Difficulty: Easy
Correct Answer: True
Explanation:
Introduction / Context:
Recognizing special cases of the polytropic relation p * v^n = C is a standard skill in thermodynamics and compressible flow. The correct identification helps select the right equations for work, heat transfer, and state changes during compression or expansion of gases.
Given Data / Assumptions:
Concept / Approach:
For an ideal gas, the equation of state is p * v = R * T (on a per-unit-mass basis). If the polytropic exponent n equals 1, then p * v^1 = constant implies p * v = constant. Combining with p * v = R * T gives R * T = constant, hence T = constant. Therefore, the polytropic case n = 1 coincides with an isothermal process for an ideal gas. Other important special cases include n = 0 (isobaric), n → ∞ (isochoric), and n = gamma (isentropic for a perfect gas with constant specific heats).
Step-by-Step Solution:
Verification / Alternative check:
On a T–s diagram, an isothermal path for an ideal gas has constant temperature; consistency is also seen on a p–v plot where n = 1 polytrope is a rectangular hyperbola, matching the classic isotherm shape for ideal gases.
Why Other Options Are Wrong:
Conditions like 'only at low pressure' or 'only if no heat transfer' are unnecessary; isothermal processes do require heat exchange to keep T constant during compression/expansion, but the identification n = 1 remains valid for ideal gases without those extra caveats.
Common Pitfalls:
Confusing isothermal with isentropic; for an ideal gas, isentropic requires n = gamma, not 1. Also, mixing up the behavior of real gases at high pressures where EOS deviations occur (outside the scope here).
Final Answer:
True
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