Solving Maxwell Relations Homework with Van der Waals Gas

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SUMMARY

The discussion focuses on solving a homework problem related to Maxwell Relations using the Van der Waals gas equation. The key equations involved are the relationship between heat capacities \(C_P\) and \(C_V\), and the Van der Waals equation \( \left(P + \frac{a}{V^2}\right)(V - b) = RT\). The user successfully derived \( \left(\frac{\partial P}{\partial T}\right)_V = \frac{R}{V - b} \) but encountered difficulties in isolating \( \left(\frac{\partial V}{\partial T}\right)_P \). The solution involves applying the product rule to differentiate the Van der Waals equation while treating pressure \(P\) as a constant.

PREREQUISITES
  • Understanding of Maxwell Relations in thermodynamics
  • Familiarity with the Van der Waals equation of state
  • Knowledge of partial derivatives in thermodynamic contexts
  • Basic principles of heat capacities \(C_P\) and \(C_V\)
NEXT STEPS
  • Study the derivation of Maxwell Relations in thermodynamics
  • Learn how to manipulate the Van der Waals equation for differentials
  • Explore the implications of heat capacity differences in real gases
  • Investigate the application of the product rule in thermodynamic equations
USEFUL FOR

Students studying thermodynamics, particularly those tackling advanced topics in heat capacity and real gas behavior, as well as educators looking for examples of applying Maxwell Relations and the Van der Waals equation.

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Homework Statement


[/B]
I'm stuck on part c of the attached problem:
SzQ4Ski.png


Homework Equations



$$C_P - C_V = \left[P + \left( \frac {∂U}{∂V} \right)_T \right]\left( \frac {∂V}{∂T} \right)_P$$

$$P + \left( \frac {∂U}{∂V} \right)_T = T \left( \frac {∂P}{∂T} \right)_V$$

$$\left(P + \frac {a}{V^2} \right)(V - b) = RT$$

The Attempt at a Solution



I need to use the bottom two equations to find to find ##P + \left( \frac {∂U}{∂V} \right)_T ## and ##\left( \frac {∂V}{∂T} \right)_P## and plug these expressions in the top equation for CP - CV.

I've found $$\left (\frac {∂P}{∂T} \right)_V = \frac {R}{V - b}$$
$$∴ P + \left( \frac {∂U}{∂V} \right)_T = \frac {RT}{V - B}$$

But I'm having trouble finding ##\left (\frac {∂V}{∂T} \right)_P## because I can't seem to make V the subject of the Van der Waals gas expression.
 

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Take the Van der Waal's equation and take a differential of both sides, using the product rule, (or just multiply out the left side), and treating ## P ## as a constant. You should get a couple of terms that are multiplied by ## dV ##. On the right side you will have ## R \, dT ##.
 
Last edited:
Charles Link said:
Take the Van der Waal's equation and take a differential of both sides, using the product rule, (or just multiply out the left side), and treating ## P ## as a constant. You should get a couple of terms that have are multiplied by ## dV ##. On the right side you will have ## R \, dT ##.

Oh I see. Thanks, I got it now :)
 
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