Plan for Mon, 13 Oct 08 • Exp 2 post-lab question • Lecture – KMT (5.6) – Effusion and Diffusion (5.7) – Real gases and the van der Waal equation (5.8) – The nature of energy?? (6.1) • Quiz 2 returned
Plan for Mon, 13 Oct 08
• Exp 2 post-lab question
• Lecture– KMT (5.6)– Effusion and Diffusion (5.7)– Real gases and the van der Waal equation (5.8)– The nature of energy?? (6.1)
• Quiz 2 returned
What can KMT do for you?• The main ideas you should take from KMT is
that we can describe T and P from a molecular perspective.
• Pressure: arises from molecules banging into the container walls.
• Temperature: arises from the kinetic energy of the gas molecules. The more KE they have, the faster they can move around, the “hotter” they are.
Temperature according to KMT
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Kinetic energy: The energy an object has by virtue of its motion.
Basically, the energy you must apply to an object to accelerate it from rest to a given velocity (u):
221 muEk
The average Ek of a molecule is directly proportional to the absolute temperature in K.
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Dr. Villarba subs. QUIZ 5
Dr. Schultz subs in lab
EXAM 2: Ch 5,6,10
Metathesis Lab (Exp3)
QUIZ 4
Vol. Anal. FORMAL RPT (Exp4)
We are here. QUIZ 3
A Closer Look at Molecular KE• Let’s consider the average KE per molecule and
see how it determines molecular speed.
3
2RTTotal KE in a mole of gas:
21
2muAverage KE per molecule:
According to KMT, and beyond the scope of this course.
Where u is an average of molecular velocity, and m is the mass of one molecule.
21 1 3
2 2A
mu RTN
We are apportioning the total KE in the mole of gas among all the molecules in an average fashion.
A Closer Look at Molecular KE
21 1 3
2 2A
mu RTN
We are apportioning the total KE in the mole of gas among all the molecules in an average fashion.
2 3
A
RTu
mN Note that mNA = M.
3rms
RTu
M
“Root-mean-square” speed, one kind of average molecular speed.
urms is the speed of a molecule that
has the average KE.
urms gives us a formal connection
between average gas speed, T, and M.
Distribution of Molecular Speeds
Petrucci, Fig 6.17
“Maxwell-Boltzmann” curve (a statistical distribution)
um – most probable speed
uav – average speed
urms – the speed of a molecule with the average molecular kinetic energy
urms Dependence on T & M
Petrucci, Fig. 6.18
E&G, Fig. 5.25M(O2) = 32 g/mol
M(H2) = 2 g/mol
M
RTurms
3
Trends
• Increased T increased average KE increased urms
– Maximum of curve shifts to higher u, and distribution spreads out.
• Increased M decreased urms
– Heavier molecules have lower average speed than lighter molecules.
• At a given T, are there more molecules at low speeds (u < urms) or high speeds (u > urms)? – There are more molecules at lower speeds than high.
M
RTurms
3
Calculating urms
• What is urms at 25oC for He(g) and N2(g)?
M(He) = 4.003 g/mol
M(N2) = 28.01 g/mol
• Already we know that urms(N2) < urms(He).• We also need T and R. What units do we need
for these values?
M
RTurms
3
Calculating urms
• What is urms at 25oC for He(g) and N2(g)?
M(He) = 4.003 g/mol
M(N2) = 28.01 g/molT = (25oC + 273) K = 298 K
• urms is in units of m/s• Will 0.08206 L atm/mol K work?• How about 8.314 J/mol K?
M
RTurms
3
Calculating urms
• How about 8.314 J/mol K?
• What’s a J (joule)?
1 J = 1 N m
• What’s a N (newton)?
1 N = 1 kg m/s2
1 J = 1 kg m2/s2
M
RTurms
3
Calculating urms for He(g)M(He) = 4.003 g/mol
T = 298 K
R = 8.314 J/mol K = 8.314 kg m2/mol K s2
M
RTurms
3
2
2
kg m3 8.314 298 K
mol K s
g 1 kg4.003
mol 1000 g
31.36 10 m/s
Calculating urms for N2(g)M(N2) = 28.01 g/mol
T = 298 K
R = 8.314 J/mol K = 8.314 kg m2/mol K s2
M
RTurms
3
2
2
kg m3 8.314 298 K
mol K s
g 1 kg28.01
mol 1000 g
515 m/s
Comparison• At 25oC,
urms(N2) = 515 m/s M(N2) = 28 g/molurms(He) = 1.36 x 103 m/s M(He) = 4 g/mol
• A car travelling at 60 mph,
ucar = 26.8 m/s
If gases travel so fast, why does it take so long for you to smell a bottle of perfume from
across the room?
Diffusion• Gas molecules travel in a
straight line only until they collide with a container wall or another gas molecule.
• Gaseous perfume molecules do not have an uninterrupted path in from of them.
• They are constantly colliding with gas molecules in the air.
Diffusion
Show Z Fig 5.24 p. 207
Diffusion is the process of mixing gases.
This is analogous to solution formation.
Diffusion of gases
In a closed container, diffusion will eventually lead to a homogeneous mixture.
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Effusion
Petrucci, Fig 6.21b
Effusion is a special case of diffusion, which exploits the difference in velocities of lighter gas molecules.
This process was used during the Manhatten Project to separate 235U and 238U isotopes.
Effusion of a Gas
Rate of effusion is proportional to urms. So lighter particles will have a higher rate of effusion.
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Real Gases
• Generally speaking, there is no such thing as an “Ideal Gas.”
• There are conditions under which a gas will behave ideally…– low P – moderate to high T
• van der Waal developed some corrections to the Ideal Gas law, based on a molecular picture, to explain these observed deviations.
Real Gases: Molecules have volume
• At high P, the volume of the individual gas molecules becomes non-negligible.
• Macroscopic gas is compressible, individual gas molecules are not.
• Under high P conditions, the space available for a gas molecule to move through is decreased by its neighbors, so the volume of the system is reduced relative to the ideal case.
Volume correction
• vdW corrected the volume available to a gas:
• P’ is a “corrected” ideal pressure. • What is the result of this volume correction, a
higher or lower pressure relative to ideal?
V V nb nRTP
V nb
Number of moles of gas
Empirical constant… different for each gas
Real Gases: Molecules attract each other• Under high P, gas molecules
get very close to each other, so intermolecular forces become significant.
• At low T, molecular Ek is reduced, and molecular speed drops, so the molecules become “trapped” by attractions to other molecules.
• Under these conditions, the molecules don’t collide with the container as frequently, so the pressure of the system is reduced relative to the ideal case.
Pressure Correction• vdW corrected for pressure, by including a mutual
attraction term.• Molecular attractions are proportional to concentration,
n/V.
• What is the result of the pressure correction?
2n
P P aV
Intermolecular
attraction termEmpirical constant… different for each gas
vdW Equation
• b generally increases with the size of the molecule• a seems to depend on the strength of intermolecular
forces.
2
obs
nP P a
V
2
obs
nRT nP a
V nb V
2
obs
nP a V nb nRT
V
vdW Equation
vdW equation corrects two major flaws in ideal gas theory:
• Gas molecules have finite volume which becomes important at high P.
• Gas molecules have nontrivial attractions that become important at low T and high P.
2
obs
nP a V nb nRT
V