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In Problem 2.32you computed the entropy of an ideal monatomic gas that lives in a two-dimensional universe. Take partial derivatives with respect to U,A, and N to determine the temperature, pressure, and chemical potential of this gas. (In two dimensions, pressure is defined as force per unit length.) Simplify your results as much as possible, and explain whether they make sense.

Short Answer

Expert verified

T=UNkP=NkTA=kTlnVN2mmkTh23/22

Step by step solution

01

Given Information

The entropy of an ideal gas is,

S=Nkln2mAU(Nh)2+2

02

Calculation

To get the temperature, we partial differentiate with respect to U,

1T=SUA,N1T=UNkln2mmAU(Nh)2+2=Nk(Nh)22xmAU2nmA(Nh)2=NkUT=UNk

Partial differentiating with respect to A, we get the pressure as,

P=TSAU,N=TANkln2mnUU(Nh)2+2=NkT(Nh)22nAU2mmU(Nh)2=NkTA

03

Chemical Potential

Partial differentiating the entropy with respect to N, we get the chemical potential as,

=TSdNUA=TdNNkln2mAU(Nh)2+2=kTln2mAU(Nh)2+2kTN(Nh)22mAU2nAUh22N3=kTln2mmAU(Nh)2+2+2kT=kTln2mmAU(Nh)2+22=kTln2mmAU(Nh)2=kTln2mmA(NkT)(Nh)2=kTlnVN2mLTN23/2

04

Conclusion

The temperature, pressure and entropy are given by:

T=UNkP=NkTA=kTlnVN2mkTh232

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Most popular questions from this chapter

Suppose you have a mixture of gases (such as air, a mixture of nitrogen and oxygen). The mole fraction xiof any species iis defined as the fraction of all the molecules that belong to that species: xi=Ni/Ntotal. The partial pressure Piof species iis then defined as the corresponding fraction of the total pressure: Pi=xiP. Assuming that the mixture of gases is ideal, argue that the chemical potential iof species i in this system is the same as if the other gases were not present, at a fixed partial pressure Pi.

The results of either of the two preceding problems can also be applied to the vibrational motions of gas molecules. Looking only at the vibrational contribution to the heat capacity graph for H2shown in Figure 1.13, estimate the value of for the vibrational motion of anH2 molecule.

A cylinder contains one liter of air at room temperature ( 300K) and atmospheric pressure 105N/m2. At one end of the cylinder is a massless piston, whose surface area is 0.01m2. Suppose that you push the piston in very suddenly, exerting a force of 2000N. The piston moves only one millimeter, before it is stopped by an immovable barrier of some sort.

(a) How much work have you done on this system?

(b) How much heat has been added to the gas?

(c) Assuming that all the energy added goes into the gas (not the piston or cylinder walls), by how much does the internal energy of the gas increase?

(d) Use the thermodynamic identity to calculate the change in the entropy of the gas (once it has again reached equilibrium).

Consider a monatomic ideal gas that lives at a height z above sea level, so each molecule has potential energy mgzin addition to its kinetic energy.

(a) Show that the chemical potential is the same as if the gas were at sea level, plus an additional term mgz:

(z)=-kTlnVN2mkTh23/2+mgz.

(You can derive this result from either the definition =-T(S/N)U,Vor the formula =(U/N)S,V.

(b) Suppose you have two chunks of helium gas, one at sea level and one at height z, each having the same temperature and volume. Assuming that they are in diffusive equilibrium, show that the number of molecules in the higher chunk is

N(z)=N(0)e-mgz/kT

in agreement with the result of Problem 1.16.

As shown in Figure 1.14, the heat capacity of diamond near room temperature is approximately linear in T. Extrapolate this function up to 500K, and estimate the change in entropy of a mole of diamond as its temperature is raised from298K to 500K. Add on the tabulated value at298K (from the back of this book) to obtain S(500K).

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