Here is a first attempt at the entropy of argon atoms (molar mass ) held at in a…
PHYSICS · Multi-part · Fermi University Physics · Thermal, Statistical & Complex Systems · Statistical foundations and the equilibrium ensembles · Statistical mechanics of ideal classical systems
Thermal Physics, Ch The classical ideal gas from the partition function
Problem
Here is a first attempt at the entropy of N=2.00×1023 argon atoms (molar mass 39.95gmol−1) held at T=250K in a rigid box of volume V=5.00L=5.00×10−3m3. Argon is monatomic, the gas is dilute enough to be treated as an ideal gas in the classical regime, and only translational states are counted. The attempt writes Z1=V/λT3 with λT=h/2πmkBT, then ZN=Z1N, so that F=−NkBTln(V/λT3) and Strial=NkB[ln(λT3V)+23]. One factor has been left out of ZN. Name it, then work through the consequences. Use h=6.626×10−34Js, kB=1.381×10−23JK−1, NA=6.022×1023mol−1, and Stirling's approximation lnN!≈NlnN−N.
((a)) Evaluate λT and the trial entropy Strial.
((b)) Evaluate the correct entropy from the Sackur-Tetrode formula.
((c)) Show that the difference Strial−S is kBlnN!, and evaluate it.
((d)) The system is now doubled at the same temperature (N→2N, V→2V). By how much does the trial formula exceed twice its original value?