$A$ current loop consists of two identical semicircular parts each of radius $R,$ one lying in the $x-y$ plane and the other in the $x-z$ plane. If the current in the loop is $i,$ the resultant magnetic field due to the two semicircular parts at their common centre is

  • A
    $\frac{\mu_0 i}{2\sqrt{2} R}$
  • B
    $\frac{\mu_0 i}{2R}$
  • C
    $\frac{\mu_0 i}{4R}$
  • D
    $\frac{\mu_0 i}{\sqrt{2} R}$

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