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Question: One mole of an ideal monoatomic gas is taken through a thermodynamic process shown in the P – V diag...

One mole of an ideal monoatomic gas is taken through a thermodynamic process shown in the P – V diagram. The heat supplied to the system in this process is K × (π\pi + 10)P0V0P_0 V_0. Determine the value of K.

Answer

1

Explanation

Solution

The process is a cycle A \to B \to A.

Process A to B is isobaric expansion at P=2P0P=2P_0 from V=2V0V=2V_0 to V=4V0V=4V_0. Work done WAB=2P0(4V02V0)=4P0V0W_{AB} = 2P_0 (4V_0 - 2V_0) = 4P_0 V_0. Change in internal energy ΔUAB=nCvΔTAB\Delta U_{AB} = n C_v \Delta T_{AB}. TA=(2P0)(2V0)R=4P0V0RT_A = \frac{(2P_0)(2V_0)}{R} = \frac{4P_0 V_0}{R}, TB=(2P0)(4V0)R=8P0V0RT_B = \frac{(2P_0)(4V_0)}{R} = \frac{8P_0 V_0}{R}. ΔTAB=4P0V0R\Delta T_{AB} = \frac{4P_0 V_0}{R}. For monoatomic gas, Cv=32RC_v = \frac{3}{2}R. ΔUAB=1×32R×4P0V0R=6P0V0\Delta U_{AB} = 1 \times \frac{3}{2}R \times \frac{4P_0 V_0}{R} = 6 P_0 V_0. Heat supplied QAB=ΔUAB+WAB=6P0V0+4P0V0=10P0V0Q_{AB} = \Delta U_{AB} + W_{AB} = 6 P_0 V_0 + 4P_0 V_0 = 10 P_0 V_0.

Process B to A is a curved path from (4V0,2P0)(4V_0, 2P_0) to (2V0,2P0)(2V_0, 2P_0) passing through (3V0,4P0)(3V_0, 4P_0). This is the upper half of an ellipse centered at (3V0,2P0)(3V_0, 2P_0) with semi-axes a=V0a=V_0 and b=2P0b=2P_0. Work done WBA=4V02V0PdVW_{BA} = \int_{4V_0}^{2V_0} P dV. The area under the curve is the area of the rectangle with height 2P02P_0 and width 2V02V_0 plus the area of the semi-ellipse with semi-axes a=V0a=V_0 and b=2P0b=2P_0. The area of the semi-ellipse is 12πab=12π(V0)(2P0)=πP0V0\frac{1}{2} \pi a b = \frac{1}{2} \pi (V_0)(2P_0) = \pi P_0 V_0. The area under the curve from V=4V0V=4V_0 to V=2V0V=2V_0 is the area of the rectangle from V=2V0V=2V_0 to V=4V0V=4V_0 at P=2P0P=2P_0 plus the area of the semi-ellipse above P=2P0P=2P_0. The area under the curve is 2P0(4V02V0)+πP0V0=4P0V0+πP0V02P_0 (4V_0 - 2V_0) + \pi P_0 V_0 = 4P_0 V_0 + \pi P_0 V_0. Since the volume is decreasing, the work done by the system is negative. WBA=(4P0V0+πP0V0)=4P0V0πP0V0W_{BA} = -(4P_0 V_0 + \pi P_0 V_0) = -4P_0 V_0 - \pi P_0 V_0. Change in internal energy ΔUBA=nCvΔTBA\Delta U_{BA} = n C_v \Delta T_{BA}. ΔTBA=TATB=4P0V0R\Delta T_{BA} = T_A - T_B = - \frac{4P_0 V_0}{R}. ΔUBA=1×32R×(4P0V0R)=6P0V0\Delta U_{BA} = 1 \times \frac{3}{2}R \times (-\frac{4P_0 V_0}{R}) = -6 P_0 V_0. Heat supplied QBA=ΔUBA+WBA=6P0V0+(4P0V0πP0V0)=10P0V0πP0V0Q_{BA} = \Delta U_{BA} + W_{BA} = -6 P_0 V_0 + (-4P_0 V_0 - \pi P_0 V_0) = -10 P_0 V_0 - \pi P_0 V_0.

The heat supplied to the system in this process (the cycle) is the net heat transfer Qcycle=QAB+QBA=10P0V0+(10P0V0πP0V0)=πP0V0Q_{cycle} = Q_{AB} + Q_{BA} = 10 P_0 V_0 + (-10 P_0 V_0 - \pi P_0 V_0) = -\pi P_0 V_0. The given heat supplied is K×(π+10)P0V0K \times (\pi + 10)P_0 V_0. If this is the net heat supplied, then πP0V0=K(π+10)P0V0-\pi P_0 V_0 = K (\pi + 10) P_0 V_0, so K=ππ+10K = -\frac{\pi}{\pi + 10}.

If the question asks for the magnitude of the heat transferred during the process from B to A, then QBA=10P0V0πP0V0=(10+π)P0V0|Q_{BA}| = |-10 P_0 V_0 - \pi P_0 V_0| = (10 + \pi) P_0 V_0. If QBA=K(π+10)P0V0|Q_{BA}| = K (\pi + 10) P_0 V_0, then (10+π)P0V0=K(π+10)P0V0(10 + \pi) P_0 V_0 = K (\pi + 10) P_0 V_0, so K=1K=1.

Given the structure of the expression, it is highly probable that the question is asking for the magnitude of the heat transferred during the process from B to A.

The final answer is 1\boxed{1}.