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1.
Summary ?The low-pressure eutectic for the coprecipitation of calcite, portlandite, and periclase/brucite (with H2O-rich vapor) has served as a model for the existence and crystallization of carbonatite magmas. Attempts to determine conditions
for the appearance of dolomite at this eutectic have been unsuccessful. We have discovered a second low-temperature eutectic
for more magnesian liquids which excludes portlandite and includes dolomite (all results are vapor-saturated). Addition of
Ca(OH)2-Mg(OH)2 to CaCO3-MgCO3 at 0.2 GPa depresses the liquidus to temperatures below the crest of the calcite-dolomite solvus; the vapor-saturated liquidus
surface falls steeply, and the field boundary for liquids coexisting with calcite and periclase reaches a peritectic at 880 °C,
where a narrow field for liquidus dolomite begins, extending down to the eutectic at 659 °C for the coprecipitation of calcite,
dolomite and periclase (brucite should replace periclase at slightly higher pressures). The calcite liquidus is very large.
The field boundary for coexistence of calcite and dolomite extends approximately in the direction from CaMg(CO3)2 towards Mg(OH)2. The results illustrate conditions for the formation of mineral-specific cumulates from variable magma compositions. Hydrous
(or sodic) carbonate-rich liquids with compositions from CaCO3 to CaMg(CO3)2 will precipitate calcite-carbonatites first, followed by calcite-dolomite-carbonatites, with the prospect of precipitating
dolomite-carbonatite alone through a limited temperature interval, and with periclase joining the assemblage in the closing
stages. Periclase in the Fe-free system may represent the ubiquitous occurrence of magnetite in natural carbonatites. The
restricted range for the precipitation of dolomite-carbonatites adds credibility to the evidence for primary magnesiocarbonatite
(near-dolomite composition) magmas. Magnesiocarbonatite magmas can precipitate much calcite-carbonatite rock.
Received July 20, 1998;/revised version accepted August 18, 1999 相似文献
Zusammenfassung ?Calciokarbonatitische und magnesiokarbonatitische Gesteine und Magmen im System CaO-MgO-CO 2 -H 2 O bei 0.2 GPa Das Niedrigdruck-Eutektikum der gemeinsamen Ausscheidung von Calcit, Portlandit und Periklas/Brucit (mit H2O-reicher Fluidphase) diente als Modell um die Existenz und Kristallisation karbonatitischer Magmen zu erkl?ren. Versuche die Bedingungen des Auftretens von Dolomit an diesem Eutektikum zu bestimmen blieben bisher ergebnislos. Wir entdeckten ein zweites Niedrigtemperatur-Eutektikum für magnesiumreichere Schmelzen, das Portlandit ausschlie?t, aber Dolomit inkludiert (alle Ergebnisse bei Fluids?ttigung). Die Zugabe von Ca(OH)2-Mg(OH)2 zu CaCO3-MgCO3 bei 0.2 GPa senkt den Liquidus auf Temperaturen unter die Solvus-Schwelle von Calcit-Dolomit. Die fluidges?ttigte Liquidusfl?che verl?uft steil und die Grenzfl?che von Schmelze, die mit Calcit und Periklas koexistiert erreicht ein Peritektikum bei 880 °C. Dort ?ffnet sich ein schmales Feld für Liquidus-Dolomit, das bis zum Eutektikum bei 659 °C reicht, an dem Calcit, Dolomit und Periklas (Brucit sollte Periklas bei geringfügig h?heren Drucken ersetzen) gemeinsam ausgeschieden werden. Der Calcit- Liquidus ist sehr gro?. Die Linie an der Calcit und Dolomit koexistieren erstreckt sich ungef?hr von CaMg(CO3)2 zu Mg(OH)2. Die Ergebnisse zeigen die Bildungsbedingungen für die Bildung mineralspezifischer Kumulate aus unterschiedlichen Magmenzusammensetzungen. Aus w?ssrigen (oder Na-reichen) karbonatreichen Schmelzen mit Zusammensetzungen zwischen CaCO3 und CaMg(CO3)2 werden sich zuerst Calcitkarbonatite und dann Calcit-Dolomitkarbonatite ausscheiden, mit der M?glichkeit Dolomitkarbonatite über ein sehr eingeschr?nktes Temperaturintervall zu bilden und mit Periklas, der zu dieser Vergesellschaftung im Endstadium hinzukommt. Periklas im Fe-freien System k?nnte das weitverbreitete Analog zu Magnetit in natürlichen Karbonatiten sein. Der enge Bereich für die Ausscheidung von Dolomitkarbonatiten untermauert die Existenz prim?rer magnesiokarbonatitischer Magmen (nahe der Zusammensetzung von Dolomit). Magnesiokarbonatitische Magmen k?nnen daher entsprechende Mengen an calcitkarbonatitischen Gesteinen ausscheiden.
Received July 20, 1998;/revised version accepted August 18, 1999 相似文献
2.
保险粉-H2O2对棉布脱色的实验研究 总被引：3，自引：0，他引：3
常用的次氯酸脱色法是在酸性条件下用次氯酸或次氯酸钠对棉布进行处理。实验研究用保险粉-H2O2多段脱色法对棉布进行脱色。保险粉处理段是在保险粉溶液中添加NaHCO3作缓冲剂，加热沸腾40min对棉布进行处理，H2O2则是在碱性H2O2溶液中，添加NaSiO3作添加剂，使棉布加热沸腾30min。与次氯酸脱色法相比，不仅脱色后的棉布强度没有减弱，而且脱色效果能达到或接近次氯酸法的脱色效果。同时脱色后的废水中不含有机氯化物，避免了致癌物质的产生。 相似文献
3.
CaCl2-H2O体系人工合成流体包裹体研究 总被引：2，自引：9，他引：2
人工合成包裹体可以作为天然包裹体参照物,提高我们对天然包裹体各种形成作用的认识,并用来模拟天然包裹体以验证许多涉及流体包裹体研究假设的有效性。本文利用人工水晶裂隙愈合方式,在一定的温压条件下合成了具有特定组成的 CaCl_2-H_2O 体系流体包裹体,并对这些合成的包裹体样品进行了详细的测温学研究,结合倪培等(2003)研究结果,进一步证实了:人工合成包裹体与天然包裹体的相似性,以及流体包裹体中捕获流体是母溶液的真实代表性。因此,合成包裹体作为天然包裹体参照物,将在流体包裹体和地质流体研究领域具有十分广阔的应用前景。 相似文献
4.
6.
三元体系NaVO3-H2NCONH2-H2O 298K相平衡及平衡液相物化性质研究 总被引：1，自引：0，他引：1
采用等温平衡溶解平衡法测定了三元体系NaVO3-H2NCONH2-H2O 298K下的溶解度及平衡液相物化性质(密度、电导率、pH值),绘制出了相应的溶解度等温图和物化性质一组成图。此三元体系等温溶解度图属简单共饱型,未产生新的复盐和固溶体。2个结晶区分别对应为盐NaVO3和H2NCONH2,无变量点平衡液相组成为：ω(NaVO3)3．99％,ω(H2NCONH2)40．17％,对应的平衡固相盐为NaVO3和H2NCONH2。 相似文献
7.
8.
利用原位低温拉曼光谱分析技术,对在设定的实验条件下合成的CaCl2-H2O体系和CaCl2-H2O体系的流体包裹体进行分析研究,结果表明低温下CaCl2水溶液和CaCl2水溶液形成的盐水合物具有各自不同的特征拉曼光谱,通过测定特征光谱,能够简易直接的鉴定这些物质,进而确定盐水体系包裹体的成分。因此,原位低温拉曼光谱技术,能够有效地测定Ca^2＋和Mg^2＋这两种盐水体系包裹体流体中常见,但显微测温过程难以观察和判别的二价阳离子。实践表明,原位低温拉曼光谱分析技术是对传统的流体包裹体显微测温技术的一个十分有效的补充,在包裹体研究领域会得到越来越广泛的应用。 相似文献
9.
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
10.
本文利用低温原位拉曼技术,对CaCl2-H2O体系和MgCl2-H2O体系人工合成流体包裹体进行了研究。结果表明：对于盐浓度不同的溶液而言,可采用不同的冷冻方式有效采集低温拉曼光谱;通过系统采集不同温度下的拉曼光谱,可以直接准确地测定包裹体中流体的成分和低温相变过程。人工合成包裹体原位低温拉曼光谱的研究,为将该技术应用于天然包裹体分研究奠定了理论基础,可以预见,该技术必将在流体包裹体研究领域发挥其它方法不可替代的重要作用。 相似文献
11.
原位低温拉曼光谱技术在人工合成CaCl2-H2O和MgCl2-H2O体系流体包裹体分析中的应用Ⅱ:低温下流体包裹体相变行为的研究 总被引：1，自引：0，他引：1
本文利用低温原位拉曼技术,对CaCl2-H2O体系和MgCl2-H20体系人工合成流体包裹体进行了研究.结果表明:对于盐浓度不同的溶液而言,可采用不同的冷冻方式有效采集低温拉曼光谱;通过系统采集不同温度下的拉曼光谱,可以直接准确地测定包裹体中流体的成分和低温相变过程.人工合成包裹体原位低温拉曼光谱的研究,为将该技术应用于天然包裹体分研究奠定了理论基础,可以预见,该技术必将在流体包裹体研究领域发挥其它方法不可替代的重要作用. 相似文献
12.
H. Fischer W. Schreyer W. V. Maresch 《Contributions to Mineralogy and Petrology》1999,136(1-2):184-191
Seeded, solid-media piston-cylinder runs of unusually long duration up to 31 days indicate growth or persistence of synthetic
gedrite of the composition □Mg6Al[AlSi7O22](OH)2(=6:1:7), prepared from the purest chemicals available, at 10 kbar water pressure and 800 °C. Conversely, breakdown was observed
at 11 kbar and 850 °C to aluminous enstatite, Al2SiO5, and a melt of the composition MgO·Al2O3·8SiO2. Thus, pure gedrite free of iron, sodium, and calcium is likely to have only a small PT stability field in the MASH system, estimated as 10 ± 1 kbar, 800 ± 20 °C, even though metastable growth of gedrite can be
observed over a larger PT range. A second starting material with the anhydrous composition 5MgO · 2Al2O3 · 6SiO2 also yielded gedrite of the composition 6:1:7, together with more aluminous phases such as kyanite, corundum or sapphirine,
thus suggesting that the end-member gedrite defined as □Mg5Al2[Al2Si6O22](OH)2(=5:2:6) by the IMA Commission on New Minerals and Mineral Names probably does not exist. With the use of this second starting
material, which contains FeNaCa impurities, growth of 6:1:7-gedrite was observed over a still wider PT-range. Seeded runs indicate that the true stability field of such slightly impure 6:1:7-gedrites may also be larger than
that of the pure MASH phase and extend at least to 15 kbar, 800 °C. There is, thus, a remarkable stabilization effect on the
orthoamphibole structure by impurities amounting only to a total of less than one weight percent of oxides in the starting
material. The gedrites synthesized are structurally well ordered amphiboles nearly free of chain multiplicity faults, as revealed
by HRTEM. The X-ray diffraction work on the gedrites synthesized yielded the smallest cell volume yet reported for this phase.
The small stability field of the pure MASH gedrite is intersected by the upper pressure stability limit of hydrous cordierite
for excess-H2O conditions, thus leading to complicated phase relations for both gedrite and cordierite involving the additional phases
aluminous enstatite, talc, quartz, Al2SiO5, melt and perhaps boron-free kornerupine.
Received: 29 July 1998 / Accepted: 7 January 1999 相似文献
13.
NaCl-CaCl2-H2O体系人工合成流体包裹体及其冷冻后的熔融行为研究 总被引：1，自引：3，他引：1
在倪培等在2003年和丁俊英等在2005年成功开展人工合成包裹体研究的基础上,利用愈合人工水晶裂隙技术,在设定的实验条件下合成了 NaCl-CaCl_2-H_2O 体系的流体包裹体。对合成的包裹体进行了岩相学观察,显微测温工作,并结合相应相图分析研究——主要对合成包襄体的低温熔融行为进行探讨。结果表明合成的包裹体捕获了既定组成的流体,其低温相变过程与相应相图吻合。因此,人工合成流体包裹体与天然包裹体相似,天然流体包襄体的各种行为可以参照人工合成流体包裹体;同时,通过人工合成流体包裹体校正补充实验相图,使其更准确的被应用于天然包襄体测定分析。 相似文献
14.
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
15.
CH4-H2O体系流体包裹体均一过程激光拉曼光谱定量分析 总被引：6，自引：2，他引：4
对南黄海盆地二叠纪地层中某石英脉中的CH4-H2O体系流体包裹体均一过程进行了激光拉曼光谱定量分析。利用甲烷与水的拉曼峰面积比值计算不同温度下流体包裹体中水溶液相中甲烷的浓度,除了在100℃附近出现最小值,随温度增加甲烷浓度呈指数增大。包裹体在214℃完全均一,均一时甲烷的浓度为0·1347mol/L。同时利用甲烷的拉曼特征对流体包裹体均一过程的内压变化作了分析。压力变化可以分为三个区间:19~100℃,随温度升高压力增大;100~150℃压力随温度升高减小;150℃之后压力迅速增大。均一温度下的内压为21·92MPa。流体包裹体内压的变化主要是由甲烷溶解行为和封闭体系的热力学特征决定的。实验表明激光拉曼光技术可以作为定量分析含甲烷流体包裹体的一种有效方法。 相似文献
16.
根据CO2-H2O体系均一法测温过程中出现的部分均一和完全均一现象,采用最新的热力学参数及相关模型,分别建立相应的热力学方程.根据同一体系的摩尔体积在均一法测温升温过程中几乎不变的特征可知,部分均一与完全均一状态下,体系的摩尔体积近似相等.据此对影响摩尔体积的充填度进行微调,通过迭代运算,直至两种条件下的摩尔体积近似相等,从而可以获得精确的摩尔体积和充填度,进而获得体系中的CO2含量、完全均—压力以及流体包裹体的总密度等热力学参数.本方法只需提供部分均一温度和完全均一温度以及部分均一方式便可求取相关热力学参数,符合地质研究方法和思路.该方法只适用于完全均—温度低于623.15K、完全均一压力小于100MPa以及最后均一至液相或临界点的CO2-H2O流体包裹体体系.对比研究表明,该方法也适用于盐度低于6％的NaCl-CO2-H2O流体体系,所获得的热力学参数相对误差在10％左右. 相似文献
17.
在倪培等在2003年和丁俊英等在2005年成功开展人工合成包裹体研究的基础上，利用愈合人工水晶裂隙技术，在设定的实验条件下合成了NaCl-CaCl2-H2O体系的流体包裹体。对合成的包裹体进行了岩相学观察，显微测温工作，并结合相应相图分析研究——主要对合成包裹体的低温熔融行为进行探讨。结果表明合成的包裹体捕获了既定组成的流体，其低温相变过程与相应相图吻合。因此，人工合成流体包裹体与天然包裹体相似，天然流体包裹体的各种行为可以参照人工合成流体包裹体；同时，通过人工合成流体包裹体校正补充实验相图，使其更准确的被应用于天然包裹体测定分析。 相似文献
18.
Two synthetic series of spinels, MgCr2O4–Fe2+Cr2O4 and MgCr2O4–MgFe2 3+O4 have been studied by Raman spectroscopy to investigate the effects of Fe2+ and Fe3+ on their structure. In the first case, where Fe2+ substitutes Mg within the tetrahedral site, there is a continuous and monotonic shift of the Raman modes A1g and Eg toward lower wavenumbers with the increase of the chromite component into the spinel, while the F2g modes remain nearly in the same position. In the second series, for low Mg-ferrite content, Fe3+ substitutes for Cr in the octahedral site; when the Mg-ferrite content nears 40 %, a drastic change in the Raman spectra occurs as Fe3+ starts entering the tetrahedral site as well, consequently pushing Mg to occupy the octahedral one. The Raman spectral region between 620 and 700 cm?1 is associated to the octahedral site, where three peaks are present and it is possible to observe the Cr–Fe3+ substitution and the effects of order–disorder in the tetrahedral site. The spectral range at 500–620 cm?1 region shows that there is a shift of modes toward lower values with the increase of the Mg-ferrite content. The peaks in the region at 200–500 cm?1, when observed, show little or negligible Raman shift. 相似文献
19.
Gennaro Ventruti Fernando Scordari Giancarlo Della Ventura Fabio Bellatreccia Alessandro F. Gualtieri Andrea Lausi 《Physics and Chemistry of Minerals》2013,40(8):659-670
The thermal stability of sideronatrite, ideally Na2Fe3+(SO4)2(OH)·3(H2O), and its decomposition products were investigated by combining thermogravimetric and differential thermal analysis, in situ high-temperature X-ray powder diffraction (HT-XRPD) and Fourier transform infrared spectroscopy (HT-FTIR). The data show that for increasing temperature there are four main dehydration/transformation steps in sideronatrite: (a) between 30 and 40 °C sideronatrite transforms into metasideronatrite after the loss of two water molecules; both XRD and FTIR suggest that this transformation occurs via minor adjustments in the building block. (b) between 120 and 300 °C metasideronatrite transforms into metasideronatrite II, a still poorly characterized phase with possible orthorhombic symmetry, consequently to the loss of an additional water molecule; X-ray diffraction data suggest that metasideronatrite disappears from the assemblage above 175 °C. (c) between 315 and 415 °C metasideronatrite II transforms into the anhydrous Na3Fe(SO4)3 compound. This step occurs via the loss of hydroxyl groups that involves the breakdown of the [Fe3+(SO4)2(OH)] ∞ 2? chains and the formation of an intermediate transient amorphous phase precursor of Na3Fe(SO4)3. (d) for T > 500 °C, the Na3Fe(SO4)3 compound is replaced by the Na-sulfate thenardite, Na2SO4, plus Fe-oxides, according to the Na3Fe3+(SO4)3 → 3/2 Na2(SO4) + 1/2 Fe2O3 + SOx reaction products. The Na–Fe sulfate disappears around 540 °C. For higher temperatures, the Na-sulfates decomposes and only hematite survives in the final product. The understanding of the thermal behavior of minerals such as sideronatrite and related sulfates is important both from an environmental point of view, due to the presence of these phases in evaporitic deposits, soils and sediments including extraterrestrial occurrences, and from the technological point of view, due to the use of these materials in many industrial applications. 相似文献
20.
Kevin J. Grant Simon C. Kohn Richard A. Brooker 《Contributions to Mineralogy and Petrology》2006,151(6):651-664
The solubility of water in coexisting enstatite and forsterite was investigated by simultaneously synthesizing the two phases in a series of high pressure and temperature piston cylinder experiments. Experiments were performed at 1.0 and 2.0 GPa at temperatures between 1,100 and 1,420°C. Integrated OH absorbances were determined using polarized infrared spectroscopy on orientated single crystals of each phase. Phase water contents were estimated using the calibration of Libowitzky and Rossman (Am Mineral 82:1111–1115, 1997). Enstatite crystals, synthesized in equilibrium with forsterite and an aqueous phase at 1,350°C and 2.0 GPa, contain 114 ppm H2O. This is reduced to 59 ppm at 1,100°C, under otherwise identical conditions, suggesting a strong temperature dependence. At 1,350°C and 1.0 GPa water solubility in enstatite is 89 ppm, significantly lower than that at 2.0 GPa. In contrast water solubility in forsterite is essentially constant, being in the range 36–41 ppm for all conditions studied. These data give partition coefficients
in the range 2.28–3.31 for all experiments at 1,350°C and 1.34 for one experiment at 1,100°C. The incorporation of Al2O3 in enstatite modifies the OH stretching spectrum in a systematic way, and slightly increases the water solubility. 相似文献