Decoding the p-T Diagram
Let's embark on a thrilling journey to decode the given p-T diagram. At first glance, it looks like a standard thermodynamic cycle, but as we dig deeper, we will uncover a fascinating physical contradiction.
First, let's analyze the process from A to B. On the p-T diagram, this is a vertical line pointing downwards. This indicates that the temperature T remains constant while the pressure p decreases. By the ideal gas law, pV=nRT, if T is constant and p drops, the volume V must increase. This is an isothermal expansion, meaning VB>VA.
Next, we look at the process from B to C. This is a horizontal line pointing to the right, meaning the pressure p is constant while the temperature T increases. According to Charles's Law, at constant pressure, volume is directly proportional to temperature (V∝T). Therefore, as the gas heats up, it expands. This is an isobaric expansion, which tells us that VC>VB.
The Adiabatic Trap
Finally, the problem states that the process from C back to A is an adiabatic process. In an adiabatic process, no heat is exchanged, and the relationship between pressure and volume is governed by pVγ=constant. Since the pressure increases from C to A, the volume must decrease.
Now, let's visualize this on a p-V diagram. At point A, two curves intersect: the isothermal curve AB and the adiabatic curve CA. We know a fundamental rule of thermodynamics: an adiabatic curve is always steeper than an isothermal curve passing through the same point. Mathematically, the slope of an adiabatic curve is γ times the slope of an isothermal curve, and since γ>1, it drops faster.
The Grand Contradiction
Because the adiabatic curve CA is steeper than the isothermal curve AB, the adiabatic curve must lie to the left of the isothermal curve for lower pressures. This implies that for any given pressure below pA, the volume on the adiabatic curve must be strictly less than the volume on the isothermal curve.
Since points B and C are at the same pressure (pB=pC), the volume at C (on the adiabatic curve) must be less than the volume at B (on the isothermal curve). So, the slope condition demands that VC<VB.
But wait! Our initial analysis of the p-T diagram clearly proved that VC>VB due to the isobaric expansion.
These two conditions are mutually exclusive. It is physically impossible for process CA to be adiabatic while simultaneously satisfying the given p-T diagram. The question itself contains a fundamental flaw, which is why none of the provided options can be correct!