Volumes at C and D in a Carnot cycle

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SUMMARY

The discussion focuses on calculating the volumes at points c and d in a Carnot cycle, given specific parameters: Va = 7.5 L, Vb = 15 L, TH = 470°C, TL = 260°C, and a diatomic gas with y = 1.4. The pressures at points a and b were determined as Pa = 4.1 x 105 Pa and Pb = 2.1 x 105 Pa. The expected volumes at points c and d are Vc = 34 L and Vd = 17 L, derived from the relationships of the Carnot cycle and the ideal gas law.

PREREQUISITES
  • Understanding of the Carnot cycle and its stages
  • Familiarity with the ideal gas law (PV = nRT)
  • Knowledge of adiabatic processes and the equation PVγ = constant
  • Basic concepts of thermodynamics, particularly relating to diatomic gases
NEXT STEPS
  • Study the derivation of the Carnot cycle equations
  • Learn about the implications of adiabatic vs. isothermal processes in thermodynamics
  • Explore the properties of diatomic gases and their behavior under varying conditions
  • Investigate the application of the ideal gas law in real-world thermodynamic systems
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Students of thermodynamics, mechanical engineers, and anyone studying the principles of heat engines and the Carnot cycle.

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Homework Statement


A Carnot cycle, shown in Fig. 20-7, has the following conditions: Va = 7.5 L, Vb = 15 L, TH = 470°C, and TL = 260°C. The gas used in the cycle is 0.50 mil of a diatomic gas, y = 1.4. Calculate (a) the pressures at a and b; (b) the volumes at c and d. (The rest of the problem...)

Homework Equations


PVy = Constant

The Attempt at a Solution


I already solved part (a), with Pa = 4.1 x 105 Pa and Pb = 2.1 x 105 Pa.

For part (b), I tried
PVy = constant
nRT⋅Vy-1 = constant.

Annnnd then I get lost. I don't understand what constant represents or if I am even on the right track. The book says Vc = 34 L and Vd = 17 L.
 
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What do the points a, b, c, and d represent in the Carnot cycle? You didn't post the figure.
 
My apologies, here is the figure:

n1723o.png


Points a, b, c, and d represent stages of the Carnot engine as it works.
 
For an adiabatic process, you have ##PV^\gamma = \text{constant}##. Since points b and c are on the same adiabat, you can say that ##P_b V_b^\gamma = P_c V_c^\gamma##.

If it still seems confusing, consider the analogous situation for an isothermal process. The righthand side of the ideal gas law, ##PV = nRT##, is constant for an isothermal process. In other words, on an isotherm, we have that ##PV = \text{constant}##. Points a and b are on the same isotherm, so you can say ##P_a V_a = P_b V_b##, which should look very familiar to you.
 

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