Why does the entropy increase in free expansion of an ideal gas?

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In the free expansion of an ideal gas, the heat transfer Q is zero, yet entropy increases, indicating that the process is not quasistatic. The discussion highlights that the formula dS = dQ/T is incorrect for irreversible processes, and the correct expression is ΔS = ∫(dQ_rev/T). It is emphasized that during free expansion, the system does not maintain equilibrium, as pressure, temperature, and entropy vary throughout the gas. The concept of temperature as a non-constant integrating factor is crucial, as it confirms the lack of equilibrium at any instant. This understanding is essential for correctly applying thermodynamic principles to irreversible processes.
Mayan Fung
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I learned that
$$ dS = \frac Q T$$
In free expansion of Ideal gas, it is obvious that Q = 0. However, the entropy increases. I guess the reason is that it is because the process is not quasistatic. If I am right, why is this process not quasistatic. If I am not, what's wrong with the formula above. Thanks!
 
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In free expansion the system does not pass through a series of equilibrium states. The P, T and S do not have the same value throughout the extent of the system at every instant. It starts with equilibrium state ends in equilibrium state but in between we are not sure rather we are sure it is not in equilibrium.
 
Chan Pok Fung said:
I learned that
$$ dS = \frac Q T$$
In free expansion of Ideal gas, it is obvious that Q = 0. However, the entropy increases. I guess the reason is that it is because the process is not quasistatic. If I am right, why is this process not quasistatic. If I am not, what's wrong with the formula above. Thanks!
The equation you wrote is incorrect. If you learned it that way, then you were taught incorrectly. The correct formula is $$\Delta S=\int{\frac{dQ_{rev}}{T}}$$
What do you think the subscript "rev" stands for?

Here is a reference to my recent Physics Forums Insights article the provides a cookbook recipe for determining the entropy change in an irreversible process: https://www.physicsforums.com/insights/grandpa-chets-entropy-recipe/
See in particular Example 3

Here is another article on entropy and the second law that should help with your understanding: https://www.physicsforums.com/insights/understanding-entropy-2nd-law-thermodynamics/
 
Thanks all for your comments
I am not sure if I am correct. Q may not always be full differential, so I guess we can't always write dQ?
 
Chan Pok Fung said:
Thanks all for your comments
I am not sure if I am correct. Q may not always be full differential, so I guess we can't always write dQ?
As I said, your exact problem is solved in Example 3.
 
But gas is pushing nothing, isn't that the work done = 0?
 
Who said that the work done is not zero? Did you read what I wrote?
 
dq is not perfect differential but [dS =(dq/T)] is perfect differential and T is called integrating factor. One may argue that for infinitesimal dq T can be considered as constant but for the process under consideration at any instant during the process if you were to measure T at different points in the mass of gas you will not get the same value which will convince you that the mass of gas does not have definite value of temperature hence the gas is not in equilibrium at any instant during the process. So formula is not applicable.
 
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Let'sthink said:
dq is not perfect differential but [dS =(dq/T)] is perfect differential and T is called integrating factor. One may argue that for infinitesimal dq T can be considered as constant but for the process under consideration at any instant during the process if you were to measure T at different points in the mass of gas you will not get the same value which will convince you that the mass of gas does not have definite value of temperature hence the gas is not in equilibrium at any instant during the process. So formula is not applicable.

Thanks for your explanation!
 
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