How Does the Entropy Change During Adiabatic Mixing of Two Gases?

AI Thread Summary
In an adiabatic mixing scenario involving two gases in separate compartments, the total change in entropy is calculated by summing the changes for each gas during free expansion. The calculations show that if the gases are identical and in the same state, removing the partition results in no change in entropy, highlighting the Gibbs paradox. This paradox emphasizes that mixing identical gases does not produce a measurable change, while mixing different gases does increase entropy. The discussion raises confusion about whether the entropy change differs for identical versus different gases, with the consensus that it does. Ultimately, the problem's specifics regarding gas identity are crucial for determining entropy changes during mixing.
KFC
Messages
477
Reaction score
4
There are two compartments, each has half volume of the total volume, separated by an insulating partition. The whole setup is adiabatic. n mole of a monatomic gas with temperature T1 and pressure P in the left while in the right m mole of monatomic gas with termparture T2 and pressure P there. Now remove the partition so two gas mix, I am trying to find out the change entropy of the whole system.

Well, I assume the total change of the entropy is the sum of change of entropy of individual gas in free expand. So I calculate the change of entropy of each gas separately. It is easy to find out the final temperature of mixture, let's call it Tf. Obviously, we need to makeup an isotermal process to let the gas expand from V to 2V; and then makeup a isochoric process to increase/decrease the temperature to Tf. With this two processes, the change of entropy for each gas should be (assume T1<T2)

\Delta S_{left} = n R\ln 2 + nC_v\ln \frac{T_f}{T_1}

\Delta S_{right} = m R\ln 2 + mC_v\ln \frac{T_2}{T_f}

The total change of entropy is \Detal S= \Delta S_{left} + \Delta S_{right}.

My question is: we didn't tell if these two gas are same or not, and this result didn't tell any different even if there are two different gas? It is so confused! I think if we are considering the mixture of two different gas, the change of entropy should be different to that of mixing two identical gas, isn't it?

I found something about mixing of entropy in wiki, and there it gives a formula that tells the total change of entropy after mixture

\Delta S_m = -nR(x_1\ln x_1 + x_2\ln x_2)

where n is the total number of moles, x_1, x_2 are the mole fraction of each of the mixed components. Again, it doesn't tell the any different for different substances being mixed ?
 
Physics news on Phys.org
KFC said:
My question is: we didn't tell if these two gas are same or not, and this result didn't tell any different even if there are two different gas? It is so confused! I think if we are considering the mixture of two different gas, the change of entropy should be different to that of mixing two identical gas, isn't it?
Right. For example, if the two parts of the container separate gasses that are identical and in identical states, then when you remove the partition, there is no change in entropy, despite the fact that your equations might say otherwise. This is known as the Gibbs paradox.
http://en.wikipedia.org/wiki/Gibbs_paradox
 
You're right, KFC, the problem must specify whether the two compartments contain the same gas or different gases. In the first case the entropy is constant; in the second the entropy increases. The reason is that "mixing" is a meaningless term when discussing identical gases in identical states. It's impossible to identify or quantify mixing in this scenario because the particles are taken to be indistinguishable.
 
Consider an extremely long and perfectly calibrated scale. A car with a mass of 1000 kg is placed on it, and the scale registers this weight accurately. Now, suppose the car begins to move, reaching very high speeds. Neglecting air resistance and rolling friction, if the car attains, for example, a velocity of 500 km/h, will the scale still indicate a weight corresponding to 1000 kg, or will the measured value decrease as a result of the motion? In a second scenario, imagine a person with a...
Scalar and vector potentials in Coulomb gauge Assume Coulomb gauge so that $$\nabla \cdot \mathbf{A}=0.\tag{1}$$ The scalar potential ##\phi## is described by Poisson's equation $$\nabla^2 \phi = -\frac{\rho}{\varepsilon_0}\tag{2}$$ which has the instantaneous general solution given by $$\phi(\mathbf{r},t)=\frac{1}{4\pi\varepsilon_0}\int \frac{\rho(\mathbf{r}',t)}{|\mathbf{r}-\mathbf{r}'|}d^3r'.\tag{3}$$ In Coulomb gauge the vector potential ##\mathbf{A}## is given by...
Thread 'Griffith, Electrodynamics, 4th Edition, Example 4.8. (First part)'
I am reading the Griffith, Electrodynamics book, 4th edition, Example 4.8 and stuck at some statements. It's little bit confused. > Example 4.8. Suppose the entire region below the plane ##z=0## in Fig. 4.28 is filled with uniform linear dielectric material of susceptibility ##\chi_e##. Calculate the force on a point charge ##q## situated a distance ##d## above the origin. Solution : The surface bound charge on the ##xy## plane is of opposite sign to ##q##, so the force will be...
Back
Top