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Use Table 3.1 to compute the temperatures of solid A and solid B when qA=1. Then compute both temperatures when qA=60. Express your answers in terms of ε/k, and then in kelvins assuming that ε=0.1eV.

Short Answer

Expert verified

For qA=1,

TA=0.187ε/k=216.8KTB=0.91ε/k=1055.07K

For qA=60,

localid="1646916582956" TA=0.57ε/k=660.87KTB=0.57ε/k=660.87K

Step by step solution

01

Given

Table of microstates, multiplicities, and entropies:

Both the solids, solid A and solid B, are sharing 100unitsof energy.

Hence,

qA+qB=100

The temperature of both the solids is to be determined when qA=1and qA=60.

role="math" localid="1646894597879" ε=0.1eV=0.1×1.6×10-19=1.6×10-20J

02

Calculation of temperatures when qA=1

Temperature can be defined in terms of entropy and energy of systems as:

T=US..........(1)

Where,

Ucan be replaced as role="math" localid="1646893107696" εdq

Hence, the simplified equation can be written as,

role="math" localid="1646893344744" T=εdqdS..........(2)

For qA=1, slope between qA=0and qA=2are used.

Similarly for solid B, qBwill be 100-qA.

Hence,

qA=0,qB=100-0=100, and

qA=2,qB=100-2=98

Now, from the table, the corresponding values of dSfor the values of qA=0,qA=2are 0,10.7krespectively.

By substituting these values in equation 2, temperature of solid A can be calculated as:

role="math" localid="1646895028376" TA=ε(2-0)SA(2)-SA(0)TA=ε(2-0)10.7k-0TA=0.187εk

We know that,

k=1.38×10-23J/K

By substituting the values, we get,

TA=0.187×1.6×10-201.38×10-23TA=216.8K

Similarly, temperature of solid B can be calculated as:

TB=ε(100-98)SB(100)-SB(98)TB=ε(100-98)(187.53-185.33)kTB=0.91εk

By substituting the values, we get,

TB=0.91×1.6×10-201.38×10-23TB=1055.07K

03

Calculation of temperatures when qA=60

Now for qA=60, the slope between qA=59and qA=61are used.

Similarly for solid B, qBwill be 100-qA.

In this case,

qA=59,qB=100-59=41, and

qA=61,qB=100-61=39

Temperature for solid A can be calculated as:

TA=ε(61-59)SA(61)-SA(59)

Now, from the table, the corresponding values of SA(61),SA(59)are 160.9,157.4respectivley.

By substituting the values in the above equation, we get,

TA=ε(61-59)(160.9-157.4)kTA==0.57εk

Now,

By substituting the values of ε,kin the above equation, we get,

TA=0.57×1.6×10-201.38×10-23TA=660.87K

Similarly, temperature of solid B can be calculated as:

TB=ε(41-39)SB(41)-SB(39)TB=ε(41-39)(107-103.5)kTB=0.57εk

By substituting the values, we get,

role="math" localid="1646916541515" TB=0.57×1.6×10-201.38×10-23TB=660.87K

04

Final answer

Hence, the temperature in both the cases for solids A and B is calculated as:

ForqA=1,

TA=0.187ε/k=216.8KTB=0.91ε/k=1055.07K

ForqA=60,

TA=0.57ε/k=660.87KTB=0.57ε/k=660.87K

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Most popular questions from this chapter

Experimental measurements of heat capacities are often represented in reference works as empirical formulas. For graphite, a formula that works well over a fairly wide range of temperatures is (for one mole)

CP=a+bT-cT2

where a=16.86J/K,b=4.77×10-3J/K2, and c=8.54×105J·K. Suppose, then, that a mole of graphite is heated at constant pressure from 298Kto 500K. Calculate the increase in its entropy during this process. Add on the tabulated value of S(298K)(from the back of this book) to obtain S(500K).

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.)

Show that the entropy of a two-state paramagnet, expressed as a function of temperature, is S=Nk[ln(2coshx)xtanhx], where x=μB/kT. Check that this formula has the expected behavior as T0and T.

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.)

The results of either of the two preceding problems can also be applied to the vibrational motions of gas molecules. Looking only at the vibrational contribution to the heat capacity graph for H2shown in Figure 1.13, estimate the value of εfor the vibrational motion of anH2 molecule.

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