The equation of state of a gas is given by $\left( P + \frac{aT^2}{V} \right) V^c = (RT + b)$,where $a, b, c$ and $R$ are constants. The isotherms can be represented by $P = AV^m - BV^n$,where $A$ and $B$ depend only on temperature. Then:

  • A
    $m = -c$ and $n = -1$
  • B
    $m = c$ and $n = 1$
  • C
    $m = -c$ and $n = 1$
  • D
    $m = c$ and $n = -1$

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