GSO003 Problem 6
Problem Statement
Thermodynamic Cycle with a Spring-Loaded and Stopper-Controlled Piston
Problem Statement
A cylindrical container with a frictionless, massless piston is fixed with its axis pointing vertically upward. The container holds a monatomic ideal gas. The atmospheric pressure outside the cylinder is constant at P0.
Above the piston, a spring with spring constant k is attached vertically. The upper end of the spring is fixed, and the lower end just touches the top face of the piston (at natural length) when the piston is at its reference position. The spring constant satisfies k=3V02P0S2.
The gas is taken through the following thermodynamic cycle (State A → State B → State C → State A):
- State A: The gas volume is V0 and pressure is P0; the piston is at rest. The spring is at natural length and just touching the piston.
- Process A → B: Heat is slowly added to the gas. The gas expands, the piston rises, and the spring compresses. When the volume reaches 4V0, heating stops. This is State B.
- Process B → C: At State B, a stopper is inserted to hold the piston fixed. Heat is then slowly removed from the gas until the pressure drops to P0. This is State C.
- Process C → A: At State C, while the piston remains fixed, the spring is gently detached from the piston. The stopper is then removed, and heat is slowly removed from the gas while keeping the pressure equal to P0 throughout, until the volume returns to V0 (State A).
Find the thermal efficiency e of this one-cycle process.
Constraints
- Atmospheric pressure: P0=1.0×105Pa
- Gas volume at State A: V0=1.0×10−3m3
- Cross-sectional area of cylinder: S=1.0×10−2m2
- Spring constant: k=3V02P0S2=320000N/m
- Gas constant: R=8.31J/(mol⋅K)
Input Format
The thermal efficiency e is expressed as an irreducible fraction ba (a,b are coprime positive integers).
Compute a+b and give the answer as a positive integer.
Solution
1. Pressure and Volume at Each State
[State A] Given: VA=V0, PA=P0.
[State B] During process A → B, let x be the upward displacement of the piston (compression of the spring) when volume is V:
V−V0=Sx⟹x=SV−V0Force balance on the massless piston (gas pressure upward; atmospheric pressure and spring force downward):
PS=P0S+kxSubstituting x:
P=P0+S2k(V−V0)At State B, VB=4V0. Using k=3V02P0S2:
PB=P0+3V0S22P0S2(4V0−V0)=P0+2P0=3P0[State C] Process B → C is isochoric (constant volume), so VC=4V0. Cooling reduces pressure to PC=P0.
2. Work and Heat in Each Process
Using the first law of thermodynamics Qin=ΔU+Wout and U=23PV for a monatomic ideal gas:
[Process A → B (heat absorption)] The P–V path is a straight line from (V0,P0) to (4V0,3P0). Work done by the gas:
WAB=21(PA+PB)(VB−VA)=21(P0+3P0)(4V0−V0)=6P0V0Change in internal energy:
ΔUAB=23(PBVB−PAVA)=23(12P0V0−P0V0)=233P0V0Heat absorbed:
QAB=ΔUAB+WAB=233P0V0+6P0V0=245P0V0[Process B → C (heat release)] Isochoric, so WBC=0.
ΔUBC=23(PCVC−PBVB)=23(4P0V0−12P0V0)=−12P0V0QBC=−12P0V0 (heat released).
[Process C → A (heat release)] Isobaric at P0 after the spring is removed.
WCA=P0(VA−VC)=P0(V0−4V0)=−3P0V0 ΔUCA=23(PAVA−PCVC)=23(−3P0V0)=−29P0V0QCA=−29P0V0−3P0V0=−215P0V0 (heat released).
3. Thermal Efficiency
Net work done per cycle:
Wnet=WAB+WBC+WCA=6P0V0+0−3P0V0=3P0V0Total heat absorbed per cycle (only process A → B absorbs heat):
Qin=QAB=245P0V0Thermal efficiency:
e=QinWnet=245P0V03P0V0=456=152So a=2, b=15, and a+b=2+15=17.
Answer: 17