The charge flowing through a resistance $R$ varies with time $t$ as $Q = at - bt^2$,where $a$ and $b$ are positive constants. The total heat produced in $R$ is

  • A
    $\frac{a^3 R}{3b}$
  • B
    $\frac{a^3 R}{2b}$
  • C
    $\frac{a^3 R}{b}$
  • D
    $\frac{a^3 R}{6b}$

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