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Verify every entry in the third line of Table 3.2 (starting with N=98.

Short Answer

Expert verified

All the entries in the third line are verified.

Step by step solution

01

Given Information

In a magnetic field B, a system of Nmagnetic dipoles arrange themselves so that their magnetic moment μpoints either parallel or anti parallel to the field.

Below is a table with the information provided.

02

Calculation

The expression for total energy is given as:

U=μBN-N..(1)

Where,

N= the number of dipoles pointing up

N= the number of dipoles pointing down

N=N+N= the total number of dipoles

The net magnetization is given as:

M=μN-N=-UB...(2)

Where,

B= the magnetic field

U= the total energy

The multiplicity of states is given as:

Ω=N!N!(NN)!=N!N!!N!.(3)

For a small system, entropy is given as:

Sk=ln(Ω)..(4)

By using these formulae, let's verify the table:

For N=98,N=2and N=100,

By substituting these values in the equation (1), we get,

U=μB(1002×98)UμB=96

By substituting this value in equation (2), we get,

M=UB=96μMNμ=96N=96100=0.96

Now, substitute the values in equation (3) to get Ω

Ω=100!98!2!=4950

By substituting this value in equation (4), we get,

Sk=ln(Ω)=ln(4950)=8.5

For N=97,N=3and N=100,

By substituting these values in equation (1), we get,

U=μB(1002×97)UμB=94

By substituting this value in equation (2), we get,

M=UB=94μMNμ=94N=94100=0.94

Substitute the values in equation (3) to get Ω

Ω=100!97!3!=161700

Now, by substituting this value in equation (4), we get,

Sk=ln(Ω)=ln(161700)=12

For N=52,N=48and N=100,

By substituting these values in equation (1), we get,

U=μB(1002×52)UμB=4

By substituting this value in equation (2), we get,

M=UB=4μMNμ=4N=4100=0.04

Now, substitute the values in equation (3) to get Ω

Ω=100!52!48!=9.32×1028

By substituting this value in equation (4), we get,

Sk=ln(Ω)=ln(161700)=12

For N=52,N=48and N=100,

by substituting these values in equation (1), we get,

U=μB(1002×51)UμB=2

By substituting this value in equation (2), we get,

M=UB=2μMNμ=2N=2100=0.02

Now, substitute the values in equation (3) to get Ω

Ω=100!51!49!=9.9×1028

By substituting this value in equation (4), we get,

Sk=ln(Ω)=ln9.9×1028=66.765

For N=50,N=50and N=100,

By substituting these values in equation (1), we get,

U=μB(1002×50)UμB=0

By substituting this value in equation (2), we get,

M=UB=0MNμ=0N=0100=0

Now substitute the values in equation (3) to get Ω

Ω=100!50!50!=1.009×1029

By substituting this value in equation (4), we get,

Sk=ln(Ω)=ln1.009×1029=66.784

For N=49,N=51and N=100,

By substituting these values in equation (1), we get,

U=μB(1002×49)UμB=2

By substituting this value in equation (2), we get,

M=UB=2μMNμ=2N=2100=0.02

Now substitute the values in equation (3) to get Ω

Ω=100!49!51!=9.9×1028

By substituting this value in equation (4), we get,

Sk=ln(Ω)=ln(9.9×1028)=66.765

For N=48,N=52and N=100,

By substituting these values in equation (1), we get,

U=μB(1002×48)UμB=4

By substituting this value in equation (2), we get,

M=UB=4μMNμ=4N=4100=0.04

Now substitute the values in equation (3) to get Ω

Ω=100!48!52!=9.32×1028

By substituting this value in equation (4), we get,

Sk=ln(Ω)=ln9.32×1028=66.7

For N=1,N=99and N=100,

By substituting these values in equation (1), we get,

U=μB(1002×1)UμB=98

By substituting this value in equation (2), we get,

M=UB=98μMNμ=98N=98100=0.98

Now substitute the values in equation (3) to get Ω

Ω=100!1!99!=100

By substituting this value in equation (4), we get,

Sk=ln(Ω)=ln(100)=4.6

For N=0,N=100and N=100,

By substituting these values in equation (1), we get,

U=μB(1002×0)UμB=100

By substituting this value in equation (2), we get,

M=UB=100μMNμ=100N=100100=1

Now substitute the values in equation (3) to get Ω

Ω=100!0!100!=1

By substituting this value in equation (4), we get,

Sk=ln(Ω)=ln(1)=0

03

Final answer

Hence, all the table values are verified.

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Most popular questions from this chapter

Polymers, like rubber, are made of very long molecules, usually tangled up in a configuration that has lots of entropy. As a very crude model of a rubber band, consider a chain of N links, each of length (see Figure 3.17). Imagine that each link has only two possible states, pointing either left or right. The total length L of the rubber band is the net displacement from the beginning of the first link to the end of the last link.

(a) Find an expression for the entropy of this system in terms of N and NR, the number of links pointing to the right.
(b) Write down a formula for L in terms of N and NR.
(c) For a one-dimensional system such as this, the length L is analogous to the volume V of a three-dimensional system. Similarly, the pressure P is replaced by the tension force F. Taking F to be positive when the rubber band is pulling inward, write down and explain the appropriate thermodynamic identity for this system.
(d) Using the thermodynamic identity, you can now express the tension force F in terms of a partial derivative of the entropy. From this expression, compute the tension in terms of L, T, N, and .
(e) Show that when L << N, the tension force is directly proportional to L (Hooke's law).
(f) Discuss the dependence of the tension force on temperature. If you increase the temperature of a rubber band, does it tend to expand or contract? Does this behavior make sense?
(g) Suppose that you hold a relaxed rubber band in both hands and suddenly stretch it. Would you expect its temperature to increase or decrease? Explain. Test your prediction with a real rubber band (preferably a fairly heavy one with lots of stretch), using your lips or forehead as a thermometer. (Hint: The entropy you computed in part (a) is not the total entropy of the rubber band. There is additional entropy associated with the vibrational energy of the molecules; this entropy depends on U but is approximately independent of L.)

Fill in the missing algebraic steps to derive equations 3.30, 3.31, and 3.33.

Use a computer to reproduce Table 3.2 and the associated graphs of entropy, temperature, heat capacity, and magnetization. (The graphs in this section are actually drawn from the analytic formulas derived below, so your numerical graphs won't be quite as smooth.)

Sketch a qualitatively accurate graph of the entropy of a substance (perhapsH2O ) as a function of temperature, at fixed pressure. Indicate where the substance is solid, liquid, and gas. Explain each feature of the graph briefly.

Figure 3.3 shows graphs of entropy vs. energy for two objects, A and B. Both graphs are on the same scale. The energies of these two objects initially have the values indicated; the objects are then brought into thermal contact with each other. Explain what happens subsequently and why, without using the word "temperature."

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