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Experimental Physics II - Molecular-kinetic theory of gases 19
The Maxwell distribution of speeds
xv
yv
zv
dxdydz
dv
24)()( vvfvF p×=!
( )þýü
îíì-÷
øö
çèæ=
kTmvv
kTmvF
2exp
24
22
2/3
pp
0 500 1000 1500 2000 2500 30000.0
2.0x10-4
4.0x10-4
6.0x10-4
8.0x10-4
1.0x10-3
1.2x10-3
hydrogen
prob
abilit
y de
nsity
velocity v (m/s)
oxygen
vm <v>vrms
The most probable speed:
0)(=
dvvdF m
kTvm2
=
The average speed:
mkTvp8
=ò= dvvvFv )(
mkTvrms3
=The rms speed:
kTvm 232
21 =
Experimental Physics II - Molecular-kinetic theory of gases 20
Experimental verification of Maxwell distribution
Classical experiments by Stern
Loven
metalvapor
(Disadvantage: detects simultaneously multiple velocities)
v
phase is shifted
Experimental Physics II - Molecular-kinetic theory of gases 24
Boltzmann distribution
2
31 vmnP =
0P
P
A
dh
2000 3
1 vmnP = kTvmvm 3220 ==
( ) AdhhPhPghM ×+-= )()()(
( )kTAdhhnhn )()( +-=
mAdhhnhM )()( »
kTmgdh
ndn
-= òò -=1
0
1
0
h
h
n
n kTmgdh
ndn
dhdhhdnhndhhn )()()( +»+
dhdhhdnkTA )(
-=
þýü
îíì D-=kThmgnn exp01
þýü
îíì-=
kTE
nn potentialexp01
Boltzmann distribution
vdkTEndn total 3
0 expþýü
îíì-=
Maxwell-Boltzmann distribution
Experimental Physics 4a - Molecular-kinetic theory of gases 25
At equilibrium, each elementary process should be equilibrated by its reverse process.
A
yv
yv'
v!
Boltzmann distribution: detailed balance
Two ensembles withequal total energies:
Experimental Physics 4a - Molecular-kinetic theory of gases 26
Avogadro’s number
Jean Baptiste Perrin3 2 0 3 2 2 5 3 1 2
3 1 1 0 3 3 4 3 4 4
0 3 1 3 1 4 2 2 1 3
1 1 2 2 3 0 1 3 4 3
0 2 2 1 0 2 1 3 2 4
2 1 0 0 1 1 3 1 0 0
0 2 0 0 0 0 1 2 2 0
2 1 3 3 1 0 0 0 3 0
1 0 2 1 0 0 1 0 1 0
1 1 0 2 4 1 0 1 0 1
Some thousands of readingsare required if some degree ofaccuracy is aimed at. To takean example, I have copiedbelow the numbers given by 50consecutive readings at twolevels 30 μ apart in one of theemulsions I have used:
Lower end Upper end
Annales de Chimie et de Physique 18, 1-114 (1909)
30 µm
The gamboge, which is used for a water-colour, comes from the desiccation of the latex secreted by Garcinia morella (guttier of Indo-China).
R = 0.212 µmrc = 1.207 g/cm3
rl = 1.0 g/cm3
T = 20°C n1/n2 = 2.08
þýü
îíì --=
kTgzmmnn lc )(exp0
)/ln(3))((4
21
123
nnTgzzRk lc --
-=rrp
The mean radius of the granules of the emulsion employed was found equal to 0.212 μm, by counting 11,000granules of a titrated emulsion, and to 0.213 μm by application of the law of Stokes. The difference of densitybetween the material of the granules and the inter-granular water was 0.2067 at 20°, the temperature to whichthe measurements refer.
J/K1013.1 23-´=
Experimental Physics II - Molecular-kinetic theory of gases 27
Ø The Maxwell velocity distribution gives the fraction
of molecules having certain velocities.
Ø There are distributions for velocity components,
for velocities and for molecular speeds.
Ø Due to occurrence of such distributions,
one may introduce different average
quantities.
ØThe Boltzmann distribution describes
variation of particle densities in an external
conservative potential field.
To remember!