/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Q. 3.39 In Problem 2.32聽you computed th... [FREE SOLUTION] | 91影视

91影视

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

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91影视!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Starting with the result of Problem 3.5, calculate the heat capacity of an Einstein solid in the low-temperature limit. Sketch the predicted heat capacity as a function of temperature.

Use a computer to study the entropy, temperature, and heat capacity of an Einstein solid, as follows. Let the solid contain 50 oscillators (initially), and from 0 to 100 units of energy. Make a table, analogous to Table 3.2, in which each row represents a different value for the energy. Use separate columns for the energy, multiplicity, entropy, temperature, and heat capacity. To calculate the temperature, evaluate U/Sfor two nearby rows in the table. (Recall that U=qfor some constant .) The heat capacity (U/T)can be computed in a similar way. The first few rows of the table should look something like this:

(In this table I have computed derivatives using a "centered-difference" approximation. For example, the temperature .28is computed as 2/(7.15-0).) Make a graph of entropy vs. energy and a graph of heat capacity vs. temperature. Then change the number of oscillators to 5000 (to "dilute" the system and look at lower temperatures), and again make a graph of heat capacity vs. temperature. Discuss your prediction for the heat capacity, and compare it to the data for lead, aluminum, and diamond shown in Figure 1.14. Estimate the numerical value of in electron-volts, for each of those real solids.

An ice cube (mass 30g)0Cis left sitting on the kitchen table, where it gradually melts. The temperature in the kitchen is 25C.

(a) Calculate the change in the entropy of the ice cube as it melts into water at 0C. (Don't worry about the fact that the volume changes somewhat.)

(b) Calculate the change in the entropy of the water (from the melted ice) as its temperature rises from 0Cto 25C.

(c) Calculate the change in the entropy of the kitchen as it gives up heat to the melting ice/water.

(d) Calculate the net change in the entropy of the universe during this process. Is the net change positive, negative, or zero? Is this what you would expect?

Use the thermodynamic identity to derive the heat capacity formula

CV=TSTV

which is occasionally more convenient than the more familiar expression in terms of U. Then derive a similar formula for CP, by first writing dHin terms of dSand dP.

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).

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.