You have six shelves, one above the other and all above the floor, and six volumes of an encyclopedia, A, B, C, D, E and F.

(a) list all the ways you can arrange the volumes with five on the floor and one on the sixth/top shelf. One way might be(ABCDE_,_,_,_,_F).

(b) List all the ways you can arrange them with four on the floor and two on the third shelf.

(c) Show that there are many more ways, relative to pans (a) and (b), to arrange the six volumes with two on the floor and two each on the first and second shelves. (There are several ways to answer

this, but even listing them all won't take forever it's fewer than.)

(d) Suddenly, a fantastic change! All six volumes are volume X-it's impossible to tell them apart. For each of the three distributions described in parts (a), (b), and (c), how many different (distinguishable) ways are there now?

(e) If the energy you expend to lift a volume from the floor is proportional to a shelf's height, how do the total energies of distributions (a), (b), and (c) compare?

(I) Use these ideas to argue that the relative probabilities of occupying the lowest energy states should be higher for hosons than for classically distinguishable particles.

(g) Combine these ideas with a famous principle to argue that the relative probabilities of occupying the lowest states should he lower for fermions than for classically distinguishable particles.

Short Answer

Expert verified

a) There are a total of six possible ways to have five books on the floor and one on the sixth shelf. The possible arrangements are as follows:

(ABCDE_,_,_,_,_F)(ABCDF,_,_,_,_,_,E)(ABCEF,_,_,_,_,_,D)(ABDEF,_,_,_,_,_,C)(ACDEF,_,_,_,_,_B)(BCDEF,_,_,_,_,_,A)

b) There are a total of 15 possible ways to have four books on the floor and two on the third shelf. The possible arrangements are as follows:

ABCD,_,_,EF,_,_,_;BCEF,_,_,AD,_,_,_ABEF,_,_,CD,_,_,_;(BDEF,_,_,AC,_,_,_)(CDEF,_,_,AB,_,_,_);(ACEF,_,_,BD,_,_,_)(ABCE_,_,DF,_,_,_);(ADEF_,_,BC,_,_,_)(ABDE,_,_,,CF,_,_,_);ABDF,_,_,CE,_,_,_(ACDE,_,_,,BF,_,_,_);ACDF,_,_,BE,_,_,_(BCDE,_,_,AF,_,_,_);ABCF,_,_,DE,_,_,_(BCDF,_,_,AE,_,_,_)

c) The total number of ways to arrange the six volumes such that two are on the floor, two are on the first shelf, and two are on the second shelf is 90

d) The number of ways to perform the arrangements described in parts (a), (b), and (c) is only one.

e) All arrangements described in parts (a). (b). and (c) share the same total energy of 6 units.

f) As we've seen, books that can be recognised from one another have a greater number of alternative configurations than books that appear to be similar. This is similar to classical particles, which have a considerably larger variety of ways to disperse their energies in lower energy states than bosons. As a result, bosons gravitate toward lower energy levels, especially the ground state.

g) Fermions have a smaller likelihood of being found in the lowest states than classical particles.

Step by step solution

01

Concept used

Binomial coefficient:

The binomial coefficient is the number of ways of picking unordered outcomes from possibilities, also known as a combination or combinatorial number.

02

Calculate all possible ways to arrange the book 

(a)

In this part, our task is to enumerate all possible ways we could arrange the books with five on the floor and one on the sixth shelf. To do so, let's first calculate the total number of ways for such an arrangement using the binomial coefficient:

W=6!5!1!=6

There are a total of six possible ways to have five books on the floor and one on the sixth shelf. The possible arrangements are as follows:

(ABCDE_,_,_,_,_F)(ABCDF,_,_,_,_,_,E)(ABCEF,_,_,_,_,_,D)(ABDEF,_,_,_,_,_,C)(ACDEF,_,_,_,_,_B)(BCDEF,_,_,_,_,_,A)

03

Calculate all possible arrangement of books using binomial coefficient

(b)

In this part, our task is to list all possible ways we could arrange the books such that four are on the floor, and two are on third shelf. Again, let us use the binomial coefficient to list down the total ways to perform such an arrangement:

W=6!4!2!=15

There are a total of 15 possible ways to have four books on the floor and two on the third shelf. The possible arrangements are as follows:

ABCD,_,_,EF,_,_,_;BCEF,_,_,AD,_,_,_ABEF,_,_,CD,_,_,_;(BDEF,_,_,AC,_,_,_)(CDEF,_,_,AB,_,_,_);(ACEF,_,_,BD,_,_,_)(ABCE_,_,DF,_,_,_);(ADEF_,_,BC,_,_,_)(ABDE,_,_,,CF,_,_,_);ABDF,_,_,CE,_,_,_(ACDE,_,_,,BF,_,_,_);ACDF,_,_,BE,_,_,_(BCDE,_,_,AF,_,_,_);ABCF,_,_,DE,_,_,_(BCDF,_,_,AE,_,_,_)

04

Calculate the number of ways to arrange the six volumes

(c)

Using the binomial coefficient, the total number of ways to arrange the six volumes such that two are on the floor, two are on the first shelf, and two are on the second shelf is thus:

W=6!2!2!2!=90

05

The number of ways to perform the arrangements

(d)

Now supposing that the volumes cannot be distinguished from one another, that is, all books are seemingly identical, then our answers in parts (a), (b), and (c) are all one. This means that if the books are indistinguishable, then the number of ways to perform the arrangements described in parts (a), (b), and (c) is only one.

06

The energy we expend to lift the books are proportional to the shelf height 

(e)

Supposing that the energy we expend to lift the books are proportional to the shelf height, let us now say that the spacing between energy levels, that is, between shelves, is one. Thus, on the floor, we have 0 units of energy to disburse, on the first shelf, we have 1 energy unit, on the second, we have 2 units, and so on.

Now for part (a), five books are on the floor, and one is on the sixth shelf. Hence the total energy we disbursed must be:

Ea=0(5)+6(1)=6units

For part (b), four books are on the floor and two are on the third shelf. The total energy expended is

Eb=0(4)+3(2)=6units

For part (c),

Ec=0(2)+1(2)+2(2)=6units

As we can see, all arrangements described in parts (a). (b). and (c) share the same total energy of 6 units.

07

The relative probabilities of occupying the lowest energy states should be higher for hosons than for classically distinguishable particles. 

(f)

As we've seen, books that can be recognised from one another have a greater number of alternative configurations than books that appear to be similar. This is similar to classical particles, which have a considerably larger variety of ways to disperse their energies in lower energy states than bosons. As a result, bosons gravitate toward lower energy levels, especially the ground state.

08

The relative probabilities of occupying the lowest states should he lower for fermions than for classically distinguishable particles. 

(g)

No two particles can have the same set of quantum numbers, according to the exclusion principle. As a result, if the spin of the particles is taken into account, the maximum number of fermions that can occupy a given energy state is two. Despite the fact that fermions are identical particles, the exclusion principle prevents particles from sharing energy levels. The number of ways they can divide their energies in the lowest levels alters as a result of this. As a result, fermions have a smaller likelihood of being found in the lowest states than classical particles

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Most popular questions from this chapter

The Debye temperature of copper is 45K .

(a) Estimate its molar heat capacity at 100 K using the plot in Figure 9.33(b) .

(b) Determine its corresponding specific heat and compare it with the experimental value of 0.254J/g·K.

To obtain equation (9-42), we calculated a total number of fermions Nas a function of EFassuming T=0. starting with equation(9.41) . But note that (9.4)is the denominator of our model for calculating average particle energy, equation (9.26). its numerator is the total (as opposed (o average particle) energy'. which we’ll callUtotalhere. In other wonts. the total system energy Uis the average particle energyE¯ times the total number of particles (n). CalculateUtotalas a function ofEF

And use this to show that the minimum (T=0)energy of a gas of spin fermions may be written asUtotal=310(3π23m3/2V)2/3N5/3

Using the relationship between temperature and MandN given in (9-16) and that betweenE andn in (9-6), obtain equation (9-17) from (9- 12). The first sum given In Exercise 30 will be useful.

Example 9.2 obtains a ratio of the number of particles expected in the n = 2state lo that in the ground state. Rather than the n = 2state, consider arbitrary n.

(a) Show that the ratio is numberofenergyEnnumberofenergyE1=n2e-13.6cV(1-n-2)/kBT

Note that hydrogen atom energies are En=-13.6eV/st2.

(b) What is the limit of this ratio as n becomes very large? Can it exceed 1? If so, under what condition(s)?

(c) In Example 9.2. we found that even at the temperature of the Sun's surface(~6000K), the ratio for n = 2 is only 10-8 . For what value of nwould the ratio be 0.01?

(d) Is it realistic that the number of atoms with high n could be greater than the number with low n ?

Show that. using equation(936), density of states(938)follows fromlocalid="1658380849671" (937)

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