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

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. block has a cavity inside, occupied by a photon gas. Briefly explain what the characteristic of this gas should have to do with the temperature of the block.

Using density of states D(E)=(2s+1)0, which generalizes equation (9-27) to account for multiple allowed spin states (see Exercise 52), the definition Nhω0/(2s+1)=εand N=0N(E)D(E)dE. Solve for Bin distributions (9-32) and (9-33) careful use of ±will cut your work by about half. Then plug back in and show that for a system of simple harmonic oscillators, the distributions become γ(E)BE=1eE/kBT1eδ/kBT1andN(E)FD=1eE/kBTe+δ/kBT1+1.

You will need the following integral:0(Be2±1)1dz=±ln(1±1B).

Determine the relative probability of a gas molecule being within a small range of speeds around 2vrmsto being in the same range of speeds around vrms.

We based the exact probabilities of equation (9-9) on the claim that the number of ways of addingN distinct nonnegative integer quantum numbers to give a total ofM is{M+N-1)!/M!(N-1)!. Verify this claim (a) for the caseN=2,M=5and(b)for the case.

N=5,M=2

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