Suppose you flip four fair coins.

(a) Make a list of all the possible outcomes, as in Table 2.1.

(b) Make a list of all the different "macrostates" and their probabilities.

(c) Compute the multiplicity of each macrostate using the combinatorial formula 2.6, and check that these results agree with what you got by bruteforce counting.

Short Answer

Expert verified

Determine the multiplicity of each macrostate and ensure that the result is agree with got by brute force counting is

Ω(0tails)=Ω(4,0)=40=1Ω(1tails)=Ω(4,1)=41=4Ω(2tails)=Ω(4,2)=42=6Ω(3tails)=Ω(4,3)=43=4Ω(4tails)=Ω(4,4)=44=1

Step by step solution

01

Step1:Given data

Assume we have four distinguishable fair (equally likely to land heads or tails) coins. There are two if we flip all four. 24=16possible outcomes, because each coin has two possible states and the four coins are distinct from one another Each of these states is referred to as a microstate. On the other hand, we might be more interested in the total number of heads or tails rather than which coins came up in either state. In this case, we'd only be interested in the overall condition of the four coin collection.

02

Step2:Possible outcomes(part a)

(a)

03

Step3:Macrostate possibilities(part b)

(b)To make things easier to count, I converted the four coin states into binary numbers usingH=0 andT=1, then simply counted how many times each number appeared. for example:

- if the sum =0, so we have0tails.

- if the sum=1so we have1tails.

- if the sum =2, so we have 2tails.

- if the sum=3,so we have3tails.

- if the sum=4, so we have3tails.

04

Step4:possible outcomes(part b)

05

Step5:final probability(part b)

06

Step6:multiplicity macrostate(part c)

(c) In general, we can calculate the probability of getting n heads in N coin flips. The problem can be thought of as the number of ways to choose n coins from a total of N and make these n coins the heads with the remaining N-n tails. We have N coins to choose from for the first of the n coins, so there are N ways to make this first selection. With that first coin selected, there areN-1coins from which we can select the next head, and so on, until we reach the final head. for which we have N-n+1choices. Thus the number of ways of choosing n coins from N in which the order of the choice does matter is:

N(N1)(Nn+1)=N!(N1)!

However, for a given macrostate, the order in which we choose the heads is irrelevant, and because there are n! ways to order each of the macrostates, the actual number of ways to choose the macrostate with n heads isΩ(N,n)=N!(N1)!n!=Nn

That is, Ω(N,n)is the binomial coefficientNn. So the multiplicity of macrostates:

Ω(0tails)=Ω(4,0)=40=1Ω(1tails)=Ω(4,1)=41=4Ω(2tails)=Ω(4,2)=42=6Ω(3tails)=Ω(4,3)=43=4Ω(4tails)=Ω(4,4)=44=1

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Most popular questions from this chapter

Fun with logarithms.
a Simplify the expressionealnb. (That is, write it in a way that doesn't involve logarithms.)
b Assuming that b<<a, prove that ln(a+b)(lna)+(b/a). (Hint: Factor out the afrom the argument of the logarithm, so that you can apply the approximation of part d of the previous problem.)

This problem gives an alternative approach to estimating the width of the peak of the multiplicity function for a system of two large Einstein solids.

(a) Consider two identical Einstein solids, each with Noscillators, in thermal contact with each other. Suppose that the total number of energy units in the combined system is exactly 2N. How many different macrostates (that is, possible values for the total energy in the first solid) are there for this combined system?

(b) Use the result of Problem2.18to find an approximate expression for the total number of microstates for the combined system. (Hint: Treat the combined system as a single Einstein solid. Do not throw away factors of "large" numbers, since you will eventually be dividing two "very large" numbers that are nearly equal. Answer: 24N/8πN.)

(c) The most likely macrostate for this system is (of course) the one in which the energy is shared equally between the two solids. Use the result of Problem 2.18to find an approximate expression for the multiplicity of this macrostate. (Answer:24N/(4πN) .)

(d) You can get a rough idea of the "sharpness" of the multiplicity function by comparing your answers to parts (b) and (c). Part (c) tells you the height of the peak, while part (b) tells you the total area under the entire graph. As a very crude approximation, pretend that the peak's shape is rectangular. In this case, how wide would it be? Out of all the macrostates, what fraction have reasonably large probabilities? Evaluate this fraction numerically for the case N=1023.

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.

Write e1023in the form 10x, for somex.

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?

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