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湖南东坡矿田金船塘、红旗岭锡多金属矿床Rb-Sr、Sm-Nd同位素年代学研究 总被引：5，自引：0，他引：5
与千里山岩体有密切时空联系的东坡矿田是我国主要钨锡多金属矿产资源基地之一。在前人对千里山复式岩体成岩时代和金船塘与千里山岩体第一期似斑状花岗岩侵入活动有关的成矿作用研究的基础上,笔者选择金船塘及红旗岭矿床含矿石英脉中的石英和金船塘矿床矽卡岩矿石中的单矿物,进行石英流体包裹体Rb-Sr和矽卡岩矿物(包括符山石和石榴石)Sm-Nd同位素年代学研究,得出金船塘及红旗岭矿床石英流体包裹体Rb-Sr等时线年龄分别为133.4±5.9 Ma(MSWD=1.3)和143.1±8.7 Ma(MSWD=47),金船塘矿床矽卡岩矿物Sm-Nd等时线年龄为141±11 Ma(MSWD=0.27)。同位素年代学研究表明金船塘矿床至少存在164 Ma±、133~141 Ma两期成矿作用,在测定误差范围内,它们分别与千里山岩体第一期似斑状花岗岩(152 Ma)和第二期等粒黑云母花岗岩(136~137Ma)的侵入活动有关,而红旗岭矿床的成矿作用与千里山岩体第二期岩浆侵入活动有关。 相似文献
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3.
广西珊瑚钨锡矿床成矿年代学研究及其地质意义 总被引：2，自引：0，他引：2
珊瑚钨锡矿床位于富贺钟钨锡多金属成矿集中区的中部,是南岭钨锡多金属成矿带内典型的热液石英脉型矿床之一。本文采用白云母~(40)Ar-~(39)Ar法和石英流体包裹体Rb-Sr法,对矿床V32号含矿石英脉进行精细年代学研究,获得石英脉中白云母~(40)Ar-~(39)Ar坪年龄为101.7±0.7 Ma(MSWD=0.34),正等时线年龄为102.0±1.0 Ma(MSWD=1.17);石英流体包裹体Rb-Sr等时线年龄为106.4±3.5 Ma(MSWD=0.83)。它们在误差范围内一致,是华南地区燕山晚期成岩成矿高峰期的产物。同时通过石英包裹体H-O同位素组成的初步分析,认为成矿流体属于"再平衡岩浆水",主要来自岩浆,在矿床深部可能存在隐伏花岗岩体。该成果对研究区域成矿规律,指导类似地区的找矿勘查工作具有重要意义。 相似文献
4.
李贵福钨锡多金属矿赋存于都庞岭复式花岗岩体东部。矿床类型主要为云英岩-石英脉型。通过对矿石中辉钼矿Re-Os同位素测年,获得等时线年龄为(211.9±6.4)Ma(n=7,MSWD=4.1),模式年龄的加权平均值为(213.3±2.9)Ma(MSWD=4.0)。结果显示成矿作用发生在印支期,表明都庞岭地区存在早中生代钨锡多金属成矿事件。 相似文献
5.
粤北连平地区钨锡多金属矿床类型主要为石英脉型.采用云母Ar-Ar法和石英包裹体Rb-Sr法.分别获得:锯板坑含钨锡石英脉中的云母Ar-Ar坪年龄为(139.2±1.5)Ma(等时线年龄为143.6±3.9 Ma,MSWD:0.30):鸡啼石含钨石英脉中石英包裹体Rb-Sr等时线年龄为(155.4±5.1)Ma(MSWD=2.1).结果表明该区存在燕山早期和燕山早晚过渡期两期钨锡多金属成矿作用,并且认为:(1)鸡啼石钨矿为南岭地区中生代大规模成岩成矿作用高峰期(150～160 Ma)的产物;(2)南岭地区140 Ma左右也有大型钨锡多金属矿的形成.这一成果为研究区域成矿规律,指导区域找矿提供了重要同位素年代学依据. 相似文献
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粤北乐昌市和尚田钨锡多金属矿是近年来新发现的一个具有"五层楼"成矿特征的大型(云英岩)-石英脉型矿床。因其主要矿体的围岩是碳酸盐岩而不是碎屑岩且矿区离出露的花岗岩体较远而受到关注。测年结果显示:一条含矿(云英岩)-石英脉中的白云母Ar-Ar坪年龄和等时线年龄分别为158.91±0.96 Ma(MSWD=0.68)和157.8±1.8Ma(MSWD=1.80)、石英矿物Rb-Sr等时线年龄为166±7Ma(MSWD=1.01);另一条含矿(云英岩)-石英脉中的石英矿物Rb-Sr等时线年龄为158.8±2.6Ma(MSWD=0.74)。它们在误差范围内一致,为粤北乃至整个南岭地区成岩成矿高峰期150~160Ma的产物。通过石英包裹体氢及石英氧同位素组成的初步分析,本文认为成矿流体主要来自岩浆水,在矿床深部可能存在隐伏花岗岩体。上述成果为研究区域成矿规律,指导类似无岩体出露的碳酸盐岩分布区的找矿勘查工作具有重要的现实意义。 相似文献
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钦杭成矿带是华南地区一条著名的中生代斑岩-矽卡岩铜铅锌多金属成矿带,其南段阳春盆地内以集中发育白垩纪钨锡多金属矿床为特征,侏罗纪成矿仅有个别铜铁钼矿床报道。因此,区内有关侏罗纪成矿特征、矿化元素组合、成岩成矿物质等问题尚不明晰。本文对阳春盆地内黑石岗矽卡岩型铅锌矿床和留洞石英脉型钨钼矿床进行了成岩成矿年代学研究。结果显示,黑石岗花岗闪长岩的锆石U-Pb等时线年龄为164.9±0.7Ma,留洞钨钼矿的辉钼矿Re-Os同位素等时线年龄为164.6±4.0Ma,加权平均值161.2±2.4Ma,表明区内铅锌钨钼成矿作用均发生于中侏罗世晚期。该结果不仅扩充了区内侏罗纪成矿作用规模,同时丰富了区内侏罗纪矿化元素组合,包括铜铁-铜铅锌-钨钼等多金属矿床。留洞矿床辉钼矿具有极低的Re含量(514.6×10-9~2365×10-9),黑石岗花岗闪长岩的εHf(t)值变化于-5.2~-2.9之间,平均为-4.3。通过对成矿带内侏罗纪铜多金属矿床的相关数据综合及对比分析,本文认为阳春盆地此时期成岩成矿物质均以壳源为主,可能混有少量幔源物质。黑石岗和留洞矿床成岩成矿年龄的确定为下一步在阳春盆地开展侏罗纪矿床找矿勘探提供了重要信息,也为进一步深入研究钦杭成矿带侏罗纪成岩成矿作用动力学背景提供了参考。 相似文献
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湖南龙山锑金矿床白云母~(40)Ar-~(39)Ar年代学及其意义初探 总被引：1，自引：1，他引：0
龙山锑金矿是湘中Sb-Au矿集区内规模最大的脉状锑金矿床,但其精确的成矿时代尚未厘定。本次工作发现该矿床第Ⅰ成矿阶段的石英硫化物脉中发育少量的热液白云母。通过40Ar-39Ar年代学测定,确定了白云母的~(40)Ar-~(39)Ar同位素坪年龄为162. 5±1. 8Ma,相应的等时线年龄为161. 1±1. 2Ma(MSWD=1. 0),反等时线年龄为161. 1±1. 2Ma(MSWD=1. 0)。根据矿物共生组合特征,认为白云母的~(40)Ar-~(39)Ar坪年龄能代表龙山锑金矿床的成矿年龄。结合湘中地区其他锑(金)矿床的年代学研究成果,本文认为,该地区在155~162Ma之间有一次热液成矿事件,与南岭地区165~150Ma与花岗岩有关的钨锡多金属矿床的成矿时代相一致。湘中地区已有的S同位素地球化学和地球物理学资料表明,该地区锑金矿床的形成可能与岩浆作用有关,类似于南岭地区晚侏罗世钨锡多金属矿床的构造背景。 相似文献
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湖南金船塘锡铋矿床辉钼矿Re-Os同位素测年及其地质意义 总被引：18，自引：14，他引：4
湖南东坡矿田位于南岭成矿带的西段,构造位置上处于扬子板块与华夏板块的对接地带,矿田内以千里山岩体为中心,发育一系列与燕山期花岗质岩浆作用有关的超大型、大型和中型钨锡钼铋多金属矿床。金船塘锡铋矿床是东坡矿田内一个以锡铋为主的大型矽卡岩型多金属矿床。本文对该矿床的矽卡岩型矿石中的辉钼矿进行了Re-Os同位素测年。结果显示,辉钼矿Re-Os同位素模式年龄范围为157.2±2.8Ma至162.4±2.4Ma,加权平均值为159.8±2.9Ma,对应的Re-Os等时线年龄为158.8±6.6Ma;这些年龄数据与柿竹园矿床辉钼矿的Re-Os等时线年龄(151.0±3.5Ma)在误差范围内基本一致,亦与区内千里山岩体锆石U-Pb年龄(152±2Ma)接近,指示金船塘Sn-Bi矿床与区内花岗岩具有密切的时间和成因关系。结合区域上已有的研究成果,包括金船塘矿床在内的东坡矿田的成岩成矿作用主要集中在149～161Ma,与南岭地区大规模的钨锡多金属成矿作用时限(150～160Ma)一致;另外,区域上的研究表明,幔源物质广泛参与了湘南钨锡矿集区晚中生代的成岩成矿作用,指示该区中-晚侏罗世爆发式的成岩成矿作用可能是区域地壳拉张-岩石圈伸展减薄背景下,强烈的壳幔相互作用的结果。 相似文献
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马卡铅锌钨矿床地处云南省马关县与麻栗坡县的南温河交界处,位于燕山晚期老君山复式花岗岩体北缘。野外地质调查发现,该矿床主要发育矽卡岩型、石英脉型铅锌矿化和萤石石英脉型白钨矿化,但它们的形成机制仍缺乏系统研究。本文通过闪锌矿Rb-Sr、锡石原位U-Pb同位素定年和硫化物原位S、Pb同位素分析,厘定了马卡矿床不同类型铅锌矿化年龄,并探讨了其成矿物质来源及成因机制。矽卡岩型和石英脉型铅锌矿石中闪锌矿分别获得了88.9±1.9Ma(MSWD=4.5)和85.18±0.72Ma(MSWD=1.2)的Rb-Sr等时线年龄,同时获得石英脉型铅锌矿石中锡石LA-ICP-MS U-Pb年龄为84.3±4.7Ma(MSWD=0.66)。结果指示锌、锡矿化时代为晚白垩世,矽卡岩型和石英脉型铅锌矿化分别与该区广泛出露的老君山花岗岩(-90Ma)和花岗斑岩年龄(80-86Ma)一致。矿石硫化物原位硫同位素测试结果显示,δ34S值范围为2.53‰-9.65‰,均值为4.7‰,与老君山花岗岩中硫化物硫同位素组成(4.07‰)相似,表明硫主要来源于老君山花岗岩,少部分源自沉积地层;原位铅同位素组成特征也表明矿石铅主要源自老君山花岗岩。综合研究认为,老君山花岗岩体南北缘地区具有相似的成矿地质条件。马卡矿床的形成主要与燕山晚期老君山复式花岗岩体有关,可能经历了与花岗岩有关的矽卡岩型矿化和与花岗斑岩有关的热液充填、交代成矿过程。 相似文献
11.
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
14.
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
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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