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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(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

Suppose you flip 20 fair coins.

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

(b) What is the probability of getting the sequence HTHHTTTHTHHHTHHHHTHT (in exactly that order)?

(c) What is the probability of getting 12 heads and 8 tails (in any order)?

Consider an ideal monatomic gas that lives in a two-dimensional universe ("flatland"), occupying an area Ainstead of a volume V. By following the same logic as above, find a formula for the multiplicity of this gas, analogous to equation 2.40.

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?

For an Einstein solid with four oscillators and two units of energy, represent each possible microstate as a series of dots and vertical lines, as used in the text to prove equation 2.9.

Rather than insisting that all the molecules be in the left half of a container, suppose we only require that they be in the leftmost 99%(leaving the remaining 1%completely empty). What is the probability of finding such an arrangement if there are 100molecules in the container? What if there are 10,000molecules? What if there are 1023?

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