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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?

Short Answer

Expert verified

Part a

aThe probability of getting exactlyP(500)≈0.02523.

part b

bhe probability of getting exactlyP(600)≈4.635×10−11.

Step by step solution

01

Step: 1 Finding probability: (part a)

A larger coin tossing experiment is underway. N=1000 coins are flipped. Stirling's approach may be used to calculate the likelihood of receiving exactly 500 head and 500 tails. The total number of possible outcomes is as follows:

2N=21000

Where n=500heads as

Ω(N,n)=Nn=N!n!(N−n)!Ω(1000,500)=1000500Ω(1000,500)=1000!500!(1000−500)!Ω(1000,500)=1000!500!2.

Using Stirling's approximation as

N!≈NNe−N2πNΩ(1000,500)=1000!500!2≈10001000e−10002π⋅1000500500e−5002π⋅5002Ω(1000,500)≈10001000×e−1000×10005001000×e−1000×500×2π

02

Step:2 Dervative: (part a)

From the above equation,

Ω(1000,500)≈(500×2)1000×10005001000×500×2πΩ(1000,500)≈(2)1000×1000500×2π

Probability approximately getting exactly role="math" localid="1650333432268" 500heads as

P(n)=Ω(N,n)2NP(500)=Ω(1000,500)21000

Substituting,we get

P(500)=Ω(1000,500)21000≈121000(2)1000×1000500×2πP(500)≈1000500×2πP(500)≈0.02523.

03

Step: 3 Derivative probability: (part b)

The number getting n=500heads as

Ω(N,n)=NnΩ(N,n)=N!n!(N−n)!Ω(1000,600)=1000600Ω(1000,600)=1000!600!(1000−600)!Ω(1000,600)=1000!600!400!.

Using Stirling's approximation as

role="math" localid="1650333713655" N!≈NNe−N2πNΩ(1000,600)=1000!600!400!≈10001000e−10002π×1000600600e−6002π×600400400e−4002π×⋅400Ω(1000,600)≈10001000×e−1000×1000400400×600600×e−1000×600×400×2π

04

Step: 4 Equating part: (part b)

From the above equation,

Ω(1000,600)≈21000×5001000×1000400400×600600×600×400×2πΩ(1000,600)≈1480π×21000×5001000400400×600600

Probability approximately getting exactly 500heads as

P(n)=Ω(N,n)2NP(600)=Ω(1000,600)21000

Substituting,we get

P(600)=Ω(1000,600)21000≈121000×1480π×21000×5001000400400×600600P(600)≈1480π×5001000400400×600600

05

Step: 5 Finding probability value: (part b)

The ratio is not applicalable, so simplify as

1480π×5001000400400×600600=1480π×(1.25×400)1000(1×400)400×(1.5×400)600→1480π×(400)1000×(1.25)1000(400)400×(1)400×(400)600×(1.5)600

But,

(400)1000(400)600×(400)400=(400)1000(400)1000=1→1480π×(1.25)1000(1)400×(1.5)600

Where,

P(600)≈1480π×(1.25)1000(1)400×(1.5)600P(600)≈4.635×10−11.

Where as Maple is working large exponents directly.

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Most popular questions from this chapter

Calculate the multiplicity of an Einstein solid with 30oscillators and 30units of energy. (Do not attempt to list all the microstates.)

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?

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?

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.

A black hole is a region of space where gravity is so strong that nothing, not even light, can escape. Throwing something into a black hole is therefore an irreversible process, at least in the everyday sense of the word. In fact, it is irreversible in the thermodynamic sense as well: Adding mass to a black hole increases the black hole's entropy. It turns out that there's no way to tell (at least from outside) what kind of matter has gone into making a black hole. Therefore, the entropy of a black hole must be greater than the entropy of any conceivable type of matter that could have been used to create it. Knowing this, it's not hard to estimate the entropy of a black hole.
aUse dimensional analysis to show that a black hole of mass Mshould have a radius of order GM/c2, where Gis Newton's gravitational constant and cis the speed of light. Calculate the approximate radius of a one-solar-mass black holeM=2×1030kg .
bIn the spirit of Problem 2.36, explain why the entropy of a black hole, in fundamental units, should be of the order of the maximum number of particles that could have been used to make it.

cTo make a black hole out of the maximum possible number of particles, you should use particles with the lowest possible energy: long-wavelength photons (or other massless particles). But the wavelength can't be any longer than the size of the black hole. By setting the total energy of the photons equal toMc2 , estimate the maximum number of photons that could be used to make a black hole of mass M. Aside from a factor of 8Ï€2, your result should agree with the exact formula for the entropy of a black hole, obtained* through a much more difficult calculation:

Sb.h.=8Ï€2GM2hck

d Calculate the entropy of a one-solar-mass black hole, and comment on the result.

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