Difficulty: Easy
Correct Answer: Disagree
Explanation:
Introduction / Context:
Thermodynamic diagrams encode energy transfers geometrically. It is crucial to know which plane corresponds to heat and which to work. Students often confuse the meaning of areas on P–v and T–s plots, leading to wrong conclusions about work and heat in cycles and processes.
Given Data / Assumptions:
Concept / Approach:
On a pressure–volume (P–v) diagram, the area under the curve equals boundary work: W = ∫ P dv. On a temperature–entropy (T–s) diagram, the area under the curve equals the heat transfer for a reversible path: Q_rev = ∫ T ds. Therefore, the statement that the T–s area represents work is incorrect; it represents reversible heat, not work. Work can be inferred on other planes (e.g., P–v, h–s with device models), but not directly from T–s area.
Step-by-Step Solution:
Verification / Alternative check:
In a reversible adiabatic process (ds = 0), area under the T–s line is zero while work is nonzero; this counterexample directly disproves the claim that T–s area is work.
Why Other Options Are Wrong:
“Agree” variants: Conflate heat with work; even for ideal gases or constant-volume paths, T–s area tracks Q_rev, not W.
Common Pitfalls:
Assuming one diagram's area rule applies universally. Always match the plane to the physical quantity represented by its integral.
Final Answer:
Disagree
Discussion & Comments