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1.
针对中、低纬太平洋ARGO测站的4个实际层结个例,计算了无背景流下准地转海洋Rossby内波的垂直模态。结果表明,海水层结垂直方向的不均匀和跃层的存在,使该垂直模态的波型发生了歪曲变形,致使其偏离了余弦波:跃层越强,这种变形也越大:层结最强的层次对应着最大的波动振幅,多极值的层结对应着多个极大振幅:该内波垂直结构函数的零点随模态序数依次递增,且其零点在海水层结较强的层次要比较弱的层次密集。  相似文献   

2.
分析了内波对多波束测深精度影响的两种机理,并指出测线方向与内波传播方向的夹角不同,多波束测深受到影响的程度也不相同。通过对实测数据的分析,获得了内波的规模、波长、运动方向等基本特征,以及初步了解了内波对多波束测深、调查船航迹线、船速等方面产生的影响。该研究结果可以用于指导野外多波束测量遇到内波时的应对措施,以及利用多波束测深系统对内波进行进一步的研究。  相似文献   

3.
内波是层结海洋中普遍存在的一种海洋动力学现象,包含内潮、内孤立波、近惯性内波等多种形式,由于其携带能量巨大,分布范围广,发生频率高,对海洋结构物造成严重威胁。对国内外关于内波生成、传播演化、海遥感观测及其与海洋结构物相互作用方面的研究进展进行综述。总结了关于内波的生成机制、浅水和深水区域内波传播演化特征、实际海洋内波特征的遥感观测以及内波与海洋平台及水下潜器相互作用的研究成果,讨论了数值模拟、模型试验、遥感观测等研究手段在海洋内波研究中的应用以及取得的相应研究成果。最后,在探讨海洋内波研究趋势的基础上对未来关于内波生成机制及其海洋学特征观测相关研究需考虑和解决的问题进行了展望。  相似文献   

4.
根据地球流体力学基本方程组,在密度垂直层结的情况下,引进行波坐标,研究非线性定形波在相平面上的几何拓扑结构。严格论证了不存在定形孤立波,并通过Hamilton函数及其角作用变把行波系统化成最简形式,由此而得到非线性惯性重力内波的解析解。  相似文献   

5.
刘式达  刘式适 《海洋学报》1982,4(5):537-544
十多年来,用摄动法研究非线性波已经取得了相当大的成就.在流体力学方面研究较多的是浅水表面波,在大气科学方面研究较多的是Rossby波.对层结流体中的内波,则研究较少.大家知道,海洋和大气都是密度随深度或高度变化的层结(分层)流体.许多重要的自然现象,如台风、飑线、积云、湍流、海洋中的温跃层等,都和重力内波有关.随着卫星技术的发展,非线性重力内波已经在大气和海洋中观测到[1,2].从理论上研究非线性重力内波较早的是Benney(1966)[3]和Benjamin(1966[4],1967[5]),最近Maslowe和Redekopp(1980)[6]对层结剪切流动的非线性内波作了系统详细的研究.  相似文献   

6.
针对传统内波重构是基于内波源基础,理论性限制太强,不适合实际应用。本文提出1种基于SAR图像反演内波参数并结合背景场密度剖面信息,对内波二维断面进行重构。在充分考虑到SAR图像反演的内波水平数据信息(数据信息均一化),垂向振幅以及垂向模态函数三者物理意义及相互关系后对内波二维断面重构,它具有物理意义清楚、实际可操作性强的特点。  相似文献   

7.
内波为发生在层结海洋内部的亚中尺度波动,是物理海洋学研究,特别是海洋混合及能量级串研究,不可或的缺环节。孤立内波的突发性巨大冲击能量可对水下航行和工程设施构成灾难性威胁,实现实时监测与预报海洋内波具有重大现实意义。南海是全球海洋中超强内波多发海区之一。长期现场观测表明,吕宋海峡以西海域内孤立波振幅高达150~200 m,且终年发生。因此,南海是目前海洋内孤立波观测与研究热点海域。本文以2015年至2021年间发表的论文为依据,评述南海内波研究新进展,认为7 a来研究成果取得质的提升。第一,实现了由卫星为主要手段2D观测到以卫星与潜标同步3D观测为主要手段的提升。由此催生出振幅240 m超强内孤立波、中尺度涡对内波的调制作用、重现周期23 h 内孤立波、浅海内孤立波裂变现象、深海盆内波及动能级串等创新成果。第二,研究区开始呈现向中部深海盆扩展趋势。迄今为止,南海内波观测与研究集中在吕宋海峡以西和北部陆架,现已出现向中部深海盆扩展趋势。第三,海洋探测高新技术应用于南海内波观测与研究,取得了突破性成果。由卫星高度计沿轨海面高度场二维平面波分解技术得出的南海M2内潮辐射图,解决了多年争论不休的南海北部内波生成机制和生成源地问题。人工智能技术成功应用于建立南海邻近的边缘海内波传播预报模式。模式预报的一个潮周期之后内波波峰线位置与后续卫星图像上显示的位置之间的平均相关系数达95%,平均距离均方根差为3 km。快速深潜剖面浮标技术应用于南海北部深海盆,得出0~3 500 m 全水深内波波段(周期为0.1~1.8 d)波动引起的水温起伏幅度垂直分布。高分辨水下声成像技术,包括人工地震技术和回声探测仪,成功应用于南海北部陆架内波观测与研究。其中回声探测仪图像空间分辨率达10 cm,清楚显示出内孤立波波包精细结构,可精确测得水平尺度仅为2 m的孤立波特征半宽度。可以预期,大量科学研究成果的积累,特别是采用人工智能技术建立内波传播预报模式的成功实例,必将为开发南海内波精准预报模式奠定基础。  相似文献   

8.
本文通过对卫星遥感图像中的内孤立波及相互作用现象进行统计分析,讨论了南海北部内孤立波及相互作用现象的时空分布特征,验证了利用卫星遥感图像反演内孤立波振幅和传播速度以及研究内波相互作用现象的可行性。统计结果表明,南海北部的内孤立波主要集中在东沙群岛以及海南岛南部,内波相互作用主要集中在东沙岛西北部以及海南岛南部。本文对此给出解释:内波传播至东沙岛附近发生绕射,绕射的内波分裂成两列后以不同的传播方向继续向西传播,相遇并发生相互作用;内波在海南岛浅滩处发生反射,与后续传来的内波发生相互作用。同时,本文利用Korteweg-de Vries (KdV)方程和Benjamin-One(BO)方程,结合观测数据,对内波振幅和传播速度进行了反演实验。反演所得的内波振幅和传播速度与南海北部实际内波振幅和传播速度相近。  相似文献   

9.
为了研究内波远距离传播过程中的演化规律,本文采用图像测速法(PIV)分别对内波近场和远场的速度场进行测量。实验中同时采用两台CCD相机对实验区域进行拍摄,根据实验结果对内波能量和垂向模态结构进行计算分析。实验结果表明,在近场区域生成的内波主要表现为内波射线结构。内波射线在经过海表面反射后,其能量在空间上出现非对称结构,能量在加强区域较减弱区增加约15%。在远场,内波射线结构不再清晰,内波主要表现为低模态内波结构。内波射线在反射时能量衰减显著,损失约为50%;低模态内波可以离开内波生成源地远距离传播,传播过程中能量损失较小,在远场传播过程中(第一模态内波半波长的距离)能量损失约20%。低模态内波的传播相速度介于垂向第一模态和第二模态相速度之间。  相似文献   

10.
粗糙地形对内波生成影响的实验研究   总被引:2,自引:1,他引:1  
王金虎  陈旭  徐洋 《海洋与湖沼》2016,47(4):706-713
为了研究粗糙地形对内波共振生成的影响,本文在实验中采用粒子图像测速法(PIV)对内波速度场进行测量。实验中设置了两种不同尺度的粗糙地形,其中一种地形的粗糙尺度大于黏性边界层厚度(δ),另一种地形的粗糙尺度小于δ。结果表明两种粗糙地形都使共振内波的能量减弱,粗糙地形一侧生成的内波强度约为光滑地形一侧生成内波强度的40%。当粗糙地形的尺度大于δ时,在粗糙地形一侧除了共振内波以外还有明显的内波射线生成,粗糙地形上的每一个凸形间断点都成为了一个新的内波源点,每条内波射线的强度约为共振内波强度的1/10,由新源点生成的内波射线相位基本一致,落后于正压潮3π/5个相位。当粗糙地形的尺度小于δ时,粗糙地形一侧仅有共振内波生成,共振内波的相位与正压潮相位十分接近。  相似文献   

11.
Oceanic pycnocline depth is usually inferred from in situ measurements. It is attempted to estimate the depth remotely. As solitary internal waves occur on oceanic pycnocline and propagate along it, it is possible to retrieve the depth indirectly in virtue of the solitary internal waves. A numerical model is presented for retrieving the pycnocline depth from synthetic aperture radar (SAR) images where the solitary internal waves are visible and when ocean waters are fully stratified. This numerical model is constructed by combining the solitary internal wave model and a two-layer ocean model. It is also assumed that the observed groups of solitary internal wave packets on the SAR imagery are generated by local semidiurnal tides. A case study in the East China Sea shows a good agreement with in situ CTD (conductivity-temperature-depth) data.  相似文献   

12.
Mathematical modelling techniques are applied to study the influence of the seasonal pycnocline on the propagation and attenuation of internal waves in an ocean with a main pycnocline. This paper discusses the peculiarities of dispersive dependences, group velocities, and of the velocity field's amplitudinal characteristics induced by the seasonal pycnocline. Short-period motions have been observed to concentrate within the latter, and the conditions causing a modification of the environment's waveguide properties for non-stationary wave packets, associated with the existence of two pycnoclines, have been identified.Translated by Vladimir A. Puchkin.  相似文献   

13.
武军林  魏岗  杜辉  徐峻楠 《海洋科学》2017,41(9):114-122
为进一步探究海洋内孤立波诱导流场对海洋工程结构物以及潜航器的影响,本文采用重力塌陷方法和粒子图像测速(Particle Image velocimetry,PIV)技术在大型分层流水槽中进行内孤立波造波以及内部流速场测量,定量分析了下凹型内孤立波诱导流场结构及其影响因素。研究表明:在密度分层流体中,PIV技术可实现对大幅面内孤立波诱导流场的精细测量以及波动结构特征的准确描述;水平流速在上下层方向相反且在跃层处最小,其剪切作用在波谷附近最强;垂向流动在波前和波后分别为上升和下沉流,两者流速值在距离波谷1/4~1/2波长位置达到最大;在相同内孤立波振幅条件下,上下层流体密度差越大、厚度比越小,则波致流场越强;随着振幅增大,流场结构与Kd V、e Kd V和MCC理论模型对应波幅适用范围的描述相吻合。  相似文献   

14.
Internal waves generated by a baroclinic internal wave impinging on an oceanic ridge are studied. Two stratification models are considered: a two-layer ocean model (with a density jump) and a continuously stratified ocean model (model pycnocline). The results yielded by different stratification models are compared analytically. The analysis makes possible the application of a piecewise-constant approximation of the fluid stratification to study topographically-generated baroclinic tides. Translated by V. Puchkin.  相似文献   

15.
应用中国近海及邻近海域海洋再分析资料(简称CORA)研究南海北部第一模态内波场运动学参数的地理分布特征及其季节变化。首先分析了Brunt-Väisälä频率的统计特征;其次,基于弱非线性变系数扩展Kortewed-de Vries (veKdv)方程模型,计算了它的输入系数,即线性长波相速度,平方和立方非线性系数和频散系数,这些参数可用于定性评估内孤立波传播可能的极性,内孤立波的形态,幅度限制以及传播速度等。分析结果表明,南海北部季节性密度跃层从2月开始出现,最大浮力频率约在20 m。它在6—7月达到最强,自8月开始减弱,在10月消退。另一密度跃层出现在8—11月,最大浮力频率约在80 m,冬季大致在120 m。季节性密度跃层在4—9月十分明显,而8—10月双跃层现象显著,冬季仅出现较弱的第二密度跃层。在1—3月和10—12月海盆深水区最大Brunt-Väisälä频率值要大于陆架浅水区;而在5—9月情况则相反。Brunt-Väisälä频率最大值所在深度随季节变化显著,冬季最深,6—7月则最浅。计算的线性内波相速度、频散系数和幅度放大因子的空间特征主要取决于地形变化;平方(立方)非线性系数与地形关系较小,随季节变化明显,它们主要取决于局地海洋环境特征。通过分析veKdv方程的系数特征,解释了为何在夏季南海北部最容易观测到大振幅内孤立波和在吕宋海峡以东海域难以观测到孤立波的原因。  相似文献   

16.
Relation between internal waves with short time scale and density distribution near the shelf break in the East China Sea is studied utilizing moored current meters, thermometers and conductivity-temperature-depth (CTD) casts. A well developed pycnocline was frequently observed around 150–200 m depth near the shelf break accompanied with the development of internal waves with short time scale. During the cruise in May 1998, the intensified internal wave motion with short time scale and the distinct offshore flow were observed just below the lower pycnocline, which shoaled and extended above the shelf area. It is suggested that vertical mixing generated by amplified internal waves would produce cross-shelf ageostophic density current around the pycnocline. During the cruise in May 1999, on the other hand, the lower pycnocline was located offshore below the shelf break, and the internal wave motion was amplified just above the lower pycnocline. In this case, the offshore flow should be generated above the lower pycnocline, but vertical profiles of current velocity were not obtained because acoustic Doppler current profiler (ADCP) data were not available around the lower pycnocline.  相似文献   

17.
High-frequency (120 and 420 kHz) sound was used to survey sound scatterers in the water over Georges Bank. In addition to the biological sound scatterers (the plankton and micronekton), scattering associated with internal waves and suspended sediment was observed. Volume backscattering was more homogeneous in the vertical dimension (with occasional patches) in the shallow central portion of the Bank where there is significant mixing. In the deeper outer portion of the Bank where the water is stratified, volume backscattering was layered and internal waves modulated the vertical position of the layers in the pycnocline. The internal waves typically had amplitudes of 5-20 m, but sometimes much higher. Species composition and size data from samples of the animals and suspended sediment used in conjunction with acoustic scattering models revealed that throughout the region the animals generally dominate the scattering, but there are times and places where sand particles (suspended as high as up to the sea surface) can dominate. The source of the scattering in the internal waves is probably due to a combination of both animals and sound-speed microstructure. Determination of their relative contributions requires further study  相似文献   

18.
Laboratory experiments are performed in a large stratified fluid flume to examine the characteristics of the load on a submerged slender body that is exerted by a nonstationary internal solitary wave (ISW) from its interaction with a gentle slope. The nonstationary ISW over the slope and its load on the body are measured by using multi-channel conductivity-probe arrays and a specially designed force measurement device, respectively, and the body’s vertical and horizontal positions on the load are determined by analyzing the effects of the incident ISW’s amplitude. The experimental results show that the load on the slender body increases as the incident ISW’s amplitude increases; additionally, the effect of oscillations is enhanced because of the ISW’s distortion, breaking and fission. The oscillating action from fission waves becomes dominant as the amplitude reaches a certain value. Additionally, the load is correlated with body’s vertical position relative to the pycnocline. The magnitudes of the vertical and horizontal forces reach a maximum and minimum in the pycnocline, respectively, and the horizontal force in this direction is the opposite above and below the pycnocline. Compared to a case without a slope, the load on the slender body increases because of the nonstationary ISW, and its effect on the maximum force is transferred to the pycnocline. When the body’s horizontal position is located close to the top of the slope, the direction of the horizontal and vertical forces remains consistent, but its acting time becomes longer. In addition, high-frequency actions on the slender body are impacted by nonstationary ISWs near the slope’s top.  相似文献   

19.
超短基线定位解算中的距离观测值是指换能器与水下应答器之间的直线距离,而海水声速的不均匀分布导致声波在海水中的实际传播路径为连续弯曲的曲线,需要结合实测声速剖面进行声线修正。根据声速在分层介质中的传播特性,本文提出了一种基于二次多项式拟合的声线跟踪算法,采用线性插值方法对声速剖面数据进行合理加密并按等深度进行分层,设定每层声速梯度是不断变化的,用二次多项式拟合声速,基于运动学原理建立了完整的数学解算模型。仿真结果表明,该方法修正后的水下目标分布具有明显的收敛性,且优于等梯度声线跟踪算法和等效声速剖面法,显著提高了超短基线水声定位系统的定位精度。  相似文献   

20.
An internal gravity wave model was employed to simulate the generation of internal solitary waves(ISWs) over a sill by tidal flows. A westward shoaling pycnocline parameterization scheme derived from a three-parameter model was adopted, and then 14 numerical experiments were designed to investigate the influence of the pycnocline thickness, density difference across the pycnocline, westward shoaling isopycnal slope angle and pycnocline depth on the ISWs. When the pycnocline thickness on both sides of the sill increases, the total barotropic kinetic energy, total baroclinic energy and ratio of baroclinic kinetic energy(KE) to available potential energy(APE) decrease, whilst the depth of isopycnal undergoing maximum displacement and ratio of baroclinic energy to barotropic energy increase. When the density difference on both sides of the sill decreases synchronously, the total barotropic kinetic energy, ratio of baroclinic energy to barotropic energy and total baroclinic energy decrease, whilst the depth of isopycnal undergoing maximum displacement increases. When the westward shoaling isopycnal slope angle increases, the total baroclinic energy increases whilst the depth of turning point almost remains unchanged. When the depth of westward shoaling pycnocline on both sides of the sill reduces, the ratio of baroclinic energy to barotropic energy and total baroclinic energy decrease, whilst the total barotropic kinetic energy and ratio of KE to APE increase. When one of the above four different influencing factors was increased by 10% while the other factors keep unchanged, the amplitude of the leading soliton in ISW Packet A was decreased by 2.80%, 7.47%, 3.21% and 6.42% respectively. The density difference across the pycnocline and the pycnocline depth are the two most important factors in affecting the characteristics and energetics of ISWs.  相似文献   

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