浅水波能谱试验研究

室内试验是研究风浪特性的一重要途径,文中首先对试验研究方法中的不足进行了改进和探讨.对比了天然风浪与试验风浪的风场特点,确定了两者特征风速间的换算关系.通过采用人工风与不规则造波机相结合来生成与模拟风浪,延长了试验条件下风浪成长所需的风区长度.在此基础上,利用试验研究的优点,完成了较大范围浅水风浪试验,对浅水波能谱进行了深入探讨.研究表明,较深水情况波能谱在浅水域其谱峰变小,谱形变得更加尖窄,反映出其波能量趋于集中,并给出了相应的表达式.     

关于风浪预报公式和风区宽度的注记

从定常波的风浪波高随风距成长的预报公式出发 ,在一定条件下 ,导出各波向上风浪波高分量与该波向上的风距之间的关系 ,以便在不规则风区上推算风浪波高和平均波向 ;同时 ,对风区宽度作了定量化的分析。     

大型风浪水槽风浪统计特征的测量和分析

研究大型风浪水槽的风浪统计特征，采用多通道测波系统，同步采集沿水槽的１２个测点在不同风速下的风浪数据，从观测事实上分析风浪波面分布和有关要素特征，并建立水槽风浪统计要素与风速，风区长度之间的关系     

小型室内水槽造波造风系统设计

小型室内风浪水槽是海气界面多种微尺度过程实验研究的基础设施.造风造波系统是风浪水槽的核心部分.针对多种微尺度过程模拟的需要,设计了造风造波系统的硬件结构与控制软件.利用该系统,开展了多种造波、造风实验.通过对实验数据的分析,证明该设计满足各项预定指标,可以有效模拟多种海气界面风浪环境.     

大洋中涌浪对风浪能量的影响

由于涌浪与风浪在特征物理参量及成长、衰亡上的显著不同,区分风涌浪以及研究涌浪对风浪的影响尤为重要。本文使用2013年及2015年大洋中的WaMoSⅡ测波雷达观测数据,研究了涌浪对风浪能量的影响。由于测波雷达仅使用了9s的有效周期作为谱分离判据,其所得风浪有效波高显著高于PM谱充分成长关系给出的波高。因此本文结合2D法与1D法,加入风速、风浪夹角、波龄等要素给出新的判据,重新对风、涌浪进行了分离。通过对比不同的波龄判据,发现当波龄取1.5时,所得结果与PM谱吻合良好。以Toba-3/2定律为基础,研究了不同类型涌浪对风浪能量的影响。发现三种类型涌浪存在时,风浪能量及有效波高整体上都有所增加,其中尤其以反向涌浪存在时增加最多。     

考虑非线性频散效应的风浪关系及其应用

随着我国沿海地区海洋经济的快速发展,相关海域的风浪规律的研究越来越受到人们的重视。依据Toba的风浪3/2指数律和非线性频散关系推导得到一个新的波陡波龄关系式,简化获得适用于深水情况下的波陡波龄关系式;基于考虑非线性频散效应的波龄波陡深水关系式,并结合有效波能量平衡方程,进一步推导出包含非线性频散效应的深水海域风浪公式。利用新的深水风浪公式,并结合Mitsuyasu开阔海域风区、风速经验公式,研究了江苏沿海海域的风浪规律,且与NCEP再分析风浪数据以及其他公式结果进行对比分析。分析结果表明所获得的新深水风浪公式适用范围更广,且在只考虑风速这个单一参数条件下计算得到的江苏外海波浪要素与NCEP再分析风浪数据吻合程度最好,且更接近其他学者的研究成果。计算过程可避免开阔海域风区长度推算的不确定性和人为因素所产生的误差,可为我国风浪成长规律的理论研究和海洋工程深海风浪要素推算提供参考。     

涌浪对风浪能量影响的实验研究

在实验室风浪水槽中进行纯风浪和混合浪波面位移观测,研究波长较长的规则波对风浪能量的影响.本文用混合浪和纯风浪中的风浪显著波的零阶谱矩之比代表混合浪中的风浪与纯风浪能量之比,并以此表征涌浪对风浪能量的影响.研究了该能量比随涌浪波陡S、风区x、波龄倒数u/C、涌浪频率与纯风浪谱峰频率之比fs/fwp的变化规律.结果表明,涌浪对风浪能量的抑制作用随涌浪波陡的增加、波龄倒数的增大及涌浪频率与纯风浪谱峰频率之比的增大而增强.发现该能量比依赖于无因次量R=(1+80(πS)2)1.9(fs/fwp)0.9(u/C)0.27,并拟合得到2者的经验关系.此外,本文实验还发现,在某些情况下,涌浪的存在使风浪能量增加.     

南麂海域风浪的平均波陡与平均波龄统计分布

利用南麂海洋站１９８１－１９９０年实测波浪资料，探讨了该海域风浪的平均波陡与平均波龄的统计分布特征。分析结果：当风浪平均波陡介于０．０２－０．０４时，其出现频率各季在８２％以上；当风浪平均波龄介于０．５－１．２时，其出现频率各季在７８％以上；当风浪的平均波陡与平均波龄介于０．０２－０．０４和０．５－１．０时，其出现频率为５３．５％－６９．６％。     

波面位移非对称性对风浪成长状态的依赖性

以二阶随机波动理论为基础，研究了刻画波面位移非对称性的偏度参量λ3对风浪成长参量(反波龄ω和无因次风区χ)的依赖性，得到了λ3与ω和λ3与χ的近似解析关系式，并利用实验室水槽风浪成长实验的实测数据对这些关系式进行了检验。     

风浪场波生横向彻体切应力的分析

使用风浪经验公式和风浪传入近岸的小振幅波动理论计算并分析了地转条件下波生横向彻体切应力随风速、风区、水深等因素的变化规律。结果表明，彻体切应力随风速、风区的增大而增大，直到波浪达到完全成长状态，但增长速度并不规则；为更加直观的显示彻体切应力的海流驱动作用，将其与定常Ekman漂流中的风生湍粘性力进行了有意义的比较，结果表明，在中、高纬度的通常海况下两者具有相同量级，因此，在有波浪场存在的条件下，由风、浪共生海流的总体强度将比理论Ekman漂流大，并且不会完全符合Ekman漂流理论的转向规律，在表层尤其明显。由此说明，在一定情况下在风生漂流研究中考虑由地转引起的波生横向彻体切应力是非常必要的。     

Altimeter Measurements of Wind and Wave Modulation by the Kuroshio in the Yellow and East China Seas

The Kuroshio is the major ocean current conveying heat and water mass in the Pacific Ocean. The impact of the Kuroshio on regional wind and wave distributions has been studied with spaceborne-altimeter measurements in the Yellow and East China Seas. In this region the Kuroshio trajectory is relatively stationary and the monsoon patterns dominate, making it an ideal natural laboratory for large scale air-sea-current interaction research. Major findings from this study include: (a) The Kuroshio exerts significant influence on the wind and wave distributions over a swath about 800-km wide along its path. (b) Seasonal average wind speeds reach a maximum near the Kuroshio axis. The magnitude of enhancement ranges between 20 and 50 percent. (c) The distribution of the surface wave heights displays similar spatial patterns to the wind-speed distribution. The Kuroshio effects on wave heights are further complicated by the hydrodynamic modulation of wave-current interaction and the influence of thermal stratification on wind-wave generation. (d) Kuroshio effects are most prominent in the first and last quarters of the year, and least prominent in the third quarter.     

基于HY-2 卫星观测分析南海风浪关系

海面有效波高(H1/3)是表征海浪的重要参数,随着卫星遥感技术的发展,雷达高度计已成为获取海面有效波高的重要手段,但也只能对卫星星下点轨迹处进行有效观测,远无法满足大范围应用的需求.本研究结合2013年10月HY-2雷达高度计观测的海面有效波高和微波散射计观测的海面风场资料,分别对高、低风速下风浪数据进行拟合,建立了适用于0~40 m/s风速范围内的南海海域风浪关系模型,经模型比对和结果验证,结果表明,基于HY-2卫星数据分析建立的南海海域风浪关系模型是可信的,特别是低风速的风浪模型与实测数据建立的风浪模型具有很好的一致性;根据建立的风浪关系模型,从卫星散射计大面观测的海面风场出发,能推算出风浪条件下海面有效波高的大面信息,数据覆盖远高于卫星高度计的星下点观测,能为分析和预报海浪、风暴潮灾害提供大范围的海面有效波高信息.     

Negative correlations of variations in near-water wind and surface wind waves

The relationship between the intensity of surface wind waves and near-water wind is analyzed. The data of measuring wind waves and near-water wind under natural conditions in the Black Sea (July 2004) and Norwegian Sea (June 2003, 16th cruise of the R/V Akademik Sergei Vavilov) are used. A phenomenon of negative correlations has been found between the intensity of wind waves and near-water wind in regions of substantial restructuring of wind waves in the field of inhomogeneous flows: wind-wave amplification during wind decay and vice versa. Examples of such observations are presented, a theoretical model is constructed for the observed phenomenon, and a good agreement is obtained between theory and experiment.     

滆湖北部人工地形重塑下风浪场变化研究

风浪是影响浅水湖泊物理生境环境重要的水动力要素之一。基于滆湖实测风浪数据, 建立了滆湖风浪模型, 验证结果表明模型可以较好模拟滆湖风浪随风场变化情况。在此基础上开展滆湖北部水域在人工地形重塑工程实施后的风浪变化情况分析。结果表明, 不同季节盛行风下, 风浪强度和湖底扰动强度均有一定程度的衰减, 这有利于水体透明度和水底光照条件的改善。风浪强度的衰减使得具有有利于水生植物生长与发育风浪条件的水域面积显著扩增。人工地形重塑的实施, 有利于滆湖北部水域水生植被物理生境环境改善, 从而为滆湖北部水域水生植被的修复提供较好的环境支撑, 也为其他浅水湖泊地形重塑工程的实施提供借鉴。     

基于多层感知器的风涌浪分离方法

风涌浪分离是研究风浪、涌浪各自特性的基础,但受限于海浪谱数据的匮乏,基于海浪谱的风涌浪分离方法难以普及应用,有效的解决办法是采用波浪观测中容易获取的基本波要素进行风涌浪分离。现有方法无法利用基本波要素全面计算出风浪、涌浪的比例及其特征参数,为此本文将机器学习引入到风涌浪分离中,以多层感知器模型为基础,提出了一种利用基本波要素、风要素准确计算出风涌浪参数的方法。该方法需要每个测站提供至少466笔、建议766笔及以上的实测波浪数据作为训练样本,适用于台湾海峡3个测站,在计算精度上显著优于基于海浪频谱的传统风涌浪分离方法,可为本海域缺乏海浪谱的测站提供替代性的风涌浪计算方案,有助于扩大实测风涌浪资料的来源,进而加强风涌浪分布特性以及预警预报研究。     

基于ERA-Interim再分析资料的南沙海域风、浪场特征分析

基于ERA-Interim再分析资料,统计分析了南沙海域的风场、海浪场的时空特征,并进一步研究了风浪成长关系,建立了适用于南沙海域的风浪模型。月平均场分析结果表明:在季风期,南沙海域的月平均有效波高与风场的时空分布特征有良好的对应关系,位于中南半岛的东南部存在一个风速和有效波高的大值中心,冬季强于夏季,中心位置随季节转换稍向下风向移动。频率分析结果表明:南沙海域全年以4级以内风力和3级以内海浪出现的频率最高,6级以上大风和5级以上海浪主要出现在冬季风期间;全年最大风速和浪高出现在10、11月,最大风速达到8级,最大有效波高可达6级,但频率非常小;整个海域风速和浪高最小的时期是4—5月。     

Gulf stream ground truth project: Results of the NRL airborned sensors

Results of an airborne study of the waves in the Gulf Stream are presented. These results show that the active microwave sensors (high-flight radar and wind-wave radar) provide consistent and accurate estimates of significant wave height and surface wind speed, respectively. The correlation between the wave height measurements of the high-flight radar and a laser profilometer is excellent.     

Modification of SAR spectra associated with surface wind fields in the sea off the Kii Peninsula: A case study

Using surface wave parameters and a high-resolution surface wind field derived from Synthetic Aperture Radar (SAR) image mode data, we have investigated the spatial modification of SAR spectra. We found a surface wind front, formed by sheltering effect of the Kii Mountains, separating high and low wind-speed regions in a sea area of an European Remote-Sensing Satellite (ERS) SAR image off the Kii Peninsula. A swell system propagating westward dominates in the whole sea area covered by the SAR image. The wavelength retrieved from the SAR spectra in the sheltered (non-sheltered) region is longer (shorter). Since the distributions of surface wave parameters and surface wind speed are so well correlated, it can be considered that the SAR spectra are modified differently by the sheltered/non-sheltered surface winds. In order to examine the phenomena observed on the SAR image we have estimated the wind-wave SAR spectrum using the SAR surface winds, a wind-wave spectrum model and a SAR wave imaging model. We assume that the SAR spectrum related to the swell is homogeneous in the area imaged by SAR, and that the SAR spectrum of the wind-wave components causes the observed SAR spectra modification. Differences between the observed SAR spectra and the estimated SAR spectra in the sheltered and non-sheltered regions agree well with each other. In the present case, it can be concluded that the observed SAR spectra can be regarded as a linear combination of the wind-wave SAR spectra and the swell SAR spectra.     

Rainfall effect on wind waves and the turbulence beneath air-sea interface

Rainfall effects on wind waves and turbulence are investigated through the laboratory experiments in a large wind-wave tank. It is found that the wind waves are damped as a whole at low wind speeds, but are enhanced at high wind speeds. This dual effect of rain on the wind waves increases with the increase of rain rate, while the influence of rainfall-area length is not observable. At the low wind speed, the corresponding turbulence in terms of the turbulent kinetic energy （TKE） dissipation rate is significantly enhanced by rain- fall as the waves are damped severely. At the high wind speed, the augment of the TKE dissipation rate is suppressed while the wind waves are enhanced simultaneously. In the field, however, rainfall usually hin- ders the development of waves. In order to explain this contradiction of rainfall effect on waves, a possibility about energy transfer from turbulence to waves in case of the spectral peak of waves overlapping the inertial subrange of turbulence is assumed. It can be applied to interpret the damping phenomenon of gas trans- fer velocity in the laboratory experiments, and the variation of the TKE dissipation rates near sea surface compared with the law of wall.     

Statistical properties of microwave backscattering from laboratory wind-wave surfaces

The microwave backscattering from wind-wave surfaces is observed in a windwave tunnel under various conditions of the wind and wind waves, and its statistical features are investigated. The dependence of the backscattered power on the wind speed and the incident angle shows similar features to those predicted by models proposed previously. However, the dependence of the backscattered power on the incident angles also corresponds to the asymmetrical feature of the wind-wave surfaces with respect to the wind direction. The spectral analyses of time series of the backscattered intensity show that the propagating speed of fine structures of the wind-wave surface contributing to the backscattering at large incident angles does not coincide with the phase speed of the freely propagating Braggwaves. Atupwind incidence, the surface structures of wind waves contributing to the backscattering propagates with the dominant waves at their phase speed. This result is inconsistent with the two-scale model in which the Bragg waves are simply superimposed on longer waves, but is consistent with the results of optical observation by Ebuchiet al. (1987). At downwind incidence, the propagating speed is slower than the phase speed of the dominant waves.