The problem of isothermal expansion against a constant external pressure is a classic application of the First Law of Thermodynamics. Let's break down the physical reality of what's happening inside the cylinder and how the math perfectly models it.
Analyzing the Setup
Imagine a sturdy cylinder fitted with a movable piston. Inside, we have 5 moles of an ideal gas. The entire system is maintained at a constant temperature of 293 K. This is our first major clue: the process is isothermal.
The gas is initially at a high pressure of 2.1 MPa. It pushes against the piston, expanding until its internal pressure drops to 1.3 MPa. However, the expansion isn't happening in a vacuum or against a slowly changing force. The gas is pushing against a heavy, constant external pressure of 4.3 MPa. Because the external pressure is constant and significantly different from the internal pressure throughout the process, this expansion is highly irreversible.
The Master Equation
To find the heat transferred (
Q), we must invoke the
First Law of Thermodynamics:
ΔU=Q+W
For an ideal gas, the internal energy (U) is solely a function of its temperature. Since our process is isothermal, the temperature doesn't change, which means the internal energy doesn't change either (ΔU=0).
This simplifies our master equation beautifully:
Q=−W
This tells us a profound physical truth: all the work done by the gas during the expansion is exactly compensated by the heat flowing into the gas from the surroundings to keep its temperature constant.
Calculating the Irreversible Work
The work done by a gas expanding against a constant external pressure is given by:
W=−pextΔV=−pext(V2−V1)
We don't know the initial and final volumes (
V1 and
V2), but we do know the pressures. We can use the Ideal Gas Law (
pV=nRT) to express volume in terms of pressure:
V=pnRT
Substituting this into our work equation gives us a powerful new form:
W=−pext(p2nRT−p1nRT)
W=−pextnRT(p21−p11)
Final Calculation
Now, we substitute our known values. The external pressure pext is 4.3 MPa, n=5 mol, R=8.314 J mol−1K−1, and T=293 K. The initial and final pressures are 2.1 MPa and 1.3 MPa respectively.
Notice a beautiful mathematical convenience here: because pext is in the numerator and p1,p2 are in the denominator, their units of Mega Pascals (MPa) will perfectly cancel out! We don't need to convert them to Pascals.
W=−4.3×5×8.314×293×(1.31−2.11)
Let's resolve the bracket first:
1.31−2.11=1.3×2.12.1−1.3=2.730.8
Plugging this back in:
W=−4.3×5×8.314×293×(2.730.8)
W≈−15347.7 J
Converting this to kilo Joules, we get W≈−15.35 kJ.
Since Q=−W, the heat transferred into the system is 15.35 kJ.
A Note on the Final Answer
The question asks for the heat transferred in kJ mol−1. Strictly speaking, we should divide our total heat by the 5 moles of gas, which would give us 3.07 kJ mol−1.
However, in the official JEE Main answer key, the total heat transferred (15 kJ) was accepted as the correct integer answer. This implies the unit kJ mol−1 in the question text was likely a typographical error intended to just be kJ. Therefore, rounding 15.35 to the nearest integer, we arrive at our final answer of 15.