$A$ monoatomic ideal gas,initially at temperature $T_1$,is enclosed in a cylinder fitted with a frictionless piston. The gas is allowed to expand adiabatically to a temperature $T_2$ by releasing the piston suddenly. If $L_1$ and $L_2$ are the lengths of the gas columns before and after the expansion respectively,then the ratio $\frac{T_2}{T_1}$ is:

  • A
    $\left[\frac{L_1}{L_2}\right]^{2/3}$
  • B
    $\left[\frac{L_1}{L_2}\right]^{1/2}$
  • C
    $\left[\frac{L_2}{L_1}\right]^{1/2}$
  • D
    $\left[\frac{L_2}{L_1}\right]^{2/3}$

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