At room temperature, what fraction of the nitrogen molecules in the air are moving at less than300m/s?

Short Answer

Expert verified

The required fraction is 0.20.

Step by step solution

01

Step 1. Given information

The maximum velocity of the nitrogen molecules in the air is 300m/s.300m/s

02

Step 2. Explanation

Maxwell speed distribution function is given by

Dv=m2πkT324πv2e-mv22kT.........................(1)

The formula to calculate the probability that the speed of the nitrogen molecules lies in the range of 0<v<300is given by

role="math" localid="1646974039312">P=0300m2πkT324πv2e-mv22kTdv=4πm2πkT320300v2e-mv22kTdv...................(2)

03

Step 3. Calculation

Change the variable vin equation (2) to x=vm2kT=vvmp, where vmpis the most probable speed.

Substitute 300m/sfor vand 422m/sfor vmpto calculate the upper limit for the variable role="math" x.

role="math" x=300m/s422m/s0.71

Substitute the required parameters into equation (2) and evaluate the integral.

role="math" localid="1646974577626" P=4πm2πkT322kTm3200.71x2e-x2dx=4π00.71x2e-x2dx0.20

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Most popular questions from this chapter

Although an ordinary H2 molecule consists of two identical atoms, this is not the case for the molecule HD, with one atom of deuterium (i.e., heavy hydrogen, 2H). Because of its small moment of inertia, the HD molecule has a relatively large value of ϵ:0.0057eV At approximately what temperature would you expect the rotational heat capacity of a gas of HD molecules to "freeze out," that is, to fall significantly below the constant value predicted by the equipartition theorem?

In problem 6.20 you computed the partition function for a quantum harmonic oscillator :Zh.o.=11-e-βε, where ε=hfis the spacing between energy levels.

(a) Find an expression for the Helmholtz free energy of a system of Nharmonic oscillators.

(b) Find an expression for the entropy of this system as a function of temperature. (Don't worry, the result is fairly complicated.)

Consider an ideal gas of highly relativistic particles ( such as photons or fast-moving electrons) whose energy-momentum relation is E=pcinstead of E=p22m. Assume that these particles live in a one-dimensional universe. By following the same logic as above, derive a formula for the single particle partition function,Z1, for one particle in the gas.

Consider a large system of Nindistinguishable, noninteracting molecules (perhaps an ideal gas or a dilute solution). Find an expression for the Helmholtz free energy of this system, in terms of Z1, the partition function for a single molecule. (Use Stirling's approximation to eliminate the N!.) Then use your result to find the chemical potential, again in terms ofZ1.

Consider a classical "degree of freedom" that is linear rather than quadratic E=cqfor some constant c. (As example would be the kinetic energy of a highly relativistic particle in one dimension, written in terms of its momentum.) Repeat derivation of the equipartition theorem for this system, and show that the average energy isrole="math" localid="1646903677918" E-=kT.

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