Thermal Physics problem: Van der Waals

AI Thread Summary
The discussion revolves around finding a relationship between temperature (T) and volume (V) for a Van der Waals gas under constant entropy (S). Participants identify a misstatement in the thermodynamic identity for entropy change, which leads to confusion in deriving the correct expressions. They emphasize the need to correctly differentiate the internal energy (U) and substitute it back into the entropy equation. After some back-and-forth, they successfully separate variables and integrate, ultimately deriving a relationship that allows them to express the final volume in terms of the initial volume and temperature. The thread concludes with a collaborative effort to clarify the integration steps and confirm the correctness of the final expression.
mmedrano8
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1. Find an expression that relates T and V in a process in which the entropy S is constant, by doing the following:

a) From thermodynamic identity dS=(1/t)dU + (p/v)dV
find the expression for dS as a function of T and V (and dT and dV).

b) Integrate the expression found in (a) along the line of constant S.


Homework Equations


I tried to use the equation of state for a Van der Waals gas

p=(NkT)/V-a(N^2/V^2)

a is constant
its energy as a function of temperature and volume is given by
U(T,V)=2NkT-a(N^2/V)

If you could give any hints that would be great!
 
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mmedrano8 said:
1. Find an expression that relates T and V in a process in which the entropy S is constant, by doing the following:

a) From thermodynamic identity dS=(1/t)dU + (p/v)dV


That equation is dimensionally inconsistent and therefore wrong.

But it's just one letter aaway from right so is probably a typo. Anyway, fix it.

Are you allowed to assume an ideal gas?
 
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As noted by rude man, the equation given for dS is incorrect. Since the equation is just a simple rearrangement of the first law (with dQ = T dS), you can see how to fix it.

To proceed with the problem, you will need to use the expression for U and find it's differential dU in terms of dT and dV.
 
OK.
You're given U(T,V) and dS = 1/T dU + p/V dV
so taking dU is just basic calculus. N, k and a are constants.

Warning: I've carried this thru to dS = 0 in terms of T and V but I wind up with an expression that I can't integrate (tried separation of parts, couldn't do it). Someone else help!
 
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ok so thermodynamic identity --> dS=(1/T)dU + (p/T)dV
 
mmedrano8 said:
ok so thermodynamic identity --> dS=(1/T)dU + (p/T)dV

Good.

What does this expression for dS become after substituting for dU and simplifying?
 
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mmedrano8 said:
ok so thermodynamic identity --> dS=(1/T)dU + (p/T)dV

Hey, how come everyone except I caught the misstatement in the problem? Now I got to start over ... :

I hope at least U(T,V) is given correctly. Someone else want to check dimensions?

Still can't seem to separate variables though ...
 
ok dU=(∂U/∂T)dT + (∂U/∂V)dV --> dU = 2NKdT + aN^2(1/V^2)dV

I plug in P and dU into dS = (1/T)dU + (P/T)dV

I get...

dS = (1/T)[2NkdT + a(N^2)/(V^2)dV] + (NKT/V - (aN^2)/(V^2))/T)dV

please correct me if I am wrong but since S is constant, then dS equals 0,
therefore the lefthand side is 0, we separate the varibales for dT and dV and simplify
i get
-2dT=(T/V)dV
integrate both parts and solve for Vf --> Vf=Vi/16

Thanks so much guys!
 
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Congartulations! Would you (or TSny or whoever) mind posting how you did the separation of variables? I couldn't do it. :blushing:

EDIT: never mind, I hadn't noticed two terms canceling each other, leaving only 2 terms to be separated.

Good show!
 
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  • #11
i forgot a step, -2dT = (T/V)dV --> (-2/T)dT=(1/V)dV
but i separated varibles by putting all T's and V's on opposite sides of the equation

-(1/T)[2NkdT] = (1/T)[a(N^2)/(V^2) + NKT/V - (aN^2)/(V^2))/T)dV

simplify a bit...
2NkdT = (NKT/V)dV

2dT = (T/V)dV

(2/T)dT = (1/v)dV then integrate both sides ---> 2ln(Tf/Ti) = ln(Vf/Vi) , where Tf = 4Ti , 2ln(4) = ln(Vf/Vi)
then solve for Vf
=)
 
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