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11.Thermodynamics
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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 column, before and after the expansion respectively, then the value of $\frac{T_{1}}{T_{2}}$ will be
A
$\left(\frac{l_{1}}{I_{2}}\right)^{\frac{2}{3}}$
B
$\frac{l_{1}}{l_{2}}$
C
$\left(\frac{l_{2}}{l_{1}}\right)^{\frac{2}{3}}$
D
$\frac{l_{2}}{l_{1}}$
Solution
For adjabatic process
$TV ^{ s -1}= K$
$T _1 V _1^{ s -1}= T _2 V _2^{ r -1}$
$\frac{ T _1}{ T _2}=\left(\frac{ A }{ A } \frac{ L _2}{ L _1}\right)^{\frac{5}{3}-1}$
$\frac{ T _1}{ T _2}=\left(\frac{ L _2}{ L _1}\right)^{\frac{2}{3}}$
Standard 11
Physics
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