Intro statistical mechanics question

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SUMMARY

The discussion centers on the relationship between macrostates and microstates in statistical mechanics, specifically addressing the principle that the most probable macrostate corresponds to the highest number of microstates. It clarifies that while an isolated box with N particles has a definite macrostate, the entropy, defined as S=k_B lnW, indicates that the macrostate with the largest number of indistinguishable microstates (W) is the most likely to be observed. This principle explains why certain macrostates, such as a calm gas distribution, are far more probable than others, like a gale force wind in a sealed room.

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  • Understanding of macrostates and microstates in statistical mechanics
  • Familiarity with the concept of entropy and its mathematical formulation
  • Basic knowledge of thermodynamics and gas behavior
  • Proficiency in using statistical mechanics terminology
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  • Study the derivation and implications of the Boltzmann entropy formula S=k_B lnW
  • Explore the concept of thermodynamic equilibrium and its relation to macrostates
  • Investigate the statistical distribution of microstates in different thermodynamic systems
  • Learn about the implications of the second law of thermodynamics in statistical mechanics
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Coffee_
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Consider the quote ''The macrostate which corresponds to the highest number of microstates which result in that macrostate, is the state which will be observed.''

Can someone specify in which context this is correct because I'm quite confused by it. If I have an isolated box with N particles in it, clearly it has some definite macrostate. Then the macrostate is definite, and not decided by the highest number of microstates. So I'd like some elaboration on what it means.
 
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What they mean is that each macrostate can be produced by a number W of indistinguishable microstates. The most probable macrostate is the one for which W is the largest. Put differently, the entropy is [itex]S=k_B lnW[/itex] in this case, so the preferred state is the one with highest entropy.
 
Coffee_ said:
Consider the quote ''The macrostate which corresponds to the highest number of microstates which result in that macrostate, is the state which will be observed.''

Can someone specify in which context this is correct because I'm quite confused by it. If I have an isolated box with N particles in it, clearly it has some definite macrostate. Then the macrostate is definite, and not decided by the highest number of microstates. So I'd like some elaboration on what it means.

At any given instant, a box containing a gas of N particles has some microstate, defined by the states of all the individual particles making up the gas. It's also true that that configuration of particles defines the macrostate of the gas (i.e., its bulk properties).

At any given instant, the particles making up the gas are randomly colliding with one another, exchanging energy and momentum. The microstate of the gas changes randomly, Since the particular microstate defines what the bulk properties are too, the macrostate changes, however slightly as the microstate changes.

Since there are many microstates that could correspond to the same macrostate, and all microstates are equally likely, we can understand the following. The macrostate that has the most microstates is the one that's most likely to be seen at any given instant. Since there are vastly more microstates where the configurations of particles is nearly evenly distributed, we almost never see, for example, a gale force wind spontaneously blow in a still, sealed room.
 

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