Thermodynamics - partial differential

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Homework Help Overview

The discussion revolves around the Joule-Thompson Expansion in thermodynamics, specifically focusing on deriving the relationship involving partial derivatives of enthalpy with respect to pressure and temperature. The original poster expresses uncertainty about the dependence of volume on pressure and temperature in the context of the problem.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the implications of treating volume as a function of pressure and temperature, questioning the validity of ignoring certain differentials in the context of the product rule. There is discussion about the application of the chain rule and the conditions under which differentials can be neglected.

Discussion Status

Participants are actively engaging with the mathematical reasoning behind the problem, with some providing guidance on the use of the product rule and the treatment of infinitesimals. There is a recognition of the need for careful consideration of variable dependencies, but no explicit consensus has been reached regarding the original poster's assumptions.

Contextual Notes

The original poster notes that enthalpy is specified as a function of pressure and temperature, which raises questions about the independence of volume in the derivation. There is an acknowledgment of the complexity introduced by the non-constant nature of volume during the expansion process.

Beer-monster
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Homework Statement



Edit: Some more details.

The question concerns Joule-Thompson Expansion and I need to derive the relationship:

[tex]\left(\frac{\partial H}{\partial P}\right)_T =V+T\left(\frac{\partial S}{\partial P}\right)_T[/tex]V is not constant as it is expansion but the enthalpy is specied as H(P,T) for the problem. Therefore I would assume that Volume is a function of P and T and not independent. However, I'm not 100% sure on this.

The Attempt at a Solution



[tex]dH=TdS+VdP[/tex]

Therefore:

[tex]\left(\frac{\partial H}{\partial P}\right)_T = T\left(\frac{\partial S}{\partial P}\right)_T + V\left(\frac{\partial P}{\partial P}\right)_T = V+T\left(\frac{\partial S}{\partial P}\right)_T[/tex]

Is this right? I know it would not be if I'm right and V is a function of P and T. Could someone please clear this up for me.Thanks

BM
 
Last edited:
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You got it, as long as you've implicitly used the chain rule and ignored the differentials as compared to non-infinitesimal values. That is,

[tex]\left(\frac{\partial}{\partial P}\right)_T\left(V\,dP\right)=\left(\frac{\partial V}{\partial P}\right)_T dP+V\left(\frac{\partial P}{\partial P}\right)_T=V.[/tex]

The differentials can be ignored in any mix of differential and non-infinitesimal values. Does this make sense?
 
I think I get it. As V is not constant and probably depends on P we can't ignore it in the differential and need to apply the product rule.

But doesn't the differential of V only equal 0 if V is constant or independent of P. In which case, why would we need to explicitly use the product rule?
 
I'm not sure if this answers your question, but we must use the product rule every time we differentiate a product. It's safest to assume every variable depends on every other variable unless it's been specifically shown not to. In this case, [itex](\partial V/\partial P)_T\,dP[/itex] goes away not because [itex]V[/itex] has any certain value, but because [itex]dP[/itex] is an infinitesimal value that vanishes when compared with the finite value [itex]V[/itex].

In summary, it's safer to use the product rule and cancel the appropriate terms than to work "fast and loose."
 
So because dp is so small (approximately zero) compared to the differential [itex] (\partial V/\partial P)_T[/itex] we can ignore it provided the differential is of something non-infintesimal?
 
Exactly. We can't automatically do the same thing for an equation like [itex]dH=T\,dS+V\,dP[/itex] because everything is infinitesimal.
 
Yeah, that occurred to me and gave me a bit of a pause. But though differentials are made of infintesimal elements they are not themselves infintesimal so would be reduced to nothing if multiplied by dP.

However, if this was worked out in a problem the product rule would have to be expressed explicitly otherwise one would think that you were treating V as constant.
 

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