Chapter 2: Q. 2.13 (page 62)
Fun with logarithms.
Short Answer
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Part
Chapter 2: Q. 2.13 (page 62)
Fun with logarithms.
Part
Part
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Get started for freeFor either a monatomic ideal gas or a high-temperature Einstein solid, the entropy is given by times some logarithm. The logarithm is never large, so if all you want is an order-of-magnitude estimate, you can neglect it and just say . That is, the entropy in fundamental units is of the order of the number of particles in the system. This conclusion turns out to be true for most systems (with some important exceptions at low temperatures where the particles are behaving in an orderly way). So just for fun, make a very rough estimate of the entropy of each of the following: this book (a kilogram of carbon compounds); a moose of water ; the sun of ionized hydrogen .
For a single large two-state paramagnet, the multiplicity function is very sharply peaked about
(a) Use Stirling's approximation to estimate the height of the peak in the multiplicity function.
(b) Use the methods of this section to derive a formula for the multiplicity function in the vicinity of the peak, in terms of
(c) How wide is the peak in the multiplicity function?
(d) Suppose you flip
Find an expression for the entropy of the two-dimensional ideal gas considered in Problem
Consider an ideal monatomic gas that lives in a two-dimensional universe ("flatland"), occupying an area
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
(a)
(b)
(c)
(d)
(e)
(f)
(g) N= anything,
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