Question #101583
An ideal gas at initial temperature (T) and initial volume(V) is expanded adiabatically to a volume (2V). The gas is then expanded isothermally a volume (5V) and thereafter compressed adiabatically so that the temperature of the gas becomes again (T).If the final volume of the gas is x(V). then the value of x is......
1
Expert's answer
2020-01-21T07:39:48-0500

The combined gas law:

pVT=const\frac{p \cdot V}{T} = const,

where pp is the pressure of the gas, VV is the volume of the gas, TT is the temperature of the gas.

Initial parameters: p1=Pp_1=P, V1=VV_1=V and T1=TT_1=T.

1) adiabatic process is characterized by the constant entropy.

Gas can be characterized by the parameters p2p_2, V2V_2 and T2T_2.

V2=2VV_2=2V

T2=(V2V1)1γT1=(2VV)1γT=(2)1γTT_2=(\frac{V_2}{V_1})^{1 - \gamma} \cdot T_1 = (\frac{2V}{V})^{1 - \gamma} \cdot T= (2)^{1 - \gamma} \cdot T

where γ\gamma is the heat capacity ratio, which is constant for a calorifically perfect gas.

2) isothermal process is characterized by the constant temperature.

Gas can be characterized by the parameters p3p_3, V3V_3 and T3T_3.

V3=5VV_3=5V

T3=T2=(2)1γTT_3=T_2= (2)^{1 - \gamma} \cdot T

3) adiabatic process is characterized by the constant entropy.

Gas can be characterized by the parameters p4p_4, V4V_4 and T4T_4.

T4=TT_4=T, so T4T3=T(2)1γT=(2)γ1\frac{T_4}{T_3}=\frac{T}{(2)^{1 - \gamma} \cdot T} = (2)^{ \gamma - 1}

V4=V3(T4T3)11γ=5V((2)γ1)11γ=(2)γ11γ5V=(2)15V=5V2=2.5VV_4=V_3 (\frac{T_4}{T_3})^{\frac{1}{1- \gamma}} = 5V ((2)^{ \gamma - 1})^{\frac{1}{1- \gamma}}=(2)^{\frac{\gamma -1}{1 - \gamma}} \cdot 5V= (2)^{-1} \cdot 5V = \frac{5V}{2} = 2.5V


Answer: If the final volume of the gas is x(V)x(V), then the value of xx is 2.5.


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