Thermodynamics is a beautiful interplay of state variables and path-dependent functions. In this problem, we are presented with a classic p−V diagram showing three distinct thermodynamic processes originating from a single state and terminating on a common isotherm. Let's break down the physics step-by-step to uncover the absolute truth, even if the given options try to trick us!
Decoding the P-V Diagram
Take a close look at the p−V diagram. We have an initial state A lying on a lower isotherm, T2. From this point, the gas undergoes three different processes: A→B, A→C, and A→D.
The crucial observation here is that all three final states—B, C, and D—lie on the exact same upper isotherm, T1. We are explicitly given that T1>T2. This geometric setup immediately tells us that regardless of the path taken, the initial and final temperatures for all three processes are identical.
The Secret of Internal Energy
Now, let's talk about the change in internal energy, denoted as E (or ΔU). For an ideal gas, the internal energy is a state function. This means it depends exclusively on the absolute temperature of the gas and is completely blind to the path taken to reach that state.
The mathematical expression for this is:
Since all three processes start at temperature T2 and end at temperature T1, the change in temperature ΔT=T1−T2 is exactly the same for paths A→B, A→C, and A→D. Consequently, the change in internal energy must be identical across the board:
The Geometry of Work Done
Next, we evaluate the work done, W. Unlike internal energy, work is a path function. Geometrically, the work done by a gas is the area under the p−V curve. Mathematically, it is given by the integral:
The sign of the work done is dictated by the change in volume. Let's analyze each path:
1. Path A→B: The arrow points to the right, indicating an expansion. The volume increases (ΔV>0), so the work done by the gas is positive. Thus, WAB>0.
2. Path A→C: This is a perfectly vertical line. The volume remains constant (ΔV=0), making it an isochoric process. With no area under the curve, the work done is zero. Thus, WAC=0.
3. Path A→D: The arrow points to the left, indicating a compression. The volume decreases (ΔV<0), so the work done by the gas is negative. Thus, WAD<0.
The Final Verdict and Beyond
Bringing our findings together, we have established the absolute truth for this system:
EAB=EAC=EAD
WAB>0,WAC=0,WAD<0
If we carefully inspect the given options, we realize that none of the options perfectly match this correct set of relations. Option (b) comes close but incorrectly states WAD>0. In competitive exams like JEE, such anomalies can occur, and they are often treated as bonus questions. The key takeaway is to trust your fundamental concepts!
As a thought experiment, consider the heat supplied (ΔQ) for these processes. According to the First Law of Thermodynamics (ΔQ=ΔU+W), since ΔU is constant, the path with the most positive work will absorb the most heat. Therefore, path A→B absorbs the maximum heat, while path A→D absorbs the least. Always keep pushing your conceptual boundaries!