The adjoining figure shows a conductor carrying a current $i$. The magnetic field at the origin is

  • A
    $ - \frac{{\mu _0 i}}{{4r}}\,\left( {\frac{{\hat i}}{\pi } + \frac{{\hat j}}{2}} \right)$
  • B
    $\frac{{\mu _0 i}}{{4r}}\,\left( {\frac{{\hat i}}{\pi } - \frac{{\hat j}}{2}} \right)$
  • C
    $\frac{{\mu _0 i}}{{4r}}\,\left( {\frac{{\hat i}}{2} - \frac{{\hat j}}{\pi }} \right)$
  • D
    $\frac{{\mu _0 i}}{{4r}}\,\left( {\frac{{2\hat i}}{\pi } + \hat j} \right)$

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