Two identical circular current loops of radius $R$ carrying equal currents $I$ are placed such that their axes are inclined at $45^\circ$ to each other. The distance from the center of each loop to point $P$ is $\sqrt{3}R$. The resultant magnetic field at $P$ is:

  • A
    $\frac{\mu_0 I}{16\sqrt{2}R} [(\sqrt{2} + 1)\hat{i} + \hat{j}]$
  • B
    $\frac{\mu_0 I}{16\sqrt{2}R} [\sqrt{2}\hat{i} + \hat{j}]$
  • C
    $\frac{\mu_0 I}{16R} [(\sqrt{2} + 1)\hat{i} + \hat{j}]$
  • D
    $\frac{\mu_0 I}{16R} [\sqrt{2}\hat{i} + \hat{j}]$

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