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Diffusion near dislocations, dislocation arrays and tensile cracks

โœ Scribed by Brotzen, F.R.; Seeger, A.


Publisher
Elsevier Science
Year
1989
Weight
731 KB
Volume
37
Category
Article
ISSN
0001-6160

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โœฆ Synopsis


Equations are developed for approximating the flow rate of mobile solutes and other point imperfections across a cylindrical surface of arbitrary radius r surrounding stationary defects such as straight edge dislocations, sharp tensile cracks and edge-dislocation pileups embedded in an infinite solid. The starting point for the calculations is Fick's generalized law which takes into account the interaction potential between the stress field of the stationary defect and the diffusing solute as well as the solute-concentration gradient. It is assumed that the initial solute concentration, c(time = 0), is uniform everywhere and that c(r = 0) = 0 for time > 0. The degree of accuracy of the approximations used in this analysis is discussed in detail. Comparisons of the calculated results with experimental data are very satisfactory.

R&un&--Nous avons diveloppt des equations pour realiser une approximations de la vitesse d'tcoulement des solutes mobiles et d'autres imperfections ponctuelles a travers une surface cylindrique, de rayon arbitraire r, entourant des defauts stationnaires tels que les dislocations coin rectilignes, les fissures de traction effilees et les empilements de dislocations coin contenus dans un solide infini. Le point de depart des calculs est la loi de Fick generaliste qui tient compte du potentiel d'interaction entre le champ de contrainte du defaut stationnaire et le solute qui diffuse, aisi que du gradient de concentration en solute. On suppose que la concentration initiale en solute, c (pour t = 0), est uniforme partout et que c(r = 0) = 0 pour t > 0. Nous discutons en detail la precision des approximations utilisees dans cette analyse. La comparaison entre les resultats calculbs et exptrimentaux est t&s satisfaisante. Zusamrnenfassung-Gleichungen werden entwickelt, urn den FluI beweglicher Losungsatome und anderer atomarer Fehlstellen durch eine zylindrische Oberflache mit beliebigem Radius r angeniihert zu beschreiben, Der Zylinder umgibt stationare Fehlstellen wie gerade Stufenversetzungen, scharf definierte Risse, erzeugt durch Zugbelastung, und Aufstauungen von Stufenversetzungen, die alle in einem unendlich grol3en .Festkdrper eingebettet sind. Ausgangspunkt der Rechnungen ist das verallgemeinerte Ficksche Gesetz, welches das Wechselwirkungspotential zwischen dem Spannungsfeld der stationiiren Fehlstelle mit der diffundierenden atomaren Fehlstelle und den Konzentrationsgradienten der atomaren Fehlstellen beriicksichtigt. Angenommen wird, dag die Anfangskonzentration der atomaren Fehlstellen, c (Zeit = 0), tiberall gleich ist und daB c(r = 0) = 0 fiir Zeiten r > 0 ist. Die Genauigkeit der in dieser Analyse benutzten Nlherungen wird ausfilhrlich diskutiert. Vergleiche der Rechnungen mit experimentellen Ergebnissen fallen zu voller Zufriedenheit aus.


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