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Use the Sackur-Tetrode equation to calculate the entropy of a mole of argon gas at room temperature and atmospheric pressure. Why is the entropy greater than that of a mole of helium under the same conditions?

Short Answer

Expert verified

The room temerperature and atmospheric pressure entropy of mole of argon gas isS=154.76JK1.

Step by step solution

01

Step: 1 Finding volume of one mole:

The entropy of sackur-tetrode formula by

S=NklnVN4mπU3Nh232+52

From ideal gas law,

At pressure of 1atm=101325Paand temperature of 300K.

The one mole occupies a volume of

V=nRTPV=8.31×300101325V=0.0246m3.

02

Step: 2 Finding Argon molecule mass:

The monatomic gas of internal energy is

U=f2NkT

where fis the degree of freedom.

Argon is monatomic gas,so it has degree of freedom as f=3.

U=32NkTU=32nRTU=32×8.31×300U=3739.5J.

The mass of argon mole is 39.948g.So the Argon mass molecule is

m=Mass of one moleNumber of atoms one moleNAm=39.948×1036.022×1023m=6.634×1026kg.

03

Step: 3 Finding the Argon gas entropy mole:

Substituting the values as k=1.38×1023J×K1;h=6.626×1034J×s,

we get

S=Nkln0.02466.022×102346.626×1026π×3739.536.022×10236.626×1034232+52S=Nkln0.0246×2.4596×10326.022×1023+52S=Nkln(10047519)+52S=6.022×10231.38×1023[18.62]S=154.76J×K1.

Because argon has a larger mass than helium, this figure is somewhat higher.

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Most popular questions from this chapter

The mathematics of the previous problem can also be applied to a one-dimensional random walk: a journey consisting of Nsteps, all the same sic, cache chosen randomly to be cither forward or backward. (The usual mental image is that of a drunk stumbling along an alley.)

(a) Where are you most likely to find yourself, after the end of a long random walk?

(b) Suppose you take a random walk of 10,000steps (say each a yard long). About how far from your starting point would you expect to be at the end?

(c) A good example of a random walk in nature is the diffusion of a molecule through a gas; the average step length is then the mean free path, as computed in Section 1.7.Using this model, and neglecting any small numerical factors that might arise from the varying step size and the multidimensional nature of the path, estimate the expected net displacement of an air molecule (or perhaps a carbon monoxide molecule traveling through air) in one second, at room temperature and atmospheric pressure. Discuss how your estimate would differ if the clasped time or the temperature were different. Check that your estimate is consistent with the treatment of diffusion in Section1.7.

For each of the following irreversible processes, explain how you can tell that the total entropy of the universe has increased.
a Stirring salt into a pot of soup.
b Scrambling an egg.
c Humpty Dumpty having a great fall.
d A wave hitting a sand castle.
e Cutting down a tree.
fBurning gasoline in an automobile.

According to the Sackur-Tetrode equation, the entropy of a monatomic ideal gas can become negative when its temperature (and hence its energy) is sufficiently low. Of course this is absurd, so the Sackur-Tetrode equation must be invalid at very low temperatures. Suppose you start with a sample of helium at room temperature and atmospheric pressure, then lower the temperature holding the density fixed. Pretend that the helium remains a gas and does not liquefy. Below what temperature would the Sackur-Tetrode equation predict that Sis negative? (The behavior of gases at very low temperatures is the main subject of Chapter 7.)

Use the methods of this section to derive a formula, similar to equation2.21, for the multiplicity of an Einstein solid in the "low-temperature" limit,qN .

Show that during the quasistatic isothermal expansion of a monatomic ideal gas, the change in entropy is related to the heat input Qby the simple formula

s=QT

In the following chapter I'll prove that this formula is valid for any quasistatic process. Show, however, that it is not valid for the free expansion process described above.

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