Question
Question: A vertical cylinder contains an ideal gas at atmospheric pressure. The cylinder has a 5kg movable pi...
A vertical cylinder contains an ideal gas at atmospheric pressure. The cylinder has a 5kg movable piston at the bottom which has a surface area 5×10−3m2. Now, the gas is heated slowly from 300K to 350K and the piston rises by 10cm. The piston is now clamped at this position and the gas is now cooled back to 300K. Find the difference between the heat provided during the heating process and the heat lost in the cooling process.

5 J
50 J
55 J
None of these
55 J
Solution
The problem involves two processes for an ideal gas: an isobaric heating process followed by an isochoric cooling process. We need to find the difference between the heat provided during heating and the heat lost during cooling.
Given Data:
- Mass of piston, m=5kg
- Surface area of piston, A=5×10−3m2
- Initial temperature, T1=300K
- Final temperature after heating, T2=350K
- Rise in piston, Δh=10cm=0.1m
- Atmospheric pressure, P0=105Pa
- Acceleration due to gravity, g=9.8m/s2
Process 1: Heating (Isobaric Process)
During heating, the piston is movable, so the pressure inside the cylinder remains constant. This constant pressure is the sum of atmospheric pressure and the pressure due to the piston's weight.
-
Calculate the total pressure (Ptotal):
Ptotal=P0+Amg
Ptotal=105Pa+5×10−3m25kg×9.8m/s2
Ptotal=105+5×10−349=105+9800=109800Pa
-
Calculate the change in volume (ΔV1):
ΔV1=A×Δh
ΔV1=(5×10−3m2)×(0.1m)=5×10−4m3
-
Calculate the work done by the gas (W1):
Since it's an isobaric process, W1=PtotalΔV1
W1=109800Pa×5×10−4m3=54.9J
-
Apply the First Law of Thermodynamics for Process 1:
ΔQ1=ΔU1+W1
Where ΔU1=nCv(T2−T1) is the change in internal energy.
ΔQ1=nCv(350K−300K)+54.9J
ΔQ1=nCv(50K)+54.9J
Process 2: Cooling (Isochoric Process)
The piston is clamped, so the volume remains constant. The gas is cooled from T2=350K back to T1=300K.
-
Calculate the work done by the gas (W2):
Since the volume is constant, ΔV2=0, so W2=PΔV2=0.
-
Apply the First Law of Thermodynamics for Process 2:
ΔQ2=ΔU2+W2
ΔQ2=ΔU2+0=ΔU2
Where ΔU2=nCv(T1−T2) is the change in internal energy.
ΔQ2=nCv(300K−350K)
ΔQ2=nCv(−50K)
Finding the Difference between Heat Provided and Heat Lost:
Heat provided during heating = ΔQ1
Heat lost in cooling process = −ΔQ2 (since ΔQ2 is negative, heat lost is a positive value)
Difference =ΔQ1−(−ΔQ2)
Difference =ΔQ1+ΔQ2
Alternatively, consider the entire process from T1 to T2 and back to T1. The net change in internal energy is zero because the gas returns to its initial temperature:
ΔUnet=ΔU1+ΔU2=nCv(T2−T1)+nCv(T1−T2)=0.
From the First Law of Thermodynamics for the entire process:
ΔQnet=ΔUnet+Wnet
ΔQ1+ΔQ2=0+(W1+W2)
ΔQ1+ΔQ2=W1+0
ΔQ1+ΔQ2=W1
The question asks for the difference between the heat provided (ΔQ1) and the heat lost (−ΔQ2).
So, the required difference is ΔQ1−(−ΔQ2)=ΔQ1+ΔQ2.
As derived above, this is equal to W1.
Difference =W1=54.9J
Rounding to the nearest integer, the value is approximately 55 J.