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Interdiffusion of Sn and Pb in Liquid Pb-Sn Alloys

机译:液态Pb-Sn合金中Sn和Pb的相互扩散

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Coefficients for the interdiffusion of Sn in Pb-richalloys and Pb in Sn-rich alloys were established using 1.5-mm-diameter capillaries and the semi-infinite rod technique.Interdiffusion coefficients are presented for the entireconcentration range from pure Pb to pure Sn, for temperaturesfrom 668 to 1031 K. The concentration dependence of theinterdiffusion coefficients was determined by establishing theconcentration along the length of the capillaries and calculatingthe coefficients using a finite-difference technique. Theinterdiffusion of Sn in Pb, extrapolated to 0 at. pct Sn, is given byD valence 8.8 X 10~(-8) exp - (22, 600/RT) m~2/sand that for Pb in Sn, extrapolated to 0 at. pct Pb, byD valence 2.4 X l0~(-8) exp - (19, 300/RT) m~2/sThe "average" value for the interdiffusion of Sn in Pb, for theconcentration range from 0 to 74 at. pct Sn, is given byD valence 1.1 X 10~ (-7) exp - (25, 200/RT) m~2/sand the average value for the interdiffusion of Pb in Sn, for theconcentration range from 0 to 26 at. pct Pb, is given byD valence 1.3 X 10~ (-8)exp - (22, 600/RT) m~2/sThe values obtained for the coefficients agree reasonably wellwith previous results for the diffusion of Sn in Pb-rich alloysand are consistent with solvent self-diffusion coefficients forpure Pb and pure Sn. However, while the diffusion coefficientsobtained from these Arrhenius equations are likely of the rightorder of magnitude, it is concluded that the results are affectedby fluid flow in the capillaries, resulting in higher than actualactivation energies. It is suggested that, for the capillary-reservoir technique, convective flow in the reservoir across theopen end of the capillaries induces "lid-driven" flow in theupper portions of the capillaries, resulting in higher than actualdiffusion coefficients, particularly for the Sn-rich alloys, sincethe Sn-rich end of the capillaries was open to the reservoir.Because of fluid motion induced in the capillaries, all of theresults for solute and self-diffusion in Pb, both present andprevious, are likely erroneous because they were obtained usingthe capillary-reservoir technique.Some previous results for solvent self-diffusion in liquid Snwere obtained using either the thin disk or the semi-infinite rodtechnique and, since these results agree with results obtained inmicrogravity, it is concluded that the nonreservoir methods mayprovide a means of obtaining more accurate liquid diffusion data.
机译:利用直径为1.5 mm的毛细管和半无限杆技术,建立了富铅合金中锡和富锡合金中铅的相互扩散系数,并给出了从纯铅到纯锡的整个浓度范围的扩散系数。扩散系数的浓度依赖性是通过建立沿毛细管长度的浓度并使用有限差分技术计算该系数来确定的。 Sn在Pb中的相互扩散,外推至0 at。 pct Sn由D价8.8 X 10〜(-8)exp-(22,600 / RT)m〜2 / s给出,而Sn中Pb的外推为0 at。 pct Pb,按D价2.4 X l0〜(-8)exp-(19,300 / RT)m〜2 / s锡在Pb中相互扩散的“平均值”值,浓度范围为0至74 at。 pct Sn由D价1.1 X 10〜(-7)exp-(25,200 / RT)m〜2 / s给出,Pb在Sn中扩散的平均值为0至26 at。 pct Pb由D价1.3 X 10〜(-8)exp-(22,600 / RT)m〜2 / s给出。系数值与先前关于Sn在富Pb合金中扩散的结果相当吻合,并且与纯Pb和纯Sn的溶剂自扩散系数一致。然而,尽管从这些Arrhenius方程获得的扩散系数可能处于正确的数量级,但可以得出结论,结果受到毛细管中流体流动的影响,导致活化能高于实际。建议对于毛细管储层技术,储层中穿过毛细管开放端的对流在毛细血管的上部引起“滑动驱动”流,导致扩散系数高于实际扩散系数,尤其是富锡的扩散系数。合金,因为毛细管中富锡的末端向储层开放。由于毛细管中引起的流体运动,Pb中的溶质和自扩散的所有结果(现在和以前)都可能是错误的,因为它们是通过毛细管获得的以前使用薄盘法或半无限杆技术获得了液体Snwe中溶剂自扩散的一些结果,由于这些结果与在微重力下获得的结果相符,因此得出结论,非储层方法可以提供一种获得水的方法。更准确的液体扩散数据。

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