Normalization of Hydrodynamic Coefficients in Morison Equation     

LI Yucheng Professor  the State Key Laboratory of Coastal  Offshore Engineering  Dalian University of Technology  Dalian  P. R. China. 《中国海洋工程》1999,(2)

-The hydrodynamic coefficients C_d and C_m are not only dependent on the size of slender cylin-der,its location in water,KC number and Re number,but also vary with environmental conditions,i.e.,in regular waves or in irregular waves,in pure waves or in wave-current coexisting field.In this paper,thenormalization of hydrodynamic coefficients for various environmental conditions is discussed.When aproper definition of KC number and proper characteristic values of irregular waves are used,a unified re-lationship between C_d,C_m and KC number for regular waves,irregular waves,pure waves and wave-cur-rent coexisting field can be obtained.  相似文献   

基于遗传算法的浮式防波结构物形状最优化设计     

黄衍顺  林莉  胡云昌 《海洋工程》1999,17(4)

采用遗传算法作为优化手段,以透射系数为目标函数,对给定横剖面面积的浮式防波结构物在规则波中的消波性能及剖面形状进行了最优化计算研究,探讨了透射系数最小的剖面形状与波浪周期之间的关系,为浮式防波结构物的设计提供了一定的理论依据  相似文献   

Scattering of S waves diffracted at the core–mantle boundary: forward modelling     

Valérie Emery  Valérie Maupin  & Henri-Claude Nataf 《Geophysical Journal International》1999,139(2):325-344

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The effect of angle-dependent non-coherent electron scattering and partial redistribution on the polarization of resonance lines     

K. E. Rangarajan 《Monthly notices of the Royal Astronomical Society》1999,308(4):1053-1060

The polarized radiative transfer equation is solved when angle-dependent partial redistribution and non-coherent electron scattering are included as line-scattering mechanisms. A static atmosphere with plane parallel symmetry is assumed. Test calculations are used to illustrate the effects of the electron-scattering coefficient, the thermalization parameter and the continuous absorption coefficient on the line polarization. Results of angle-averaged and angle-dependent redistribution functions are compared and it is shown that angle-dependent functions should be used to model the wing polarization of optically thin lines. The lower the continuous absorption compared with the electron scattering, the higher the wing polarization.  相似文献   

Numerical simulation of the propagation of P waves in fractured media   总被引：1，自引：0，他引：1  

Sylvie Kelner  Michel Bouchon  & Olivier Coutant 《Geophysical Journal International》1999,137(1):197-206

We study the propagation of P waves through media containing open fractures by performing numerical simulations. The important parameter in such problems is the ratio between crack length and incident wavelength. When the wavelength of the incident wavefield is close to or shorter than the crack length, the scattered waves are efficiently excited and the attenuation of the primary waves can be observed on synthetic seismograms. On the other hand, when the incident wavelength is greater than the crack length, we can simulate the anisotropic behaviour of fractured media resulting from the scattering of seismic waves by the cracks through the time delay of the arrival of the transmitted wave. The method of calculation used is a boundary element method in which the Green's functions are computed by the discrete wavenumber method. For simplicity, the 2-D elastodynamic diffraction problem is considered. The rock matrix is supposed to be elastic, isotropic and homogeneous, while the cracks are all empty and have the same length and strike direction. An iterative method of calculation of the diffracted wavefield is developed in the case where a large number of cracks are present in order to reduce the computation time. The attenuation factor Q ⁻¹ of the direct waves passing through a fractured zone is measured in several frequency bands. We observe that the attenuation factor Q ⁻¹ of the direct P wave peaks around kd = 2, where k is the incident wavenumber and d the crack length, and decreases proportionally to ( kd ) ⁻¹ in the high-wavenumber range. In the long-wavelength domain, the velocity of the direct P wave measured for two different crack realizations is very close to the value predicted by Hudson's theory on the overall elastic properties of fractured materials.  相似文献   

Migration of scattered teleseismic body waves   总被引：3，自引：0，他引：3  

M. G. Bostock  & S. Rondenay 《Geophysical Journal International》1999,137(3):732-746

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宽甸岩金预测区指示元素的优选     

杜德文  陈永良 《地质与资源》1996,5(2):103

本文介绍了在宽甸无已知金矿床地区岩金预测工作中优选指示元素的思路。依据金矿地球化学理论,参考成矿带内已知金矿地球化学资料初选指示元素作为化学分析项目。化学分析结果出来后,编制地球化学图件时,考虑到减轻图幅负担和编图工作量,突出有用找矿信息,我们利用元素的变异性和致矿系数筛选出具有明显变异性和较高致矿性的元素,在此基础上利用元素间统计相关性和空间相关性,保留与成矿元素Au有明显相关性的元素,作为优选出的指示元素。  相似文献   

随机介质的声散射(Ⅰ)——广义Born近似反演     

王宁  付圣雪  魏俊  赵犁丰 《中国海洋大学学报(自然科学版)》1998,(4)

运用泛函微分方法给出弱随机介质中散射问题的散射幅度Ｂｏｒｎ近似的推广形式。讨论了关于阻尼最小二乘法反演介质参数的各价相关函数的方法,并讨论具有有限支集势函数扰动的逆问题的唯一性,其结果对运用Ｎｅｗｔｏｎ法等数值方法有实际意义。  相似文献   

Monitoring regional sea ice of the Bohai Sea by SSM/I scattering index     

Jin Yaqiu 《海洋学报(英文版)》1998,(1):53-61

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An analysis of horizontal dispersion due to the drift current with an Ekman layer     

Hidekazu Yasuda 《Journal of Oceanography》1998,54(2):151-164

An analytical method for describing horizontal matter dispersion in shear currents is presented using a tensor expression from the point of view that matter dispersion due to the shear effect should be one of the principal mixing dilution processes. Although the behavior of horizontal dispersion is considerably more complicated than common longitudinal dispersion, the present study elucidates the vertical structure of dispersion and the dispersing process from the initial to the stationary stage, besides the usual depth-averaged dispersion coefficient at the stationary stage. As one of the typical applications of horizontal dispersion, dispersion due to the pure drift current with an Ekman layer is examined theoretically using the present method. This examination reveals that the displacement of the centroid and the major axis of dispersion are twisted in the vertical direction more than the direction of the current vector forming the Ekman spiral; that the variance increases in proportion to the third power of the elapsed time; and that the dispersion coefficient at the stationary stage remains constant, independent of the depth normalized by an Ekman layer thickness. Such dependence of the dispersion coefficient in the steady current is shown to be different from that in the oscillatory current, which is inversely proportional to the depth normalized by a Stokes layer thickness. This is considered to be induced by the difference of the vertical profiles of the first order moment in both currents, that is, the shear region of the first order moment is restricted around the floor by the alternation of the current shear in the oscillatory current while it is diffused in the whole depth in the steady current.  相似文献