The Mordor Alkaline Igneous Complex,Central Australia: PGE-enriched disseminated sulfide layers in cumulates from a lamprophyric magma

The Mordor Alkaline Igneous Complex (MAIC) is a composite intrusion comprising a body of syenite and a funnel-shaped layered mafic–ultramafic intrusion of lamprophyric parentage, the Mordor Mafic–Ultramafic Intrusion or MMUI. The MMUI is highly unusual among intrusions of lamprophyric or potassic parentage in containing primary magmatic platinum-group element (PGE)-enriched sulfides. The MMUI sequence consists largely of phlogopite-rich pyroxenitic cumulates, with an inward dipping conformable layer of olivine-bearing cumulates divisible into a number of cyclic units. Stratiform-disseminated sulfide accumulations are of two types: disseminated layers at the base of cyclic units, with relatively high PGE tenors; and patchy PGE-poor disseminations within magnetite-bearing upper parts of cyclic units. Sulfide-enriched layers at cycle bases contain anomalous platinum group element contents with grades up to 1.5 g/t Pt+Pd+Au over 1-m intervals, returning to background values of low parts per billion (ppb) on a meter scale. They correspond to reversals in normal fractionation trends and are interpreted as the result of new magma influxes into a continuously replenished magma chamber. Basal layers have decoupled Cu and PGE peaks reflecting increasing PGE tenors up-section, due to increasing R factors during the replenishment episode, or progressive mixing of between resident PGE-poor magma and more PGE-enriched replenishing magma. The presence of PGE enriched sulfides in cumulates from a lamprophyric magma implies that low-degree partial melts do not necessarily leave sulfides and PGEs in the mantle restite during partial melting. Electronic supplementary material  The online version of this article (doi:) contains supplementary material, which is available to authorized users.     

内蒙古天和永玄武岩成因：岩相学与矿物学分析

天和永地区南北向出露的小面积单层碱性玄武岩,岩石中出现至少三种矿物共生组合关系。所有岩石均以橄榄石作为主要斑晶矿物,大颗粒环带橄榄石斑晶中心镁值为89．5,边缘镁值为70．3,小颗粒环带橄榄石镁值46．2～78．9。粒径最小的橄榄石聚集体和散布的基质橄榄石均无明显环带,前者镁值67．4～68．1,后者镁值65．5—72．1;单斜辉石由相对高钛高铝贫硅的散布柱状辉石和相对低钛低铝富硅的聚集粒状辉石组成,前者形成于低压快速淬火环境,镁值65．1—77．1,后者形成于富含挥发份的低压低过冷度环境,镁值77．7～78．0。所有单斜辉石均以次透辉石为主,个别为深绿辉石;斜长石以包含结构产出为主,为相对偏酸性的中长石An=33．7～37．4,CaO含量低与早期大量单斜辉石结晶有关。由于残余岩浆内K,0和Na20含量富集且极不均一,晚期结晶的长石同时出现了高钠长石、K-高钠长石（歪长石）和K-透长石;钛铁氧化物多数为晚期结晶的细粒基质矿物,少量以0．3ram左右的斑晶和橄榄石斑晶中的包裹体形式存在,可归属为钛铁尖晶石（Usp）-磁铁矿（Mt）固溶体系列,晚期逐渐向贫铝、铬和富钛方向演化。由于以上各种造岩矿物的晶出,导致残余岩浆形成的火山玻璃向贫镁、铁、钙和富铝、钾方向演化,火山玻璃的全碱含量变异趋势与全岩类似,均和SiO2含量无明显相关性,火山玻璃具有响岩和粗面安山岩成分特征,K2O／Na2O值变化大0．68～1．61,均为钾玄岩系列,Na2O含量依然呈现宽区间特征,是天和永玄武岩由钾质过渡到钠质的主要原因。天和永玄武质岩浆从地幔运移到地表仅需5小时-5天,大颗粒斑晶橄榄石和小颗粒基质橄榄石生长仅需几小时到几天,前者形成无须深部岩浆房停留,后者近似晚期岩浆快速淬火时间。高镁橄榄石斑晶与残余岩浆的扩散平衡时间约42天～252天。深部结晶的橄榄石在运移途中和地表流动过程中缺乏足够的时间和适宜的动力学条件而无法离开岩浆体系。全岩与火山玻璃间缺少中间过渡成分,呈两个相对集中的端元组分存在亦由晶出矿物无法离开岩浆体系所致。天和永玄武岩的成岩时间尺度远小于同化混染和岩浆分异的时间尺度,是岩浆作用过程未能明显影响其不均一原生岩浆性质的主要原因。因此,岩浆作用的某些物理过程分析是认识岩浆起源与岩浆作用过程及其对火成岩多样性的贡献的重要方面,同时对于理解和约束岩浆作用的某些化学过程也是十分有益的。     

新疆东天山葫芦岩体岩石学与地球化学研究

葫芦岩体位于康古尔—黄山韧性剪切带东段,地表出露面积0.75km²。主要岩石类型有辉长闪长岩、辉长岩、辉石岩、辉橄岩、橄揽岩。岩相之间多呈渐变过渡关系,局部也有侵入接触。主量元素化学组成基本上属拉斑玄武岩系列。岩石相对富集LREE、适度亏损高场强元素(Nb、Ta、Ti)。岩浆演化过程中发生了较弱的同化混染作用。橄榄石、斜方辉石、单斜辉石和斜长石的分离结晶作用是岩浆演化的主要机制。四件样品ε_Nd(t)值(＋6.4~+7.1),一件样品的ε_Sr(t)=+3.4,其余三件的ε_Sr(t)值(-10.1~-9.3),²⁰⁶Pb/²⁰⁴Pb(18.091~18.513)、²⁰⁷Pb/²⁰⁴Pb(15.459~15.528)、²⁰⁸Pb/²⁰⁴Pb(37.526~38.126)。元素地球化学和Nd、Sr、Pb同位素体系表明,源区软流圈来源的岩浆中混入了富集岩石圈地幔来源的岩浆。稀土元素地球化学证明,熔融作用发生于尖晶石稳定域内。由此可见,岩体是尖晶石稳定域内占主体的软流圈地幔与富集岩石圈地幔相互作用的结果。     

胶州湾海水微表层粘度及其在海-气通量计算中的作用

物质海 -气通量计算新建议中将物质海 -气通量计算公式 F=K(CL- b Cg)中的 CL 用CL ( SML ) 代替。本文着重于对公式中质量迁移系数 K的讨论。在测定了海水微表层、次表层水粘度并同时测定了其它一些化学参量基础上 ,得出如下结论 :海水粘度与盐度、碱度有一定相关性 ;微表层与次表层海水的粘度变化小于 3%。因此 ,海水微表层效应影响 K值 ,与海水微表层效应影响物质浓度相比 ,可以不考虑。     

浅海流体动力学一种含变湍粘性系数的流速分解模型(Ⅱ)——模型在超浅海风暴潮零阶问题中的应用

本文将流速分解模型应用于作为超浅海风暴潮的渤海风潮,并讨论了变湍粘性系数的确定。作为一个初步的,但较为成功的数值试验例子,描述了实际风场作用下的渤海风潮,比较了变湍粘性系数模型与常湍粘性系数模型的计算结果间的差异。     

Modeling of the eddy viscosity by breaking waves

Breaking wave induced nearsurface turbulence has important consequences for many physical and biochemical processes including water column and nutrients mixing,heat and gases exchange across air-sea interface.The energy loss from wave breaking and the bubble plume penetration depth are estimated.As a consequence,the vertical distribution of the turbulent kinetic energy(TKE),the TKE dissipation rate and the eddy viscosity induced by wave breaking are also provided.It is indicated that model results are found to be consistent with the observational evidence that most TKE generated by wave breaking is lost within a depth of a few meters near the sea surface.High turbulence level with intensities of eddy viscosity induced by breaking is nearly four orders larger than υwl(=κuwz),the value predicted for the wall layer scaling close to the surface,where uw is the friction velocity in water,κ with 0.4 is the von Kármán constant,and z is the water depth,and the strength of the eddy viscosity depends both on wind speed and sea state,and decays rapidly through the depth.This leads to the conclusion that the breaking wave induced vertical mixing is mainly limited to the near surface layer,well above the classical values expected from the similarity theory.Deeper down,however,the effects of wave breaking on the vertical mixing become less important.     

湍流数值模拟中封闭模式应用的局限性

通过对琼州海峡的潮流场特征进行数值模拟，指出了选择不同的特征混合长度表达式对数值模拟结果的影响，表明了基于特征混合长度理论的流封闭模式在近海湍流数值模拟中应用的局限性。     

Effects of scattering and resonance on energy dissipation of an internal tide in a narrow shelf

The effects of scattering and resonance on the energy dissipation of an internal tide were investigated using a two-dimensional model which is a reassembled version of the theoretical generation model devised by Rattray et al. (1969) for internal tide. The basic character of the scattering process at the step bottom was first investigated with a wide shelf model. When the internal wave incited from a deep region (Region II) into the shallow shelf region (Region I), a passing wave into the shallow region, a reflected wave into the deep region, and a beam-like wave, i.e. a scattered wave (SW), emanated at the step bottom. The SW, which consists of the superposition of numerous internal modes, propagated upward/downward into both regions. The general properties of the SW were well expressed around the shelf edge, even in the present model with viscosity effect. The amplitude of the SW decreased dramatically when the depth of the velocity maximum of the incident internal wave in Region II corresponded with the depth of the shelf edge. In the narrow shelf model, where the decay distance of the internal wave in Region I is longer than the shelf width, the incident internal wave reflected at the coast to form a standing wave. When the internal wave in Region I is enhanced by the resonance, the energy of the SW in Region II is also intensified. Furthermore, the energy of the modes in Region II predominated when the velocity maximum is identical to that of the dominant mode in Region I. These results suggest that the spatial scale of shelf region is a very important factor governing the energy dissipation of the internal tide through reflection and scattering in a narrow shelf.     

渤海垂直湍流混合强度季节变化的数值模拟

渤海为极浅陆架海 ,其中湍流耗散作用显著。将三维斜压陆架海模式 HAMSOM应用于渤海 ,以渤海周边台站每天 4次的常规气象资料作为风和热驱动 ,渤海海峡开边界以 5个主要分潮调和常数计算水位强迫 ,计算了渤海 1982年水文要素和流场变化 ,并用模式以湍的局地平衡理论封闭计算出垂直湍流粘性的时空分布。结果表明 :渤海湍流混合冬强夏弱 ,变化幅度较大 ( 10～ 2 0 0 cm2 / s) ,这是风搅拌和潮混合的湍流输入在密度层化调整下的结果 ;风的作用在冬季强于潮的作用 ,而底层则由潮混合控制呈现半月周期 ;渤海湍粘性系数的空间分布十分复杂 ,这是在渤海地形和岸形轮廓限制下 ,由一定大气条件驱动的流场和密度场导致的湍流混合强度不同所致