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Question: Certain amount of an ideal gas are contained in a closed vessel. The vessel is moving with a constan...

Certain amount of an ideal gas are contained in a closed vessel. The vessel is moving with a constant velocity v. The molecular mass of gas is M. The rise in temperature of the gas when the vessel is suddenly stopped is (γ=CP/CV)(\gamma = C_{P}/C_{V})

A

Mv22R(γ+1)\frac{Mv^{2}}{2R(\gamma + 1)}

B

Mv2(γ1)2R\frac{Mv^{2}(\gamma - 1)}{2R}

C

Mv22R(γ+1)\frac{Mv^{2}}{2R(\gamma + 1)}

D

Mv22R(γ+1)\frac{Mv^{2}}{2R(\gamma + 1)}

Answer

Mv2(γ1)2R\frac{Mv^{2}(\gamma - 1)}{2R}

Explanation

Solution

If m is the total mass of the gas then its kinetic energy=12mv2= \frac{1}{2}mv^{2}

When the vessel is suddenly stopped then total kinetic energy will increase the temperature of the gas (because process will be adiabatic) i.e. 12mv2=μCvΔT=mMCvΔT\frac{1}{2}mv^{2} = \mu C_{v}\Delta T = \frac{m}{M}C_{v}\Delta T

[As Cv=Rγ1C_{v} = \frac{R}{\gamma - 1}]

mMRγ1ΔT=12mv2\frac{m}{M}\frac{R}{\gamma - 1}\Delta T = \frac{1}{2}mv^{2}ΔT=Mv2(γ1)2R\Delta T = \frac{Mv^{2}(\gamma - 1)}{2R}.