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Use Stirling's approximation to show that the multiplicity of an Einstein solid, for any large values ofNandlocalid="1650383388983" q,is approximately

Omega(N,q)q+Nqqq+NNN2πq(q+N)/N

The square root in the denominator is merely large, and can often be neglected. However, it is needed in Problem2.22. (Hint: First show thatΩ=Nq+N(q+N)!q!N!. Do not neglect the2πNin Stirling's approximation.)

Short Answer

Expert verified

The square root and the large values are neglect

Ω(N,q)q+Nqqq+NNN2πq(q+N)N

Step by step solution

01

Macroscopic solid

For any macroscopic solid, both qand Nare large numbers (on the order of Avogadro's number, or1023) so the factorials in Ωare very large numbers, not calculable on most computers. To get estimates of Ωwe can use Stirling's approximation for the factorials. The multiplicity is given by:

Ω(N,q)=q+N-1q

Writing out the binomial coefficient:

q+N-1q=(q+N-1)!q!(N-1)!

we can write the factorial (q+N-1)! in the following form:

(q+N-1)!=(q+N-1)!×q+Nq+N

we can write the factorial (q+N-1)! in the following form:

(q+N-1)!=(q+N-1)!×q+Nq+N

but,(q+N-1)!(q+N)=(q+N)so

(q+N-1)!=(q+N)!(q+N)

and also we can write the factorial (N-1)! in the following form:

(N-1)!=(N-1)!×NN=N!N

Assume that qand Nare large numbers, so:

02

Substitution 

substitute from (2) and (3) into (1), so:

Ω(N,q)=q+N-1q=N(q+N)(q+N)!N!q!

Assume that qand Nare large numbers, so we can use Stirling's approximation for the factorials:

n!2πnnne-n

so we get:

N!2πNNNe-Nq!2πqqqe-q(q+N)!2π(q+N)(q+N)(q+N)e-(q+N)

substitute from (5),(6)and (7)into (4), so:

Ω(N,q)N(q+N)2π(q+N)(q+N)(q+N)e-(q+N)2πNNNe-N2πqqqe-q

cancel e^{-(q+N)}withe^{-q}e^{-N}so:

Ω(N,q)N(q+N)2π(q+N)(q+N)(q+N)2πNNN2πqqq

Ω(N,q)N2π(q+N)(q+N)(2πq)(2πN)(q+N)(q+N)NNqq

Ω(N,q)N2πq(q+N)(q+N)(q+N)NNqq

03

Substitution 

but, (q+N)^{(q+N)}=(q+N)^{q}(q+N)^{N}, so:

Ω(N,q)N2πq(q+N)(q+N)q(q+N)NNNqq

Ω(N,q)N2πq(q+N)q+Nqqq+NNN

Ω(N,q)q+Nqqq+NNN2πq(q+N)N

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Most popular questions from this chapter

Consider a system of two Einstein solids, Aand B, each containing 10 oscillators, sharing a total of 20units of energy. Assume that the solids are weakly coupled, and that the total energy is fixed.

(a) How many different macro states are available to this system?

(b) How many different microstates are available to this system?

(c) Assuming that this system is in thermal equilibrium, what is the probability of finding all the energy in solid A?

(d) What is the probability of finding exactly half of the energy in solid A?

(e) Under what circumstances would this system exhibit irreversible behavior?

Consider a two-state paramagnet with 1023elementary dipoles, with the total energy fixed at zero so that exactly half the dipoles point up and half point down.

(a) How many microstates are "accessible" to this system?

(b) Suppose that the microstate of this system changes a billion times per second. How many microstates will it explore in ten billion years (the age of the universe)?

(c) Is it correct to say that, if you wait long enough, a system will eventually be found in every "accessible" microstate? Explain your answer, and discuss the meaning of the word "accessible."

Use a computer to plot formula 2.22directly, as follows. Define z=q_{A}/q, so that (1-z)=q_{B}/q. Then, aside from an overall constant that we'll ignore, the multiplicity function is [4z(1-z)]N, where zranges from 0to1and the factor of 4ensures that the height of the peak is equal to 1for any N. Plot this function forN=1,10,100,1000, and 10,000. Observe how the width of the peak decreases asNincreases.

The natural logarithm function, ln, is defined so that elnx=xfor any positive numberx.
aSketch a graph of the natural logarithm function.
b Prove the identities
localid="1650331641178" lnab=lna+lnbandlocalid="1650331643409" lnab=blna
(c) Prove thatlocalid="1650331645612" ddxlnx=1x.
(d) Derive the useful approximation

localid="1650331649052" ln(1+x)x

which is valid when localid="1650331651790" |x|1. Use a calculator to check the accuracy of this approximation for localid="1650331654235" x=0.1and localid="1650331656447" x=0.01.

Use the Sackur-Tetrode equation to calculate the entropy of a mole of argon gas at room temperature and atmospheric pressure. Why is the entropy greater than that of a mole of helium under the same conditions?

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