{\mu _0}\pi {r^3}n\sigma }}{{{y^3}}}$
  • C$\frac{{\left( {\frac{{{\mu _0}}}{{4\pi }}} \right){r^3}n\sigma }}{{{y^3}}}$
  • D$\frac{{\left( {\frac{{{\mu _0}}}{{2\pi }}} \right){r^3}n\sigma }}{{{y^3}}}$
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