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海水是一种高电导率的流体。不停运动的海水因切割地磁场而产生感应电流,从而产生感应电磁场。本文从麦克斯韦方程出发推导了地磁场三分量作用下一维海流感应磁场表达式,并分析了地磁场水平分量对海流感应电磁场的影响。计算表明地磁场水平分量的影响随纬度变化。在高纬度地区地磁场水平分量对海流感应电磁场影响很小,而在低纬度地区它会对海流感应电磁场产生明显的影响。本文还分析了变化的海水电导率对海流感应电磁场的影响。 相似文献
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海洋背景磁场模拟计算及东中国海表层磁场分布 总被引：1，自引：0，他引：1
海洋中海水的运动会切割地球磁场,生成微弱的电场,进而在海洋内部和周围空间激发感生电磁场,即约为地球磁场一万至十万分之一的微弱海洋背景磁场.文中针对海洋背景磁场的生成机制及近几十年来对海洋背景磁场的理论研究,结合世界磁场模型WMM2005,模拟计算了三种典型的海洋运动--海浪、海流、内波所产生的感应磁场,建立了海洋背景磁场的数值计算模型,并在此基础上设计开发了海洋背景磁场的模拟计算软件.最后用卫星多传感器资料驱动普林斯顿海洋动力学模式,得到的东中国海2005年海洋表层环流数据,模拟计算了东中国海海表层磁场分布,对其磁场变化与分布规律作了简要分析. 相似文献
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海水是一种高导电率的流体,处于不停的运动之中。海水运动因切割地磁场而产生感应电流,从而产生感应磁场。本文从毕奥-萨伐尔定律出发,推导出了二维海水运动磁场方程,并利用形函数将其转换成二维离散速度场感应磁场积分表达式,采用高斯数值积分方法计算二维离散速度场感应磁场响应。算例表明,本文计算方法具有较高计算精度。文章还分析了海水运动频率、振幅和水深对感应磁场的影响。 相似文献
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根据麦克斯韦电磁理论,在地磁场中运动的海水将产生感应电磁场。利用一个简单的数学物理模型对感应电磁场在海水内部的分布进行了计算,结果表明海浪产生的电磁场明显依赖于海浪波动的周期及浪高。在100 m的海水深度内,海浪产生的磁感应强度的大小为纳特数量级,而电场强度的大小为几个微伏每米。在同一海水深度处,磁感应强度随海水波动的周期呈现近线性变化,而电场强度的大小有一个极值,该极值随海水深度的增加向长周期方向移动。海浪产生的电磁场是影响海洋电磁探测数据精度的主要噪声之一。 相似文献
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海水是一种高电导率的流体,根据电磁感应定律,运动的海水切割地磁场会在海水中产生感应电流,从而产生感应电磁场。本文从麦克斯韦方程出发,推导出一维速度场海水运动感应电磁场偏微分方程,利用电磁场水平分量在海表面和海底面上的连续性条件,得到海水运动感应电磁场表达式,并编写了Fortran计算程序。计算了常速度海水运动感应电磁场,并与格林函数法计算结果进行了对比,两种方法的计算结果一致。计算了变速度(即海水运动速度随深度变化)海水运动感应电磁场,并讨论了海水运动周期和海底介质电导率对海水运动感应电磁场的影响。计算结果表明:海水运动周期和海底介质电导率对常速度海水运动和变速度海水运动感应电磁场都有影响,但影响程度不同。在本文所述模型和参数条件下,海水运动感应电场和感应磁场振幅分别可达6μV/m和10nT,这与海洋大地电磁响应的量级相当。因而在处理海洋大地电磁数据时,海水运动感应电磁响应是不可忽略的噪音干扰,需要采用必要的压制手段。 相似文献
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The behavior of a highly deformable membrane to ocean waves was studied by coupling a nonlinear boundary element model of the fluid domain to a nonlinear finite element model of the membrane. The hydrodynamic loadings induced by water waves are computed assuming large body hydrodynamics and ideal fluid flow and then solving the transient diffraction/radiation problem. Either linear waves or finite amplitude waves can be assumed in the model and thus the nonlinear kinematic and dynamic free surface boundary conditions are solved iteratively. The nonlinear nature of the boundary condition requires a time domain solution. To implicitly include time in the governing field equation, Volterra's method was used. The approach is the same as the typical boundary element method for a fluid domain where the governing field equation is the starting point. The difference is that in Volterra's method the time derivative of the governing field equation becomes the starting point.The boundary element model was then coupled through an iterative process to a finite element model of membrane structures. The coupled model predicts the nonlinear interaction of nonlinear water waves with highly deformable bodies. To verify the coupled model a large scale test was conducted in the OH Hinsdale wave Research Laboratory at Oregon State University on a 3-ft-diameter fabric cylinder submerged in the wave tank. The model data verified the numerical prediction of the structure displacements and of the changes in the wave field.The boundary element model is an ideal modeling technique for modeling the fluid domain when the governing field equations is the Laplace equation. In this case the nonlinear boundary element model was coupled with a finite element model of membrane structures, but the model could have been coupled with other finite element models of more rigid structures, such as a pontoon floating breakwater. 相似文献
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The size and shape of the effective test area are crucial to consider when short-crested waves are created by segmented wavemakers. The range of the effective test area of short-crested waves simulated by two-sided segmented wavemakers is analyzed in this paper. The experimental investigation on the wave field distribution of short-crested waves generated by two-sided segmented wavemakers is conducted by using an array of wave gauges. Wave spectra and directional spreading function are analyzed and the results show that when the main direction is at a certain angle with the normal line of wave generators, the wave field of 3D short-crested waves generated by two-sided segmented wavemakers has good spatial uniformity within the model test area. The effective test area can provide good wave environments for seakeeping model tests of various ocean engineering structures in the deep ocean engineering basin. 相似文献
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合成孔径雷达(SAR)海面场景原始数据仿真是研究海洋动力参数(表面波浪、风矢量和洋流)的有效工具。目前海面场景原始数据仿真方法已经基于逆Omega-K算法实现了海洋运动参数的空间变化。但是目前仅仅讨论了正侧视情况下的海面场景仿真,应用范围有限,同时没有考虑Stokes漂流以及Bragg相速度的影响,而这两者都是存在于真实海面的。通常情况下为了反演得到海面流场的二维速度矢量,雷达需要从两个不同的方位方向观察海面的同一个区域,因此这就需要考虑大斜视的雷达波束,同时Stokes漂流和Bragg相速度是SAR海表面流场观测不容忽视的两种运动。本文在不改变原有正侧视逆Omega-K算法的情况下,通过增加重新计算零方位时刻的斜视波束中心位置坐标,并据此确定SAR原始数据在多普勒域的位置来将其扩展到大斜侧视逆Omega-K算法,并通过时域Stokes漂流公式到频域内离散化Stokes漂流公式的推导来加入Stokes漂流,以及根据Bragg散射机制加入了Bragg相速度。仿真结果表明,经过聚焦成像后的SAR图像很好的体现了真实海面波浪场的形状,同时能够很好地反演出设定的雷达径向流场速度,且流速精度误差控制在6%以内。最后也证明了Bragg相速度以及Stokes漂流对于海面流场的影响不可忽视。 相似文献
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A new approach to detecting ocean eddies automatically from remote sensing imageries based on the ocean eddy's eigen-pattern in remote sensing imagery and "force field-based shape extracting method" is proposed. First, the analysis on extracting eddies' edges from remote sensing imagery using conventional edge detection arithmetic operators is performed and returns digitized vector edge data as a result. Second, attraction forces and fusion forces between edge curves were analyzed and calculated based on the vector eddy edges. Thirdly, the virtual significant spatial patterns of eddy were detected automatically using iterative repetition followed by optimized rule. Finally, the spatial form auto-detection of different types of ocean eddies was done using satellite images. The study verified that this is an effective way to identify and detect the ocean eddy with a complex form. 相似文献
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Numerical calculation of acoustic field perturbation expressions can be used to predict fluctuations after propagation through ocean sound-speed structures, but before the onset of multipath. The general form of the expressions for signal spectra or correlation functions allow numerical evaluation for an unlimited quantity of vector wave-number spectral models of refractive index. In order to help define the bounds of applicability of the theory, log-intensity fluctuation variances have been calculated for three major situations: ocean internal waves, ocean turbulence, and continuous strong large-scale turbulence. Propagation through ocean thermocline internal waves, realistically weak thermocline turbulence, and unrealistically strong turbulence show that scintillations of intensity can be predicted and understood to first order up to ranges of tens of kilometers, given the proper transmission geometry. Internal wave effects dominate over any effects from expected microstructure. Nonhorizontal transmission yields small fluctuations, but eventually refractive effects of the sound channel will contribute some additional spatial variability and multipath, complicating the use of the theory. Multipath due to the sound channel can exist at ranges where the random small-scale structures would contribute only small perturbations (no multipath from small structures) 相似文献