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紫金山地区斑岩-浅成热液成矿系统的成矿流体演化 总被引：25，自引：2，他引：23
本文从流体包裹体和热液矿物的年代学方面追踪了紫金山地区的斑岩-浅成热液成矿系统中成矿流体的演化过程和演化轨迹。研究表明,汇聚到岩体顶部的岩浆流体在104．5Ma左右、650～550℃温度区间减压沸腾,形成的不混溶流体导致了钾硅酸盐化蚀变及初始Cu(Mo)矿化。其后流体继续向花岗闪长斑岩的外接触带上升运移和降温,在102．5Ma左右、420～380℃区间,再次减压沸腾,分离出的富液相H2O-NaCl流体进一步与对流循环中的大气降水混合,导致体系的温度和盐度逐步降低,演化出绢英岩化蚀变及含铜-硫化物矿化的流体。流体进一步向花岗闪长斑岩外接触带汇聚,在不同构造部位、不同时期分别氧化形成两种不同的流体：其一是在100Ma左右,流体到达花岗闪长斑岩顶面之上800～2000m的火山岩穹部位,温度降至280～250℃时又一次减压沸腾和不混溶,不混溶流体进一步与对流循环中的大气降水混合,使之冷却、稀释和酸化．演化成酸性硫酸盐型浅成热液蚀变和Cu—Au矿化的流体;其二是在94．7Ma左右,形成绢英岩化后的流体侧向扩散到远离花岗闪长斑岩的大型低平火山洼地中,由于大气降水的大量注入,使其演化成为低盐度、较低的温度的H2o-NaCl体系,其沿不整合面附件的断裂-裂隙系统充填,形成冰长石-石英细-网脉及Ag-Au矿化。 相似文献
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查册桥金矿是近年来在江南过渡带发现的一个金多金属矿床,本文对该矿床与矿化有关的蚀变花岗闪长斑岩中绢云母进行了~(40)Ar-~(39)Ar年龄测试,获得蚀变岩金矿石绢云母坪年龄156.9±1.6 Ma,等时线年龄152±28 Ma和矿化强蚀变花岗闪长斑岩绢云母坪年龄142.1±1.3 Ma,等时线年龄137±13 Ma。程檀矿段与牛头高家矿段流体包裹体均一温度为160℃左右,氢氧同位素特征显示成矿热液以岩浆热液为主。结合本区及邻近矿区相关研究成果,本区金矿主要为浅成、低温型,成矿物质和热液具有多来源特征,原生金矿以微细粒浸染型为主,具类卡林型金矿矿化特征,其年龄值分别对应于燕山期不同阶段构造活动和成岩成矿作用时代,其成矿过程经历了中侏罗世韧-脆性挤压构造变形和蚀变、矿化,晚侏罗世-早白垩世早期与岩体侵入相关的金多金属矿化,以及早白垩世中、晚期浅成低温热液成矿作用。 相似文献
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春都斑岩铜矿床地处著名的印支期中甸-义敦岛弧成矿带南端。矿区出露闪长玢岩-花岗闪长斑岩复式岩体,成矿岩体为印支晚期的花岗闪长斑岩。围绕成矿岩体,围岩蚀变强烈,蚀变分带明显,由中心向外,依次出现硅化钾化带→绢英岩化带→硅化带→硅化黑云母化带→青磐岩化带→绢云母化及泥化带。区内蚀变与矿化关系密切,蚀变类型决定矿化程度,蚀变... 相似文献
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福建碧田金银铜矿床冰长石的^40Ar／^39Ar年龄 总被引：10，自引：1，他引：10
采用40Ar/39Ar快中子活化年代学方法对采自碧田金银铜矿床的冰长石进行了年龄测定.结果表明,冰长石年龄为91.47土0.39Ma,代表了碧田矿床金-银矿化的形成时代.作为紫金山-碧田地区大规模铜金(银)矿化作用冰长石-绢云母型浅成低温热液贵金属矿床的典型代表,碧田矿床成矿年龄的确定,为本区不同类型铜金(银)矿床时空关系和成因机制的探讨提供了重要的依据. 相似文献
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冈底斯中段尼木斑岩铜矿田的K-Ar、^40 Ar/^39 Ar年龄：对岩浆-热液系统演化和成矿构造背景的制约 总被引：7，自引：0，他引：7
青藏高原冈底斯斑岩成矿带不同于经典的产于岛弧和大陆边缘的斑岩铜矿,而形成于后碰撞挤压向伸展转变期,显示了极好的成矿前景。本文对冈底斯中段尼木矿田白容、厅宫和冲江斑岩铜矿区斑岩体进行了系统研究,确定出斑岩体演化和侵入序列为:似斑状二长花岗岩→成矿二长花岗斑岩→石英闪长玢岩→花岗闪长斑岩。K-Ar和~(40)Ar/~(39)Ar年代学研究获得白容矿区似斑状二长花岗岩中角闪石的K-Ar年龄为16.9±2.4Ma;石英闪长玢岩中黑云母的K-Ar年龄为12.3±0.2Ma、~(40)Ar/~(39)Ar坪年龄为12.5±0.2Ma;花岗闪长斑岩中黑云母的K-Ar年龄为11.5±0.2Ma、~(40)Ar/~(39)Ar坪年龄为12.4±0.2Ma;厅宫矿区石英闪长玢岩中黑云母的K-Ar年龄为13.8±0.2Ma、~(40)Ar/~(39)Ar坪年龄为14.9±0.2Ma;花岗闪长斑岩中黑云母的K-Ar年龄为13.5±0.3Ma、~(40)Ar/~(39)Ar坪年龄为14.2±0.2Ma,这些年龄表明:石英闪长玢岩晚于似斑状二长花岗岩,略早于花岗闪长斑岩。成矿与二长花岗斑岩有关,其侵位时间晚于似斑状二长花岗岩,早于石英闪长玢岩和花岗闪长斑岩。尼木斑岩铜矿田这种复式杂岩体较充分的分异演化有利于含矿热液的集中与逐渐富集成矿。白容斑岩铜矿蚀变矿化二长花岗斑岩的蚀变绢云母的K-Ar年龄为11.8±0.2Ma,~(40)Ar/~(39)Ar坪年龄为12.0±0.1Ma,代表了中低温蚀变和矿化末期的年龄。白容矿区绢云母化带的蚀变年龄与石英闪长玢岩和花岗闪长斑岩的黑云母~(40)Ar/~(39)Ar年龄基本一致,与厅宫矿区辉钼矿Re-Os年龄及石英闪长玢岩和花岗闪长斑岩的黑云母~(40)Ar/~(39)Ar年龄同样基本一致,暗示两个矿区石英闪长玢岩和花岗闪长斑岩的岩浆结晶冷却与成矿二长花岗斑岩后期热液成矿时间上有重叠。结合前人年龄数据大致确定出白容矿区岩浆-热液活动时限为0.5～5Ma,厅宫为4Ma,冲江为4.5Ma。尼木矿田成矿斑岩~(40)Ar/~(39)Ar年龄晚于冈底斯碰撞后第一次快速隆升时间≈21Ma,15Ma冈底斯中段NS向正断层开始活动,表明含矿斑岩体可能侵位于地壳加厚、冈底斯山大规模隆升到一定程度后出现弱伸展环境的构造背景下,即斑岩铜矿形成于从南北向挤压隆升到东西向伸展初始发育的过渡构造背景。 相似文献
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银岩斑岩锡矿产于花岗质岩浆演化晚期所形成的浅成侵位的隐伏花岗斑岩小岩株中。花岗斑岩自下而上表现出强烈的蚀变分带：较新鲜的花岗斑岩(其中发育弱钾长石化)→黑鳞云母云英岩化→黄玉云英岩化→绢英岩化→顶部硅化核。矿化主要富集在黄玉云英岩化带。通过对矿物学、岩石学和微量元素等一系列地球化学特征的研究，作者认为银岩斑岩锡矿应属于华南陆壳改造型花岗岩类成岩成矿系列的斑岩锡矿。 相似文献
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鄂东南铁铜矿集区铜山口铜(钼)矿床40Ar/39Ar年代学及对区域成矿作用的指示 总被引：11，自引：0，他引：11
铜山口铜-钼矿床发育有夕卡岩型和斑岩型两类矿化,是鄂东南矿集区内典型的夕卡岩-斑岩复合型矿床。成矿作用与铜山口花岗闪长斑岩岩株和大冶群碳酸盐岩有关,矿体主要沿两者的接触带分布。本文利用激光阶段加热技术分别对两类矿化有关的蚀变矿物金云母和绢云母进行40Ar／39Ar年龄测定。结果表明,铜山口矿区经历了两次蚀变一矿化事件:铜山口矿床成矿作用发生于约143±0．3 Ma,而矿区东南缘的牛鼻峰石英二长斑岩的热液蚀变发生于约129 Ma。牛鼻峰石英二长斑岩的侵位及蚀变对铜山口矿床斑岩型矿化的部分地段产生热扰动, 导致绢云母40Ar／39Ar年龄比实际矿化蚀变年龄偏年轻。铜山口矿区两次蚀变-矿化年龄分别与长江中下游成矿带早晚两期成岩成矿事件(145-133 Ma和130-120 Ma)一致。岩石圈伸展及幔源玄武质岩浆底侵作用可能是区域上大规模岩浆活动与成矿作用的深部地球动力学因素。 相似文献
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浅成低温水热酸性硫酸盐型和冰长石绢云母型金矿床形成于陆相火山岩活动区地热系统内,成矿流体以大气水为主,成矿温度小于３００℃,压力小于ｎ×１０ＭＰａ。酸性硫酸盐型金矿床以出现硫砷铜矿＋黄铁矿±铜蓝±自然铜和明矾石、高岭石等高级泥岩化蚀变为特征;冰长石绢云母型矿床以出现冰长石±绢云母和绢云母化、硅化蚀变为特征。酸性硫酸盐型矿床形成于酸性（ｐＨ＜４）相对氧化的流体环境,冰长石绢云母型矿床形成于近中性（ｐＨ＞６）相对还原的流体环境。 相似文献
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西藏铁格隆南超大型铜(金、银)矿床地质、蚀变与矿化 总被引：5，自引：1，他引：4
铁格隆南是班公湖-怒江成矿带西段重要的斑岩-浅成低温热液铜(金、银)矿床,也是西藏地区首个铜资源量超过1000万吨的超大型铜(金、银)矿床,其蚀变与矿化结构的精细解剖,对完善区域成矿理论和指导找矿实践有重要的指导意义。文章基于详细的野外地质调查、钻孔编录和镜下鉴定,识别出铁格隆南矿床具有斑岩和浅成低温热液叠加成矿作用特征。其中,斑岩成矿作用主要位于矿床深部及外围,以细脉状、脉状、浸染状黄铁矿、黄铜矿、斑铜矿及少量辉钼矿等为主,蚀变为钾硅化、青磐岩化、黄铁绢英岩化,发育A、B、D型脉体。浅成低温热液成矿作用主要产于矿床中-浅部,叠加于斑岩成矿作用之上,以浸染状-脉状黄铁矿、硫砷铜矿、斑铜矿、铜蓝、蓝辉铜矿、斯硫铜矿、雅硫铜矿、久辉铜矿等Cu-S体系矿物为特征,蚀变为高级泥化,广泛发育N脉(即高岭石或明矾石-硫化物脉)。蚀变、矿化特征及脉体穿切关系揭示,矿床成岩成矿作用可细分为岩浆期(Ⅰ)、岩浆-热液期(Ⅱ)和表生期(Ⅲ)。成岩成矿年代学结果揭示,矿区内闪长玢岩侵位时代较早(123 Ma),代表岩浆活动上限;花岗闪长斑岩(122～120 Ma)是主要的含矿斑岩,与成矿作用关系最为密切;火山岩覆盖于地表,喷发时代较晚(111 Ma),代表成矿后岩浆活动的产物。钾硅化的黑云母和黄铁绢英岩化的绢云母40Ar-39Ar年龄分别(121.1±0.5) Ma、(120.8±0.9)Ma与斑岩成矿作用的辉钼矿Re-Os年龄((121.2±1.2) Ma)一致,而高级泥化的明矾石40Ar-39Ar年龄为(117.9±1.6)Ma与浅成低温热液矿化的黄铁矿Rb-Sr年龄((117.5±1.8)Ma)一致。所以,依据时空关系,铁格隆南超大型矿床成矿作用可细分为岩浆热液成矿作用(123～119 Ma)、浅成低温热液成矿作用(118～117 Ma)和火山岩覆盖保存(111～110 Ma)3个阶段。 相似文献
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Enthalpies of solution in 2PbO· B2O3 at 712°C have been measured for glasses in the systems albite anorthite diopside, NaAlO2-SiO2, Ca0.5AlO2-SiO2 and albite-anorthite-quartz. The systems albite-anorthite and diopside-anorthite show substantial negative enthalpies of mixing, albite-diopside shows significant positive heats of mixing. For compositions up to NaAlO2 = 0.42 (which includes the subsystem albite-silica) the system NaAlO2-SiO2 shows essentially zero heats of mixing. A negative ternary excess heat of mixing is found in the plagioclase-rich portion of the albite-anorthite-diopside system. The join Si4O8-CaAl2Si2O8 shows small but significant heats of mixing. In albite-anorthite-quartz. ternary glasses, the ternary excess enthalpy of mixing is positive.Based on available heat capacity data and appropriate consideration of the glass transition, the enthalpy of the crystal-glass transition (vitrification) is a serious underestimate of the enthalpy of the crystal-liquid transition (fusion) especially when the melting point, Tf, is many hundreds of degrees higher than the glass transition temperature, Tg. On the other hand, the same heat capacity data suggest that the enthalpies of mixing in albite-anorthite-diopside liquids are calculated to be quite similar to those in the glasses. The enthalpies of mixing observed in general support the structural models proposed by Taylor and Brown (1979a, b) and others for the structure of aluminosilicate glasses. 相似文献
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Enthalpies of solution in 2PbO · B2O3 at 981 K have been measured for glasses in the system albite-orthoclase-silica and along the join Na1.6Al1.6Si2.4O8-K1.6Al1.6Si2.4O8. The join KAlSi3O8-Si4O8 shows zero heat of mixing similar to that found previously for NaAlSi3O8-Si4O8 glasses. Albite-orthoclase glasses show negative heats of mixing symmetric about Ab50Or50 (Wn = ? 2.4 ± 0.8 kcal). Negative heats of (Na, K) mixing are also found at Ternary excess enthalpies of mixing in the glassy system Ab-Or-4Q are positive but rarely exceed 1 kcal mol?1.Using earlier studies of the thermodynamic properties of the crystals, the present calorimetric data and the “two-lattice” entropy model, the albite-orthoclase phase diagram is calculated in good agreement with experimental data. Attempts to calculate albite-silica and orthoclase-silica phase diagrams reveal complexities probably related to significant (but unknown) mutual solid solubility between cristobalite and alkali feldspar and to the very small heat and entropy of fusion of SiO2. 相似文献
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An end member of the tourmaline series with a structural formula □(Mg2Al)Al6(BO3)3[Si6O18](OH)4 has been synthesized in the system MgO-Al2O3-B2O3-SiO2-H2O where it represents the only phase with a tourmaline structure. Our experiments provide no evidence for the substitutions Al → Mg + H, Mg → 2H, B + H → Si, and AlAl → MgSi and we were not able to synthesize a phase “Mg-aluminobuergerite” characterized by Mg in the (3a)-site and a strong (OH)-deficiency reported by Rosenberg and Foit (1975). The alkali-free tourmaline has a vacant (3a)-site and is related to dravite by the □ + Al for Na + Mg substitution. It is stable from at least 300°C to about 800°C at low fluid pressures and 100% excess B2O3, and can be synthesized up to a pressure of 20 kbars. At higher temperatures the tourmaline decomposes into grandidierite or a boron-bearing phase possibly related to mullite (“B-mullite”), quartz, and unidentified solid phases, or the tourmaline melts incongruently into corundum + liquid, depending on pressure. In the absence of excess B2O3 tourmaline stability is lowered by about 60°C. Tourmaline may coexist with the other MgO-Al2O3-B2O3-SiO2-H2O phases forsterite, enstatite, chlorite, talc, quartz, grandidierite, corundum, spinel, “B-mullite,” cordierite, and sinhalite depending on the prevailing PTX-conditions.The (3a)-vacant tourmaline has the space group R3m with , , and . However, these values vary at room temperature with the pressure-temperature conditions of synthesis by , , and , probably as a result of MgAl order/disorder relations in the octahedral positions. Despite these variations intensity calculations support the assumed structural formula. Refractive indices are no = 1.631(2), nE = 1.610(2), Δn = 0.021. The infrared spectrum is intermediate between those of dravite and elbaite. The common alkali and calcium deficiencies of natural tourmalines may at least partly be explained by miscibilities towards (3a)-vacant end members. The apparent absence of (3a)-vacant tourmaline in nature is probably due to the lack of fluids that carry boron but no Na or Ca. 相似文献
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Richard L. Hervig Derry Scott Alexandra Navrotsky 《Geochimica et cosmochimica acta》1985,49(7):1497-1501
Enthalpies of solution in 2PbO · B2O3 at 974 K have been measured for glasses along the joins Ca2Si2O6 (Wo)-Mg2Si2O6 (En) and Mg2Si2O6-MgAl2SiO6 (MgTs). Heats of mixing are symmetric and negative for Wo-En with WH = ?31.0 ± 3.6 kJ mol?. Negative heats of mixing were also found for the En-MgTs glasses (WH = ?33.4 ± 3.7 kJ mol?).Enthalpies of vitrification of pyroxenes and pyroxenoids generally increase with decreasing alumina content and with decreasing basicity of the divalent cation.Heats of mixing along several glassy joins show systematic trends. When only non-tetrahedral cations mix (outside the aluminosilicate framework), small exothermic heats of mixing are seen. When both nontetrahedral and framework cations mix (on separate sublattices, presumably), the enthalpies of mixing are substantially more negative. Maximum enthalpy stabilization near compositions with Al/Si ≈ 1 is suggested. 相似文献
15.
Five hundred eighty-five viscosity measurements on 40 melt compositions from the ternary system CaMgSi2O6 (Di)-CaAl2Si2O8 (An)-NaAlSi3O8 (Ab) have been compiled to create an experimental database spanning a wide range of temperatures (660-2175°C). The melts within this ternary system show near-Arrhenian to strongly non-Arrhenian properties, and in this regard are comparable to natural melts. The database is used to produce a chemical model for the compositional and temperature dependence of melt viscosity in the Di-An-Ab system. We use the Vogel-Fulcher-Tammann equation (VFT: log η = A + B/(T − C)) to account for the temperature dependence of melt viscosity. We also assume that all silicate melts converge to a common viscosity at high temperature. Thus, A is independent of composition, and all compositional dependence resides in the parameters B and C. The best estimate for A is −5.06, which implies a high-temperature limit to viscosity of 10-5.06 Pa s. The compositional dependence of B and C is expressed by 12 coefficients (bi=1,2.6, cj=1,2..6) representing linear (e.g., bi=1:3) and higher order, nonlinear (e.g., bi=4:6) contributions. Our results suggest a near-linear compositional dependence for B (<10% nonlinear) and C (<7% nonlinear). We use the model to predict model VFT functions and to demonstrate the systematic variations in viscosity due to changes in melt composition. Despite the near linear compositional dependence of B and C, the model reproduces the pronounced nonlinearities shown by the original data, including the crossing of VFT functions for different melt compositions. We also calculate values of Tg for melts across the Di-An-Ab ternary system and show that intermediate melt compositions have Tg values that are depressed by up to 100°C relative to the end-members Di-An-Ab. Our non-Arrhenian viscosity model accurately reproduces the original database, allows for continuous variations in rheological properties, and has a demonstrated capacity for extrapolation beyond the original data. 相似文献
16.
Guy L. Hovis 《Geochimica et cosmochimica acta》1984,48(3):523-525
Glasses in the systems NaAlSi3O8-KAlSi3O8 and NaAlSi3O8-Si4O8 have been studied by means of hydrofluoric acid solution calorimetry at 50°C. Results indicate small negative enthalpies of mixing in the former system and small positive departures from ideality in the latter. 相似文献
17.
18.
R.C. Newton T.V. Charlu P.A.M. Anderson O.J. Kleppa 《Geochimica et cosmochimica acta》1979,43(1):55-60
Enthalpies of solution of synthetic clinopyroxenes on the join CaMgSi2O6-Mg2Si2O6 have been measured in a melt of composition Pb2B2O5 at 970 K. Most of the measurements were made on samples crystallized at 1600°–1700°C and 30 kbar pressure, which covered the range 0–78 mole per cent Mg2Si2O6, and whose X-ray patterns could be satisfactorily indexed on the diopside (C2/c) structure. For the reaction: Mg2Si2O6→-Mg2Si2O6 enstatite diopside the present data, in conjunction with previous and new measurements on Mg2Si2O6 enstatite, determine ΔH° ~ 2 kcal and WH (regular solution parameter) ~ 7 kcal. These values are in good agreement with those deduced by Saxena and Nehru (1975) from a study of high temperature, high pressure phase equilibrium data under the assumption that the excess entropy of mixing is small, but, in light of the recent theoretical treatment of Navrotsky and Loucks (1977, Phys. Chem. Min.1, 109–127), the meanings of these parameters may be ambiguous.Heat of solution measurements on Ca-rich binary diopsides made by annealing glasses at 1358°C in air gave slighter higher values than the higher temperature high pressure samples. This may be evidence for some (Ca, Mg) disorder of the sort postulated by Navrotsky and Loucks (1977, Phys. Chem. Min.1, 109–127), although no differences in heat of solution dependent on synthesis temperature in the range 1350°–1700°C could be found in stoichiometric CaMgSi2O6. 相似文献
19.
D. E. Kelsey R. W. White T. J. B. Holland R. Powell 《Journal of Metamorphic Geology》2004,22(6):559-578
Sapphirine, coexisting with quartz, is an indicator mineral for ultrahigh‐temperature metamorphism in aluminous rock compositions. Here a new activity‐composition model for sapphirine is combined with the internally consistent thermodynamic dataset used by THERMOCALC, for calculations primarily in K2O‐FeO‐MgO‐Al2O3‐SiO2‐H2O (KFMASH). A discrepancy between published experimentally derived FMAS grids and our calculations is understood with reference to H2O. Published FMAS grids effectively represent constant aH2O sections, thereby limiting their detailed use for the interpretation of mineral reaction textures in compositions with differing H2O. For the calculated KFMASH univariant reaction grid, sapphirine + quartz assemblages occur at P–T in excess of 6–7 kbar and 1005 °C. Sapphirine compositions and composition ranges are consistent with natural examples. However, as many univariant equilibria are typically not ‘seen’ by a specific bulk composition, the univariant reaction grid may reveal little about the detailed topology of multi‐variant equilibria, and therefore is of limited use for interpreting the P–T evolution of mineral assemblages and reaction sequences. Calculated pseudosections, which quantify bulk composition and multi‐variant equilibria, predict experimentally determined KFMASH mineral assemblages with consistent topology, and also indicate that sapphirine stabilizes at increasingly higher pressure and temperature as XMg increases. Although coexisting sapphirine and quartz can occur in relatively iron‐rich rocks if the bulk chemistry is sufficiently aluminous, the P–T window of stability shrinks with decreasing XMg. An array of mineral assemblages and mineral reaction sequences from natural sapphirine + quartz and other rocks from Enderby Land, Antarctica, are reproducible with calculated pseudosections. That consistent phase diagram calculations involving sapphirine can be performed allows for a more thorough assessment of the metamorphic evolution of high‐temperature granulite facies terranes than was previously possible. The establishment of a a‐x model for sapphirine provides the basis for expansion to larger, more geologically realistic chemical systems (e.g. involving Fe3+). 相似文献
20.
The short range distribution of interatomic distances in three feldspar glasses has been determined by X-ray radial distribution analysis. The resulting radial distribution functions (RDF's) are interpreted by comparison with RDF's calculated for various quasi-crystalline models of the glass structure.The experimental RDF's of the alkali feldspar glasses were found to be inconsistent with the four-membered rings of tetrahedra associated with crystalline feldspars; the structures of these glasses are probably based on interconnected six-membered rings of the type found in tridymite, nepheline, or kalsilite. In contrast, the RDF of calcic feldspar glass is consistent with a four-membered ring structure of the type found in crystalline anorthite. T-O bond lengths (T = Si,Al) increase from 1.60 Å in SiO2 glass [J. H. Konnert and J. Karle (1973) Acta Cryst.A29, 702–710] to 1.63 Å in the alkali feldspar glasses to 1.66 Å in the calcic feldspar glass due to the substitution of Al for Si in the tetrahedra] sites. The T-O-T bond angles inferred from the RDF peak positions are 151° in SiO2 glass (see reference above), 146° in the alkali feldspar glasses, and 143° in the calcic feldspar glass. Detail in the RDF at distances greater than 5 Å suggests that the alkali feldspar glasses have a higher degree of long range order than the calcic feldspar glasses.Assuming that the structural details of our feldspar glasses are similar to those of the melts, the observed structural differences between the alkali feldspar and calcic feldspar glasses helps explain the differences in crystallization kinetics of anhydrous feldspar composition melts. Structural interpretations of some thermodynamic and rheologic phenomena associated with feldspar melts are also presented based on these results. 相似文献