第三章 地磁条带与海底扩张

(一)海洋地磁测量与处理 地球磁场总强度的测量使用G-801/3型质子旋进磁力仪。测量工作与多道地震、重力测量等同步进行。探头电缆长500m,以降低船磁的影响。由于船磁影响与探头至船距离的三次方成反比,目前的措施可将此影响降至1nT以下,故可忽略不计。 为消除区域场的影响,理应使用国际地磁参考场IGRF1985来进行改正,但为节约时间起见,本次采用多项式来逼近IGRF,两者的差在整个测区内不足1nT,其结果是可信赖     

Numerical Solution of Lock-Release Gravity Current with Viscous Self-Similar Regime

Lock-release gravity currents with a viscous self-similar regime are simulated by use of the renormalization group(RNG) k - ε model for Reynolds-stress closure. Besides the turbulent regime with initially a slumping phase of a conslant current front speed and later an inviseid self-similar phase of front speed decreasing as t^-1/3(where t is the time measured from release), the viseous self-similar regime is satisfactorily reproduced with front speed decreasing as t^-4/5,consistent with well known experimental observations.     

标志沉积层磁组构特征及其古环境意义研究

通过对长江三角洲及其邻近区域埋藏古土壤、潮坪、长江下游河道浸滩、舟山滨岸风成沙丘、南京黄土古土壤序列沉积体的磁组构测量统计分析，取得了各自的标志特征。该２特征揭示出，舟山滨岸风成沙丘与南京黄土吉土壤序列沉积的搬运介质能量位相基本一致，其物源来向却显示出巨大差异；上述两类沉积体与上述现今潮坪、河道漫滩沉积体地搬运介质能量位相及物源来向均显示出绝然不同的标志特征。然而浸滩物源来民南京黄土的物尖兵为向却     

加拿利区域的热点

以 ДВЕрошенко为首的俄罗斯科学院海洋研究所大西洋分部的专家们 ,审查了有关加拿利群岛、马德拉岛和佛得角群岛是由于上升地幔流在热点区活动而产生的假说。对这个假说有利的证据是 ,在加拿利群岛上火山岩的年龄由西向东随着远离强烈的火山活动区而增加。但是认为这只是一种趋向 ,还带有很大的不确定性 ,再加上群岛不是位于同一海岭上 ,还有在非洲沿岸未发现年龄更为古老的同类岩石。地幔流在其上部运动的板块上留下了火山形成物的痕迹。它们呈东西向弧状延伸 ,并不进入大陆。科学家们研究了深海钻探计划和大洋钻探计划报告中有…     

用Geosat高度计数据观测黑潮流系的低频变化

对Ｇｅｏｓａｔ高度计ＥＲＭ Ｔ２－ＧＤＲｓ共２．３ａ的海面高度数据进行了处理，研究区域为西北太产洋１０°￣４５℃Ｎ，１２０℃￣１６０°Ｅ，包括整个黑潮流系，时间段为１９８６年１１月至１９８９年３月，经过数据筛选，地球物理、环境因子校正及轨道误差较正后，用客观分析方法得到时空均匀的５０个时间序列的海面高度异常场，Ｇｅｏｓａｔ高度计的海面高度异常与验潮站实测水位高度符合较好，之证明处理结果是可信的，海     

希尔伯特变换快速计算及其在磁二度体△T解释中的应用

重磁数据处理的根本任务是从观测数据中提取更多的信息，以丰富重磁异常解释的方法，提高地质解释结果的准确性和可靠性。希尔伯特变换是数据处理的一种方法，近几年在重磁异常中已有所应用，主要有利用希尔伯特变换进行二维位场分量的互算；通过二度体重磁异常的某一分量与其希尔伯特变换来反演异常体埋藏深度和产状要素。     

地形和流同时影响下波向线的数值计算

本文提出一种同时考虑地形和均匀流影响的波向线数值解法及其具体的计算步骤。作为例子，对一种理想的简单地形作了数值计算并绘出波向线图．计算结果表明．流对波浪折射有明显的作用。     

Numerical Study on Instantaneous Discharge of Unsorted Particle Cloud in Cross Flow

The mixing characteristics of particles such as dredged sediment of variable size discharged into cross flow are studied by a 3D numerical model, which is developed to model the particle-fluid two-phase flow. The Eulerian method with the modified k-ε parameterization of turbulence for the fluid phase is used to solve fluid phase, while a Lagrangian method for the solid phase (particles), both the processes are coupled through the momentum sources. In the model the wake turbulence induced by particles has been included as additional source term in the k-ε model; and the variable drift velocities of the particles are treated efficiently by the Lagrangian method in which the particles are tracked explicitly and the diffusion process is approximated by a random walk model. The hydrodynamic behavior of dumping a cloud of particles is governed by the total buoyancy of the cloud, the drag force on each particle and the velocity of cross-flow. The computed results show a roughly linear relationship between the displacement of the frontal position and the longitudinal width of the particle cloud. The particle size in the cloud and the velocity of cross flow dominate the flow behavior. The computed results are compared with the results of laboratory experiments and satisfactory agreement is obtained.     

The Mathematical and Parameterized Expressions for Wave Induced Excess Flow of Momentum

Wave induced excess flow of momentum(WIEFM)is the averaged flow of momentum over a wave period due to wave presence,which may also be called 3-D radiation stress.In this paper,the 3-D current equations with WIEFM are derived from the averaged Navier-Stokes equations over a wave period,in which the velocity is separated into the large-scale background velocity,the wave particle velocity and the turbulent fluctuation velocity.A concept of wave fluctuating layer(WFL)is put forward,which is the vertical column from the wave trough to wave ridge.The mathematical expressions of WIEFM in WFL and below WFL are given separately.The parameterized expressions of WIEFM are set up according to the linear wave theory.The integration of WIEFM in the vertical direction equals the traditional radiation stress(namely 2-D radiation stress)given by Longuet-Higgins and Stewart.