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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 again the system of two large, identical Einstein solids treated in Problem 2.22.

(a) For the case N=1023, compute the entropy of this system (in terms of Boltzmann's constant), assuming that all of the microstates are allowed. (This is the system's entropy over long time scales.)

(b) Compute the entropy again, assuming that the system is in its most likely macro state. (This is the system's entropy over short time scales, except when there is a large and unlikely fluctuation away from the most likely macro state.)

(c) Is the issue of time scales really relevant to the entropy of this system?

(d) Suppose that, at a moment when the system is near its most likely macro state, you suddenly insert a partition between the solids so that they can no longer exchange energy. Now, even over long time scales, the entropy is given by your answer to part (b). Since this number is less than your answer to part (a), you have, in a sense, caused a violation of the second law of thermodynamics. Is this violation significant? Should we lose any sleep over it?

Show that during the quasistatic isothermal expansion of a monatomic ideal gas, the change in entropy is related to the heat input Qby the simple formula

∆s=QT

In the following chapter I'll prove that this formula is valid for any quasistatic process. Show, however, that it is not valid for the free expansion process described above.

Suppose you flip1000 coins.
a What is the probability of getting exactly 500heads and 500tails? (Hint: First write down a formula for the total number of possible outcomes. Then, to determine the "multiplicity" of the 500-500"macrostate," use Stirling's approximation. If you have a fancy calculator that makes Stirling's approximation unnecessary, multiply all the numbers in this problem by 10, or 100, or1000, until Stirling's approximation becomes necessary.)
bWhat is the probability of getting exactly 600heads and400 tails?

Suppose you flip 50fair coins.

(a) How many possible outcomes (microstates) are there?

(b) How many ways are there of getting exactly25heads and25tails?

(c) What is the probability of getting exactly 25heads and 25tails?

(d) What is the probability of getting exactly 30heads and 20tails?

(e) What is the probability of getting exactly 40heads and 10 tails?

(f) What is the probability of getting 50heads and no tails?

(g) Plot a graph of the probability of getting n heads, as a function of n.

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

(a) How many different macrostates 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?

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