To solve the given problem, we analyze each step of the cyclic process J→K→L→M→J for n=1 mole of a monatomic ideal gas.
For a monatomic ideal gas, the molar heat capacity at constant volume is:
CV=23R
From the given P−T diagram, the thermodynamic states are:
- State J: (P0,T0)
- State K: (P0,3T0)
- State L: (2P0,3T0)
- State M: (2P0,T0)
Step-by-Step Analysis of Each Process:
1. Process J→K (Isobaric process at P=P0):
- Temperature changes from T0 to 3T0.
- Work done (WJK):
WJK=nR(TK−TJ)=1⋅R⋅(3T0−T0)=2RT0
- Change in internal energy (ΔUJK):
ΔUJK=nCV(TK−TJ)=1⋅(23R)(3T0−T0)=3RT0
This corresponds to (Q) → (3).
2. Process K→L (Isothermal process at T=3T0):
- Pressure changes from P0 to 2P0.
- Change in internal energy (ΔUKL):
ΔUKL=0
- Work done (WKL):
WKL=nRTln(PLPK)=1⋅R(3T0)ln(2P0P0)=−3RT0ln2
- By the First Law of Thermodynamics, the heat given to the gas (QKL) is:
QKL=ΔUKL+WKL=−3RT0ln2
This corresponds to (R) → (5).
3. Process L→M (Isobaric process at P=2P0):
- Temperature changes from 3T0 to T0.
- Work done (WLM):
WLM=nR(TM−TL)=1⋅R⋅(T0−3T0)=−2RT0
4. Process M→J (Isothermal process at T=T0):
- Pressure changes from 2P0 to P0.
- Change in internal energy (ΔUMJ):
ΔUMJ=0 (since TM=TJ=T0)
This corresponds to (S) → (2).
- Work done (WMJ):
WMJ=nRTln(PJPM)=1⋅RT0ln(P02P0)=RT0ln2
Total Work Done in the Cyclic Process (P):
Wtotal=WJK+WKL+WLM+WMJ
Wtotal=2RT0+(−3RT0ln2)+(−2RT0)+(RT0ln2)=−2RT0ln2
This corresponds to (P) → (4).
Final Matching Summary:
- (P) Work done in complete cyclic process → (4)
- (Q) Change in internal energy in JK → (3)
- (R) Heat given to gas in KL → (5)
- (S) Change in internal energy in MJ → (2)
P→4;Q→3;R→5;S→2
Thus, the correct option is B.