地幔流体与地球的放气作用

地幔流体的形成、聚集和渗透是引起地幔交代作用的主要营力。地幔交代作用发育的强弱决定着所生成岩浆的碱性程度。地幔流体和部分熔融体高度富集不相容元素,它们与亏损地幔的相互作用可以使后者发生ＬＲＥＥ和不相容元素的局部富集。通过板块俯冲作用使地球表层的ＣＯ２进入地幔,参加地球的碳循环。热点岩浆来源的ＣＯ２中含有部分循环的ＣＯ２,而大洋中脊玄武岩中的ＣＯ２主要是原始地球的ＣＯ２。携带ＣＨ４和Ｈ２Ｏ的流体渗透至被俯冲带带入地幔的物质,使碳酸盐化的榴辉岩还原而形成含金刚石的榴辉岩和富水流体,并诱发局部熔融,所形成的熔体以火山喷发的形式上升到地表。地幔岩石中含有大量的流体,它们主要以流体包裹体的形式存在于地幔矿物中。几乎在所有的上地幔环境下形成的矿物中均找到了流体包裹体。包裹体内流体的成分主要是ＣＯ２,ＣＨ４,Ｈ２Ｏ及少量Ｈ２,Ｎ２等。     

壳幔化学不均一性与块体地球化学边界研究

壳幔派生岩石的多元同位素体系研究表明,地球存在块体的化学不均一性,可划分出地球化学省,并以地球化学急变带作为边界。全球总体上分成东冈瓦纳（如华夏与青藏—印支）、西冈瓦纳、太平洋（如佳木斯、中蒙古、辽胶渤、北疆—南戈壁）与劳亚（如华北、中朝、兴安、塔里木等）四种类型的地球化学省。地球化学急变带与地球物理场变化存在密切关系。在构造上,地球化学急变带可分成构造显性与构造隐性两种类型。应用深、浅构造立交模型及其相互转化可对两种类型地球化学急变带的出现作出较合理的解释。地球化学急变带,特别是急变带的转折端对超大型矿床和成矿密集区的分布有密切控制作用;显性急变带主要表现为与动力变质和岩浆活动有关的改造成矿作用,隐性急变带主要表现为火山与热水沉积成矿作用。具有工业意义的油气田均位于构造隐性急变带与中新生代盆地的立交地段。     

豫西中新生代地球动力学探讨

以隆断区和断陷盆地地壳厚度的显著差异,隆断区与盆地分界的深大断裂（边缘断裂,与地幔斜坡对应）,隆断区和盆地的岩浆作用及现代地热活动,盆地沉降历史四个地质特征为依据,作者认为本区盆岭构造形成的动力学机制是：中新生代上地幔起伏和下地壳不均匀岩浆熔融并由此产生的岩浆作用和热能、重力地质作用等引起的物质膨胀和岩浆侧向上侵入、岩浆冷凝和体积收缩导致同沉积断层运动,形成本区盆岭构造。     

Mantle convection with a brittle lithosphere: thoughts on the global tectonic styles of the Earth and Venus

Plates are an integral part of the convection system in the fluid mantle, but plate boundaries are the product of brittle faulting and plate motions are strongly influenced by the existence of such faults. The conditions for plate tectonics are studied by considering brittle behaviour, using Byerlee's law to limit the maximum stress in the lithosphere, in a mantle convection model with temperature-dependent viscosity.
When the yield stress is high, convection is confined below a thick, stagnant lithosphere. At low yield stress, brittle deformation mobilizes the lithosphere which becomes a part of the overall circulation; surface deformation occurs in localized regions close to upwellings and downwellings in the system. At intermediate levels of the yield stress, there is a cycling between these two states: thick lithosphere episodically mobilizes and collapses into the interior before reforming.
The mobile-lid regime resembles convection of a fluid with temperature-dependent viscosity and the boundary-layer scalings are found to be analogous. This regime has a well defined Nusselt number–Rayleigh number relationship which is in good agreement with scaling theory. The surface velocity is nearly independent of the yield stress, indicating that the 'plate' motion is resisted by viscous stresses in the mantle.
Analysis suggests that mobilization of the Earth's lithosphere can occur if the friction coefficient in the lithosphere is less than 0.03–0.13—lower than laboratory values but consistent with seismic field studies. On Venus, the friction coefficient may be high as a result of the dry conditions, and brittle mobilization of the lithosphere would then be episodic and catastrophic.     

Eigendecomposition of the two-point correlation tensor for optimal characterization of mantle convection

The two-point correlation tensor provides complete information on mantle convection accurate up to second-order statistics. Unfortunately, the two-point spatial correlation tensor is in general a data-intensive quantity. In the case of mantle convection, a simplified representation of the two-point spatial correlation tensor can be obtained by using spherical symmetry. The two-point correlation can be expressed in terms of a planar correlation tensor, which reduces the correlation's dependence to only three independent variables: the radial locations of the two points and their angular separation. The eigendecomposition of the planar correlation tensor provides a rational methodology for further representing the second-order statistics contained within the two-point correlation in a compact manner. As an illustration, results on the planar correlation are presented for the thermal anomaly obtained from the tomographic model of Su, Woodward & Dziewonski (1994 ) and the corresponding velocity field obtained from a simple constant-viscosity convection model Zhang & Christensen 1993 ). The first 10 most energetic eigensolutions of the planar correlation, which constitute an almost three orders of magnitude reduction in the data, capture the two-point correlation to 97 per cent accuracy. Furthermore, the energetic eigenfunctions efficiently characterize the thermal and flow structures of the mantle. The signature of the transition zone is clearly evident in the most energetic temperature eigenfunction, which clearly shows a reversal of thermal fluctuations at a depth of around 830  km. In addition, a local peak in the thermal fluctuations can be observed around a depth of 600  km. In contrast, due to the simplicity of the convection model employed, the velocity eigenfunctions exhibit a simple cellular structure that extends over the entire depth of the mantle and do not exhibit transition-zone signatures.     

岩浆作用过程的一种有效判别方法──(1/C_i)-(1/C_j)和(或)lgC_i-lgC_j图解法

本文利用一种新的方法和（或）lgCi－lgCi图解法，明显地区分出地幔平衡部分熔融作用和岩浆分离结晶作用。并以亚速尔群岛中Terceira岛火山岩和汉诺坝玄武岩的实际资料验证了所推导的方法。     

松辽残留地台区成因机制研究

本文在讨论松辽残留地台区特征的基础上，根据松辽地台区地幔流场的演变历史及热流演化特征，探讨了该区的成因机制。