Using the same method as in the text, calculate the entropy of mixing for a system of two monatomic ideal gases, Aand B, whose relative proportion is arbitrary. Let Nbe the total number of molecules and letx be the fraction of these that are of speciesB . You should find

ΔSmixing=Nk[xlnx+(1x)ln(1x)]

Check that this expression reduces to the one given in the text whenx=1/2 .

Short Answer

Expert verified

The entropy mixing system of two monatomic ideal gases is, ΔSmixing=Nk((1x)ln(1x)+xln(x))

Step by step solution

01

Step: 1 Equating total volume:

The Sackur-Tetrode formula by 3-dideal gas,

S=NklnVN4mπU3Nh232+52

Where,Vrepresents volume, Urepresents energy, Nrepresents the number of molecules, mrepresents the mass of a single molecule, and hrepresents Planck's constant.

NB=xNNA=(1x)N

the total volume fractions is

VB=xVVA=(1x)V

02

Step: 2 Volume changes:

From the above equation,

S=NklnVN4mπU3Nh232+52S=Nkln(V)+ln1N4mπU3Nh232+52ln1N4mπU3Nh232

The change in entropy process where the volume changes is

ΔS=SfSi=NklnVflnViΔS=NklnVfVi

The volume change for two gases is

ΔSA=NAklnVA,fVA,iΔSB=NBklnVB,fVB,i

03

Step: 3 Finding entropy mixing:

The volume of gas part Astarts from VA=(1x)Vand ends with total volume container role="math" localid="1650278031887" V.

The part Bstarts from VB=xVand ends with total volume container V.

ΔSA=(1x)NklnV(1x)VΔSB=xNklnVxVΔSA=(1x)Nkln1(1x)=(1x)Nkln(1x)ΔSB=xNkln1x=xNkln(x)

After mixing the total entropy change is entropy of mixing by

ΔSmixing=ΔSA+ΔSB=Nk((1x)ln(1x)+xln(x))ΔSmixing=Nk((1x)ln(1x)+xln(x))

Both logarithms are negative so 0<x<1, soΔSmixing>0.If x=12so,the two equal quantities of gases starting by

ΔSmixing=Nkln2

Since Nis the number of molecules of each gas,not total number.

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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.

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.)

According to the Sackur-Tetrode equation, the entropy of a monatomic ideal gas can become negative when its temperature (and hence its energy) is sufficiently low. Of course this is absurd, so the Sackur-Tetrode equation must be invalid at very low temperatures. Suppose you start with a sample of helium at room temperature and atmospheric pressure, then lower the temperature holding the density fixed. Pretend that the helium remains a gas and does not liquefy. Below what temperature would the Sackur-Tetrode equation predict that Sis negative? (The behavior of gases at very low temperatures is the main subject of Chapter 7.)

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?

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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