Entropy change during wet compression

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Discussion Overview

The discussion revolves around the entropy change during wet compression, specifically examining the apparent paradox between mathematical and physical interpretations of entropy in an isentropic process. Participants explore the implications of thermodynamic principles and statistical physics in the context of adiabatic compression of a gas transitioning from a mixture of vapor and water to superheated vapor.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant notes that mathematically, the entropy change (ΔS) is zero for isentropic compression, yet physically, the transition from a less disordered state to a more disordered state suggests an increase in entropy.
  • Another participant argues that if compression occurs slowly and without heat exchange, the second law of thermodynamics supports the constancy of entropy, independent of disorder concepts.
  • A participant requests clarification on the relationship between entropy and disorder as mentioned in the previous post.
  • It is suggested that thermodynamic entropy can be calculated without referencing disorder, indicating that it is a distinct concept from statistical entropy.
  • One participant summarizes the situation as a balance between increasing temperature (which increases entropy) and decreasing volume (which decreases entropy), leading to a net unchanged entropy.
  • A later reply emphasizes that during isentropic compression, the temperature increase and volume decrease counterbalance each other, resulting in no change in entropy.

Areas of Agreement / Disagreement

Participants express differing views on the relationship between entropy and disorder, with some emphasizing thermodynamic principles while others focus on statistical interpretations. The discussion does not reach a consensus on the implications of these perspectives.

Contextual Notes

The discussion highlights the complexity of relating thermodynamic and statistical definitions of entropy, as well as the assumptions involved in interpreting the effects of temperature and volume changes on entropy.

kulkajinkya
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I have a quick question. Consider the process S2 to S1 in the figure below

rnkTs.gif.gif


Since this represents wet (isentropic) compression, mathematically we have ΔS=0 (assuming adiabatic compression). But if we consider the process in a physical way, we are going from a region of less disorder (mixture of vapour and water) to a state of more disorder (superheated vapour). Hence physically speaking entropy should increase since we are going to a highly disordered state from a low disorder state. So here is my paradox. How can the process have mathematically 0 change in entropy, but physically it does seem to increase?
 
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But if we consider the process in a physical way, we are going from a region of less disorder (mixture of vapour and water) to a state of more disorder (superheated vapour)

If the compression is done slowly and without heat exchange, that the entropy is constant follows from the second law of thermodynamics. There is no connection to disorder in this theory.

This connection is a subject of statistical physics, where the statistical entropy is connected to disorder in a mathematical way. You have to quantify the disorder by a number which is proportional to the number of microstates of the system that are compatible with the macroscopic variables, like pressure and volume.

When you do that, you will find out that the "disorder" is proportional to the volume raised to power of N, where N is the number of molecules of the gas.

Now, in order to perform the transition to superheated vapour, we have to push the piston and thus shrink the volume V. This decreases the number of accessible microstates and hence "disorder". If the statistical entropy is to have the same value as the thermodynamic entropy, the decrease of the accessible states has to compensate exactly for the increase of them due to higher kinetic energy of the molecules.
 
I didn't get this line: 'If the compression is done slowly and without heat exchange, that the entropy is constant follows from the second law of thermodynamics. There is no connection to disorder in this theory'.
Will you please elaborate?
 
The above behavior of the entropy can be calculated in thermodynamics without any use of idea of "disorder", if entropy means "thermodynamic entropy". Thermodynamic entropy is a concept that does not depend on such statistical notions.
 
So essentially you mean to say that on one hand we are increasing disorder by increasing the temp, but simultaneously decreasing disorder by reducing the volume? Like balancing both of them and getting a 'net' result of an 'unchanged' disorder, right?
 
Just consider isentropic compression of a gas without a phase change. This corresponds to the portion of path S2 to S1, starting from the 100% saturated vapor location. The temperature is increasing, which acts to increase the entropy, but the volume is decreasing, which acts to decrease the entropy. The two effects cancel out so that there is no change in entropy. Are you still wondering why decreasing the volume of a gas acts to decrease its entropy?

Chet
 
Thank you people for the answers!
 

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