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Calculate the Fermi energy for copper, which has a density of8.9103kg/m3and one conduction electron per atom. Is room temperature "cold"?

Short Answer

Expert verified

The Fermi energy for the copper is7.0eV . The room temperature is cold.

Step by step solution

01

Formula Used:

The energy of fermions at absolute zero temperature is known as Fermi energy. The mathematical equation for the Fermi energy is,

EF=22m[3(2s+1)2NV]23 鈥︹. (1)

Here,

NNumber of oscillators

Planck's reduced constant

VVolume

sSpin

02

Given information from question and calculate the fermi energy 

Density of copper=8.9103kg/m3

The NN in the equation (1) can be rewritten as the mass per unit volume over the mass per atom, or the bulk density D over the atomic mass:

role="math" localid="1658381923377" EF=22m[3(2s+1)2NV]23=22m[3(2s+1)2DmA]23

Substitute9.11031kgfor mass of the electron (m),8.9103kg/m3for density of copper(D), 1.0551034J.sfor ,12forthe spin of the electron and 1.0551025kgformA.

role="math" localid="1658381931536" EF=2(1.0551034J.s)2(9.11031kg)[3(2(12)+1)2(8.9103kg/m3)(1.0551025kg)]23=1.1261018J

Convert the unit for Fermi energy for copper energy from JtoeV .

role="math" localid="1658381943480" EF=1.1261018J=(1.1261018J)(1eV1.6109J)=7.04eV

Therefore, the Fermi energy for the copper is7.04eV .

Since the energy that a particle at room temperature would have been 0.04eV(from 32kBT), as opposed to the Fermi energy of 7.0eV, room temperature would be considered cold in comparison.

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Most popular questions from this chapter

(a) From equation (9.34) and the Fermi-Dirac distribution given in Exercise 53, obtain an expression for EF(T), the Fermi temperature for a collection of fermion oscillators, (b) Show that EFo=. (c) Plot EF(T)versuskBTfrom 0tokBT6=1.5. (d) By what percent does the Fermi energy drop from its maximum T=0value when kBTrises to 25%of?

Example 9.4 investigated one criterion for quantum indistinguishability with reference to atmospheric nitrogen. Here we investigate the other, (a) Calculate the avenge separation between nitrogen molecules in the air. Assume a temperature of 300K a pressure of1atmand air that is 80% nitrogen. (b) Calculate the wave length of a typical nitrogen molecule in the air. (c) How does your result relate to Example 9.4?

When would a density of states be needed: in a sum over states? in a sum over energies? in an integral over energies? in an integral over states?

The diagram shows two systems that may exchange both thermal and mechanical energy via a movable, heat-conducting partition. Because both Eand Vmay change. We consider the entropy of each system to be a function of both:S(E,V). Considering the exchange of thermal energy only, we argued in Section 9.2 that was reasonable to define1TasSE. In the more general case, PTis also defined as something.

a) Why should pressure come into play, and to what mightPTbe equated.

b) Given this relationship, show thatdS=dQT(Remember the first law of thermodynamics.)

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.

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