结构海床耦合系统动力分析数值模型及考察

基于改进的哈丁模型建立了结构海床耦合系统的等效线性化动力分析模型。等效阻尼比是对土体进行等效线性化分析的重要组成,论文着重对土体阻尼对结构海床耦合系统的影响效应进行了考察。接触面分离力是运用滑动库仑摩擦模型进行接触面效应模拟的重要参数,在以前的工作基础上,文中提出了新的结构-海床接触面分离力模型并进行了考察,使其更符合实际情况     

Time domain method for calculating free field motion of a layered half-space subjected to obliquely incident body waves

In numerical simulation of wave scattering under oblique incident body waves using the finite element method, the free field motion at the incident lateral boundary induced by the background layered half-space complicates the computational area. In order to replace the complex frequency domain method, a time-domain method to calculate the free field motion of a layered half-space subjected to oblique incident body waves is developed in this paper. The new method decouples the equations of motion used in the finite element method and offers an interpolation formula of the free field motion. This formula is based on the fact that the apparent horizontal velocity of the free field motion is constant and can be calculated exactly. Both the theoretical analysis and numerical results demonstrate that the proposed method offers a high degree of accuracy.     

紫色土典型三角形层状剖面入渗模拟

通过室内特制的土壤水分入渗试验装置,分别设置上粗下细和上细下粗两种典型不同质地紫色土三角形层状剖面,探讨典型不规则层次结构的土壤入渗特性。结果显示,同一三角形层状剖面入渗,粗质土半剖面的垂直湿润锋随时间推进速度快于细质土。对于粗质土,上细下粗剖面设置下其半剖面的垂直湿润锋随时间推进速度快于上粗下细,但对于细质土,两种层状剖面设置下其垂直湿润锋随时间推进速度差异不明显。无论上粗下细,还是上细下粗,两种层状剖面对斜面湿润锋变化曲线影响不大。两种层状剖面入渗,湿润锋、入渗速率与时间均呈极显著幂函数关系。建立的紫色土典型三角形层状剖面入渗模型,经验证,模拟值与实测值具有非常好的一致性,且可与经验模型相互转换,模型参数也具有一定的物理意义。     

Storm-induced turbidity currents on a sediment-starved shelf: Insight from direct monitoring and repeat seabed mapping of upslope migrating bedforms

The monitoring of turbidity currents enables accurate internal structure and timing of these flows to be understood. Without monitoring, triggers of turbidity currents often remain hypothetical and are inferred from sedimentary structures of deposits and their age. In this study, the bottom currents within 20 m of the seabed in one of the Pointe-des-Monts (Gulf of St. Lawrence, eastern Canada) submarine canyons were monitored for two consecutive years using Acoustic Doppler Current Profilers. In addition, multibeam bathymetric surveys were carried out during deployment of the Acoustic Doppler Current Profilers and recovery operations. These new surveys, along with previous multibeam surveys carried out over the last decade, revealed that crescentic bedforms have migrated upslope by about 20 to 40 m since 2007, despite the limited supply of sediment on the shelf or river inflow in the region. During the winter of 2017, two turbidity currents with velocities reaching 0·5 m sec⁻¹ and 2·0 m sec⁻¹, respectively, were recorded and were responsible for the rapid (<1 min) upstream migration of crescentic bedforms measured between the autumn surveys of 2016 and 2017. The 200 kg (in water) mooring was also displaced 10 m down-canyon, up the stoss side of a bedform, suggesting that a dense basal layer could be driving the flow during the first minute of the event. Two other weaker turbidity currents with speeds <0·5 m sec⁻¹ occurred, but did not lead to any significant change on the seabed. These four turbidity currents coincided with strong and sustained wind speed >60 km h⁻¹ and higher than normal wave heights. Repeat seabed mapping suggests that the turbidity currents cannot be attributed to a canyon-wall slope failure. Rather, sustained windstorms triggered turbidity currents either by remobilizing limited volumes of sediment on the shelf or by resuspending sediment in the canyon head. Turbidity currents can thus be triggered when the sediment volume available is limited, likely by eroding and incorporating canyon thalweg sediment in the flow, thereby igniting the flow. This process appears to be particularly important for the generation of turbidity currents capable of eroding the lee side of upslope migrating bedforms in sediment-starved environments and might have wider implications for the activity of submarine canyons worldwide. In addition, this study suggests that a large external trigger (in this case storms) is required to initiate turbidity currents in sediment-starved environments, which contrasts with supply-dominated environments where turbidity currents are sometimes recorded without a clear triggering mechanism.     

攀西地区红格层状岩体的地球化学特征

红格岩体赋存有大型钒钛磁铁矿床，在橄辉岩相带和辉石岩相带底部有铂族元素（PEG）的矿化，是攀西层状岩体中重要的岩体之一，系统分析了红格层状岩体不同岩相带的微量元素和稀土元素特征，探讨了岩浆的结晶分异演化过程，提出岩体主体上是由一个岩浆房经正常的结晶分异形成的，底层的硫化物富集带和中上层位的钒钛磁铁矿是岩浆结晶分异产生的堆积相，并非是岩浆多次脉动式补给的结果。     

平面SV波在层状半空间中沉积谷地周围的散射

采用间接边界元方法求解了入射平面SV波在层状半空间中沉积谷地周围的散射问题.问题的解答包含自由场和散射场两部分.自由场可由直接刚度法求得,散射场由层状半空间中斜线荷载动力格林函数来模拟.文中以入射平面SV波在基岩上单一土层中沉积谷地周围散射为例研究了土层和沉积谷地周围的影响.结果表明,由于考虑了土层的动力特性,平面SV...     

南阿尔金山清水泉镁铁-超镁铁质侵入体LA-ICP-MS 锆石U-Pb同位素定年及其意义

清水泉镁铁-超镁铁质层状侵入体位于南阿尔金山阿帕—茫崖构造带中-北部的清水泉地区,其北部与南阿尔金山超高压变质带紧邻。该岩体包含有3～4个由辉石橄榄岩-角闪辉长岩构成的岩浆旋回,与元古宙变质沉积岩系呈侵入接触关系。对其中的角闪辉长岩进行了LA-ICP-MS锆石U-Pb同位素测年,其206Pb/238U表面年龄为(461±2)Ma～(471±2)Ma,其加权平均值为(467.4±1.4)Ma(n=21,MSWD=2.5),所测锆石具有明显的岩浆振荡环带,Th/U比值为0.32～1.16(平均0.64)。测年结果显示,清水泉镁铁-超镁铁质岩体的形成时代晚于南阿尔金山超高压变质岩的峰期变质时代(504～487 Ma),而老于该地区A型花岗岩的时代(425 Ma左右)。分析认为,伴随着同时代的"双峰式"岩浆侵入作用及广泛的变质热事件,大约465 Ma时的南阿尔金山已经由前期的陆-陆碰撞造山阶段转入到了碰撞后的裂谷伸展作用阶段。     

HiPAP 100水下定位系统在海底摄像中的应用

分析了HiPAP100高精度声学定位系统及其水下定位原理,阐述了影响水声传播的因素及HiPAP100的解决办法,介绍了水下定位系统在我国海洋区域地质调查海底摄像测站作业中的应用,分析比较海底摄像常规定位与HiPAP100超短基线的定位精度,说明水下定位在海底摄像等水下拖曳和定点作业中的必要性和重要性。     

A superposition scheme to obtain fundamental boundary element solutions in multi‐layered elastic media

A superposition scheme is proposed to obtain a fundamental solution for boundary elements in multi‐layered elastic media. A three‐layered elastic region is obtained by superposing two sets of bonded half‐planes and subtracting one infinite plane. Therefore, the solution for an element in a layered media can be expressed in terms of bonded half‐plane solutions and an infinite‐plane solution. The major advantages of this superposition scheme are: (1) it is unnecessary to introduce elements at the interface, (2) it can be extended to higher‐order element, and (3) it may be applicable to three dimensions easily. The accuracy and performance of the developed model is illustrated by two examples. For the problem of a pressurized two‐dimensional crack within a three‐layered system, the comparison with other numerical results shows the model is quite accurate and efficient. The model is also used for a study of a practical two‐dimensional mining problem in South Africa, i.e. stoping through a dyke with material properties different from the host rock. Copyright © 2000 John Wiley & Sons, Ltd.