In the $P-V$ diagram shown,there are two adiabatic parts of the same gas intersecting two isothermals at $T_1$ and $T_2$. The ratio $\left(\frac{V_b}{V_a}\right)$ is equal to

  • A
    $\left(\frac{V_c}{V_d}\right)^2$
  • B
    $\left(\frac{V_c}{V_d}\right)$
  • C
    $\frac{1}{2}\left(\frac{V_c}{V_d}\right)$
  • D
    $2\left(\frac{V_c}{V_d}\right)$

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