The magnetic induction at the centre $O$ of the current-carrying bent wire shown in the adjoining figure is:

  • A
    $\frac{{\mu _0}I}{{4\pi {R_1}}}\alpha $
  • B
    $\frac{{\mu _0}I}{{4\pi {R_2}}}\alpha $
  • C
    $\frac{\mu_0 I \alpha}{4\pi} \left( \frac{1}{R_1} - \frac{1}{R_2} \right)$
  • D
    $\frac{\mu_0 I \alpha}{4\pi} \left( \frac{1}{R_1} + \frac{1}{R_2} \right)$

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