Clarification on derivations of specific heats in fluids

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SUMMARY

This discussion clarifies the derivation of specific heats in fluids, focusing on the definitions and relationships involving internal energy (U), enthalpy (H), and heat transfer (Q). The correct definition of enthalpy is established as H = U + pV, leading to the derivation of specific heat at constant pressure (Cp) and constant volume (Cv). The confusion surrounding the incremental form of enthalpy is resolved by correctly applying the first law of thermodynamics and recognizing the role of pressure-volume work (PdV) in the equations. The final clarification emphasizes that the state function Q cannot be used in defining enthalpy.

PREREQUISITES
  • Understanding of the first law of thermodynamics
  • Familiarity with thermodynamic state functions (U, H, T, V, p)
  • Knowledge of heat transfer concepts (Q)
  • Basic calculus, particularly differentiation and the chain rule
NEXT STEPS
  • Study the derivation of the first law of thermodynamics in detail
  • Explore the relationship between internal energy and enthalpy in thermodynamics
  • Learn about the implications of state functions in thermodynamic processes
  • Investigate the applications of specific heats in real-world fluid systems
USEFUL FOR

Students and professionals in thermodynamics, mechanical engineers, and anyone involved in fluid mechanics or heat transfer analysis will benefit from this discussion.

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.
 
Absolutely.
 

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