What is the difference between Cp and Cv for an ideal gas?

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SUMMARY

The discussion clarifies the distinction between heat capacities Cv and Cp for ideal gases. Cv, the heat capacity at constant volume, is used for calculating changes in internal energy, as it directly relates to temperature changes via the equation ΔU = nCvΔT. Cp, the heat capacity at constant pressure, is significant for understanding thermodynamic processes but is not utilized for internal energy calculations in ideal gas scenarios. The ratio of Cp to Cv, known as gamma (γ), is also highlighted as an important thermodynamic parameter.

PREREQUISITES
  • Understanding of thermodynamic concepts, specifically internal energy and heat capacities.
  • Familiarity with the ideal gas law and its applications.
  • Knowledge of kinetic theory and its relation to temperature and energy.
  • Basic grasp of thermodynamic processes and their path dependencies.
NEXT STEPS
  • Study the derivation and implications of the ideal gas law.
  • Learn about the significance of the ratio γ = Cp/Cv in thermodynamics.
  • Explore applications of Cv and Cp in real-world heat engine calculations.
  • Investigate the relationship between heat capacities and phase changes in substances.
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Students and professionals in thermodynamics, mechanical engineers, and anyone involved in the design and analysis of heat engines and energy systems.

sachi
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I'm just checking that it's okay to use Cv all the time as a heat capacity of an ideal gas, even when the volume's not constant. This is because the average energy per molecule is 3/2*Kb*T from kinetic theory, therefore the average energy per mole is equal to 3RT/2 = CvT etc.
I'm currently doing a calculation for a heat engine and I'm working out the change in internal energy at a constant volume and I need to make sure that we use Cv and not Cp as the heat capacity.
Also, what is the significance of Cp if it's not used? Is it just so that we can set gamma=Cp/Cv?

Thanks
 
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The heat capacity C of a substance is the amount of heat required to change its temperature by one degree.

So, in your thermodynamic processes, the value of the heat capacity depends on the path chosen.

That is why you have heat capacites at constant pressure(Cp) and constant volume(Cv) .

Now, for an ideal gas, the change in internal energy for any process depends on the temperature only and the relation is given by [itex]\Delta U = nC_v \Delta T[/itex].
That is why in most of the problems you are doing(which involves ideal gases), you are using C_v to calculate the change in internal energy.

Did that help?
 
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