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Find an expression for the entropy of the two-dimensional ideal gas considered in Problem 2.26. Express your result in terms of U,AandN.

Short Answer

Expert verified

The Entropy of the two-dimensional ideal gaas isS=Nkln2mUA(Nh)2+2.

Step by step solution

01

Step: 1 Definition of Entropy:

Entropy is described as a measure of the degree of unpredictability in a system, or in other words, the growth in disorder.Entropy is a measure of disarray that has an impact on many facets of our existence. In reality, it's akin to a tax imposed by nature. If problem is not addressed, it will worsen over time. Energy dissipates, and systems disintegrate. We consider something to be more entropic if it is more disordered.

02

Step: 2 Derivative part

The entropy substance as

S=kln()

where,

localid="1650262053991" is the number of microstates substance accessible.

The localid="1650262058146" 2-dideal gas multipilicity is

=(A)N(N!)2h2N(2mU)N

where,localid="1650262061679" Ais the area gas.

By using Stirling's approximation,

n!2nnnenN!2NNNeN(N!)22N2N+1e2N

03

Step: 3 Finding Ω value:

Substituting we get,

(2mUA)N2N2N+1e2Nh2N

Where localid="1650262075329" Nis the large,the couple of factors away is

(2mUA)NN2Ne2Nh2N(2mUA)N(Nh)2Ne2N(2mUA)(Nh)2e2N

04

Step: 4 Finding entropy of ideal gas:

Taking logarithm on both sides,

ln(ab)=ln(a)+ln(b)andlnab=ln(a)ln(b)

is taking into account,so

ln()Nln(2mUA)(Nh)2e2ln()Nln(2mUA)(Nh)2+Nlne2ln()Nln2mUA(Nh)2+2

The entrpy of ideal gas gives as,

S=Nkln2mUA(Nh)2+2.

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Most popular questions from this chapter

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.

Compute the entropy of a mole of helium at room temperature and atmospheric pressure, pretending that all the atoms are distinguishable. Compare to the actual entropy, for indistinguishable atoms, computed in the text.

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=21030kg .
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 82, your result should agree with the exact formula for the entropy of a black hole, obtained* through a much more difficult calculation:

Sb.h.=82GM2hck

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

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.

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