State Functions and Order of Diff and Enthelpy

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State functions in thermodynamics, such as internal energy (U), temperature (T), pressure (P), Gibbs free energy (G), and Helmholtz free energy (A), are exact differentials, while non-state functions are inexact differentials. The order of differentiation for state functions does not affect the result, meaning mixed partial derivatives yield the same value. Enthalpy (H) is independent of the process path, and while it can be calculated at constant volume, it still depends on pressure, which explains the use of qp in bomb calorimetry. The equation dH = dU + PdV is preferred in certain contexts, possibly when initial and final pressures are constant, rather than expanding d(PV). Understanding these principles is crucial for accurate thermodynamic derivations.
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I am working on some basic derivations for thermodyhnamics, my book doesn't explicitly state things so I am not sure if my current assumptions are correct?

1) All state functions (U,T,P,G,A) are exact differentials AND all non-state functions are INexact differntials. So if I take the 2nd derivative, I will get the same function for M and N in the example of dz = M(x,y) + N(x,y)

2) What does my book mean when it says that the order of differentiation doesn't matter for state functions?

- what do they mean by order of differentiation? does t

3) How do I calculate (delta)Enthalpy when volume is constant? It looks like it would be qv but when it comes to bomb calorimeters my book keeps using qp?

If H = U + PV, shouldn't constant volume make H = U? for reversible and irrev?

H = q/T only pressure is constant + reversible?

Why is it that my book shows dH = dU + PdV RATHER THAN d(PV) = dU+ VdP+PdV (expanding for chainge P and V?)

Thank YOU :D
 
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cns said:
I am working on some basic derivations for thermodyhnamics, my book doesn't explicitly state things so I am not sure if my current assumptions are correct?

1) All state functions (U,T,P,G,A) are exact differentials AND all non-state functions are INexact differntials. So if I take the 2nd derivative, I will get the same function for M and N in the example of dz = M(x,y) + N(x,y)

2) What does my book mean when it says that the order of differentiation doesn't matter for state functions?

- what do they mean by order of differentiation? does t
It means that $$\frac{\partial ^2 U}{\partial T\partial V}=\frac{\partial^2 U}{\partial V\partial T}$$
3) How do I calculate (delta)Enthalpy when volume is constant? It looks like it would be qv but when it comes to bomb calorimeters my book keeps using qp?
Enthalpy is independent of process path, so it is not specifically related to qv or qp, except when employed to analyze a particular process.
If H = U + PV, shouldn't constant volume make H = U? for reversible and irrev?
Again, it is independent of process path and, if V is constant, you still have H depending on P. Reversible or irreversible is irrelevant.
H = q/T only pressure is constant + reversible?
Neither. The units don't match.
Why is it that my book shows dH = dU + PdV RATHER THAN d(PV) = dU+ VdP+PdV (expanding for chainge P and V?)
Maybe your book is referring to a case in which the initial and final pressures are the same.
 
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