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探讨差应力对熔体分布和成分演化的关系,利用细粒闪长岩进行高温高压条件下的岩石变形,主要包括静态熔融实验和有差应力参与的动态熔融2种类型。实验首先统计了熔体含量、确定了实验重要参数,然后分别描述了动、静态熔融实验后闪长岩的显微特征;并且通过对动、静态熔融实验结果熔体分布情况的对比,结合熔体成分电子探针数据进行分析。结果表明:在细粒闪长岩的部分熔融中,熔体在差应力的作用下沿一定的方向展布,并从差应力大的地方向差应力小的地方运移,差应力的作用使得高含水矿物(角闪石)先于熔点低的斜长石发生熔融,说明差应力促进了岩石的熔融,使得熔体成分向Si、Al等方向转化,即从基性向酸性转化。 相似文献
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利用高温高压的实验分别对辉长岩进行差应力和温度与岩石熔融程度测试,并进一步分析讨论差应力和温度等岩石熔融程度的关系。动、静态的实验结论表明:(1)静态熔融条件下,岩石的熔融程度主要受温度的影响并且岩石熔融程度与温度呈正相关关系;(2)在保持一定温度不变的动态熔融条件下,岩石的熔融程度还与差应力呈正相关的关系;(3)差应力可以降低熔点,促使熔融提前发生并且使熔融强度增大;(4)差应力对岩石的熔融具有明显的控制作用;(5)以700℃为基准,差应力每增加5MPa其带来的影响与温度升高50℃的效果相当;(6)基性岩石的熔融对差应力的敏感程度最高。该实验结果还表明在研究岩石深熔作用时尤其是在构造作用较强烈地区要考虑差应力的影响因素。 相似文献
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为了探讨差应力和温度与岩石熔融程度的关系,利用角闪变粒岩进行高温高压条件下的岩石变形实验。包括差应力条件下的动态实验,围压100 MPa,温度700℃,施加相当于差应力为0~25 MPa,且以每5 MPa为间隔进行天然块状岩石样品的动态熔融;在相同的围压条件下,温度由700 ℃到900 ℃每50 ℃为间隔,进行无差应力条件下天然块状岩石的静态熔融实验,并进行对比研究。结果表明,在相同温度条件下,岩石的熔融程度随着差应力的增加明显增高。通过对斜率的对比分析表明:以700 ℃为基准,差应力每增加5 MPa,其带来的影响与温度升高40 ℃的效果相当,也说明中性岩石的熔融对差应力的敏感程度比酸性岩要高。 相似文献
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以河北省平山县阜平群的黑云片麻岩为实验样品,有差应力条件下的动态实验,围压10MPa,温度800℃条件下,施加相当于差应力为O～25MPa,且以每5MPa为间隔进行了天然块状岩石样品的动态熔融,在相同的围压条件下,温度由800～900℃每20℃为间隔,进行了无差应力条件下天然块状岩石的静态熔融实验,并进行了对比研究。结果表明,在相同温度条件下,岩石的熔融程度随着差应力的增加明显增高,当差应力达到25MPa时,800℃条件下岩石的熔融程度与900℃静态熔融条件下岩石的熔融程度相当。实验力学分析计算表明,动态实验中构造附加压力增加了围压,差应力每增加5MPa相当于1．67MPa的增压,其与静态实验中温度升高20℃的效果一样。该实验结果对研究岩石深熔作用的深度问题有一定的参考意义。 相似文献
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利用脉冲透射-反射法,在YJ-3000 t高压装置弹性波速测量系统上,测量了0.6、1.0和2.0 GPa,最高1141℃条件下闪长岩的纵波波速(vp)。结果显示,高压下闪长岩的vp随温度升高首先缓慢降低,分别到769℃(0.6 GPa)、810℃(1.0 GPa)和925℃(2.0 GPa)后转而快速下降。实验产物观测显示,0.6 GPa下岩石在758℃时发生脱水熔融并有新生单斜辉石生成,1.0 GPa和2.0 GPa下,闪长岩分别在865℃和921℃的实验产物中出现熔体,新生矿物有单斜辉石和石榴子石。温度升高导致闪长岩中熔体含量增加,斜长石、角闪石和绿泥石等逐渐减少直至消失,单斜辉石和石榴子石呈先增加后减少趋势。探针分析显示,熔体含水量较高,且随温度升高熔体成分向基性方向演化。单斜辉石化学成分变化不明显,2.0 GPa下,随温度从1030℃升高到1138℃,新生石榴子石成分逐渐向钙铝榴石变化。vp变化和熔体含量关系表明,熔体含量增加导致了闪长岩在高温阶段波速的持续快速降低。 相似文献
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高温高压条件下实验变形石英闪长岩微观结构与熔体特征研究 总被引：1，自引：0，他引：1
本文以高温高压条件下石英闪长岩流变实验样品为研究对象,利用偏光显微镜进行微观结构观察,研究了样品在实验温度压力条件下的变形机制与斜长石结构对流变强度的影响;通过透射电镜能谱与电子探针,分析了熔体分布和成分特征,讨论了角闪石脱水熔融的影响因素与脱水熔融对岩石流变的影响。结果表明,随着温度升高,岩石从脆塑性过渡域逐渐向高温位错攀移和动态重结晶为主的塑性域转化。在高温条件下,角闪石出现了脱水与部分熔融,脱水熔融的熔体分布和成分体现出非均匀与非平衡熔融的特点,空间分布上,熔体主要出现在角闪石和黑云母矿物颗粒的边缘以及角闪石和长石颗粒之间的区域内;成分分布上,熔体的成分与参与熔融的矿物成分密切相关。角闪石边缘的熔体和黑云母边缘的熔体具有低硅铝、高铁镁特征,斜长石边缘的熔体具有高硅铝、低铁镁的特征,处于角闪石和斜长石颗粒中间的熔体,其成分间于斜长石与角闪石成分之间。实验中出现的非平衡非均匀部分熔融可以解释混合岩中的浅色体与暗色体的成因,富硅熔体可以形成富硅铝的花岗质岩石,而贫硅富铁镁的熔体可以形成基性岩。角闪石的脱水熔融程度依赖于样品的封闭条件,处于封闭环境的样品,角闪石不易脱水熔融,而处于开放环境时,角闪石脱水熔融显著。拆离断层带及其附近具备这样的开放环境,有利于角闪石发生脱水熔融。实验力学数据和微观结构显示,随机分布的斜长石对岩石强度影响并不明显,但斜长石的长轴方向与最大主应力方向呈大角度相交(近90°)会显著强化岩石的强度,这意味着岩石组构与主应力方向大角度相交或呈垂直方向时,不利于岩石变形和拆离断层的形成,反之,均匀岩石或岩石组构与最大主应力方向小角度相交,有利于岩石的变形,容易发育拆离断层。 相似文献
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以岩石粉末试样的熔融实验为基础的 Ｑ Ａｂ Ｏｒ Ａｎ Ｈ２ Ｏ 体系的相关系表明,地壳岩石的熔融作用遵循矿物相消失所制约的固 液相平衡规律。然而,地壳岩石块状样品开放体系的熔融作用,其熔融机制、矿物相转变、初熔液相成分、残余固相等方面,均与地壳岩石封闭体系的熔融作用有很大差别。石英闪长岩开放体系的熔融实验表明,岩石的熔融首先从含水矿物的脱水熔融开始,从而熔体成分由基性逐渐转变为中酸性,残余固相趋于超酸性。这一实验结果对大陆地区岩浆起源和深部地壳物质组成的研究可能有新的启示。 相似文献
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矿物反应与变形关系研究——以糜棱岩高温高压实验为例 总被引：1，自引：1，他引：0
矿物反应和变形局部化在中下地壳普遍存在,两者相互影响和促进。实验研究表明,矿物反应与变形关系非常复杂。本文在糜棱岩高温高压流变实验的基础上,分析了实验变形样品中的矿物反应分布特征以及矿物反应引起的化学成分变化,讨论了矿物反应与变形的相互影响。微观结构分析表明,实验变形后的糜棱岩样品在温度800~890℃时,角闪石和黑云母出现脱水反应,生成微晶角闪石和黑云母,并伴有局部熔融。受应变局部化控制,脱水反应产物主要出现在黑云母、角闪石条带边缘。微晶和熔体的成分分析表明,不仅脱水反应形成的微晶与熔体的SiO 2含量非常低,而且黑云母周围的反应产物和熔体主要来自于黑云母的脱水,角闪石边缘的反应产物和熔体主要来自于角闪石脱水,石英、钾长石和斜长石没有参与反应与熔融。本研究中的脱水反应产物中,没有发现辉石和石榴石,这种脱水反应与文献中报道的无局部化的均匀样品在静高压和高熔融比例条件的脱水反应产物和熔体的成分有很大差别。黑云母和角闪石的局部化分布和脱水程度低,可能是造成脱水反应产物有差别的巨大原因。在本实验结果中,脱水反应对变形的影响主要体现为,脱水反应产生了细粒混合矿物相,使得在局部化的剪切带内变形机制从位错蠕变转变为扩散蠕变,导致样品出现应变弱化。另外脱水反应还引起了局部脆性破裂。变形引起晶体塑性变形,增加了位错密度和矿物细粒化,促进了晶体内部成核和黑云母与角闪石的脱水分解;差应力作用增加了局部的正应力和平均应力,增加了黑云母和角闪石能够稳定存在的压力范围,这可能是反应产物以微晶黑云母和角闪石为主,而没有转化为辉石的原因。 相似文献
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深熔作用是大陆地壳分异、元素迁移富集和混合岩化作用的主要机制和关键地质过程.吉南地区出露的太古宙基底普遍经历了角闪岩相-麻粒岩相变质及深熔作用,长英质淡色体及淡色花岗岩广泛分布.吉南和龙花岗-绿岩地体出露的太古宙变质石英闪长岩及相关的长英质浅色体和含斜方辉石(角闪石)淡色伟晶花岗岩的野外地质特征、相互关系及岩相学特征指... 相似文献
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This paper presents a model for the partial melting of quartz diorite and greywacke in the upper crust based on the mineralogy and geochemistry of enclaves within the Loch Doon granitic intrusion of southern Scotland. The melting of quartz diorite was modelled using autoliths, which represent fragments of cogenetic igneous rocks that became incorporated in the fractionating magma. Compared to their quartz diorite parents, the autoliths are enriched to varying degrees in some elements (notably Rb, Nb, Ta, Sm, Y, Yb) and depleted in others (Sr, and Ba); Eu and P are also depleted in the more assimitated autoliths. The compositions of melts that could be derived from assimilation of the autoliths have also been calculated: their REE patterns reveal a light REE enrichment, low concentrations of heavy REEs (1–3 x chondrite) and a positive Eu anomaly. The calculated degrees of melting vary from 35% in the least assimilated to 84% in the most assimilated autolith (assuming a bulk distribution coefficient of 10 for the most compatible element). Results from modelling of xenolith compositions (derived from metasediments) are also reported, but because of uncertainties in the composition of the parental sediment, these data are subject to larger errors. They do, however, indicate that resultant partial melts are distinctly different from those derived by partial melting of autoliths. In particular, the REE pattern of a greywacke-derived melt shows a slight enrichment in light REEs, greater concentrations of heavy REEs (10 x chondrite) and a small negative Eu anomaly. The calculated degrees of melting of the xenoliths fall in the range of 66–88% (assuming a bulk distribution coefficient of 10 for the most compatible element). The results have direct implications for assimilation and melting of the upper crust. By taking into account how the nature of residual phases is likely to change with depth, it can be demonstrated that some Archaean tonalite gneisses could represent liquids derived by partial melting of igneous material. 相似文献
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中生代华北克拉通岩石圈减薄的证据——以河北武安固镇杂岩体为例 总被引：3，自引：3，他引：0
本文对位于华北克拉通中部的固镇侵入杂岩体(闪长岩、二长岩、石英二长岩和正长岩)进行了野外地质调查、岩相学、矿物学、地球化学、锆石U-Pb定年、Sr-Nd同位素和Lu-Hf同位素研究,进而探讨其形成时代、源区和成因,以期得到关于华北克拉通中部中生代岩石圈减薄研究的新启示。研究区岩体形成时代和岩石结构有一定关联性,总体来看,等粒结构的岩体形成时代早于似斑状结构岩体,研究区岩浆活动可分为两个期次:第一期次岩浆活动形成等粒结构的深成岩体,包括中细粒闪长岩、二长岩、石英二长岩和正长岩,形成时代约为130～135Ma;第二期次岩浆活动形成浅部的似斑状岩体,包括似斑状闪长岩和石英二长岩,形成时代约为127Ma。结合野外观察、岩相学、矿物学、地球化学等特征,讨论分析了固镇杂岩体的成因:固镇闪长岩富镁,高Mg~#值,Cr、Ni含量较高,富集LILE和LREE,亏损HFSE,铕异常不明显,具有高镁安山岩(HMA)性质,是与其相对应的侵入岩。固镇高镁闪长岩是被俯冲板片熔体和流体交代后的地幔橄榄岩部分熔融的产物,岩浆在上升途中与地壳发生了较弱的同化混染。固镇正长岩形成于加厚陆壳的部分熔融,地壳厚度约为40～67km。固镇二长岩是由区内正长岩和高镁闪长岩混合形成。研究区石英二长岩是区内高镁闪长岩与另一种更富硅的岩浆混合形成。俯冲板片物质(流体+熔体)对固镇高镁闪长岩的形成有重要贡献,显示出古太平洋板块俯冲作用的影响也涉及到了NCC中部,但受影响的程度小于NCC东部;正长岩形成于加厚陆壳部分熔融,显示出拆沉作用在中生代NCC中部岩石圈减薄过程中发挥了重要作用。结合角闪石温压计的计算结果和前人研究成果可以推测,NCC中部大规模拆沉作用发生的时间节点为127Ma。 相似文献
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Fluid‐fluxed melting and melt loss in a syntectonic contact metamorphic aureole from the Variscan eastern Pyrenees 
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下载免费PDF全文 Open‐system behaviour through fluid influx and melt loss can produce a variety of migmatite morphologies and mineral assemblages from the same protolith composition. This is shown by different types of granulite facies migmatite from the contact aureole of the Ceret gabbro–diorite stock in the Roc de Frausa Massif (eastern Pyrenees). Patch, stromatic and schollen migmatites are identified in the inner contact aureole, whereas schollen migmatites and residual melanosomes are found as xenoliths inside the gabbro–diorite. Patch and schollen migmatites record D1 and D2 structures in folded melanosome and mostly preserve the high‐T D2 in granular or weakly foliated leucosome. Stromatic migmatites and residual melanosomes only preserve D2. The assemblage quartz–garnet–biotite–sillimanite–cordierite±K‐feldspar–plagioclase is present in patch and schollen migmatites, whereas stromatic migmatites and residual melanosomes contain a sub‐assemblage with no sillimanite and/or K‐feldspar. A decrease in X Fe (molar Fe/(Fe + Mg)) in garnet, biotite and cordierite is observed from patch migmatites through schollen and stromatic migmatites to residual melanosomes. Whole‐rock compositions of patch, schollen and stromatic migmatites are similar to those of non‐migmatitic rocks from the surrounding area. These metasedimentary rocks are interpreted as the protoliths of the migmatites. A decrease in the silica content of migmatites from 63 to 40 wt% SiO2 is accompanied by an increase in Al2O3 and MgO+FeO and by a depletion in alkalis. Thermodynamic modelling in the NCKFMASHTO system for the different types of migmatite provides peak metamorphic conditions ~7–8 kbar and 840 °C. A nearly isothermal decompression history down to 5.5 kbar was followed by isobaric cooling from 840 °C through 690 °C to lower temperatures. The preservation of granulite facies assemblages and the variation in mineral assemblages and chemical composition can be modelled by ongoing H2O‐fluxed melting accompanied by melt loss. The fluids were probably released by the crystallizing gabbro–diorite, infiltrating the metasedimentary rocks and fluxing melting. Release of fluids and melt loss were probably favoured by coeval deformation (D2). The amount of melt remaining in the system varied considerably among the different types of migmatite. The whole‐rock compositions of the samples, the modelled compositions of melts at the solidus at 5.5 kbar and the residues show a good correlation. 相似文献
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青藏高原西部班公湖-怒江缝合带西端的班公湖地区分布着一系列南北向和东西向岩脉: 花岗斑岩和闪长玢岩.通过岩石地球化学系统分析和锆石U-Pb LA-ICP-MS年龄测定, 指出这些岩脉代表了班公湖中特提斯洋盆闭合后的地壳伸展事件.呈南北向产出的花岗斑岩脉13个锆石颗粒测试结果给出了79.59±0.32Ma(MSWD=1.08)的加权平均年龄; 既有南北向也有东西向产出的闪长玢岩脉6个锆石颗粒给出了75.9±1.2Ma(MSWD=2.8)的加权平均年龄.这些结果表明班公湖岛弧带发生在晚白垩世的地壳伸展作用一开始只沿东西向进行, 稍后南北向也开始伸展.岩石地球化学特征表明, 2种脉岩都具有岛弧岩浆特征, 这是由于岩浆源区的印度洋MORB型地幔受到了来自俯冲沉积物熔体的交代.处于较深部位的闪长玢岩源区参与交代的沉积物熔体大体在1%~10%之间, 部分熔融程度约为8%~15%;处于较浅部位的花岗斑岩源区参与交代的沉积物熔体约在10%~15%之间, 部分熔融程度大于15%. 相似文献
16.
安徽铜陵矿集区是我国长江中下游构造—岩浆—成矿带中一个重要的铜金多金属成矿区,区内广泛发育晚中生代以石英闪长岩和花岗闪长岩为主的中酸性闪长质侵入岩体,且其与成矿关系密切。关于铜陵矿集区侵入岩的成因,前人已有大量研究成果发表,但仍存有一定争议。本文在广泛收集前人研究资料和成果的基础上,选择区内铜官山石英闪长岩体和新屋里、胡村花岗闪长岩体开展全岩Sr-Nd同位素和锆石原位Hf-O同位素分析,以进一步探讨其成因机制。研究表明,石英闪长岩和花岗闪长岩的结构构造和矿物组成特征相似,全岩主量元素、微量元素和稀土元素组成特征也基本一致,均属高钾钙碱性岩石系列,并具有埃达克质岩石特征。石英闪长岩ISr值为0.707 2～0.709 0,εNd（t）值为-13.0～-8.3,锆石εHf（t）值为-23.5～-8.7,δ18O值为6.5‰～7.4‰;花岗闪长岩ISr值0.707 7～0.709 8,εNd（t）值为-13.6～-8.5,锆石εHf（t）值为-19.0～-7.4,δ18O值为6.7‰～8.1‰。石英闪长岩和花岗闪长岩Sr-Nd同位素组成特征和锆石Hf-O同位素组成特征亦基本一致,指示它们具有相同的成岩物质来源。结合区域地质背景和构造演化,本文认为,铜陵矿集区石英闪长岩和花岗闪长岩为富集岩石圈地幔岩浆与壳源埃达克质岩浆混合并上升侵位所形成,富集岩石圈地幔岩浆并非起源于古太平洋俯冲洋壳或俯冲洋壳析出流体交代的富集岩石圈地幔,而是新元古代华夏洋俯冲析出流体交代扬子板块岩石圈地幔所形成,壳源埃达克质岩浆为新元古代华夏板块与扬子板块碰撞之后形成的新生地壳熔融而成。铜陵矿集区晚中生代大规模岩浆作用的诱因是大陆板内构造背景下富集岩石圈地幔部分熔融岩浆上涌加热以及受古太平洋板块挤压和地壳加厚再转向拉张应力下的减压熔融。 相似文献
17.
Pelitic hornfelses within the inner thermal aureole of the Etive igneous complex underwent limited partial melting, generating agmatic micro‐stromatic migmatites. In this study, observed volume proportions of vein leucosomes in the migmatites are compared with modelled melt volumes in an attempt to constrain the controls on melting processes. Petrogenetic modelling in the MnNCKFMASHT system was performed on the compositions of 15 analysed Etive pelite samples using THERMOCALC. Melt modes were calculated at 2.2 kbar (the estimated pressure in the southern Etive aureole) from solidus temperatures to 800 °C for both fluid‐absent and fluid‐present conditions. Volume changes accompanying fluid‐absent melting at 2.2 kbar were also calculated. P–T pseudosections reproduce the zonal sequence of the southern Etive aureole fairly well. The modelled solidus temperatures of silica‐rich pelitic compositions are close to 680 °C at 2.2 kbar and, in the absence of free fluid, melt modes in such compositions rise to between 12 and 29% at 800 °C, half of which is typically produced over the narrow reaction interval in which orthopyroxene first appears. Silica‐poor compositions have solidus temperatures of up to ～770 °C and yield <11.4% melt at 800 °C under fluid‐absent conditions. For conditions of excess H2O, modelled melt modes increase dramatically within ～13 °C of the solidus, in some cases to >60%; by 800 °C they range from 61 to 88% and from 29 to 74% in silica‐rich and silica‐poor compositions, respectively. Calculated volume changes for fluid‐absent melting are positive for all modelled compositions and reach 4.5% in some silica‐rich compositions by 800 °C. Orthopyroxene formation is accompanied by a volume increase of up to 1.48% over a temperature increase of as little as 2.7 °C, supporting the arguments for melt‐induced ‘hydrofracturing’ as a viable melt‐escape mechanism in low‐P metamorphism. Mineral assemblages in the innermost aureole support previous conclusions that partial melting took place predominantly under fluid‐absent conditions. However, vein leucosome proportions, estimated by image analysis, do not show the expected correlation with grade, and are locally greatly in excess of melt modes predicted by fluid‐absent models, particularly close to the melt‐in isograd. Melting of interlayered psammites, addition of H2O from interlayered melt‐free rocks, and metastable persistence of muscovite are ruled out as major causes of the excess melt anomaly. The most likely cause, we believe, is that local variations existed in the amount of fluid available at the onset of melting, promoted by focussing of fluid released by dehydration in the middle and outer aureole; however, some redistribution of melt by compaction‐driven flow through the vein channel network cannot be ruled out. The formation of melt‐filled fractures in the inner Etive aureole was assisted by stresses that caused extension at high angles to the igneous contact. The fractures were probably caused either by transient pressure reduction in the diorite magma chamber associated with a second phase of intrusion, or by sub‐solidus thermal contraction in the diorite pluton during the early stages of inner‐aureole cooling. 相似文献