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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(N−1)…(N−n+1)=N!(N−1)!

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!(N−1)!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

For an Einstein solid with each of the following values of N and q , list all of the possible microstates, count them, and verify formula Ω(N,q)=q+N−1q=(q+N−1)!q!(N−1)!

(a) N=3,q=4

(b)N=3,q=5

(c) N=3,q=6

(d) N=4,q=2

(e) N=4,q=3

(f) N=1,q=anything

(g) N= anything, q=1

Use Stirling's approximation to find an approximate formula for the multiplicity of a two-state paramagnet. Simplify this formula in the limit N↓≪Nto obtain Ω≈Ne/N↓N↓. This result should look very similar to your answer to Problem 2.17; explain why these two systems, in the limits considered, are essentially the same.

Problem 2.20. Suppose you were to shrink Figure2.7until the entire horizontal scale fits on the page. How wide would the peak be?

Use a computer to reproduce the table and graph in Figure2.4: two Einstein solids, each containing three harmonic oscillators, with a total of six units of energy. Then modify the table and graph to show the case where one Einstein solid contains six harmonic oscillators and the other contains four harmonic oscillators (with the total number of energy units still equal to six). Assuming that all microstates are equally likely, what is the most probable macrostate, and what is its probability? What is the least probable macrostate, and what is its probability?

Use a computer to produce a table and graph, like those in this section, for the case where one Einstein solid contains 200 oscillators, the other contains100 oscillators, and there are 100 units of energy in total. What is the most probable macrostate, and what is its probability? What is the least probable macrostate, and what is its probability?

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