Relation between entropy and pressure at constant temperature

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Discussion Overview

The discussion revolves around the relationship between entropy and pressure at constant temperature, exploring whether a decrease in pressure leads to an increase in entropy. Participants examine this concept from various theoretical and practical perspectives, considering ideal and non-ideal gases, as well as reversible and irreversible processes.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants suggest that a decrease in pressure at constant temperature may lead to an increase in entropy, but this requires further discussion on the nature of the system and the process involved.
  • One participant argues that the relationship can be derived mathematically, indicating that as pressure increases, entropy decreases, or vice versa, depending on the system's characteristics.
  • Another viewpoint emphasizes that for a decrease in pressure to occur at constant temperature, an increase in volume must happen, which necessitates heat flow into the gas, thus increasing entropy.
  • Concerns are raised about the applicability of these principles to non-ideal gases, where the heat absorbed may not follow the same rules as for ideal gases, potentially leading to a negative entropy change under certain conditions.
  • There is a discussion about the implications of free expansion and how it affects the definition of temperature and entropy, with some participants arguing that entropy must increase in any case where pressure decreases, regardless of the process being reversible or irreversible.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between pressure and entropy, with some supporting the idea that entropy increases with decreasing pressure, while others highlight conditions under which this may not hold true, particularly for non-ideal gases. The discussion remains unresolved with multiple competing perspectives.

Contextual Notes

Participants note that the conclusions drawn may depend on the definitions of the system and the processes involved, including whether they are reversible or irreversible. The discussion also touches on the limitations of applying ideal gas behavior to non-ideal systems.

bill nye scienceguy!
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if there is a decrease in pressure at constant temperature will there be an increase in entropy?
 
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bill nye scienceguy! said:
if there is a decrease in pressure at constant temperature will there be an increase in entropy?
Maybe...
 
Very interesting question, Bill. My first knee-jerk reaction is to say yes, because energy is lost from the system. But the fact that it's mechanical potential energy (pressure) rather than electromagnetic energy (heat) is a bit strange, so maybe the question requires more discussion.
 
Increase in the entropy of what? Only the system or the system and the surroundings together?

I think it depends on how the system is defined and what process the system is subject to (reversible/irreversible).
 
I would say yes.
Starting from
T dS = dE + P dV

and dividing by dP at constant T gives
T\left( \frac{\partial S}{\partial P} \right)_T = \left( \frac{\partial E}{\partial P} \right)_T + P\left( \frac{\partial V}{\partial P} \right)_T

If you use the idea gas equations E = \lambda NkT and PV = NkT then energy derivative reduces to zero and you're left with the pressure/change in volume term. The final result I get is
\left( \frac{\partial S}{\partial P} \right)_T = -\frac{V}{T}

which is negative, indicating that as pressure goes up, entropy goes down, or vice versa.

For a real system, the energy derivative is likely to be positive and the volume derivative will always be negative (for P > 0) so these two terms will compete.
 
bill nye scienceguy! said:
if there is a decrease in pressure at constant temperature will there be an increase in entropy?
The only way to have a decrease in pressure at constant temperature is to have an increase in volume. Work must be done in order to increase the volume (unless it is a free expansion). From the first law, if temperature remains the same (ie. internal energy remains constant) there must be heat flow into the gas. Since entropy is dQ/T, and dQ is positive (ie. into the gas) there is an increase in entropy of the gas.

If there is an adiabatic free expansion of a gas, the temperature is unchanged (isothermal) so you might think that there is no increase in entropy (dQ = 0 so dQ/T = dS = 0). However, this is not correct. dQ = TdS is defined only for reversible processes. While the gas is expanding, the speed distribution of the molecules is no longer a Maxwell-Boltzmann speed distribution. So temperature is undefined. In order to determine the entropy (which since it is a state function it is independent of the process by which the state changed) you have to determine an equivalent reversible process. In any reversible process, work must be done during the expansion, so heat must flow into the gas. Therefore, dS>0.

So in all cases, there is an increase in entropy of the gas where there is a decrease in pressure but no change in temperature.

There is a very easy conceptual way to see this. Entropy measures the energy concentration. If the same amount of energy disperses into a larger volume, entropy must increase.

AM
 
Andrew Mason said:
From the first law, if temperature remains the same (ie. internal energy remains constant) there must be heat flow into the gas

That's true for an ideal gas. But for a non-ideal gas (or a general homogeneous substance), the heat absorbed will be,

dQ= C_p dT - TV \alpha dp

where \alpha is the coefficient of volume expansion. So, if you look at a quasi-static equilibrium process for a substance with a negative coefficient which expands on cooling in a certain temperature range (like water), the entropy change can be negative depending on the value of the integral,

\int TV \alpha dp
 
siddharth said:
That's true for an ideal gas. But for a non-ideal gas (or a general homogeneous substance), the heat absorbed will be,

dQ= C_p dT - TV \alpha dp

where \alpha is the coefficient of volume expansion. So, if you look at a quasi-static equilibrium process for a substance with a negative coefficient which expands on cooling in a certain temperature range (like water), the entropy change can be negative depending on the value of the integral,

\int TV \alpha dp
But in this case, temperature is constant. I am not aware of any substance which, if pressure is decreased its volume reduces. So if pressure decreases and temperature is constant, you have expansion which does work. Therefore, heat must flow into the system, regardless of the type of substance.

AM
 

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