Kinetic-Molecular Theory
The Physics Hypertextbook™
© 1998-2008 by Glenn Elert -- A Work in Progress
All Rights Reserved -- Fair Use Encouraged
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Discussion
Postulates
- all matter is composed of microscopic particles (molecules in general, but
also atoms, ions, and free electrons)
- molecules are very small relative to the distance between them
- molecules are in constant random (chaotic) motion
- collisions between particles are perfectly elastic
Macroscopic--Microscopic
- density is the sum of the mass of the molecules divided by the volume that
the gas occupies
- pressure is a measure of the mean linear momentum of the molecules
- temperature is a measure of the mean kinetic energy of the molecules
root mean square
[animate]
six modes of freedom
- heave
- sway
- thrust
- roll
- pitch
- yaw
degrees of freedom
- translational: radio frequencies
- rotational: microwave-infrared
- vibrational: infrared-visible-ultraviolet
- electronic: infrared-visible-ultraviolet-x ray
Photons created at the sun's center travel a distance of 2 × 1010 times the sun's radius before emerging. The trip takes something
like 30,000 years.
Summary
Problems
practice
- How about a simple, straightforward problem?
- Compute the rms speed of an oxygen molecule at room temperature.
- Use the results of part a. to determine the rms speed of a hydrogen molecule at room temperature.
- Use the results of part b. to determine the rms speed of a mercury atom at 1200 K.
Here come the solutions …
- Use the formula. Recall that oxygen is a diatomic molecule in everyday
situations. Let's not go nuts here with precision. Just use the approximate
molecular mass of oxygen (2 × 16 u = 32 u)
and the approximate value of room temperature (300 K). Let's try
calculating it both ways: first with the mass of a molecule …
| |
| vO = √ |
⎛ ⎝ |
3kT |
⎞ ⎠ |
= √ |
⎛ ⎝ |
3(1.38 × 10−23 J/K)(300 K) |
⎞ ⎠ |
= 483.5 m/s |
| m |
(32 u)(1.66 × 10−27 kg/u) |
| |
and then with the mass of a mole …
| |
| vO = √ |
⎛ ⎝ |
3RT |
⎞ ⎠ |
= √ |
⎛ ⎝ |
3(8.31 J/mol K)(300 K) |
⎞ ⎠ |
= 483.4 m/s |
| M |
(0.032 kg/mol) |
| |
The two answers are slightly different in the fourth significant digit,
but I said to be reasonable with the precision. Let's just say the answer
is …
- Exploit the simple ratio of the two molecular masses. Oxygen is 16
times heavier than hydrogen on a per atom or per molecule comparison
(since both gases are diatomic in our everyday lives). RMS speed
is inversely proportional to the square root of mass (molecular or molar).
This means the rms speed of hydrogen should be √16 = 4
times faster. If you would like to see the mathematical reasoning presented
formally, here it is …
| vH |
|
√ |
⎛ ⎝ |
3kT |
⎞ ⎠ |
|
| = |
mH |
= √ |
⎛ ⎝ |
mO |
⎞ ⎠ |
= √ |
⎛ ⎝ |
32 u |
⎞ ⎠ |
= 4 |
| vO |
√ |
⎛ ⎝ |
3kT |
⎞ ⎠ |
mH |
2 u |
| |
mO |
|
| |
| vH = 4 vO = 4(480 m/s) = 1920 m/s |
| |
- Another question with rigged numbers. The atomic mass of mercury (200 u)
is 100 times that of molecular hydrogen (2 u). This difference reduces
the speed by 1/√100 = 1/10. In a similar vein, the temperature
of these mercury atoms is 4 times that of the hydrogen molecules in part b.
This change raises the rms speed by a factor of √4 = 2.
Combining both changes gives a new rms speed that's 2/10 of the old one.
Again, if you would like to see the mathematical reasoning presented
formally, here it is …
| vHg |
|
√ |
⎛ ⎝ |
3kTHg |
⎞ ⎠ |
|
| = |
mHg |
= √ |
⎛ ⎝ |
THgmH |
⎞ ⎠ |
= √ |
⎛ ⎝ |
(1200 K) |
(2 u) |
⎞ ⎠ |
= |
2 |
= |
1 |
| vH |
√ |
⎛ ⎝ |
3kTH |
⎞ ⎠ |
THmHg |
(300 K) |
(200 u) |
10 |
5 |
| |
mH |
|
| |
| vHg = ⅕ vH = 0.2(1920 m/s) = 384 m/s |
| |
- Write something else.
- Write something different.
- Derive the law of Dulong and Petit by applying the equipartition of energy to the atoms in a solid.
Solution …
Atoms in a solid have six degrees of freedom. (Why?) Therefore, the energy
per atom is
Multiply by Avogadro's constant to get the internal energy in a mole of atoms.
Specific heat is the rate of change in internal energy with respect to
temperature. Molar specific heat is this derivative applied to the internal
energy in
one mole of atoms.
This shows that molar specific heat is a constant for all material since
Boltzmann's constant (k) and Avogadro's constant (NA) are both constant. Substitution using unusually precise values for the
two constants yields the usually stated value of this constant.
| CV = 3(1.3806503 × 10−23 J/K)(6.0221415 × 1023 atoms/mol) = 24.94 J/mol·K |
numerical
- What is the average speed of a hydrogen atom in the interplanetary medium
(the very thin, cold plasma between the planets) if it has a temperature of 16 K?
- What is the speed of a typical free electron in copper at
room temperature? (Free electrons in a metal are those which are
so loosely bound that they wander from atom to atom like the molecules in
a gas.)
- Weapons grade uranium is enriched by the diffusion of gaseous uranium
hexafluoride (UF6) through a stack of very tight metal screens. The lighter,
fissionable isotope U235 has a slightly faster rms speed and is more likely
to diffuse through the screens than the heavier, non-fissionable isotope
U238. Determine the ratio of the rms speed of UF6 made
from the light, desirable isotope to the heavier, undesirable isotope. (The
atomic mass of fluorine is approximately 19 u.)
Resources
- no resources for this topic
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