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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

Use the Sackur-Tetrode equation to calculate the entropy of a mole of argon gas at room temperature and atmospheric pressure. Why is the entropy greater than that of a mole of helium under the same conditions?

Consider a system of two Einstein solids, \(A\) and \(B\), each containing 10 oscillators, sharing a total of 20 units of energy. Assume that the solids are weakly coupled, and that the total energy is fixed.

(a) How many different macrostates 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?

Use a computer to plot formula 2.22directly, as follows. Define z=q_{A}/q, so that (1-z)=q_{B}/q. Then, aside from an overall constant that we'll ignore, the multiplicity function is [4z(1-z)]N, where zranges from 0to1and the factor of 4ensures that the height of the peak is equal to 1for any N. Plot this function forN=1,10,100,1000, and 10,000. Observe how the width of the peak decreases asNincreases.

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?

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?

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