Proving Internal Pressure of Ideal & VdW Gases

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Homework Help Overview

The discussion revolves around proving the internal pressure of ideal gases and Van der Waals gases, focusing on the mathematical relationships and equations governing these systems.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the derivation of internal pressure using various equations of state for ideal and Van der Waals gases. There is an attempt to apply thermodynamic identities and Maxwell relations, with some participants expressing uncertainty about their calculations and methods.

Discussion Status

Several participants are actively engaging with the problem, sharing their attempts and questioning the steps involved in deriving the internal pressure. Some guidance has been offered regarding the relationship between caloric and thermal equations of state, but there is no explicit consensus on the correct approach yet.

Contextual Notes

Participants note challenges in applying the equations correctly and express uncertainty about the derivations, indicating a learning process that is ongoing. There is mention of homework constraints and the need to clarify certain mathematical tools and concepts.

Jennifer Lyn
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Like in the other problem I posted- This is the other question that I missed and just can't find a solution for.

Homework Statement


Prove the internal pressure is 0 for an ideal gas and ((n^2)a)/(v^2) for a Van der Waals gas.

Homework Equations


1. VdQ Eqn: p= (nRT)/(v-b) - ((n^2)a)/(v^2)
2. (partial S/partial V) for constant T = (partial p/partial T) for contant V.
3. dU = TdS - pdV
4. pi sub t (internal pressure) = (partial U/partial V) for constant T


The Attempt at a Solution



a) Ideal Gas
0 = (partial U/partial V) for const T
int 0 dv = int du
0 = int (TdS - pdV)
int p dv = int T ds
int (nRT/v) dv = int (Pv/nR) dS
nRT x int(1/V) dv = pv/nR x int 1 dS
... and I get kind of lost here, though I know that what I've already done is wrong.. :(

b) VdW gas
I actual have to get going to school, but I'll come back and type up what I've done (incorrectly :( for this part afterwards).
 
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Hello Jennifer,

I suppose you are given the so called thermal equation of state [itex]p=p(T,V,n)[/itex] for both

the ideal gas

[tex]p=\frac{nRT}{V}[/tex]

and the Van der Waals gas

[tex]p=\frac{nRT}{V-nb}-\frac{n^2a}{V^2}[/tex]

The inner pressure [itex]\left(\frac{\partial U}{\partial V}\right)_T[/itex] can be calculated after finding the so called caloric equation of state [itex]U=U(T,V,n)[/itex] for both cases.

Another straightforward method would be to use the following identity which shows that the caloric and thermal equations of state are not independent of each other:

[tex]\left(\frac{\partial U}{\partial V}\right)_T=T\left(\frac{\partial p}{\partial T}\right)_V-p[/tex]

Do you know how to derive this identity?
 
I think so..
[tex]\Pi[/tex]t = [tex]\partial[/tex]u/[tex]\partial[/tex]v for constant t
= ( 1/[tex]\partial[/tex]v[tex]\times[/tex](Tds - pdv) )
= T [tex]\times[/tex] ([tex]\partial[/tex]p/[tex]\partial[/tex]t) - p

I think that's right. I still don't know how to get from that Maxwell relation to the ideal gas and Van der Waals eqn, though.
 
Last edited:
Ok, I think I figured it out, from my previous post (sorry- I am still getting used to using the tools for math on this board) I replace the vanderwaals eqn into P in my partial p and then just solve from there.
 
Thanks everyone!
 

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