What is the Derivative of P/T with respect to T?

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The discussion focuses on finding the derivative of temperature with respect to volume in a gas undergoing free expansion, where there is no heat exchange or work done. The user is trying to demonstrate that (dT/dv)u equals -(T^2/Cv)(d/dT)(P/T) at constant volume. Initial attempts lead to an expression involving the heat capacity at constant volume, Cv, and the pressure derivative, but the user struggles to connect the two forms of the equation. Clarifications reveal that the scenario describes an adiabatic free expansion, and participants guide the user toward rearranging their findings to achieve the desired result. The conversation emphasizes understanding the thermodynamic principles involved in the process.
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Homework Statement



Hi, i have a little problem with a demostration, I hope you can help me.

Homework Equations


this said that we have a system, a gas is containing in a recipe, there's no heat exchange neither work with the enviroment, only an expansion v to 2v, we have to find that

(dT/dv)u=-(T^2/Cv)(d/dT)(P/T)v

The Attempt at a Solution



I start with
dU=(dU/dT)vdT+(dU/dv)t dU=0
(dT/dv)u=-(dU/dv)(dT/dU)vdv

(dT/du)v=1/Cv

(dT/du)=-(1/cv)(T(dP/dT)-P)

I don't know how continue!
 
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Welcome to PF;

Have I understood you correctly:
An ideal(?) gas in a container (recipe?!), no heat may enter or leave the container(?), and no work is done on or by the gas(?) ... yet there is an expansion? How can this be?

It sounds like you are trying to describe an adiabatic expansion.
 
Simon Bridge said:
Welcome to PF;

Have I understood you correctly:
An ideal(?) gas in a container (recipe?!), no heat may enter or leave the container(?), and no work is done on or by the gas(?) ... yet there is an expansion? How can this be?

It sounds like you are trying to describe an adiabatic expansion.


yes! Sorry i have some problems lol! In fact it's a free expansion U=0 Q=0 and w=0
 
A free expansion

I try to find the Joule coefficient (dT/dv) constant U.
I must find that it's equal to -(T^2/Cv)d/dT(P/T) constant V, but
I found that it's equal to (-1/Cv)(T(dP/dT)v-P)
 
Oh you mean - like in the title ?!

All right: you got
$$\left.\frac{dT}{dv}\right|_U = -\frac{1}{C_v}\left(T\left.\frac{dP}{dT}\right|_v -P \right)$$

You need to get from there to:$$\left.\frac{dT}{dv}\right|_U = -\frac{T^2}{C_v}\left. \frac{d}{dT}\frac{P}{T}\right|_v$$

... it looks like you are almost there since you expression rearranges as:

$$\left.\frac{dT}{dv}\right|_U = -\frac{T^2}{C_v}\left(\frac{1}{T}\left.\frac{dP}{dT}\right|_v -\frac{P}{T^2} \right)$$

So what is $$\frac{d}{dT}\frac{P}{T}$$
 
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