华北地块南部巨型陆内俯冲带与秦岭造山带岩石圈现今三维结构

豫西横穿秦岭造山带的反射地震为主的综合地球物理探测，发现秦岭现今北界存在华北地块南部自北向南向秦岭的巨型陆内俯冲带，深达Ｍｏｈｏ面以下，与之相伴而生，在中上地壳发育自南向北的逆冲推构造带，千公里东西向延伸，主要发生于晚白垩世１００Ｍａ±，成为秦岭与华北地区块间中新生代重要陆内构造，它是秦岭造山带岩石圈现今三维结构的基本要素和组成部分，秦岭造山带岩石圈现今结构具有流变学分层的“立交桥”三维结构框架模型。显然它们具有统一的动力学背景，是秦岭造山带现今处于印度－青藏、太平洋和欧亚板块的西伯利亚地块等三大构造动力学体系复合部位，导致其从深部地幔动力学的最新调整到上部地壳响应所发生的壳幔等圈层相互作用的综合产物，可能是大陆长期保存、演化的主要途径与形式之一，具有重要的大陆动力学意义，对中国大陆构造、灾害、环境研究也具重要意义。     

Mianlüe tectonic zone and Mianlüe suture zone on southern margin of Qinling-Dabie orogenic belt

The Mianlue tectonic zone (Mianlue zone), an ancient suture zone in addition to theShangdan suture in the Qinling-Dabie orogenic belt, marks an important tectonic division geo-logically separating north from south and connecting east with west in China continent. To de-termine present structural geometry and kinematics in the Mianlue tectonic zone and to recon-struct the formation and evolution history involving plate subduction and collision in theQinling-Dabie orogenic belt, through a multidisciplinary study, are significant for exploring themountain-building orogenesis of the central orogenic system and the entire process of the majorChinese continental amalgamation during the Indosinian.     

The effects of the thermal state of overriding continental plate on subduction dynamics: Two-dimensional thermal-mechanical modeling

The dynamic process of ocean-continent subduction depends on not only the properties of the subducting oceanic plate, but also the characteristics and state of the overriding continental plate. Numerical models conducted to date have mostly focused on the oceanic lithosphere in this regard; research on the properties of overriding continental lithosphere remains relatively limited, especially the influence of its thermal state on subduction dynamics. Here we explored the performance of continental lithosphere with different thermal states during the subduction process using two-dimensional thermal-mechanical modeling and systematically investigated the effects of the thermal state of overriding continental plate, the age of subducting oceanic plate, and relative convergence rate on subduction dynamics. Modeling results show that:(1) When the geothermal gradient of continental crust is low(between 10 and 15 ℃ km~(-1)), the oceanic plate first subducts at a low angle. As subduction continues, the slab dip gradually increases and the slab begins to retreat rapidly driven by its negative buoyancy, opening an ocean basin ranging from 600 to 1100 km in width. This leads to the decoupling between the overriding continental plate and oceanic plate. As the trench retreat continues, the horizontal deviatoric stress inside the overriding continental crust alternates between being positive and negative in a local area. Thinning of the overriding lithosphere mainly occurs at the region adjacent to the subduction zone, where the surface experiences significant subsidence.(2) When the geothermal gradient of continental crust is higher(greater than 15 ℃ km~(-1)), oceanic plate retreat causes the overriding continental plate to be strongly stretched. In this case, the trench retreat distance decreases and the width of the ocean basin also reduces by between 100 and 1000 km. The horizontal deviatoric stress inside the whole overriding continental crust first manifests as compression and then changes into extension, which causes the surface to first uplift and then slowly subside.(3) Increasing the age of oceanic lithosphere accelerates trench retreat and promotes overriding plate thinning.(4) An advancing overriding continental plate slows down trench retreat. In cases where the geothermal gradient of continental crust is greater than 17.5 ℃ km~(-1), the hot continental crust experiences gravitational collapse and is overthrusted onto oceanic lithosphere, resulting in slow trench retreat. We analyzed the subduction process of the western Paleo-Pacific Plate in the Early Cretaceous based on our modeling results and discussed its possible control on the tectonic evolution of the rift basins in east Asia. We suggest that the development of a wide rift basin system on the Amurian Superterrane in the Early Cretaceous was likely related to slow trench retreat and the collapse of the hot crust, and the formation of a series of passive rift basins in the North China Craton was likely caused by the relatively cold thermal state of the lithosphere and the rapid retreat of the Paleo-Pacific Plate.     

空间节省型堰式沉箱波浪反射与结构优化试验研究

为了同时提升消浪效果和节省海岸空间,对低反射防波堤进行改进,提出了一种空间节省型堰式沉箱结构。通过物理模型试验研究了堰式沉箱在规则波作用下的消能机理,然后采用单因子分析法分析了相对淹没深度、波陡和相对波高对反射系数的影响,并且利用SPSS软件对无因次参数进行非线性回归分析得到了反射系数计算公式。结果表明,内堰消浪室可以形成良好的波能耗散机制,随着有效消浪室个数的增多,消浪效果逐渐增强,使得反射系数的最小值和最大值较非透空直立结构分别降低了60%～90%和10%～30%。基于以上研究成果,给出关于特征水位与内堰的相对位置关系的合理建议,并总结了堰式沉箱结构的优化设计要点,对实际工程应用具有一定的指导意义。     

大别造山带折返剥露历史:来自合肥盆地南缘中生界变质岩碎屑的证据

在合肥盆地南缘广泛分布的中生界内,砾石主要由变质岩碎屑组成。碎屑在地层中分布及垂向上的变化,为重塑造山带折返剥露历史提供了证据。防虎山组和三尖铺组底部砾岩碎屑组合为:石英片岩+云母片岩+石墨片岩+千枚岩+石英岩+脉石英+片麻岩(局部),表明在早侏罗世晚期Pliensbachian期(距今195Ma)之前,佛子岭群和卢镇关群已经折返到地表并遭受剥露。早白垩世凤凰台组、毛坦厂组和周公山组中砾岩碎屑组合为:片岩+石英岩+片麻岩+混合岩+榴辉岩+角闪岩+斜长岩+花岗岩+大理岩等,榴辉岩以及其它基性岩的微量元素特征表明它们可能是一个在早白垩世以前(距今135Ma)折返到地表并遭受完全剥露,而现在已经从造山带消失的超高压构造地层单元。大别造山带出露的超高压变质带(大别杂岩)在北缘中生代地层中目前尚未发现有可靠的沉积记录,推测它们的大规模折返和剥露可能在新生代,并持续到现在。据此认为大别造山带大规模的折返剥露分为3个阶段:早侏罗世之前、晚侏罗世—早白垩世早期和新生代。     

大别造山带超高压变质岩折返隆升的地层学证据—毛坦厂组榴辉岩砾石的启示

大别山北缘地区发育厚达近万米的中新生代碎屑岩，它们记录着大别山造山带和在株罗纪以来的演化历史。在安徽省六安地区毛坦厂组中，发现多块榴辉岩砾石。砾石新鲜，质地坚硬，表明属于第一旋回砾石。榴辉岩由石榴子石、多硅白云母、绿帘石、石英、金红石等组成。具有明显的退变质作用，发育以钠长石和闪石类组成的后合成晶、以及石榴子石周边的次为边。石榴子石以铁铝榴石和钙铝榴石为主，恪地C类榴辉岩。根据其特征应该属于大别山南部和北部超高压榴辉岩。毛坦厂组层位确切，古生物化石和同位素年龄都表明以晚株罗世为主，这一发现表明，在晚株罗世，以榴辉岩为代表的造山带根部物质，即：超高压变质岩已经出露地表，并作为毛坦厂组的物源。因此，大别造山带超高压为质岩折返到地表，最迟在晚株罗世。     

秦岭俯冲板块前缘石炭纪构造-沉积环境

石炭纪处于秦岭南、北板块由俯冲到全面碰撞的重要阶段。在俯冲板块前缘,石炭系发育在两种不同类型的沉积盆地之中。前缘南带盆地的形成与俯冲板块边缘弯曲而导致的浅层水平伸展有关,前缘北带主要为一些小型残余盆地,并明显遭受定向滑移构造的改造。两种不同沉积作用演化是在不同的构造过程中形成的。     

地层证据——对大别造山带汇聚历史的制约

大别造山带的汇聚演化历史一直存在不同的认识,来自扬子陆块和华北陆块显生宙以来的地层记录以及北淮阳地区的地层记录可能为两个陆块的汇聚模式提供制约。通过对扬子陆块与华北陆块显生宙以来岩相古地理进行比较,其中3个阶段相似, 2个阶段差别很大。以浊积岩发育作为俯冲阶段的标志,磨拉石建造出现作为闭合的标志,显生宙以来,大别造山带曾经历了两次俯冲和两次汇聚,俯冲时间分别是晚奥陶世—早志留世和早三叠世,汇聚的时间分别为中 晚泥盆世和中三叠世,早期的汇聚具有软碰撞特征,以上认知得到了北淮阳地区地层、古生物和沉积记录的支持,同时也与大别山造山带榴辉岩的同位素年龄数据基本吻合。高压 超高压变质岩在晚三叠世处于快速折返阶段,早侏罗世以前到达地表,其平均折返隆升速率为39～66mm/a。     

不同破碎波气液混合区发展特征及其运动特性研究

了解波浪破碎速度场的分布特性对于波浪破碎物理机制的研究极为重要,同时,对比研究不同类型破碎产生的气液混合区的演化特征有利于波浪白冠覆盖率模型的完善。在实验室水槽,生成了深水临界波、单次崩破波和单次卷破波,采用图像测速技术获取了波浪破碎图像、波面下水体和气液混合区速度场。结果表明,崩破波的水平向速度u和垂直向速度v在波峰前和波峰后的分布极为不对称,其水平向最大速度u_max并不位于峰顶,而是在主导波峰前0.7η_{m ax}处;卷破波的u_max出现在波峰峰顶前端极小的区域内,且该区域与周围区域的速度梯度极大。崩破波和卷破波生成的气液混合区发展特征也存在差异：崩破波的u_max值大、影响区域长、混合区厚度较小、各区域影响时间短;而卷破波的各项特征参数与崩破波形成对比。