Thermodynamics Cv = Cp + R Question

In summary, the equation of state for an ideal gas is pΔV = nRΔT, and the first law of thermodynamics applies to an ideal gas undergoing a isochoric process.
  • #1
drcrabs
47
0
Can someone tell me why Cv = Cp + R
 
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  • #2
Well first of all its Cp - Cv = nR, where is your moles of gas, and its only true for an ideal gas. You find this about about halfway through the first semester of physical chemistry.

The formal definitions of Cv and Cp are

[tex] C_v = \frac{\partial U}{\partial T} [/tex] and

[tex] C_p = \frac{\partial H}{\partial T}[/tex]

Where U is the internal energy and H is the enthalpy, defined to be H = U + pV. But for an ideal gas, pV = nRT. Substitutiotn this into the defition for Cp we get

[tex] C_p = \frac{\partial (U + nRT)}{\partial T}[/tex]

[tex] C_p = \frac{\partial U }{\partial T} + \frac{\partial (nRT)}{\partial T}[/tex]

[tex] C_p = \frac{\partial U}{\partial T} + nR[/tex]

[tex] C_p = C_v + nR[/tex]
 
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  • #3
What are on?
 
  • #4
Are you talking about [tex]\partial[/tex] ? Thats the symbol for a partial deriviative. Its like a deriviative but for functions of mroe than one variable. To calculate it, you treat the other variables as constants, except for the one youare differentiating against.
 
  • #5
Can u prove the equation by the consideration of an isobaric process?
 
  • #6
No, path has nothing to do with it. It follows directly from the definition of U, H, Cp and Cv, and our assumption of an ideal gas. If our gas it is not ideal, that equation does not hold.
 
  • #7
But what if we consider an ideal gas undergoing a isochoric process and
how the first law of thermodynamics applies to it.
ΔU= Q - W

Since the work is defined by the pressure * the change in volume
W = pΔV
then work is 0

Hence ΔU = Q - 0 = Q

but Q = nCvΔT hence ΔU = nCvΔT

But since the change in internal energy is independant of path taken
for any process ΔU = nCvΔT.

Now let us consider a isobaric process
In this case Q = nCpΔT.

Now taking the definition of work to be W = pΔV
and using the defition of the equation of state pΔV = nRΔT

then W = nRΔT

Now consider the first law of thermodynamics again

ΔU= Q - W

then nCvΔT = nCpΔT + nRΔT

leaving us with Cv = Cp + R
 

What is the definition of Cv and Cp in thermodynamics?

Cv and Cp refer to specific heat capacities used in thermodynamics to describe the amount of heat required to raise the temperature of a substance by 1 degree Celsius. Cv is the specific heat capacity at constant volume, while Cp is the specific heat capacity at constant pressure.

What is the relationship between Cv, Cp, and the universal gas constant R?

The relationship between Cv, Cp, and R is Cv = Cp + R. This equation is known as the Mayer's relation and it states that the specific heat capacity at constant volume is equal to the specific heat capacity at constant pressure plus the universal gas constant.

Why is the value of Cv less than Cp for most substances?

For most substances, the value of Cv is less than Cp because at constant pressure, the substance is allowed to expand and do work on its surroundings, which requires more energy and thus a higher specific heat capacity. At constant volume, the substance cannot do work on its surroundings, resulting in a lower specific heat capacity.

What is the significance of the Cv = Cp + R equation in thermodynamics?

The Cv = Cp + R equation is significant because it provides a way to relate the specific heat capacities of a substance at different conditions (constant volume and constant pressure) to a fundamental physical constant, the universal gas constant. This allows for the calculation of one specific heat capacity if the other two values are known.

How is the Cv = Cp + R equation used in practical applications of thermodynamics?

The Cv = Cp + R equation is used in various practical applications of thermodynamics, such as in the design of heat exchangers, refrigeration systems, and engines. It is also used in the calculation of thermodynamic properties, such as enthalpy and entropy, which are important for understanding and predicting the behavior of substances under different conditions.

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