The magnetic field at the origin due to the current $I$ flowing in the wire as shown in the figure is:

  • A
    $ - \frac{{\mu _0 I}}{{8\pi a}}\left( {\hat i + \hat k} \right)$
  • B
    $\frac{{\mu _0 I}}{{2\pi a}}\left( {\hat i + \hat k} \right)$
  • C
    $\frac{{\mu _0 I}}{{8\pi a}}\left( { - \hat i + \hat k} \right)$
  • D
    $\frac{{\mu _0 I}}{{4\pi a\sqrt 2 }}\left( {\hat i - \hat k} \right)$

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