Diffusion - Thermal Physics - Assignment 5 | PHYS 213, Assignments of Physics

Material Type: Assignment; Class: Univ Physics: Thermal Physics; Subject: Physics; University: University of Illinois - Urbana-Champaign; Term: Fall 2008;

Typology: Assignments

Pre 2010

Uploaded on 03/13/2009

koofers-user-ira
koofers-user-ira 🇺🇸

5

(1)

10 documents

1 / 2

Toggle sidebar

This page cannot be seen from the preview

Don't miss anything!

bg1
Physics 213 Problem 5 Week 3
Diffusion
1. A few atoms of Argon (atomic weight = 40) are released from a storage tank into a room full
of air at 300 K. Assume that the Ar atoms have an average energy of (3/2)kT and a mean free
path of 0.1 micrometer. Determine the diffusion constant of the Ar gas and the average radial
displacement of the atoms from their point of origin at 1 second and at 1 hour after their release.
Plot a few points of rav(t) to get a feeling for the t1/2 function.
The Ar atoms have mass m = 0.040 kg/6.022x1023 = 6.64 x 10-26 kg,
v = (3kT/m)1/2 = (3 x 1.38 x 10-23 x 300/6.64 x 10-26) = 432.6 m/s
= 0.1 µm = 10-7 m
D = v / 3 = (433 m/s )(10-7)/3 = 1.44 x 10-5 m2/s
Diffusion distance in 1 sec = (6Dt)1/2 = (6 x 1.44 x 10-5 x )1/2 = 0.93 cm
Diffusion distance in 3600 sec = 0.93 cm x (3600)1/2 = 56 cm
2. Now calculate the average displacement in the x-direction at 1 second and 1 hour.
This basically the same problem, realizing that <r2> = <x2> + <y2> + <z2> 3<x2>
Therefore, <x2> = <r2>/3 xrms = rrms/3.
xrms(1 s) = 0.93 cm/3 = 0.54 cm
xrms(3600 s) = 56 cm/3 = 32.3 cm
Note: You can get the same results by using the formula <x2> = 2Dt.
rav(cm)
0 1 2 3 4 5 6 t (s)
2.5
2.0
1.5
1.0
0.5
0.0
pf2

Partial preview of the text

Download Diffusion - Thermal Physics - Assignment 5 | PHYS 213 and more Assignments Physics in PDF only on Docsity!

Physics 213 Problem 5 Week 3 Diffusion

  1. A few atoms of Argon (atomic weight = 40) are released from a storage tank into a room full of air at 300 K. Assume that the Ar atoms have an average energy of (3/2)kT and a mean free path of 0.1 micrometer. Determine the diffusion constant of the Ar gas and the average radial displacement of the atoms from their point of origin at 1 second and at 1 hour after their release. Plot a few points of rav(t) to get a feeling for the t 1/ function. The Ar atoms have mass m = 0 .040 kg/6.022x 23 = 6.64 x 10 - 26 kg, v = (3kT/m)1/2^ = (3 x 1.38 x 10-^23 x 300/6.64 x 10-^26 ) = 432.6 m/s

 = 0.1 μm = 10

  • 7 m

D = v  / 3 = (433 m/s )(10-^7 )/3 = 1.44 x 10-^5 m^2 /s

Diffusion distance in 1 sec = (6Dt)1/2^ = (6 x 1.44 x 10-^5 x )1/2^ = 0.93 cm

Diffusion distance in 3600 sec = 0.93 cm x (3600) 1/ = 56 cm

  1. Now calculate the average displacement in the x-direction at 1 second and 1 hour. This basically the same problem, realizing that <r 2 > = <x 2 > + <y 2 > + <z 2 > ≈ 3<x 2 > Therefore, <x 2 > = <r 2 >/3  xrms = rrms/√3. xrms(1 s) = 0.93 cm/√3 = 0.54 cm xrms(3600 s) = 56 cm/√3 = 32.3 cm Note: You can get the same results by using the formula <x^2 > = 2Dt.

rav(cm)

0 1 2 3 4 5 6 t (s)

  1. Note that we’ve treated these gas atoms as ideal, i.e., there’s nothing attracting them to or repelling them from one another. Why do they spread out? That is, why do they move outward on average instead of inward or sitting still? Would your answer change if we released these argon atoms into a room full of ARGON instead of air? If we counted the states of the Argon in air and compared to Argon in Argon, do we get the same answers? Ask your other group members and see if you come to a consensus. The argon atoms spread out because the more volume they fill, the more arrangements are possible. The most likely configuration is to have all the gas molecules spread evenly (on average) around the entire room. We’re watching the system approach that configuration. As for releasing argon into a room full of argon, we lose track of our particular argon atoms (they’re indistinguishable from the ones in the room). Since we can’t tell them from the ones in the room, all that we could see would be a higher density of argon atoms near the container. Over time, this high density “blob” would smear out and the pressure in the room would be slightly increased. The strange thing is, we would count LESS possible states in this case, since our molecules are indistinguishable from those already in the room. Getting more entropy from mixing different gases is something that used to puzzle folks working on thermodynamics before we know to count states—it’s called “entropy of mixing”.