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1.
采用等温溶解平衡法研究了288K时Li+,Mg2+//SO42-,B4O72--H2O四元体系的固液相平衡关系,测定了该四元体系在288K时平衡液相的溶解度和密度。依据实验测定的平衡溶解度数据及对应的平衡固相,绘制了该四元体系的平衡相图及密度组成图。研究结果表明:交互四元体系Li+,Mg2+//SO42-,B4O27--H2O288K时平衡相图中有2个共饱点,5条单变量曲线,4个结晶区对应的平衡固相分别为Li2B4O7.3H2O,Li2SO4.H2O,MgB4O7.9H2O和MgSO4.7H2O。 相似文献
2.
采用等温溶解平衡法研究了288K时Li+, Mg2+//SO2-4, B4O2-7- H2O四元体系的固液相平衡关系,测定了该四元体系在288K时平衡液相的溶解度和密度。依据实验测定的平衡溶解度数据及对应的平衡固相,绘制了该四元体系的平衡相图及密度组成图。研究结果表明：交互四元体系Li+, Mg2+//SO2-4, B4O2-7- H2O 288K时平衡相图中有2个共饱点,5条单变量曲线,4个结晶区对应的平衡固相分别为Li2B4O7·3H2O,Li2SO4·H2O,MgB4O7·9H2O和MgSO4·7H2O。 相似文献
3.
采用等温溶解平衡法开展了三元体系K+,Mg2+∥B4O72--H2O 348K的稳定相平衡研究,获得溶解度数据及平衡液相的密度,折光率,pH值。根据溶解度数据绘制了三元体系稳定相图。该三元体系在348K时的稳定相图含有一个共饱点E、两条单变量曲线AE,BE和两个结晶相区MgB4O7.9H2O(AECA)和K2B4O7·4H2O(BEDB)。共饱点的平衡固相组成为MgB4O7·9H2O和K2B4O7·4H2O,对应的平衡液相组成为w(K2B4O7)=42.28%、w(MgB4O7)=8.11%。研究结果表明,该三元体系属于简单共饱和型,无复盐和固溶体形成。K2B4O7·4H2O和MgB4O7·9H2O互相存在盐溶作用,使得这两种盐的溶解度明显增大。平衡液相的密度、折光率均随溶液中K2B4O7质量分数的增大而增大。 相似文献
4.
采用等温蒸发法研究简单四元体系Na+//CI-,CO32-,B4O72---H2O 273 K时的介稳相平衡,并测定该体系273 K平衡液相中各组分的溶解度及密度,该体系的介稳相图和密度组成图显示:该四元体系在273 K时的相图由3条溶解度单变量线、3个结晶区及1个共饱和点组成.体系属简单共饱型,无复盐或固溶体形成,3个结晶区分别对应单盐Na2CO3?10H2O,NaCI和Na2B4O7?10H2O.共饱点E处于Na2CO3?10H2O,NaCI及Na2B4O,?10H2O3盐共饱和,所对应的平衡液相组成为ω(Na2CO3)=6.81%,ω(NaCl)=21.69%,ω(Na2B4O7)=0.65%.ω(H20)=70.85%.研究体系在273 K下,Na2CO3?10H2O是碳酸钠盐的唯一析出形式,且硼酸钠对碳酸钠有盐析作用. 相似文献
5.
《矿物岩石》2008,(4)
采用等温蒸发法研究简单四元体系Na ∥Cl-,CO32-,B4O72--H2O273K时的介稳相平衡,并测定该体系273K平衡液相中各组分的溶解度及密度,该体系的介稳相图和密度组成图显示:该四元体系在273K时的相图由3条溶解度单变量线、3个结晶区及1个共饱和点组成。体系属简单共饱型,无复盐或固溶体形成,3个结晶区分别对应单盐Na2CO3·10H2O,NaCl和Na2B4O7·10H2O。共饱点E处于Na2CO3·10H2O,NaCl及Na2B4O7·10H2O3盐共饱和,所对应的平衡液相组成为w(Na2CO3)=6.81%,w(NaCl)=21.69%,w(Na2B4O7)=0.65%,w(H2O)=70.85%。研究体系在273K下,Na2CO3·10H2O是碳酸钠盐的唯一析出形式,且硼酸钠对碳酸钠有盐析作用。 相似文献
6.
7.
四元体系K_2SO_4-K_2B_4O_7-K_2CO_3-H_2O 273K时介稳相平衡研究 总被引：1，自引：1，他引：0
采用等温蒸发法研究K2SO4-K2B4O7-K2CO3-H2O四元体系在低温273K时的介稳固液相平衡关系,测定了介稳平衡液相的溶解度和密度。研究发现,该四元体系273K时的介稳平衡相图有3个固相结晶相区分别为K2SO4,K2B4O7.4H2O和K2CO3.3/2H2O;3条单变量曲线E1E,E2E和E3E;一个共饱点E,在共饱点E处的液相中各盐的溶解度分别为K2CO3(43.46%),K2SO4(2.52%)和K2B4O7(3.10%);研究结果表明K2CO3对K2B4O7和K2SO4有强烈的盐析作用。实验证明在富含硼钾的扎布耶盐湖卤水中,低温平衡条件下硫酸钾和硼酸钾极易从溶液中结晶析出,而碳酸钾则由于溶解度大,介稳性强,即使在低温条件下也难以从溶液中析出。 相似文献
8.
针对西藏扎布耶盐湖卤水组成,采用等温蒸发法分别研究了含钾四元体系Na+,K+//Cl-,B4O27--H2O308.15K、五元体系K+//Cl-,CO23-,SO42-,B4O72--H2O273.15K下的介稳相关系。分别测定了上述体系308.15K、273.15K时介稳平衡液相组成及密度、pH值。根据实验数据绘制了相应的介稳相图、水图。结果表明,本文研究的两个体系均为简单共饱型,无复盐和固溶体生成。其中,四元体系介稳相图由2个共饱点,5条单变量曲线,4个结晶区组成。平衡固相分别为Na2B4O7.10H2O、K2B4O7.4H2O、NaCl和KCl。对比四元体系308.15K和273.15K下的介稳相图发现,平衡固相盐的种类及结晶形式均没有发生变化,但结晶区大小产生变化:在308.15K下,Na2B4O7.10H2O结晶区变小,K2B4O7.4H2O结晶区变大。五元体系投影图中有1个共饱点、3条单变量曲线和3个结晶相区。结晶相区分别为K2CO3.3/2H2O、K2SO4和KCl。K2CO3.3/2H2O结晶区面积最小,K2SO4结晶区面积最大。K2CO3对KCl有较强的盐析作用。 相似文献
9.
用等温溶解平衡法研究了四元体系K+,Na+∥Clˉ,Brˉ-H2O 348 K条件下的相平衡关系,测定了该交互四元体系在相应温度条件下平衡溶液的溶解度和密度,并根据相平衡实验数据绘制了相应的相图.研究结果表明:四元体系K+,Na+∥Clˉ,Brˉ-H2O348 K条件下属于固溶体型,相图中含有1条单变量曲线,2个平衡固相结晶区,无共饱和点.其平衡固相分别为固溶体K(Cl,Br)和Na(Cl,Br),其中固溶体K(Cl,Br)结晶区较大,固溶体Na(Cl,Br)结晶区较小.与同体系313 K条件下的相图相比,348 K时固溶体Na(Cl,Br)·2H2O结晶区消失. 相似文献
10.
采用等温蒸发法研究简单四元体系Na＋／／Cl-,CO3^2-,B4O7^2--H2O273K时的介稳相平衡,并测定该体系273K平衡液相中各组分的溶解度及密度,该体系的介稳相图和密度组成图显示：该四元体系在273K时的相图由3条溶解度单变量线、3个结晶区及1个共饱和点组成。体系属简单共饱型,无复盐或固溶体形成,3个结晶区分别对应单盐Na2CO3·10H2O,NaCl和Na2B4O7·10H2O。共饱点E处于Na2CO3·10H2O,NaCl及NaB4O7·10H2O3盐共饱和,所对应的平衡液相组成为w（Na2CO3）=6．81％,w（NaCl）=21．69％,w（Na2B4O7）=0．65％,w（H2O）=70．85％。研究体系在273K下,Na2CO3·10H2O是碳酸钠盐的唯一析出形式,且硼酸钠对碳酸钠有盐析作用。 相似文献
11.
298K时三元体系K^＋／CO3^2—,B4O7^2——H2O和Li^＋／CO3^2—,B4O7^2——H2O相关系 总被引：2，自引：0，他引：2
研究了二个三元体系Ｌｉ＋／ＣＯ２－３,Ｂ４Ｏ２－７Ｈ２Ｏ（１）和Ｋ＋／ＣＯ２－３,Ｂ４Ｏ２－７Ｈ２０（２）２９８Ｋ时的相平衡关系和平衡液相的物化性质（密度、折光密、粘度、电导率、ｐＨ值）。研究表明：这二个三元体系均属简单共饱型,无复盐或固溶体形成。体系（１）的两段溶解度曲线对应于无水Ｌｉ２ＣＯ３和Ｌｉ２Ｂ４Ｏ７·３Ｈ２Ｏ结晶区,体系（２）的两段溶解度曲线对应于Ｋ２ＣＯ３·３／２Ｈ２Ｏ和Ｋ２Ｂ４Ｏ７·４Ｈ２Ｏ结晶区。 相似文献
12.
为了计算高温，高压和高密度流体的热力学性质，提出了一个具有19个参数的维里型状态方程，其中参数与温度间的函数关系采用由Sutherland位能函数导出的维里系数近似式。除临界点附近以外，在已报道的pVT数据所覆盖的大部分超临界区域内，该方程均可适用。用该方程对H2O，CH4，H2，CO2，CO和O2等流体pVT关系的计算结果令人满意，其中pVT上限分别为：91-610GPa,1.6-11.0cm^3/mol,4000-5000K。计算体积的平均偏 小于0．8％，最大偏差小于5．4％。 相似文献
13.
According to the compositions of the underground gasfield brines in the west of Sichuan Basin,the phase equilibria in the ternary systems KBr-K2B4O7-H2O and KCl-K2B4O7-H2O at 373 K were studied using the isothermal dissolution equilibrium method.The solubilities of salts and the densities of saturated solutions in these ternary systems were determined.Using the experimental data,phase diagrams and density-composition diagrams were constructed.The two phase diagrams were simple co-saturation type,each having an invariant point,two univariant curves and two crystallization regions.The equilibrium solid phases in the ternary system KBr-K2B4O7-H2O are potassium bromide （KBr） and potassium tetraborate tetrahydrate （K2B4O7·4H2O）,and those in the ternary system KCl-K2B4O7-H2O are potassium chloride （KCl） and potassium tetraborate tetrahydrate （K2B4O7·4H2O）.Comparisons of the phase diagrams of the two systems at different temperatures show that there is no change in the crystallization phases,but there are changes in the size of the crystallization regions.As temperature increases,the solubility of K2B4O7·4H2O increases rapidly,so the crystallization field of K2B4O7·4H2O becomes smaller. 相似文献
14.
离子色谱法测定水样中S2-、SO2-3、SO2-4、S2O2-3 总被引：1，自引：0，他引：1
该种方法利用离子色谱仪的电导检测器与电化学检测器串联,十几分钟即可连续完成水中S2-、SO2-3、SO2-4、S2O2-3的测定,方法具有快速、高效、方便、灵敏、选择性好等特点.方法的检出限分别为S2-12.5μg/L;SO2-3 22.4μg/L;SO2-4 5.0μg/L;S2O2-3 5.0μg/L.相对标准偏差在1.5%～6.9%之间,能够满足水中S2-、SO2-3、SO2-4、S2O2-3四种阴离子分析测试的需要. 相似文献
15.
Dr. K. Mereiter 《Mineralogy and Petrology》1982,30(2):129-139
Summary The crystal structure of walpurgite has been determined from three-dimensional X-ray single crystal data and has been refined toR=0.041 for 1381 independent reflections using a crystal from Schneeberg, Sachsen. Walpurgite crystallizes triclinic, space group
, witha=7.135 (2),b=10.426 (4),c=5.494 (1) Å, =101 47 (2), =110.82 (2), =88.20 (2)o andV-374 A3. Cell content and chemical formula are (UO2)Bi4O4(AsO4)2·2H2O, which is one H2O less than previously known. The structure consists of complex layers Bi4O4(AsO4)2·2H2O extending parallel to (010). Each layer is built up from a network of bismuth and oxygen atoms, to both sides of which AsO4 groups and water molecules are attached. (UO2)O4 octahedra link the layers parallel tob via the AsO4 groups and thus simultaneously from UO2(AsO4)2 chains parallel toc. The two independent Bi atoms are trivalent and form pronounced one-sided BiO polyhedra: 4–5 oxygens are at distances of 2.11–2.48 Å, 4 additional oxygens are at distances of 2.63–3.35 Å.
With 4 Figures 相似文献
Die Kristallstruktur des Walpurgins, (UO2)Bi4O4(AsO4)2·2H2O
Zusammenfassung Die Kristallstruktur des Walpurgins wurde anhand eines Kristalls von Schneeberg, Sachsen, mit dreidimensionalen Röntgen-Einkristalldaten bestimmt und für 1381 Reflexe aufR=0,041 verfeinert. Walpurgin kristallisiert triklin, Raumgruppe ,a=7,135 (2),b=10,426 (4),c=5,494 (1) Å, =101,47 (2), =110,82 (2), =88,20 (2)o undV=374 Å3. Zellinhalt und chemische Formel lauten (UO2)Bi4O4(AsO4)2·2H2O, das ist um ein H2O-Molekül weniger als bislang bekannt. Die Struktur enthält kompliziert gebaute Bi4O4(AsO4)2·2H2O-Schichten, die sich parallel (010) erstrecken. Jede Schicht besteht aus einem Netz von Wismut- und Sauerstoffatomen, an das zu beiden Seiten AsO4-Gruppen und H2O-Moleküle anknüpfen. (UO2)O4-Oktaeder verbinden die Schichten über die AsO4-Gruppen parallel zub und bilden so gleichzeitig (UO2)(AsO4)2-Ketten parallel zuc aus. Die zwei unabhängigen, dreiwertigen Wismutatome des Walpurgins sind von 4–5 Sauerstoffatomen in Abständen von 2,11–2,48Å einseitig koordiniert und darüber hinaus noch von vier weiteren Sauerstoffatomen in Abständen von 2,63–3,35 Å umgeben.
With 4 Figures 相似文献
16.
The morphological theory of Hartman and Perdok (1955, 1956) allows to deduce the character of a growth form {hkl} on the basis of structural data alone. Its application to the structure of whewellite leads to the identification of forms {100}, {010}, {021}, {011}, {12 \(\bar 1\) } and {121} which show during the growth a flat surface profile (flat forms F). These forms occur very frequently in the crystals we grew from pure aqueous solutions at supersaturation β≦1,90. Other forms, {001} and {10 \(\bar 1\) }, possibly show a double character (F or S, where S stays for related faces showing a stepped profile during the growth) according to the bonds assumed within some periodic bond chains (PBCs). Alternative ways of bonding water molecules lead to different structures of the same PBC. The different energy corresponding to these structures may explain the complex morphology of both natural and synthetic crystals grown at high β values. 相似文献
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19.
Various members of the KAlSi3O8-BaAl2Si2O8 feldspar series are hydrothermally synthesized. Cellparameters of these are calculated from diffractometer patterns and found to be similar to those of Gay and Roy. A variation diagram is constructed correlating Cn-content and values of ΔFeKα(2θ(111)CaF2—2θ(004)Fsss), which gives $${\text{Mol}}\% {\text{ Cn = 229}}{\text{.83}}\Delta {\text{2}}\theta ---{\text{190}}{\text{.81}}$$ by a least square regression fitting. Phase equilibria relation in the solidus-liquidus-region for the KAlSi3O8-BaAl2Si2O8-H2O system at 1000 kg/cm2 are investigated. It is found to be a case of simple solid solution in a binary system, with reservations at the potassium-rich side of the system. Goranson (1938) gives a temperature of about 1000°C at 1000 kg/cm2 \(P_{{\text{H}}_{\text{2}} {\text{O}}} \) for the incongruent melting of sanidine, but the authors prefer a value around 930°C at the same \(P_{{\text{H}}_{\text{2}} {\text{O}}} \) . Reaction products of starting materials on the join KAlSi2O6-BaAl2Si2O8 and KAlSiO4-BaAl2Si2O8 gave no experimental hint for replacement of K+ by Ba++. 相似文献
20.
Spinelloid phases have been observed and characterized by powder X-ray diffraction and high-resolution electron microscopy. Mg3Ga2GeO3(III), with a narrow composition range of approximately 3 mole percent Mg2GeO4, is stable at atmospheric pressure up to about 1,420° C, and is isostructural with β-Mg2SiO4 and the spinelloid Phase III of the NiAl2O4-Ni2SiO4 system. This represents the first occurrence of a β-phase structure stable at 1 atm pressure. Above 1,420° C (1 atm) Mg3Ga2GeO8 (III) decomposes reversibly into a mixture of spinel and olivine. At high pressure (around 30 kbar at 1,100° C) it transforms into another spinelloid phase, Mg3Ga2GeO8 (IV), isostructural with Phase IV of the NiAl2O4-Ni2SiO4 system. In terms of crystal structures and phase relations therefore there exists a close analogy between the magnesium gallo-germanate and nickel alumino-silicate systems, the former being a lower-pressure analogue of the latter. Our investigation of a number of other pseudo-binary spinel-olivine oxide systems suggests that the formation of spinelloid phases can be associated with the inverse character of the spinel component. 相似文献