Physique Des Solides [physics] by N. Ashcroft, et. al., [FRENCH]
By N. Ashcroft, et. al., [FRENCH]
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Source : G. W. Kaye et T. H. Laby, Table of Physical and Chemical Constants, Longmans, London, 1966. libre parcours moyen jusqu’à lo3 A et plus ; ce qui est environ mille fois plus grand que la distance entre les ions. Aujourd’hui, en travaillant à des températures suffisamment basses, et en utilisant des échantillons soigneusement préparés, on peut atteindre des valeurs du libre parcours moyen de l’ordre du centimètre (c’est-à-dire los distances interatomiques). 3 ~ 11 Temps de relaxation de Drude en unités de lop" s".
6 - Valeurs expérimentales de la conductivité thermique et du nombre de Lorenz pour quelques métaux. K-2) 2,22 x 10-8 2,12 2,23 2,42 2,20 2,31 2,32 2,36 2’14 2’90 2,61 2,28 2,49 2,14 2’58 2,75 2,48 2,64 3,53 2,57 0,73 2,43 x 10-8 3’82 4,17 371 177 2,29 2,38 2,36 2,42 2,25 2,78 2,88 2,30 1,5 0,54 0,73 171 170 2,30 0,80 0,45 0760 0,35 0,08 0717 &/UT 2,19 2,60 2,75 2,54 2,53 3’35 2,69 Source : G. W. C. Kaye et T. B. Laby, Table of Physical and Chemical Constants, Longmans Green, London, 1966. 6). tures.
6). tures. Si & ( T )est l’énergie thermique par électron dans un métal à l’équilibre à une température T , alors, un électron ayant subi sa dernière collision en un point x’, aura, en moyenne, une énergie thermique € ( T [ z ’ ] )Les . électrons arrivant en J: par les hautes températures, auront subi, en moyenne, leur dernière collision au point *-~* Chapitre 1 : Théorie de Drude des métaux 26 Haute température Basse température FIG. 6 Vue schématique de la relation entre le gradient de température et le courant thermique.