共查询到20条相似文献，搜索用时 78 毫秒
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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
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在１＊１０＾５Ｐａ,１４００℃条件下实验合成了不同成分的Ｎｉ（１－ｘ）ＺｎｘＦｅ２Ｏ４尖晶石,并将部分尖晶石在１１００℃和１６１０℃条件下重新平衡。采用粉晶Ｘ射线衍射法测定了尖晶石的晶胞参数。将实测的尖晶石晶胞参数与理论计算值进行对比,结果发现,在温度小于１４００℃时Ｎｉ（１－ｘ）ＺｎｘＦｅ２Ｏ４尖晶石中的四面体主要由Ｚｎ＾２＋、Ｆｅ＾３＋占据,而八面体主要由Ｎｉ＾２＋、Ｆｅ＾３＋占据,但至少当温 相似文献
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我们利用Holland和Powell(1990)的内部一致的热动力学数集,在0～18kb,460～720℃温压范围内计算出了KFMASH(K_2O—FeO—MgO—Al_2O3—SiO_2—H_2O)体系和KFASH、KMASH亚体系中的单变平衡线和不变平衡点,这些体系中含有十字石、硬绿泥石、绿泥石、黑云母、堇青石、石榴石、红柱石、矽线石和蓝晶石组合及过剩的白云母、石英和水。我们不仅获得了这些平衡的温压位置,而且还确定了涉及到MgFe—1和MgSiAl—2置换的矿物成分。除了在我们的KFMASH体系格子中由于没有Fe~(+3)而无硬绿泥石+黑云母或红柱石+黑云母组合的稳定范围以外,Harte和Hudson(1979)所确立的岩石一致格子是特别出色的。但考虑到格子中反应位置的不确定性以及黑云母和硬绿泥石可能富集了更多的那部分Fe,这些组合在格子中即是稳定的。我们检验了一个内部一致的数集是否象我们合理预测的与那些天然泥质岩石一样复杂的相关系,尽管结果与岩石学观察是有惊人的一致性,但仍需进一步的实验工作,特别是含堇青石和十字石的反应,在进一步改进以前,可以得出这种推算出的格 相似文献
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本文根据物理化学基本原理，提出HF的表面吸附催化机制对于CaF2-HCl-H2O固－液反应体系溶解振荡起着关键性作用。同时建立了该 体系的动力学模型，研究其振荡现象的非线性动力学起因，虽然这一数学模型是基于CSTR反应器为对象而建立的，不过其基本的结论对叠层式流动反应器的情况也是适用的。 相似文献
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Li2B4O7—Na2B4O70H2O三元体系25℃相关系及物化性质实验 总被引：3，自引：0，他引：3
通过实验研究了Ｌｉ２Ｂ４Ｏ７－Ｎａ２Ｂ４Ｏ７－Ｈ２Ｏ三元体系２５℃相关 溶液的物化性质，其２５℃相图由二条溶解度曲线构成，分别对应于Ｌｉ２Ｂ４Ｏ７．３Ｈ２Ｏ、Ｎａ２Ｂ４Ｏ７．１０Ｈ２Ｏ相区，属简单共饱和型。简要讨论了该体系硼酸盐在水听溶解行为，并用经验公式描述了物有浓度的变化规律。 相似文献
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Based on the physical chemistry principle ,this paper proposes that the surface adsorption catalytic mechanism of HF is the key to dissolving the oscillation of the CaF2-HCl-H2OL solid-liquid reaction system.Meanwhile the dynamical model of this system has been established in order to study its non-linear dynamical genesis.Although this mathematics model is based on CSTR reaction apparatus,it is applicable to the foliate flow reaction apparatus,too. 相似文献
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The configurational heat capacity, shear modulus and shear viscosity of a series of Na2O–Fe2O3–Al2O3–SiO2 melts have been determined as a function of composition. A change in composition dependence of each of the physical properties
is observed as Na2O/(Na2O + Al2O3) is decreased, and the peralkaline melts become peraluminous and a new charge-balanced Al-structure appears in the melts.
Of special interest are the frequency dependent (1 mHz–1 Hz) measurements of the shear modulus. These forced oscillation measurements
determine the lifetimes of Si–O bonds and Na–O bonds in the melt. The lifetime of the Al–O bonds could not, however, be resolved
from the mechanical spectrum. Therefore, it appears that the lifetime of Al–O bonds in these melts is similar to that of Si–O
bonds with the Al–O relaxation peak being subsumed by the Si–O relaxation peak. The appearance of a new Al-structure in the
peraluminous melts also cannot be resolved from the mechanical spectra, although a change in elastic shear modulus is determined
as a function of composition. The structural shear-relaxation time of some of these melts is not that which is predicted by
the Maxwell equation, but up to 1.5 orders of magnitude faster. Although the configurational heat capacity, density and shear
modulus of the melts show a change in trend as a function of composition at the boundary between peralkaline and peraluminous,
the deviation in relaxation time from the Maxwell equation occurs in the peralkaline regime. The measured relaxation times
for both the very peralkaline melts and the peraluminous melts are identical with the calculated Maxwell relaxation time.
As the Maxwell equation was created to describe the timescale of flow of a mono-structure material, a deviation from the prediction
would indicate that the structure of the melt is too complex to be described by this simple flow equation. One possibility
is that Al-rich channels form and then disappear with decreasing Si/Al, and that the flow is dominated by the lifetime of
Si–O bonds in the Al-poor peralkaline melts, and by the lifetime of Al–O bonds in the relatively Si-poor peralkaline and peraluminous
melts with a complex flow mechanism occurring in the mid-compositions. This anomalous deviation from the calculated relaxation
time appears to be independent of the change in structure expected to occur at the peralkaline/peraluminous boundary due to
the lack of charge-balancing cations for the Al-tetrahedra. 相似文献
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