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Experimental Physics II - Molecular-kinetic theory of gases 19 The Maxwell distribution of speeds x v y v z v dx dy dz dv 2 4 ) ( ) ( v v f v F p × = ! () þ ý ü î í ì - ÷ ø ö ç è æ = kT mv v kT m v F 2 exp 2 4 2 2 2 / 3 p p 0 500 1000 1500 2000 2500 3000 0.0 2.0x10 -4 4.0x10 -4 6.0x10 -4 8.0x10 -4 1.0x10 -3 1.2x10 -3 hydrogen probability density velocity v (m/s) oxygen v m <v> v rms The most probable speed: 0 ) ( = dv v dF m kT v m 2 = The average speed: m kT v p 8 = ò = dv v vF v ) ( m kT v rms 3 = The rms speed: kT v m 2 3 2 2 1 =

The Maxwell distribution of speeds · Ø The Maxwell velocity distribution gives the fraction of molecules having certain velocities. Ø There are distributions for velocity components,

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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 4a - Molecular-kinetic theory of gases 23

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!