Difficulty: Medium
Correct Answer: > R
Explanation:
Introduction / Context:
The difference between the constant-pressure and constant-volume specific heats, Cp − Cv, is a fundamental quantity that links caloric and thermal equations of state. For an ideal gas, Cp − Cv equals the universal gas constant R on a molar basis. For real gases described by the van der Waals model, non-ideality changes thermal expansion and compressibility, which in turn modifies Cp − Cv. This question checks your understanding of the general identity relating Cp − Cv to measurable volumetric properties and why real-gas behavior typically yields a value larger than R under stable conditions.
Given Data / Assumptions:
Concept / Approach:
The general identity is Cp − Cv = T * V * α^2 / κ_T (molar basis: replace V with molar volume). Here α is the volumetric thermal expansion coefficient and κ_T is the isothermal compressibility. For an ideal gas, α = 1/T and κ_T = 1/P, giving Cp − Cv = R. For a van der Waals gas at the same T and P, κ_T is usually smaller (the fluid is less compressible) and α does not decrease proportionally, so the ratio α^2/κ_T is larger, making Cp − Cv greater than R in stable regions.
Step-by-Step Solution:
Verification / Alternative check:
Another exact form is Cp − Cv = −T * (∂P/∂T)_V^2 / (∂P/∂V)_T. For stable fluids, (∂P/∂V)_T < 0, making the fraction positive. Real-gas deviations generally make the magnitude larger than the ideal case at the same conditions.
Why Other Options Are Wrong:
Common Pitfalls:
Confusing per-mole vs per-mass bases; forgetting that α and κ_T govern Cp − Cv in all fluids; applying the ideal-gas result blindly to real fluids at high pressures.
Final Answer:
> R
Discussion & Comments