Compute the quantum volume for an N2molecule at room temperature, and argue that a gas of such molecules at atmospheric pressure can be

treated using Boltzmann statistics. At about what temperature would quantum statistics become relevant for this system (keeping the density constant and pretending that the gas does not liquefy)?

Short Answer

Expert verified

The quantum volume for an N2molecule at room temperature is 6.9×10-33m3. The temperature of system at which quantum statistics become relevant is 5.681K.

Step by step solution

01

Step 1. Formula quantum volume

Formula for quantum volume is:

νQ=h2πmkT3

where,Tis temperature,role="math" localid="1647248715772" mis molecule mass,his Planck's constant,kis Boltzmann constant.

02

Step 2. Calculation quantum volume

Mass of N2 is calculated as:

role="math" localid="1647249031293" m=(28u)1.67×10-27kg1u=46.48×10-27kg

Substitute variables in quantum volume formula:

νQ=6.63×10-34J·s2π(46.48×10-27kg)(1.38×10-23J/K)(300K)3=6.63×10-34347.91×10-503=6.9×10-33m3

So, quantum volume ofN2molecule is6.9×10-33m3.

03

Step 3. Calculation ideal gas equation

Ideal gas equation is PV=NkT

So, VN=kTP

Substitute Pressure,P=1.013×105N/m2, Temperature,T=300K.

role="math" localid="1647253225593" VN=(1.38×10-23J/K)(300K)1.013×105N/m2=4×10-26m3

04

Step 4. Calculation temperature

In quantum statistics, VNνQ

kTPh2πmkT3T.T32h3(2πmK)32×PkT52Ph3(2πm)32k52T1kP2h6(2πm)315

Substitute the values of variables in above equation:

T11.38×10-23J/K(1.013×105N/m2)2(6.63×10-34J·s)6(2π(28×1.67×10-27kg))315T=5.681K

So, temperature of the system is5.681K.

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Most popular questions from this chapter

For a gas of particles confined inside a two-dimensional box, the density of states is constant, independent of ε(see Problem 7.28). Investigate the behavior of a gas of noninteracting bosons in a two-dimensional box. You should find that the chemical potential remains significantly less than zero as long as T is significantly greater than zero, and hence that there is no abrupt condensation of particles into the ground state. Explain how you know that this is the case, and describe what does happen to this system as the temperature decreases. What property must ε have in order for there to be an abrupt Bose-Einstein condensation?

The argument given above for why CvTdoes not depend on the details of the energy levels available to the fermions, so it should also apply to the model considered in Problem 7.16: a gas of fermions trapped in such a way that the energy levels are evenly spaced and non-degenerate.

(a) Show that, in this model, the number of possible system states for a given value of q is equal to the number of distinct ways of writing q as a sum of positive integers. (For example, there are three system states for q = 3, corresponding to the sums 3, 2 + 1, and 1 + 1 + 1. Note that 2 + 1 and 1 + 2 are not counted separately.) This combinatorial function is called the number of unrestricted partitions of q, denoted p(q). For example, p(3) = 3.

(b) By enumerating the partitions explicitly, compute p(7) and p(8).

(c) Make a table of p(q) for values of q up to 100, by either looking up the values in a mathematical reference book, or using a software package that can compute them, or writing your own program to compute them. From this table, compute the entropy, temperature, and heat capacity of this system, using the same methods as in Section 3.3. Plot the heat capacity as a function of temperature, and note that it is approximately linear.

(d) Ramanujan and Hardy (two famous mathematicians) have shown that when q is large, the number of unrestricted partitions of q is given approximately by

p(q)eπ2q343q

Check the accuracy of this formula for q = 10 and for q = 100. Working in this approximation, calculate the entropy, temperature, and heat capacity of this system. Express the heat. capacity as a series in decreasing powers of kT/η, assuming that this ratio is large and keeping the two largest terms. Compare to the numerical results you obtained in part (c). Why is the heat capacity of this system independent of N, unlike that of the three dimensional box of fermions discussed in the text?

Consider a two-dimensional solid, such as a stretched drumhead or a layer of mica or graphite. Find an expression (in terms of an integral) for the thermal energy of a square chunk of this material of area , and evaluate the result approximately for very low and very high temperatures. Also, find an expression for the heat capacity, and use a computer or a calculator to plot the heat capacity as a function of temperature. Assume that the material can only vibrate perpendicular to its own plane, i.e., that there is only one "polarization."

Consider a gas of nidentical spin-0 bosons confined by an isotropic three-dimensional harmonic oscillator potential. (In the rubidium experiment discussed above, the confining potential was actually harmonic, though not isotropic.) The energy levels in this potential are ε=nhf, where nis any nonnegative integer and fis the classical oscillation frequency. The degeneracy of level nis(n+1)(n+2)/2.

(a) Find a formula for the density of states, g(ε), for an atom confined by this potential. (You may assume n>>1.)

(b) Find a formula for the condensation temperature of this system, in terms of the oscillation frequency f.

(c) This potential effectively confines particles inside a volume of roughly the cube of the oscillation amplitude. The oscillation amplitude, in turn, can be estimated by setting the particle's total energy (of order kT) equal to the potential energy of the "spring." Making these associations, and neglecting all factors of 2 and πand so on, show that your answer to part (b) is roughly equivalent to the formula derived in the text for the condensation temperature of bosons confined inside a box with rigid walls.

(a) Estimate (roughly) the total power radiated by your body, neglecting any energy that is returned by your clothes and environment. (Whatever the color of your skin, its emissivity at infrared wavelengths is quite close to 1; almost any nonmetal is a near-perfect blackbody at these wavelengths.)

(b) Compare the total energy radiated by your body in one day (expressed in kilocalories) to the energy in the food you cat. Why is there such a large discrepancy?

(c) The sun has a mass of 2×1030kgand radiates energy at a rate of 3.9×1026watts. Which puts out more power per units mass-the sun or your body?

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