河口海岸底部边界层和细颗粒泥沙过程??

水动力、细颗粒泥沙过程是淤泥质河口海岸变化的重要物理过程 ;并具有这样的特征 :强密度梯度、高度不稳定和非均匀流、高浓度泥沙、底床与流相互作用、难确定的底床／水界面。淤泥质河口海岸水动力、细颗粒泥沙过程的研究主要起因于：１）海洋科学的基础理论研究 ;２）港口航道的建设、维持（整治、疏浚）、海岸防护工程实践等需要。就淤泥质河口海岸水动力、细颗粒泥沙过程而言 ,水流最重要的部分是底部边界层。为计算河口海岸水流中的底床切应力 ,必需考虑边界层。在淤泥质河口海岸底部边界层内 ,强劲的潮流、波致流可以引起淤泥底床沉积…     

台风期间厦门湾潮流边界层特征研究

本文基于2007年8月圣帕台风影响台湾海峡期间的厦门湾垂向海流流速剖面观测资料，运用Karman-Prandtl模型统计和分析了流速对数剖面的出现频率和边界层参数（摩阻流速与粗糙长度）．结果表明流速剖面满足对数分布出现频率都超过50％，但进行内部一致性原则分析后，流速剖面满足对数分布情况均不足30％．造成流速剖面偏离对数分布的因素主要有：台风、径流、流速加减速、水体分层、底床结构、海底悬沙浓度等等．台风期间的摩阻流速和粗糙长度都大于非台风期间的数值．     

海底边界层水流结构及底移质搬运研究进展

海底边界层包括从底底至受其显著影响的水体之间的水层厚度,对海底动力过程,尤其是沉积物搬运及近海底化学物质输运有重要影响,不同的水动力（潮流、波浪及浪流共同作用）形成完全不同的边界层。边界层厚度与水流周期有关,但目前对其理解及计算公式并不统一,边界层内的流带分布与摩阻流速的床底糙率有关,目前已经发展了多种估算这两个参数的方法,对于边界层内的沉积物搬运率的计算,关键在于弄清沉积物在边界层内的沉降、起动     

悬沙浓度分布对鸭绿江河口流速结构的影响

对鸭绿江河口1994和1996两年两个站位共4个潮周期的数据进行了分析,通过流速对数剖面公式计算了边界层参数,并对各个潮周期内的边界层参数的变化规律进行了分析,同时也对悬沙输送可能对垂向流速结构以及边界层参数造成的影响进行了探讨,分析结果表明,正是由于悬沙分布的影响,打破了原有的温度、盐度、水体密度在水层间的分布格局,改变了原有水体的纵向密度梯度,除少数时刻对应的水体Rf值减小之外,水体的Rf值被普遍提高,并且分层稳定。应用改造后的Von karmen-Prandtl流速对数分布剖面公式,重新对原先公式计算的边界层参数进行了修正,修正后结果表明,u*、C100和τ分别比通过原公式的计算值平均减少了21%、56%和36%,而由于水体悬沙则使τ比在没有悬沙存在的情况下的τ值平均减少了22%。     

长江口南港底部边界层特征的观测与分析

对长江口2002年和2003年共4个潮周期的数据进行了分析,通过流速对数剖面公式计算边界层参数,并对各个潮周期内的边界层参数的变化规律进行了分析,同时也对悬沙输送可能对垂向水流结构以及边界层参数造成的影响进行了探讨。结果表明,悬沙的时间分布特征对温度、盐度、水体密度的分布格局有重要影响,主要表现在水体的Rf值普遍较高,分层稳定。此外,悬沙也可影响边界层参数,从而对水流结构产生影响。由于水体的层化作用,使层间的摩擦阻力增大,相当于在垂向上产生不同内边界层,因而影响了流速在垂向上的变化。     

瓯江口水流挟沙力公式探讨

采用瓯江口实测泥沙资料,对多个典型挟沙力公式进行了系统比较;对瓯江口同步的平均流速和平均含沙量进行分析,探讨适合该河口的挟沙力关系,并引入泥沙因子,考虑泥沙粒径对水流挟沙力的影响。结果认为:各挟沙力公式的计算结果过程曲线趋势一致,只是存在量级上的差别;结合实测泥沙资料进行分析,采用河口、海岸适用性较好的水流挟沙力公式,考虑泥沙粒径对挟沙力的影响,引入泥沙因子分析拟合瓯江口水流挟沙力公式。旨在揭示不同挟沙力公式之间的联系,以及河口海域水流挟沙力拟合过程,为进一步探讨河口海岸含沙量分布和悬浮泥沙输运提供思路。     

海洋底边界层中实测海流的垂直分布Ⅰ.余流边界层

海底以上1-2m水层的海流垂直分布和变化,对于海底泥沙运动和海洋工程设计具有十分重要的意义.迄今为止,研究者分别从实测资料、实验室实验和理论等方面对底边界层中稳定流动的垂直分布进行了研究,其结果均难以直接满足工程需要.本文基于现有的理论和实验结果,发展了现有海底边界层理论,运用把稳定流的底Ekman层与对数层相配匹的方法确定了实测余流的垂直分布,并给出了在渤海石油平台区的应用实例.结果表明,本文给出的原理和方法在应用中与实测结果符合良好,可以直接满足工程需要.     

海洋底边界层中实测海流的垂直分布I. 余流边界层

海底以上 1— 2m水层的海流垂直分布和变化 ,对于海底泥沙运动和海洋工程设计具有十分重要的意义。迄今为止 ,研究者分别从实测资料、实验室实验和理论等方面对底边界层中稳定流动的垂直分布进行了研究 ,其结果均难以直接满足工程需要。本文基于现有的理论和实验结果 ,发展了现有海底边界层理论 ,运用把稳定流的底Ekman层与对数层相配匹的方法确定了实测余流的垂直分布 ,并给出了在渤海石油平台区的应用实例。结果表明 ,本文给出的原理和方法在应用中与实测结果符合良好 ,可以直接满足工程需要     

潮滩水流加减速阶段边界层流速剖面的比较

江苏大丰地区潮滩由于水深较浅,潮流、波浪等动力较强,整个水层可视为边界层,其主体部分是对数层,即水流流速在垂向上呈对数分布。在潮流的加减速阶段,流速剖面将可能偏离对数分布,从而使对数剖面法计算出来的边界层参数造成误差。使用MIDAS-400用户化数据采集系统,在大丰潮滩获得了多层流速、浊度等同步高频观测数据,基于修正后的von Karman-Prandtl模型对u-lnz进行回归分析、数据内部一致性分析来定义流速对数剖面并与未修正前经典理论得到的边界层参数进行比较。分析结果表明,修正后的流速剖面更符合实际情况,边界层参数除了受水流加速度的影响外,还和沙纹等因素有关。另外,边界层参数的变化量与特征加速度负相关。     

江苏大丰潮间带粉砂滩的潮流边界层特征

对江苏大丰潮间带粉砂滩的潮流观测数据，运用Karman-parndtl模型分析了流速对数剖面的出现频率和边界层参数（摩阻流速与粗糙长度）。结果表明，不同时间尺度（10^1-10^3s）的平均流速对计算u-lnz线性关系出现频率的影响不大，而不同层位组合的影响较为显著，影响流速对数剖面分布的自然因素为波浪、风、潮流旋转、表底层流向差异、滩面坡度和水流加减速等。相邻层位的流速在时间序列上存在很高的线性关系，回归直线的斜率与水层距底床的高度、粗糙长度和摩阻流速有关。涨潮阶段床面粗糙长度大于落潮阶段，涨潮阶段摩阻流速小于落潮阶段。     

基于分段自适应算法的浅海水深遥感反演融合模型研究

对于水深光学遥感反演研究，虽然已经建立了大量的模型方法，然而对于不同水深段，同一模型的反演精度各异，且采用单一模型进行水深反演得到的整体反演精度未必最佳。为了提高水深光学遥感反演的整体精度，本文提出一种分段自适应水深反演融合模型，模型在误差估计的基础上，结合了对数线性模型、对数转换比值模型、改进的对数转换比值模型与多调节因子模型的优势。利用模型在西沙群岛东岛开展了水深遥感反演实验，从整体反演精度、不同水深段反演精度及逐米水深精度等角度进行分析，结果表明，分段自适应融合模型的整体精度最高，平均绝对误差为1.09 m，平均相对误差达到16.06%；分水深段来看，分段自适应融合模型在多数不同水深段内的反演效果均最好；从逐米精度来看，分段自适应融合模型在大部分逐米水深段的反演能力均优于其他模型。     

Study on the Log-Linear Velocity Profile of Near-Bed Tidal Current in Estuarine and Coastal Waters

Many observed data show that the near-bed tidal velocity profile deviates from the usual logarithmic law. The amount of deviation may not be large, but it results in large errors when the logarithmic velocity profile is used to calculate the bed roughness height and friction velocity （or shear stress）. Based on their investigation, Kuo et al. （1996） indicate that the deviation amplitude may exceed 100%. On the basis of fluid dynamic principle, the profile of the near-bed tidal velocity in estuarine and coastal waters is established by introducing Prandtl＇ s mixing length theory and Von Kannan selfsimilarity theory. By the fitting and calculation of the near-bed velocity profde data observed in the west Solent, England, the results are compared with those of the usual logarithmic model, and it is shown that the present near-bed tidal velocity profile model has such advantages as higher fitting precision, and better inner consistency between the roughness height and friction velocity. The calculated roughness height and friction velocity are closer to reality. The conclusions are validated that the logarithmic model underestimates the roughness height and friction velocity during tidal acceleration and overestimates them during tidal deceleration.     

近地层风廓线与垂直湍流强度关系研究

通过改进Prandtl 混合长理论,得出近地层风廓线形式     

有无1墨水点亚对数空间限定交替式下推自动机之间的关系

该文引入 1墨水点 2方向交替式下推自动机 ,它是 1个具有额外能力的 2方向交替式下推自动机 ,能够用 1个墨水点在输入带上标记出最多 1个单元格。对具有 1个墨水点的和没有墨水点的亚对数空间限定交替式下推自动机之间的关系进行研究。实例证明了具有 1个墨水点的亚对数空间限定交替式下推自动机的语言受理能力强于没有墨水点的亚对数空间限定交替式下推自动机     

海面风的特征分析

作者利用在渤海进行的不同时距的平均风速观测值,经统计分析求得1秒、2分和10分钟平均风速间的线性关系。同时根据风速梯度观测值给出风速指数廓线的指数值,并且给定风速对数廓线的特征值:海面摩擦速度和海面粗糙度。此外,作者还提出了海面风应力的经验公式。     

多光谱遥感影像的两种浅海水深反演模型对比与分析

利用WorldView-2高分辨率卫星影像,以南海北岛附近海域为研究区,研究了两种水深反演模型——对数变换模型(Stumpf 2003)和双波段线性回归模型(Lyzenga 1985)。分析了不同底质情况下水深与各波段的相关性,并利用L-M(Levenberg-Marquardt)算法求解模型参数,然后对两种模型反演的水深结果的精度进行了对比分析。对于珊瑚底质,Lyzenga 1985模型水深反演的决定系数和均方根误差分别为0.902和1.651,均优于Stumpf 2003模型(0.882,6.421);对于砂质底质,Lyzenga 1985模型水深反演的决定系数和均方根误差分别为0.897和0.529,均优于Stumpf 2003模型(0.779,0.723)。可见,在水体清澈的珊瑚底质和砂质底质区域,Lyzenga 1985模型的水深反演精度均优于Stumpf 2003模型,Lyzenga 1985模型普适性更强,能够呈现出较为稳定的反演效果。     

Study on the double-logarithmic profile of tidal flow velocity in the near-bed layers

Tidal current velocity profile in the near-bed layers has been widely studied. The results showed that velocity profile in the near-bed layer obviously departure from the traditional logarithmic profile, due to the acceleration or deceleration. Although the logarithmic linear profile can reduce the rate of deviation from this, only it is a lower-order approximate solution. In this paper, considering the unsteady and non-linear features of tidal motion, the double logarithmic profile near-bed layers in estuarine and coastal waters is established on the assumption that the turbulent shear stress along the water depth was parabolic distribution, and on the basis of Prandtl''s mixing length theory and von Karman''s self-similar theory. Having been verified the data observed at the West Solent in the south of England, and comparison of the logarithmic linear profile, it found that the double logarithmic profile is more precious than the latter. At last, the discussed results showed that:(1) The parabolic distribution of the tidal shear stresses verified good by the field data and experimental data, can be better reflected the basic features of the tidal shear stress deviating from linear distribution that is downward when to accelerate, upward when to decelerate. (2) The traditional logarithmic velocity profile is the zero-order approximation solution of the double logarithmic profile, the logarithmic linear profile is the first order, and the logarithmic parabolic profile is the second order. (3) Ignoring the conditions of diffusion and convection in the tidal movement, the double logarithmic profile can reflect the tidal properties of acceleration or deceleration, so that the calculation of the friction velocity and roughness length are more reasonable. When the acceleration or the deceleration is about zero, the double logarithmic profile becomes the logarithmic profile.     

几种经典海洋环境噪声谱分析

目前风关海洋环境噪声实验研究结果较多,其中较为经典的是Knudsen谱、Wenz谱、Piggott谱、Crouch谱,以及风速与噪声谱级的对数关系等。对这几种经典的海洋环境噪声谱进行了概述,分析了其数据来源,并对Wenz谱、Piggott谱和Crouch谱进行了比较,探究了其差异产生的原因,并给出了不同情况下进行风关海洋环境噪声估计时的参考建议。     

Microbial Biomass and Organic Nutrients in the Deep-Sea Sediments of the Central Indian Ocean Basin

In order to assess the impact of deep-sea mining on the in situ benthic life, we measured the microbial standing stock and concentration of organic nutrients in the deep-sea sediments of the Central Indian Ocean Basin in the Indian pioneer area. Sediments were collected using box core and grab samples during September 1996. The total bacterial numbers ranged from 10 10 -10 11 cells per g -1 dry weight sediment. There was a marginal decrease in the number of bacteria from surface to 30 cm depth, though the subsurface section registered a higher number than did the surface. The highest numbers were encountered at depths of 4-8 cm. The retrievable number of bacteria were two orders less in comparison with the direct total counts of bacteria. An almost homogeneous distribution of bacteria, total organic carbon, living biomass, and lipids throughout the depth of cores indicates active microbial and benthic processes in the deep sea sediments. On the other hand, a uniform distribution of total counts of bacteria, carbohydrates, and total organic carbon in all the cores indicates their stable nature and suggests that they can serve as useful parameters for long-term monitoring of the area after the benthic disturbance. Further studies on temporal variability in this region would not only verify the observed norms of distribution of these variables but would also help to understand restabilization processes after the simulated benthic disturbance.     

Assessing the Validity of Seismo-Acoustic Predictor Equations for Obtaining Seabed and Sub-Surface Sediment Physical Properties

The interdependence between the seismo-acoustic properties of a marine sediment and its geotechnical/physical parameters has been known for many years, and it has been postulated that this should allow the extraction of geotechnical information from seismic data. Though in the literature many correlations have been published for the surficial layer, there is a lack of information for greater sediment depths. In this article, a desktop study on a synthetic seafloor model illustrates how the application of published near-surface prediction equations to subsurface sediments (up to several tens of meters burial depth) can lead to spurious predictions. To test this further, acoustic and geotechnical properties were measured on a number of sediment core samples, some of which were subjected to loading in acoustically-equipped consolidation cells (oedometers) to simulate greater burial depth conditions. For low effective pressures (representing small burial depths extending to around 10 meters subsurface), the general applicability of established relationships was confirmed: the prediction of porosity, bulk density, and mean grain size from acoustic velocity and impedance appears generally possible for the investigated sedimentary environments. As effective pressure increases through, the observed relationships deviate more and more from the established ones for the near-surface area. For the samples tested in this study, in some instances increasing pressure even resulted in decreasing velocities. There are several possible explanations for this abnormal behavior, including the presence of gas, overconsolidation, or bimodal grain size distribution. The results indicate that an appropriate depth correction must be introduced into the published prediction equations in order to obtain reliable estimates of physical sediment properties for greater subsurface depths.