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Fun with logarithms.
a Simplify the expressionealnb. (That is, write it in a way that doesn't involve logarithms.)
b Assuming that b<<a, prove that ln(a+b)(lna)+(b/a). (Hint: Factor out the afrom the argument of the logarithm, so that you can apply the approximation of part d of the previous problem.)

Short Answer

Expert verified

Part a

aThe expressions is ealn(b)=ba.

Part b

bThe equationln(a+b)ln(a)+bais proved.

Step by step solution

01

Step: 1 Simplify steps: (part a)

We know that,

ealn(b)

The logarithm rule is

lnba=aln(b)ealn(b)=elnbaeln(x)=xealn(b)=elnba=ba

02

Step: 2  Equating part: (part b)

Consider b<<aand factor aas

ln(a+b)ln(a+b)=lna1+baln(a+b)=ln(a)+ln1+ba

Using Taylor formula as

f(x)=fx0+dfdxx0xx0+ln1+ba=ln(1+x)

03

Step: 3 Proving part: (part b)

We have,

ln(1+x)atx0=0as,

ln(1+x)ln(1+0)+(x0)d(ln(1+x))dx0ln(1+x)0+(x)11+x0=(x)11+0ln(1+x)xln1+babaln(a+b)ln(a)+ba

Hence,the equation is proved.

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Most popular questions from this chapter

For 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 N=N/2.

(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 xN(N/2). Check that your formula agrees with your answer to part (a) when x=0.

(c) How wide is the peak in the multiplicity function?

(d) Suppose you flip 1,000,000coins. Would you be surprised to obtain heads and 499,000 tails? Would you be surprised to obtain 510,000 heads and 490,000 tails? Explain.

Find an expression for the entropy of the two-dimensional ideal gas considered in Problem 2.26. Express your result in terms of U,AandN.

Consider an ideal monatomic gas that lives in a two-dimensional universe ("flatland"), occupying an area Ainstead of a volume V. By following the same logic as above, find a formula for the multiplicity of this gas, analogous to equation 2.40.

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 Ω(N,q)=q+N1q=(q+N1)!q!(N1)!

(a) N=3,q=4

(b)N=3,q=5

(c) N=3,q=6

(d) N=4,q=2

(e) N=4,q=3

(f) N=1,q=anything

(g) N= anything, q=1

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