one and a half century of diffusion fick, einstein before...

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One and a Half Century of Diffusion FICK, EINSTEIN before and beyond Jean Philibert Diffusion Fundamentals I, Leipzig September 2005

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One and a Half Century of Diffusion

FICK, EINSTEINbefore and beyond

Jean Philibert

Diffusion Fundamentals I, Leipzig September 2005

Some MILESTONES

• Thomas Graham A Scottish Chemist

1830 (gas) 1863 (liquids)• Adolf Fick 1855 A German Physiologist

• Josef Stefan 1879 An Austrian Physicist

• W.C. Roberts-Austen 1896 An English Metallurgist

• G. Von Hevesy 1920 A Hungarian Physicist

Random Walk

• Robert Brown 1828• J.C. Maxwell 1867• Albert Einstein 1905• Maryan Smoluchowski 1906• Jean Perrin 1912• J. Bardeen , C. Herring 1950

Temperature dependence

• Svante Arrhenius 1889• Henry Eyring 1935 / 1941• C. Wert, C. Zener 1949• G.H. Vineyard 1957

Fruitful as the miscibility of the gases has been an interestingspeculation,the experimental information we possess on the subject amounts to little more than the well established fact,that gases of different nature, when brought into contact, do not arrange themselves according to their density, ….but they spontaneouly diffuse, mutually and equally,through each otherand so remain in the intimate state of mixture for any length of time.

Thomas Graham, 1829

Adolf FICK1829-1901

Fick’s experimental Set-up

Fick’s results (tube)

1

1.05

1.1

1.15

1.2

specific gravity

0 50 100 150 200 250depth under surface (mm)

FICK ( cylindrical tube)

y = 1.0045 + 0.00088321x R= 0.99908

FICK / funnel

d2cdx 2 = −

d ln Adx

dcdx

Cone :d2cdx 2 = −

2x + dO

dcdx

c(x)csat

=dO

d − dO

−1+d

x + dO

⎣ ⎢

⎦ ⎥

Fick’s results (funnel)250 mm is a guess for the position of the cone apex

-0.02

0

0.02

0.04

0.06

0.08

0.1

0.12

Specific gravity(-1)

0.004 0.005 0.006 0.007 0.008 0.009 0.01 0.011(250-depth) -1 ( mm -1 )

Fick (funnel)

y = -0.078707 + 17.248x R= 0.99922

Fick revisited• Theory and Simulation of Fick’s historical

verification of the 2nd LawM.E. Glicksman, R. DiDomizio, A. Lupulescu

This Conference

• Fick’s Diffusion Experiments revisitedT.W. Patzak, unpublished, available at

http://petroleum.berkeley.edu/papers/patzek/Fick%20Revisited%20V2.pdf

Joseph Fourier1768-1830

• . Josef STEFAN

1836-1893

Is solid state diffusion possible ?

Corpora non agunt nisi solutaGay-Lussac, 1846

However, diffusion in solids has been used for centuries in many metallurgical processes : e.g. cementation described by the Roman author PLINY.

W.C. ROBERTS-AUSTEN

Chemist and essayer, The Mint, London

Bakerian Lecture on the Diffusion in Metals1) Diffusion of molten Metals2) Diffusion of solid Metals

London, 1896

“To make accurate experiments on diffusion is one of the most difficult problems in practical physics”Ostwald, 1891“My long connection with Graham’s researches made it almost a duty to attempt to extend is work on liquide diffusiontometals…”Roberts-Austen, 1896

W. C. ROBERTS-AUSTEN

Diffusion of Gold In Lead

The evidence gathered by the metallurgist of active atomicmovements in fluid and solid metals sustain hope of the Physiologist that …

he will ultimately be able to measure theatomic movements upon which vitalityand thought depend.

Roberts-Austen

• Robert BROWN1773-1858

Robert Brown

Havingfound motion in the particles of the pollenof allthe living plants which Ihad examined, I was led next to inquire whether this property continued after thedeath of the plant, and for what length of time it was retained In plants, eitherdried or immersed in spirit for a few days only, the particles of pollen of bothkinds were found in motion equally evident with that observed in the living plant; specimens of several plants, some of which had been dried and preserved in anherbarium for upwards of twenty years, and others not less than a century, stillexhibited the molecules or. smaller spherical particles in considerable numbers,and in evident motion,…

Albert EINSTEIN1879-1955

Drunkard’s walkfrom G. GAMOW

Jean PERRIN1870-1942

Fractal trajectory D =2Si on faisait des pointés à

des intervalles de temps 100 fois plus rapprochés, chaque segment seraitremplacé par un contour polygonal relativementaussi compliqué que le dessin entier, et ainsi de suite. On voit comment s’évanouit … la notion de trajectoire.

Jean Perrin

György HEVESY1885-1966

1920: natural radioactive Lead

Pb*/PbCl2

1935: artificial 32P