Stat mech-microstates and macrostates

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SUMMARY

The discussion focuses on the fundamentals of statistical mechanics, specifically the concepts of microstates and macrostates. The analogy of coins is used to illustrate two-state systems, where "heads" represent particles in an upper energy state. The conversation emphasizes the importance of understanding energy exchange between closed subsystems and introduces the binomial distribution for calculating microstates. Additionally, the discussion references the multinomial distribution and the entropy formula S=-∑i pi ln pi as key components in this area of study.

PREREQUISITES
  • Understanding of statistical mechanics principles
  • Familiarity with microstates and macrostates
  • Knowledge of binomial and multinomial distributions
  • Basic grasp of entropy and its mathematical representation
NEXT STEPS
  • Study the derivation of the entropy formula S=-∑i pi ln pi
  • Explore the implications of the binomial distribution in statistical mechanics
  • Investigate the differences between microstates and macrostates in closed systems
  • Learn about the applications of multinomial distributions in thermodynamics
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Students of physics, researchers in statistical mechanics, and anyone interested in the foundational concepts of thermodynamics and entropy.

Dawei
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Hello,

I'm trying to make sure I understand the basics of statistical mechanics and microstates/macrostates.

Being the nerd that I am, I have attempted to draw a diagram, as if I were explaining it to someone. If some one who is familiar with this topic could please review it and tell me if they see anything at all wrong, I would very much appreciate it.

The two systems are each two state systems, and to keep things simple I used the common "coin" analogy, where the total number of coins represents the total number of particles, and if they are "heads" then that means they are in the upper energy state. The two individual subsystems, as well as the final combined system, are all assumed to be completely closed. The only energy exchange allowed is between the two subsystems after they are in contact.

4301178262_d90074aaf3_o.jpg
 
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That's a very good explanation that one rarely finds in a book.

You could even write it out with formulas.

Also you could write out the number of microstates explicitely. In your case it is the binomial distribution. In the more general case it is the multinomial distribution and this is the origin of the well known
S=-\sum_i p_i\ln p_i
 

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