Use the definition of temperature to prove the zeroth law of thermodynamics, which says that if system A is in thermal equilibrium with system B, and system B is in thermal equilibrium with system C, then system A is in thermal equilibrium with system C. (If this exercise seems totally pointless to you, you're in good company: Everyone considered this "law" to be completely obvious until 1931, when Ralph Fowler pointed out that it was an unstated assumption of classical thermodynamics.)

Short Answer

Expert verified

When the slopes of all three systems A, B, and C are equal, the systems are considered to be in thermal equilibrium, or at the same temperature.

Step by step solution

01

Concept Introduction

Temperature is a measure of hotness or coldness represented on one of several arbitrary scales that describes the natural flow of heat energy.

02

Explanation

If two items are in thermal equilibrium, their temperatures are said to be the same. The entropy and energy of a system can be used to express temperature. The gauge of randomness is entropy. The Zeroth law states that if a system A and a system B are in thermal equilibrium with another system C individually, then systems A and B will be in thermal equilibrium as well.

Mathematically, temperature can be stated as:

1T=SU

By rearranging the terms,

T=US

The entropy vs energy graph will have equal slopes if the system is in thermal equilibrium. Because any two systems in thermal equilibrium have the same SUvalues, system B and C must have the same slope as system A, resulting in their slopes being identical. The zeroth law, which asserts that a system A can be set in thermal equilibrium with any other systems that are all in thermal equilibrium with each other, is the foundation of thermodynamics.

03

Final answer

As a result, if the slopes of all three systems A, B, and C are similar, the systems are said to be in thermal equilibrium, or at the same temperature.

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Most popular questions from this chapter

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.

In Section 2.5 I quoted a theorem on the multiplicity of any system with only quadratic degrees of freedom: In the high-temperature limit where the number of units of energy is much larger than the number of degrees of freedom, the multiplicity of any such system is proportional to UNf/2, whereNf is the total number of degrees of freedom. Find an expression for the energy of such a system in terms of its temperature, and comment on the result. How can you tell that this formula forΩ cannot be valid when the total energy is very small?

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.)

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.)

A liter of air, initially at room temperature and atmospheric pressure, is heated at constant pressure until it doubles in volume. Calculate the increase in its entropy during this process.

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