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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=m2Ï€kT324Ï€v2e-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=4πm2πkT32∫0300v2e-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/s≈0.71

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

role="math" localid="1646974577626" P=4πm2πkT322kTm32∫00.71x2e-x2dx=4π∫00.71x2e-x2dx≈0.20

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Most popular questions from this chapter

Derive equation 6.92 and 6.93 for the entropy and chemical potential of an ideal gas.

In this problem you will investigate the behavior of ordinary hydrogen, H2, at low temperatures. The constant εis0.0076eV. As noted in the text, only half of the terms in the rotational partition function, equation6.3, contribute for any given molecule. More precisely, the set of allowed jvalues is determined by the spin configuration of the two atomic nuclei. There are four independent spin configurations, classified as a single "singlet" state and three "triplet" states. The time required for a molecule to convert between the singlet and triplet configurations is ordinarily quite long, so the properties of the two types of molecules can be studied independently. The singlet molecules are known as parahydrogen while the triplet molecules are known as orthohydrogen.

(a) For parahydrogen, only the rotational states with even values of j are allowed.Use a computer (as in Problem6.28) to calculate the rotational partition function, average energy, and heat capacity of a parahydrogen molecule. Plot the heat capacity as a function of kT/t

(b) For orthohydrogen, only the rotational states with odd values of jare allowed. Repeat part (a) for orthohydrogen.

(c) At high temperature, where the number of accessible even-j states is essentially the same as the number of accessible odd-j states, a sample of hydrogen gas will ordinarily consist of a mixture of 1/4parahydrogen and 3/4orthohydrogen. A mixture with these proportions is called normal hydrogen. Suppose that normal hydrogen is cooled to low temperature without allowing the spin configurations of the molecules to change. Plot the rotational heat capacity of this mixture as a function of temperature. At what temperature does the rotational heat capacity fall to half its hightemperature value (i.e., to k/2per molecule)?

(d) Suppose now that some hydrogen is cooled in the presence of a catalyst that allows the nuclear spins to frequently change alignment. In this case all terms in the original partition function are allowed, but the odd-j terms should be counted three times each because of the nuclear spin degeneracy. Calculate the rotational partition function, average energy, and heat capacity of this system, and plot the heat capacity as a function of kT/t.

(e) A deuterium molecule, D2, has nine independent nuclear spin configurations, of which six are "symmetric" and three are "antisymmetric." The rule for nomenclature is that the variety with more independent states gets called "ortho-," while the other gets called "para-." For orthodeuterium only even-j rotational states are allowed, while for paradeuterium only oddj states are allowed. Suppose, then, that a sample of D2gas, consisting of a normal equilibrium mixture of 2/3ortho and 1/3para, is cooled without allowing the nuclear spin configurations to change. Calculate and plot the rotational heat capacity of this system as a function of temperature.*

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?

Show explicitly from the results of this section thatG=Nμfor an ideal gas.

Consider a hypothetical atom that has just two states: a ground state with energy zero and an excited state with energy 2 eV. Draw a graph of the partition function for this system as a function of temperature, and evaluate the partition function numerically at T = 300 K, 3000 K, 30,000 K, and 300,000 K.

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