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Question: Two moles of an ideal monatomic gas occupies a volume \[V\] at \[{27^\circ }{\text{C}}\]. The gas ex...

Two moles of an ideal monatomic gas occupies a volume VV at 27C{27^\circ }{\text{C}}. The gas expands adiabatically to a volume 2V2V.Calculate (a) the final temperature of the gas and (b) change in its energy.
(A) (a) 189K (b)2.7kJ(a){\text{ }}189{\text{K (b)}} - {\text{2}}{\text{.7}}\,{\text{kJ}}
(B) (a) 195K (b)2.7kJ(a){\text{ }}195{\text{K (b)2}}{\text{.7}}\,{\text{kJ}}
(C) (a) 189K (b)2.7kJ(a){\text{ }}189{\text{K (b)2}}{\text{.7}}\,{\text{kJ}}
(D) (a) 195K (b)2.7kJ(a){\text{ }}195{\text{K (b)}} - {\text{2}}{\text{.7}}\,{\text{kJ}}

Explanation

Solution

Adiabatic process happens in a system in which there is no exchange of heat and mass with surroundings. The change in the internal energy is defined as negative of change in the work done in the adiabatic process. Use the relationship between the temperature and volume for adiabatic processes.

Complete step by step answer:(a)
Write down the expression for the adiabatic process in terms of temperature
T1V1γ1=T2V2γ1{T_1}{V_1}^{\gamma - 1} = {T_2}{V_2}^{\gamma - 1}
Here T1{T_1} and V1{V_1} are initial temperature and volume of gas respectively. T2{T_2} And V2{V_2} are initial temperature and volume of gas. γ\gamma is adiabatic constant.
Rearrange
T2=T1V1γ1V2γ1{T_2} = \dfrac{{{T_1}{V_1}^{\gamma - 1}}}{{{V_2}^{\gamma - 1}}}
Substitute VV forV1{V_1}, 2V2V forV2{V_2}, 53\dfrac{5}{3} for γ\gamma and 27C{27^\circ }{\text{C}} for T1{T_1}

(27C)1(2)531 (27C+373 K)1(2)23 300 K1(2)23 189 K  \Rightarrow ({27^\circ }{\text{C}})\dfrac{1}{{{{\left( 2 \right)}^{\dfrac{5}{3} - 1}}}} \\\ \Rightarrow \left( {{{27}^\circ }{\text{C}} + 373{\text{ K}}} \right)\dfrac{1}{{{{\left( 2 \right)}^{\dfrac{2}{3}}}}} \\\ \Rightarrow 300{\text{ K}}\dfrac{1}{{{{\left( 2 \right)}^{\dfrac{2}{3}}}}} \\\ \Rightarrow 189{\text{ K}} \\\

(b)

Write down the expression for the change in internal energyΔU\Delta U for adiabatic processes.
ΔU=nR(T2T1)γ1\Delta U = \dfrac{{nR({T_2} - {T_1})}}{{\gamma - 1}}
Here, nn is the number of moles and RR is gas constant.
Substitute 22 fornn, 8.318.31 forRR, 189K189{\text{K}} forT2{T_2}, 300 K300{\text{ K}} for T1{T_1}

ΔU=2×8.31(189300 K) 531  2767 K  \Delta U = \dfrac{{2 \times 8.31(189 - 300{\text{ K}}){\text{ }}}}{{\dfrac{5}{3} - 1}} \\\ \Rightarrow {\text{ }} - 2767{\text{ K}} \\\

Note: We have used ideal gas law here because it was mentioned in the question that the gas is ideal. Otherwise, we would have to use real gas laws. If in the question it was mentioned that the process is sudden but not mentioned adiabatic, then also the process would also be adiabatic. The adiabatic process does not involve any transfer of heat to or inside the system. γ\gamma is the ratio of specific heat at constant pressure to specific heat at constant volume. It is also given by relation called Mayer’s formula