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Some advances textbooks define entropy by the formula

S=-k∑sPslnPs

where the sum runs over all microstates accessible to the system and Psis the probability of the system being in microstate s.

(a) For an isolated system, role="math" localid="1647056883940" Ps=1Ωfor all accessible states s. Show that in this case the preceding formula reduces to our familiar definition of entropy.

(b) For a system in thermal equilibrium with a reservoir at temperatureT,role="math" localid="1647057328146" Ps=e-EskTZ. Show that in this case as well, the preceding formula agrees with what we already know about entropy.

Short Answer

Expert verified

Part (a): S=klnΩ

Part (b):S=E-FT

Step by step solution

01

Part (a): Step 1. Given information

The entropy of the system is defined as

S=-k∑sPslnPs........................(1)

and the probability of finding the system in a microstate sis given by

Ps=1Ω........................(2)

02

Part (a): Step 2. Calculation

Substitute the value of Psfrom equation (2) into equation (1) and simplify to obtain the entropy of the system.

S=-k∑s1Ωln1Ω=klnΩΩ∑s1=klnΩΩΩ=klnΩ

03

Part (b): Step 1. Given information

The probability is given by

Ps=e-EskTZ..................(3)

04

Part (b): Step 2. Calculation

Take logarithm from both sides of equation (3).

lnPs=lne-EskTZ=-βEs-lnZ=1kT-Es+F.................(4)

Substitute the values of the parameters from equation (3) and equation (4) into equation (1) and simplify to obtain the required entropy of the system.

S=-k∑se-EskTZ1kT-Es+F=1T∑sEse-βEsZ-FT∑se-βEsZ=E-FT

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