For a room3.0mtall, by roughly what percent does the probability of an air molecule being found at the ceiling differ from that of an equal speed molecule being found at the floor? Ignore any variation in temperature from floor to ceiling.

Short Answer

Expert verified

The percentage of the relative difference between the probability of finding an air molecule at height y=3mto that of another air molecule with the same speed at the floor is roughly 0.04%.

Step by step solution

01

Concept used

Boltzmann probability distribution:

PEn=Ae-En/kBT,

where is a normalization constant, and T is temperature. This corresponds to the probability of finding a particle at an energy stateEn for a system of N particles at temperature T .

02

Use the Boltzmann probability distribution

To tackle this problem, we will be using the Boltzmann probability distribution:

PEn=Ae-En/kBT, ……. (1)

03

Calculate the total energy of an air molecule

Under the influence of gravity, the total energy of an air molecule is the sum of its kinetic energy K and gravitational potential energy Ug:

E=K+Ug=12mv2+mgy ……. (2)

where m is the mass of the molecule, V is its speed, and Y is its position.

Using eq. (2), the total energy of an air molecule located at the floor must be:

Ey=0=12mv2.

For an air molecule at a height y=3m, the total energy is:

Ey=3m=12mv2+3mg.

04

Ratio of the probability of finding an air molecule

The ratio of the probability of finding an air molecule at the height to that of another air molecule at the floor with the same speed is

Py=3mPy=0=Ae-12mv2+3mg/kBTAe-12mv2/kBT=e-12mv2+3mg-12mv2/kBT=e-3mg/kBT=e-35.6×10-26(9.8)/1.38×10-28(300)=0.9996.

05

Calculate relative difference in percentage

To find the relative difference in percentage, we subtract the above value from 1 and multiply by ,100% we get:

percent difference=(1-0.9996)×100%=0.04%

Hence, the percentage of the relative difference between the probability of finding an air molecule at height y=3mto that of another air molecule with the same speed at the floor is roughly 0.04%.

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Most popular questions from this chapter

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.

Derivation of equation(940): Our model for calculatingE¯is equation (9-26), whose denominator is the total number of particlesNand whose numerator is the total energy of the system, which we here callUtotal. State with the denominator:

N=0N(E)(E)dE

Insert the quantum gas density of states and an expression for the distribution. using±to distinguish the Bose-Einstein from the Fermi-Dirac. Then change variables:E=y2, and factorBe+r2/kUTout of the denominator. In the integrand will be a factor

(11Bey2/kBT)1

Using,(lε)11±ε a sum of two integrals results, each of Gaussian form. The integral thus becomes two terms in powers of1/B. Repeat the process. but instead find an expression forUtotalin terms of1/B, using

U|ntal=0EN(E)D(E)dE

Divide your expression forUtotalby that forN. both in terms of1/B. Now1/Bcan safely be eliminated by using the lowest-order expression forNin terms of1/B.

A two-sided room contains six particles, a, b, c, d, e and f, with two on the left and four on the right.

(a) Describe the macrostate.

(b) Identify the possible microstates. (Note: With only six particles, this isn't a thermodynamic system, but the general idea still applies, and the number of combinations is tractable.)

Obtain equation (9- 15) from (9-14). Make use or the following sums, correct when |x|<1 :

n=0xn=11-xn=0nxn=x(1-x)2

Exercise 52 gives the Boltzmann distribution for the special case of simple harmonic oscillators, expressed in terms of the constantε, Nω0/(2s+1)and Exercise 53 gives the two quantum distributions in that case. Show that both quantum distributions converge to the Boltzmann in the limitkBT.

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