The magnetic flux through a stationary loop with resistance $R$ varies during an interval of time $T$ as $\phi = at(T - t)$. The heat generated during this time,neglecting the inductance of the loop,will be

  • A
    $\frac{a^2 T^3}{3R}$
  • B
    $\frac{a^2 T^2}{3R}$
  • C
    $\frac{a^2 T}{3R}$
  • D
    $\frac{a^2 T^3}{R}$

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