As per the Bose-Einstein system,
The particles are indistinguishable.
Let total number of particle in the system is ni , energy Ei
and let the statistical weight factor(degeneracy) is gi
.Now, the way of the distribution of ni particle into gi space,
So, the distribution ni(gi−1)!(ni−gi−1)!
for no particle,
we know that thermodynamic probability w=no(go−1)!(no−go−1)!.n1(g1−1)!(n1−g1−1)!.........ni(gi−1)!(ni−gi−1)!
So, we can write it as w=Πni(gi−1)!(ni−gi−1)!
Hence lnw=∑ln((ni−gi−1)!)−lnni−ln(gi−1)!
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