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How many possible arrangements are there for a deck of 52playing cards? (For simplicity, consider only the order of the cards, not whether they are turned upside-down, etc.) Suppose you start w e in the process? Express your answer both as a pure number (neglecting the factor of k) and in SI units. Is this entropy significant compared to the entropy associated with arranging thermal energy among the molecules in the cards?

Short Answer

Expert verified

The Boltzmann constant Swith and without.

  • With Boltzmann constant S=2.157 *10^21 J.K^1
  • With Boltzmann constant S = 156.36

Step by step solution

01

The entropy create in the process

  • In a standard pack of playing cards there are N=52different cards, so they can be arranged in:

ฮฉ=N!=52!=8.07ร—1067ways

  • The size of this number is why it's highly unlikely that any card game that relies on dealing cards from a shuffled deck will ever repeat itself. The entropy of a shuffled deck is therefore:

S=klnฮฉ

substitute withk=1.38ร—10โˆ’23Jโ‹…Kโˆ’1 S=1.38ร—10-23ln8.07ร—1067=2.157ร—10-21JยทK-1

S=1.38ร—10โˆ’23ln8.07ร—1067=2.157ร—10โˆ’21Jโ‹…Kโˆ’1

02

Calculate without Boltzmann Constants

Without Boltzmann's constant we have,

S=lnฮฉ=ln(8.07x1067)=156.36

  • Although playing cards aren't made of an Einstein solid, the multiplicity of the macrostate in which thermal energy is exchanged among the cards will be something of similar order. The approximate multiplicity in the high temperature case for an Einstein solid with oscillators and q >> N energy quanta is

ฮฉโ‰ˆqeNN

  • For Non the order of 1023 ,ฮฉis a very large number, so the thermal entropy of the cards is vastly greater than the entropy generated by shuffling the deck.

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Most popular questions from this chapter

Suppose you flip 20 fair coins.

(a) How many possible outcomes (microstates) are there?

(b) What is the probability of getting the sequence HTHHTTTHTHHHTHHHHTHT (in exactly that order)?

(c) What is the probability of getting 12 heads and 8 tails (in any order)?

Fun with logarithms.
a Simplify the expressionealnโกb. (That is, write it in a way that doesn't involve logarithms.)
b Assuming that b<<a, prove that lnโก(a+b)โ‰ˆ(lnโกa)+(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.)

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.

The natural logarithm function, ln, is defined so that elnโกx=xfor any positive numberx.
aSketch a graph of the natural logarithm function.
b Prove the identities
localid="1650331641178" lnโกab=lnโกa+lnโกbandlocalid="1650331643409" lnโกab=blnโกa
(c) Prove thatlocalid="1650331645612" ddxlnโกx=1x.
(d) Derive the useful approximation

localid="1650331649052" lnโก(1+x)โ‰ˆx

which is valid when localid="1650331651790" |x|โ‰ช1. Use a calculator to check the accuracy of this approximation for localid="1650331654235" x=0.1and localid="1650331656447" x=0.01.

Problem 2.20. Suppose you were to shrink Figure2.7until the entire horizontal scale fits on the page. How wide would the peak be?

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