Durch elektrolytische Ionenwanderung wurde an der Grenzfläche zwischen geschmol-zenem LiCl mit 2 Molprozent KCl einerseits und geschmolzenem PbCl2 andererseits bei einer Stromdichte von 5 A/cm 2 in 48 Stdn. K stark angereichert, das Mischungsverhält-nis [ 7 Li]/[ 6 Li] von 12,3 auf. 44,3 und das Mischungsverhältnis [41K]/[39K] von 0,0714 auf 0,0885 verschoben. Als Quotienten der Ionenwanderungsgeschwindigkeiten wurden gefunden:wLi/wK =1,156, w6/w7= 1,021 und w39/w41 = 1,016. Faßt man diese Quotienten als Trennfaktoren einer Stufe auf, so bedeuten die angegebenen Anreiche-rungen eine wirksame gesamte Trennstufenzahl von 61,5 bei den Li-Isotopen und 13,4 bei den K-Isotopen. Für den Masseneffekt μ = ln (wj/wk)/ In (mj / mk), (m = Isotopen-masse), folgt μ = - 0,135 für Li und μ= - 0,32 für K. Der große Masseneffekt und die kleine Trennstufenzahl beim K kann durch dessen geringe Konzentration erklärt werden.
The 180 / 160 ratio under the m-and r-faces of smoky quartz has been measured; the ratio of the growth velocities was vm/vr = \ß. The obtained separation factor 1.00020 is compared with that obtained previously for amethyst (1.00043), where the ratio vm/vr was unity.Recently we reported on a new isotope effect [1]: During the growth of natural amethyst, Si02 with different lsO content is incorporated at crystallo graphically different faces of the crystal, the 180 / 160 ratio increasing in the order z-face, r-face, m-face. Meanwhile a similar effect in natural calcite was re ported by J. A. D. Dickson [2].Care must be taken if one wants to single out such an effect because during the hydrothermal growth of the crystal the isotope composition of the mother liquid may have varied, this leading to a corresponding iso topic layering ("mantle zoning") inside the crystal, which is superimposed on the sought for isotopic "sec tor zoning".In a polished plane-parallel slice of quartz, which is cut out from the crystal parallel to the c-axis and perpendicular to an m-face, one sees the boundary between the r-and m-sectors if during the growth impurities, which cause colouring, have been incorpo rated preferentially at one of the two faces. This was the reason why for our first study we had chosen amethyst and in the present one we deal with smoky quartz. The colours of both smoky quartz and amethyst are due to aluminium and iron impurities. If the aluminium impurity Al3 + substituting silicon exReprint requests to Prof. Dr. A. Klemm, Max-Planck-Institut für Chemie, Saarstraße 23, W-6500 Mainz, FRG. ceeds the interstitial Fe3+ impurity by a large amount, radioactivity will turn the colourless quartz to a smoky quartz. On the other hand, if the amount of interstitial Fe3+ exceeds the Al3+ impurity, the amethystine colour will appear after irradiation [3].If one chooses two points on such a visible boundary between r-and m-sectors and cuts through these points parallel to the corresponding r-and m-faces, the material between these cuts in the r-and m-sectors has grown within the same time span. In order to secure that the proportion of the amounts of material m 1 m 3 Fig. 1. The position of the samples in a slice of smoky quartz, cut parallel to the c-axis and perpendicular to the m-face. Height 6 cm, thickness 3 mm. In this case, where the average ratio of the growth velocities vr and vm was 3, sampling by scraping material from the surfaces, as was done in [2], would have given results where the isotopic mantle zoning is fully involved. Near the surface the sectorial boundary changes its direction. It would therefore have been better to exclude the corresponding layers from the samples.0932-0784 / 91 / 1200-0001 $ 01.30/0. -Please order a reprint rather than making your own copy.
The concentration of ls O within well formed crystals of amethyst was found to vary beneath the different growth faces, increasing in the order z -»• r m. The 18 0/ 16 0 fractionation factor between the faces m and z was measured as 1.0007.
Mit einem CLUSius–DiCKELschen Trennrohr, in dem zur Vermeidung von Austausch das Versuchsgas bei höchstens 230°C nur mit Glas, Quecksilber und Hahnfett Kontakt hatte, wurden die Thermodiffusionsfaktoren α von HT und DT in DEs wurde eine starke Anreicherung von HT in DDie Thermodiffusionsfaktoren in binären Gemischen von isotopen Wasserstoffmolekülen lassen sich einheitlich darstellen, wenn man α
Self-diffusion measurements on molten LiCl in the temperature range 610 °C ≦ ϑ ≦ 760 °C, obtained with a capillary-reservoir technique, result in the expressionsDD_ = [ 5.8 + 0.0117 ϑ - 610) ±0.3] × 10These results fit well into the pattern of the other alkali halides. As with these, it is observed that (D + /R T) + (D_/R T) - (Λ/F
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