Obtain equation (9- 15) from (9-14). Make use or the following sums, correct when |x|<1 :

n=0xn=11-xn=0nxn=x(1-x)2

Short Answer

Expert verified

Equation E¯=n=0nhω0e-mω0kBTn=0emhω0kBT simplifies to equation E¯=hω0ehω0kBT-1

Step by step solution

01

Average Energy. 

Let us consider the expression for the average energy:

E¯=n=0nhω0e-nhω0kBTn=0e-nhω0kBT

Performing some minor modifications, we have:

E¯=hω0n=0ne-nhω0kBTn=0e-nhω0kBT

E¯=n=0nhω0e-nhω0kBTn=0e-nhω0kBT

02

Properties

Making use of the propertyx=e-hω0kBT.

n=0xn=11-xn=0[e-hω0kBT]n=11-e-hω0kBT

And,

n=0nxn=x(1-x)2n=0n[e-hω0kBT]n=e-hω0kBT(1-e-hω0kBT)2

03

Final Average Energy.

E¯=hω0e-hω0kBT(1-e-hω0kBT)211-e-hω0kBT=hω0e-hω0kBT1-e-hω0kBT=hω0(ehω0kBT)(1-e-hω0kBT)=hω0ehω0kBT-(ehω0kBT)(e-hω0kBT)=hω0ehω0kBT-1

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 Vaia!

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

Consider a room divided by imaginary lines into three equal parts. Sketch a two-axis plot of the number of ways of arranging particles versus NleftandNrightfor the caseN=1023, Note that Nmiddleis not independent, being of courseNNnghtNleftYour axes should berole="math" localid="1658331658925" NleftandNright, and the number of ways should be represented by density of shading. (A form for numbers of ways applicable to a three-sided room is given in Appendix I. but the question can be answered without it.)

At high temperature, the average energy of a classical one-dimensional oscillator is kBT, and for an atom in a monatomic ideal gas. it is 12kBT. Explain the difference. using the equipartition theorem.

The electrons’ contribution to the heat capacity of a metal is small and goes to 0as T0. We might try to calculate it via the total internal energy, localid="1660131882505" U=EN(E)D(E)dE, but it is one of those integrals impossible to do in closed form, and localid="1660131274621" N(E)FDis the culprit. Still, we can explain why the heat capacity should go to zero and obtain a rough value.

(a) Starting withN(E)FDexpressed as in equation (34), show that the slope N(E)FDdEatE=EFis-1(4kBT).

(b) Based on part (a), the accompanying figure is a good approximation to N(E)FDwhen Tis small. In a normal gas, such as air, whenTis raised a little, all molecules, on average, gain a little energy, proportional to kBT. Thus, the internal energy Uincreases linearly with T, and the heat capacity, UT, is roughly constant. Argue on the basis of the figure that in this fermion gas, as the temperature increases from 0to a small value T, while some particles gain energy of roughly kBT, not all do, and the number doing so is also roughly proportional to localid="1660131824460" T. What effect does this have on the heat capacity?

(c)Viewing the total energy increase as simply U= (number of particles whose energy increases) (energy change per particle) and assuming the density of states is simply a constant Dover the entire range of particle energies, show that the heat capacity under these lowest-temperature conditions should be proportional to kBREFT. (Trying to be more precise is not really worthwhile, for the proportionality constant is subject to several corrections from effects we ignore).

Exercise 54 calculates the three oscillator distributions'E=0values in the special case wherekBTis15ξ. Using a very common approximation technique. show that in the more general low-temperature limit,kBTε,theoccupation numbers becomeδ/kBT,e5/kBT, and 1, for the distinguishable. boson. and fermion cases, respectively. Comment on these results. (Note: Although we assume thatkBTNω0/(2s+1). we also still assume that levels are closely spaced-that is kBhω0.),

We based the exact probabilities of equation (9-9) on the claim that the number of ways of addingN distinct nonnegative integer quantum numbers to give a total ofM is{M+N-1)!/M!(N-1)!. Verify this claim (a) for the caseN=2,M=5and(b)for the case.

N=5,M=2

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.

Sign-up for free