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Problem 2.20. Suppose you were to shrink Figure2.7until the entire horizontal scale fits on the page. How wide would the peak be?

Short Answer

Expert verified

Fraction of the total width of the graph is around the hydrogen atom

1×10-12m

Step by step solution

01

Distance between the two points

Schroeder shows thatΩbecomes, near the peak:

Ω=Ωmax·e-N2xq2

which is a Gaussian curve. The width can be defined as the distance in xbetween the points where the curve is 1eof its maximum value, so:

Ωmaxe=Ωmax·e-N2xq2

e1=eN2xq2

1=N2xq2

x=q2N

so the width of the curve is twice this, or:

x=qN

02

Peak is a fraction

Since we're assumingq>>N, this width is still a large number, but since the total width of the graph is q+1, the width of the peak as a fraction of the total width of the graph is around:

q(q+1)N1N

which for any macroscopic value of N, is vanishingly small. For example, if Nis on the order of 1020, and we drew the graph so that the total width of the graph fits on a page 10cmwide, , the width of the central peak is around:

10×10-3m1020=1×10-12m

which is about frac1120the size of a hydrogen atom.

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Most popular questions from this chapter

Use the methods of this section to derive a formula, similar to equation2.21, for the multiplicity of an Einstein solid in the "low-temperature" limit,qN .

Show that during the quasistatic isothermal expansion of a monatomic ideal gas, the change in entropy is related to the heat input Qby the simple formula

s=QT

In the following chapter I'll prove that this formula is valid for any quasistatic process. Show, however, that it is not valid for the free expansion process described above.

For an Einstein solid with each of the following values of N and q , list all of the possible microstates, count them, and verify formula Ω(N,q)=q+N1q=(q+N1)!q!(N1)!

(a) N=3,q=4

(b)N=3,q=5

(c) N=3,q=6

(d) N=4,q=2

(e) N=4,q=3

(f) N=1,q=anything

(g) N= anything, q=1

Consider a two-state paramagnet with 1023elementary dipoles, with the total energy fixed at zero so that exactly half the dipoles point up and half point down.

(a) How many microstates are "accessible" to this system?

(b) Suppose that the microstate of this system changes a billion times per second. How many microstates will it explore in ten billion years (the age of the universe)?

(c) Is it correct to say that, if you wait long enough, a system will eventually be found in every "accessible" microstate? Explain your answer, and discuss the meaning of the word "accessible."

The mathematics of the previous problem can also be applied to a one-dimensional random walk: a journey consisting of Nsteps, all the same sic, cache chosen randomly to be cither forward or backward. (The usual mental image is that of a drunk stumbling along an alley.)

(a) Where are you most likely to find yourself, after the end of a long random walk?

(b) Suppose you take a random walk of 10,000steps (say each a yard long). About how far from your starting point would you expect to be at the end?

(c) A good example of a random walk in nature is the diffusion of a molecule through a gas; the average step length is then the mean free path, as computed in Section 1.7.Using this model, and neglecting any small numerical factors that might arise from the varying step size and the multidimensional nature of the path, estimate the expected net displacement of an air molecule (or perhaps a carbon monoxide molecule traveling through air) in one second, at room temperature and atmospheric pressure. Discuss how your estimate would differ if the clasped time or the temperature were different. Check that your estimate is consistent with the treatment of diffusion in Section1.7.

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