Total multiplicity is product of individual multiplicities?

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SUMMARY

The discussion centers on the concept of total multiplicity in statistical mechanics, specifically regarding two independent 3-harmonic oscillators with a total of 6 units of energy. Each oscillator has an individual multiplicity of 10, leading to a total multiplicity of 100 when combined, as confirmed by the formula Ω(X_{i},Y_{j}) = Ω(X_{i})Ω(Y_{j}). This principle is rooted in the rule of statistical independence, which states that the probabilities of independent systems can be factored, thereby allowing for the multiplication of their individual multiplicities.

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mishima
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Hi, I was looking for a proof or explanation of this. From Schroeder's Thermal Physics, pg 56, explaining interacting systems in equilibrium.

The example in the text is two 3-harmonic oscillators with a total of 6 units of energy. So one macrostate is where each has 3 units of energy. The individual multiplicity of each is 10, but the total multiplicity is 100 when considered together (10*10).

The explanation is "because the systems are independent of each other." I know there is something from introductory combinatorics which explains this (which is why he went no further), but I myself don't know.

Any help?
 
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For each microstate of the first oscillator, there are 10 microstates of the other oscillator, so there are 10 microstates of the oscillator-pair given that the first one is in a particular microstate.

Since there are 10 pair microstates for each microstate of the first oscillator, and there are 10 microstates of the first oscillator, there are 100 total microstates for the pair.
 
Yes, if the system are independent the total multiplicity is the product of the individual multiplicity. Example: one die has 6 possible states [1; 2; 3; 4; 5; 6] and two dice have 6X6=36 states [(1,1); (1,2); (1,3); (1,4); (1,5); (1,6); (2,1); (2,2); (2,3); (2,4); (2,5); (2,6); (3,1); (3,2); (3,3); (3,4); (3,5); (3,6); (4,1); (4,2); (4,3); (4,4); (4,5); (4,6); (5,1); (5,2); (5,3); (5,4); (5,5); (5,6); (6,1); (6,2); (6,3); (6,4); (6,5); (6,6)].
 
Hi, that makes sense. Is there a name for this rule?
 
It's generally referred to as statistical independence. If two systems together have a specific probability distribution P(X_{i},Y_{j})for each being in given microstates X_{i}and Y_{j} respectively, and these two systems are statistically independent of one another, then the probabilities will factor out.
P(X_{i},Y_{j}) = P(X_{i})P(Y_{j})

Where these probabilities are ratios of multiplicities:
P(X_{i})=\frac{\Omega(X_{i})}{\Omega_{total}}, P(Y_{j})=\frac{\Omega(Y_{j})}{\Omega_{total}}, P(X_{i},Y_{j})=\frac{\Omega(X_{i},Y_{j})}{\Omega_{total}}
If the probabilities factor, than so do the multiplicities.

If P(X_{i},Y_{j}) = P(X_{i})P(Y_{j})
then \Omega(X_{i},Y_{j}) = \Omega(X_{i})\Omega(Y_{j})
 

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