Change in entropy of an ideal gas during thermodynamic cycle

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SUMMARY

The discussion focuses on the thermodynamic cycle of an ideal gas characterized by an adiabatic index γ. The cycle consists of three steps: isochoric heating from P1 to P2, adiabatic expansion from P2 to P1, and isobaric compression back to the initial state. The total change in entropy for the complete cycle is determined to be zero, confirming the reversibility of the process. The equation used for entropy change is ΔS = CP*ln(V/V0) + CV*ln(P/P0), which is essential for calculating the entropy changes in each step.

PREREQUISITES
  • Understanding of thermodynamic cycles and processes
  • Familiarity with the concepts of entropy and the adiabatic index γ
  • Knowledge of heat capacities (CP and CV) for ideal gases
  • Ability to interpret PV diagrams
NEXT STEPS
  • Study the derivation of the adiabatic relations for ideal gases
  • Learn how to construct and analyze PV diagrams for thermodynamic processes
  • Explore the implications of the second law of thermodynamics on entropy changes
  • Investigate the relationship between heat capacities and the adiabatic index γ
USEFUL FOR

This discussion is beneficial for students studying thermodynamics, particularly those focusing on ideal gas behavior, entropy calculations, and the principles of reversible processes.

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Homework Statement


An ideal gas with adiabatic index γ is taken around a complete thermodynamic cycle consisting of three steps. Starting at point A, the pressure is increased at constant volume V1 from P1 to P2 at point B. From point B to point C, the gas is allowed to expand adiabatically from volume V1 and pressure P2 to volume V2 and the original pressure P1. Finally, from point C to point A, the volume of the gas is decreased at constant pressure P1 back to the original volume V1.

a) Make a PV diagram of the complete cycle.

b) For each step of the cycle, determine the change in the entropy of the gas. Sum your results to find the total entropy change for the whole cycle. Note that every step is reversible.

c) Use the adiabatic relations to eliminate the pressure from your result for part b. Show that the resulting expression gives a total entropy change for the complete cycle equal to zero.

Homework Equations


ΔS = CP*ln(V/V0) + CV*ln(P/P0)

The Attempt at a Solution


I did part a.) which is in the attachment, as well as my work so far for part b.). I'm not sure how to express the heat capacities in terms of the adiabatic index... any hints?
 

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What you have is correct so far. How do P1, P2, V1, and V2 have to be related for the adiabatic expansion?
 

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