Question #75613
Description:
Define thermodynamic probability (W) of the macrostate. Establish the relation between entropy (S) and W.
Solution.
Thermodynamic probability (W) the number of ways in which this macroscopic state of the system can be implemented,
such a value according to the probability theory has the following property, even if our system consists of two parts 1 and 2 then we will have
W=W12=W1W2,S12=S1+S2
since entropy is defined as a measure of disorder in a system of bodies, it clearly depends on the probability of a given state and hence on W, we differentiate the function S=f(W) by W1 and W2
W12=W1W2,S12(W12)=S12(W1W2)=S1(W1)+S2(W2),∂W1∂S12=W2∗S′(W1W2)=S′(W1),⇒∂W1∂W2∂2S12=S′(W1W2)+W1W2S′′(W1W2)=0S′(W)+WS′′(W)=0
the solution of this differential equation has the form
S=kBlnW
where kB is called Boltzmann constant = 1.38×10−23J/K
for gas with particles N
W=N1!∗N2!∗N3!∗…N!
where N is the total number of molecules of the gas in the considered volume. Ni-number of molecules, moving at speeds corresponding to the i-th cell of the conditional velocity space
Answer
S=kBlnW
for gas with particles N
W=N1!∗N2!∗N3!∗…N!
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