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2 - The Second Law of Thermodynamics

Published online by Cambridge University Press:  05 June 2012

Ralph Baierlein
Affiliation:
Wesleyan University, Connecticut
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Summary

Chapter 2 examines the evolution in time of macroscopic physical systems. This study leads to the Second Law of Thermodynamics, the deepest principle in thermal physics. To describe the evolution quantitatively, the chapter introduces (and defines) the ideas of multiplicity and entropy. Their connection with temperature and energy input by heating provides the chapter's major practical equation.

Multiplicity

Simple things can pose subtle questions. A bouncing ball quickly and surely comes to rest. Why doesn't a ball at rest start to bounce? There is nothing in Newton's laws of motion that could prevent this; yet we have never seen it occur. Why? (If you are skeptical, recall that a person can jump off the floor. Similarly, a ball could—in principle—spontaneously rise from the ground, especially a ball that had just been dropped and had come to rest.)

Or let us look at a simple experiment, something that seems more “scientific.” Figure 2.1 shows the context. When the clamp is opened, the bromine diffuses almost instantly into the evacuated flask. The gas fills the two flasks about equally. The molecules seem never to rush back and all congregate in the first flask. You may say, “That's not surprising.” True, in the sense that our everyday experience tells us that the observed behavior is reasonable. But let's consider this “not surprising” phenomenon more deeply.

Type
Chapter
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Thermal Physics , pp. 24 - 50
Publisher: Cambridge University Press
Print publication year: 1999

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