Clarification on derivations of specific heats in fluids

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The discussion centers on the derivation of specific heats, CV and CP, using the first law of thermodynamics and the definition of enthalpy. There is a clarification on the correct definition of enthalpy, which is H = U + pV, and how it relates to the incremental form of enthalpy, dH = δQ + Vdp. The confusion arises from the treatment of pressure-volume work and the state function Q, leading to a misunderstanding in the derivation process. Ultimately, the participant resolves their confusion by recognizing the proper relationship between the terms and correcting their earlier mistakes. This highlights the importance of accurate definitions and careful application of thermodynamic principles.
Kori Smith
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Hello! I understand what specific heats are and how to derive them. I just feel that I'm missing a little something in the methodology.

Consider the 1st law of thermodynamics and the definition of enthalpy:

1) dU = δQ -δW = δQ - PdV
2) H = Q - VP

For the derivation of CV, dV = 0 and the relationship becomes

(∂U/∂T)V = (∂Q/∂T)V = CV

For the derivation of CP, something happens that I don't quite understand. Sources I've found say that the incremental form of the enthalpy relation is given as

3) dH = δQ - VdP

since dP = 0, it becomes

(∂U/∂T)P = (∂Q/∂T)P = CP

but why do we write it like this? Wouldn't the chain rule for differentiation apply to d(VP) s.t. it becomes

d(VP) = VdP + PdV

in which case, where does the PdV component in EQ (3) go? Thanks ahead of time for the clarification!
 
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The definition of enthalpy is not correct. Enthalpy is a state function, like U, T, V or p. It is defined by:
H = U + pV. Then instead of your equ. (3):

dH = dU + pdV + Vdp = δQ + Vdp, so that, for a constant pressure process, dp = 0, and
dH = δQ,
(∂H/∂T)p = (∂Q/∂T)p = Cp

The problem with the definition of enthalpy that you gave is that there is no state function called Q, so you cannot define any state function in terms of something called Q.
 
Chandra Prayaga said:
The definition of enthalpy is not correct. Enthalpy is a state function, like U, T, V or p. It is defined by:
H = U + pV. Then instead of your equ. (3):

dH = dU + pdV + Vdp = δQ + Vdp, so that, for a constant pressure process, dp = 0, and
dH = δQ,
(∂H/∂T)p = (∂Q/∂T)p = Cp

The problem with the definition of enthalpy that you gave is that there is no state function called Q, so you cannot define any state function in terms of something called Q.

Woops! I made a typo. As usual, my issue boils down to simple errors. When I look at it again, I see that

dH = dU + pdV + Vdp = δQ - δW +pdV + Vdp = δQ + Vdp + (pdV - δW) = δQ + Vdp

since δW = pdV (pressure-volume work). Which is exactly as it should be and explains where the missing pdV went.
 
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