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1.
一种白浪覆盖率与风要素关系模式   总被引:2,自引:0,他引:2  
采用Glazm an 提出的“微尺度平均”的方法,在合理选择平均尺度的基础上计算了JONSWAP谱的四阶矩,并将此结果与Snyder提出的白浪覆盖率模式结合,从而建立起依赖于风速和风区两者的半经验、半理论的白浪覆盖率与风要素关系模式。此模式给出的结果与Monahan 等汇集的海洋白浪覆盖率测量数据总体符合良好。  相似文献   

2.
海洋白浪覆盖率模式的研究   总被引:2,自引:0,他引:2  
在波面位移为均匀正态分布的假定下,导出以海浪谱矩为参量的波面斜率分布函数,依此函数,利用极限波面斜率为波浪破碎判据导出依赖于海浪谱四阶矩的白浪覆盖率的表示式,又通过Krylov谱和SMB海浪预报方法的经验公式,将海浪谱四阶矩代之以风要素,从而首次建立了一个依赖于风速和风区两者的半理论,半经验的海洋白浪覆盖率模式,此模式给出了结果与Monahan汇集的海洋白浪覆盖测量数据符合颇佳。  相似文献   

3.
将Adler关于二维随机波场跨水平特征量的理论应用于二维线性随机海浪,严格导出了二维海浪波包的跨水平特征量表达式,并利用该式讨论了给定时刻二维海浪的一种几何结构——大波簇集情况。对于海面上波高均超过较高参考水平的一簇大波,给出了一个计算其中波峰平均个数的公式,它与Glazman所给出的公式不同另外还给出计算上述大波簇平均面积的公式。最后结合现有的海浪万向谱给出一些具体计算结果,并对这些结果进行了讨论。  相似文献   

4.
基于江苏沿海辐射沙洲南翼实测波浪资料,采用波包线理论计算实测波包谱,利用改进的公式对无因次化平均波包谱曲线进行拟合,得到了一个能够反映辐射沙洲南翼海域风浪波包能量分布的波包谱经验公式.同时,考虑了基于波包线理论的群高参数和群长参数,结合实测资料初步建议了此海域群高及群长参数的取值.此外,结合相关统计参数对波包谱经验公式进行了简化,并将计算所得的谱峰值和零阶矩与实测统计值进行对比验证,谱峰值相对误差范围为0.1%~80.0%,均值为23.5%,零阶矩的相对误差范围为0.0%~23.5%,均值为5.0%.从总体上来说,经验公式确定的波包谱与实测波包谱符合较好,对今后辐射沙洲南翼海域的波群理论研究及工程建设具有一定的参考价值.  相似文献   

5.
应用理论推导及数值计算方法,对Stokes随机波的谱特性进行了分析。首先将波面方程,海水质点水平速度用一阶波面分量的非线性组合表示,应用平稳随机高阶短的降阶计算法则,得到了波面方程及海水质点水平速度与一阶波面分量的自相关函数之间的关系,从而确定了Stokes随机波浪的波浪谱密度及海水质点水平速度和加速度谱密度,进而求得有关波浪要素的均方根值。文章还应有数值计算方法,分析了波浪基本参数对均方根值的影响。  相似文献   

6.
海浪周期关系的研究   总被引:2,自引:0,他引:2  
本文利用现场观测数据、实验室风浪槽观测数据和由文氏谱及JONSWAP谱生成的模拟数据,研究了有效周期与谱平均周期、谱峰周期与谱平均周期以及有效周期与谱峰周期的关系,通过数据拟合给出了相应的关系式.研究发现,有效周期与由谱的负阶矩计算的平均周期之间的关系更加稳定,并且有效周期与负2阶矩计算的平均周期几乎相等,均代表了海浪主导波对海浪平均周期的贡献.  相似文献   

7.
王伟  徐德伦  楼顺里 《海洋学报》1990,12(5):638-647
本文报告首次进行的海洋白浪、泡沫和沫流带与海面摩擦速度的直接同步测量结果.由此结果得海洋白浪覆盖率Wc与海面摩擦速度U*的经验关系为Wc=1.34×10-5U*1.93.这一关系式支持白浪覆盖率正比于海面风应力的论断;显著不同于白浪覆盖率正比于摩擦速度3次方的物理分析结果.基于此经验关系式,还对白浪在海-气交换中的作用进行了讨论.  相似文献   

8.
徐德伦  赵锰  楼顺里 《海洋学报》1990,12(3):291-297
本文报告波群统计特性研究结果的第二部分.提出用波包谱零阶、二阶矩和波面谱零阶、二阶矩计算平均历时长度和平均连长的新方法.用不规则波造波系统在水槽内产生的具有不同群性的三列不规则波作了验证,并与按Nolte和Hsu公式计算的平均历时长度和按Ewing公式计算的平均连长作了比较.验证和比较结果表明,本文提出的方法不仅可行,且具有一定的优越性.  相似文献   

9.
在波面位移为正态过程的假定下,推导出一种以平均周期和风速为参量的白浪覆盖率公式W=1-Φ[5.11094[-T/U10]0.7576].依据摩擦风速和U10的表达式,进一步推导出白浪覆盖率依赖于摩擦风速的形式W=1-Φ[0.5227[-T/U]0.7576]].考虑到在实际应用中,经常需要用波龄描述波浪的状态,将白浪覆盖率表示成一种形式简单的波龄的函数W=1-Φ(3.6496ξ0.7576),与Monahan等的海上测量数据符合良好.  相似文献   

10.
白浪覆盖率法(白浪法)是被广泛应用的计算气溶胶粒子通量的方法,但是公式本身还存在一些问题,且其在低纬度海域的应用情况还未见报道。本文利用2012年8月25日—10月12日在中国南海走航实验观测的气溶胶粒子浓度数据,对Monahan等的白浪覆盖率-风速的公式进行了修正,并利用最小二乘法推导出单位白浪面积上次微米气溶胶产生通量与风速的关系。对半径小于0.3μm的粒子,通量的分布符合对数正态分布,通量的对数与风速呈幂函数关系。与高纬度海域的研究相比,中国南海飞沫气溶胶粒子的排放通量特征表现为较小粒子(r800.2μm)较其他海域偏高,而较大粒子略偏低。当风速在7~13m·s-1时,用新的源函数计算的通量与观测值保持较高的一致性。  相似文献   

11.
More and more researches show that neither the critical downward acceleration nor the critical slope of water waves is a universal constant. On the contrary, they vary with particular wave conditions. This fact moders the models either for the probability of wave breaking B or for the whitecap coverage W based on these criteria difficult to apply. In this paper and the one which follows we seek to develop models for the prediction of both B and W based on the kinematical criterion. First, several joint probabihstic distribution functions (PDFs) of wave characteristics are derived, based on which the breaking properties B and W are estimated. The estimation is made on the assumption that a wave breaks ff the horizontal velocity of water particles at its crest exceeds the local wave celerity, and whitecapping occurs in regions of fluid where water particles travel faster than the waves. The consequent B and W depend on wave spectral moments of orders 0 to 4.Then the JONSWAP spectrum is used to represent the fetch-limited sea waves in deep water, so as to relate the probahility of wave breaking and the whitecap coverage with wind parameters. To this end, the time-averaging technique proposed by Glazman (1986) is applied to the estimation of the spectral moments involved, and furthermore, the theoretical models are compared with available observations collected from published literature. From the comparison, the averaging time scale is determined. The final models show that the probability of wave breaking as well as the whitecap coverage depends on the dimensionless fetch. The agreement between these models and the database is reasonable.  相似文献   

12.
The propagation,shoaling and breaking of solitary waves on mild slopes are simulated byboundary element method.In this paper,the criterion of breaking solitary waves on mild slopes is discussed.The criterion is that the ratio of horizontal velocity of water particles on the wave crest to wave celerity equalsone.However,the case that the ratio of horizontal velocity of water particles on the wave crest to wave ce-lerity is below one but the front face of wave profile becomes vertical is also considered as a breaking criteri-on.According to the above criteria,the breaking index for slopes 1:10 to 1:25 is studied.The result is com-pared to other researchers'.The deformation of solitary waves on slopes is discussed and the distribution offluid velocities at breaking is shown.  相似文献   

13.
When waves propagate from deep water to shallow water, wave heights and steepness increase and then waves roll back and break. This phenomenon is called surf. Currently, the present statistical calcula...  相似文献   

14.
为了探寻波浪破碎与波形不对称性的关系,通过对1/200缓坡上波浪破碎实验研究结果的进一步分析,运用最小二乘法,拟合了波形不对称性参数与相对水深的关系,以及用波形不对称性参数表示的波浪破碎指标表达式。所得规则波的结果与Kjeldsen的深水波结果相同,而不规则波的结果比规则波的小。研究还表明,这一破碎指标与相对水深有关系,随着水深变浅,指标值增大。  相似文献   

15.
近岸波浪破碎区不规则波浪的数值模拟   总被引:2,自引:0,他引:2       下载免费PDF全文
唐军  沈永明  崔雷  邱大洪 《海洋学报》2008,30(2):147-152
基于近岸不规则波浪传播的抛物型缓坡方程和两类波浪破碎能量损耗因子,对近岸波浪破碎区不规则波浪的波高分布进行了数值模拟,并结合实验结果对数值模拟结果进行了验证分析,结果表明采用两类波浪破碎能量损耗因子所模拟的破碎区波高与实测值均吻合良好,波浪破碎能量损耗因子及波浪破碎指标对破碎区波浪波高分布影响较明显。  相似文献   

16.
一个新的破碎波统计模式   总被引:6,自引:1,他引:6       下载免费PDF全文
由运动方程和涡度方程所导得的两个首次积分估计给出了海波破碎的发生条件和破碎波的波面限制。由这两个条件所构造的新的破碎波统计模式,可导出海波的破碎面积率、破碎体积率和破碎能量损耗率的解析表达式,加之一个简单的白冠物理模型又导出了一个新的白冠覆盖率的解析表达式。  相似文献   

17.
The characteristics of wave and turbulence velocities created by a broad-banded irregular wave train breaking on a 1:35 slope were studied in a laboratory wave flume. Water particle velocities were measured simultaneously with wave elevations at three cross-shore locations inside the surf zone. The measured data were separated into low-frequency and high-frequency time series using a Fourier filter. The measured velocities were further separated into organized wave-induced velocities and turbulent velocity fluctuations by ensemble averaging. The broad-banded irregular waves created a wide surf zone that was dominated by spilling type breakers. A wave-by-wave analysis was carried out to obtain the probability distributions of individual wave heights, wave periods, peak wave velocities, and wave-averaged turbulent kinetic energies and Reynolds stresses. The results showed that there was a consistent increase in the kurtosis of the vertical velocity distribution from the surface to the bottom. The abnormally large downward velocities were produced by plunging breakers that occurred from time to time. It was found that the mean of the highest one-third wave-averaged turbulent kinetic energy values in the irregular waves was about the same as the time-averaged turbulent kinetic energy in a regular wave with similar deep-water wave height to wavelength ratio. It was also found that the correlation coefficient of the Reynolds stress varied strongly with turbulence intensity. Good correlation between u′ and w′ was obtained when the turbulence intensity was high; the correlation coefficient was about 0.3–0.5. The Reynolds stress correlation coefficient decreased over a wave cycle, and with distance from the water surface. Under the irregular breaking waves, turbulent kinetic energy was transported downward and landward by turbulent velocity fluctuations and wave velocities, and upward and seaward by the undertow. The undertow in the irregular waves was similar in vertical structure but lower in magnitude than in regular waves, and the horizontal velocity profiles under the low-frequency waves were approximately uniform.  相似文献   

18.
响水近岸海域波浪特性研究   总被引:3,自引:0,他引:3  
基于响水波浪站累计一整年的现场观测资料,分析了波高和波周期的年内变化特性,研究了波浪的统计特性和波谱特性,并总结归纳了该海域各特征波要素之间以及各波谱参数之间的转换关系。结果显示:响水海域全年有效波高的变化幅度在0.10~2.80 m之间,年平均值为0.56 m;最大波高的变化幅度在0.15~5.58 m之间,年平均值为0.93 m;平均波周期的变化范围为1.91~9.02 s,年平均值为3.90 s。夏季大波高发生频率明显要小于冬、春季节,波浪季节性变化较为显著。就波高和波周期分布而言,通过拟合得出的Weibull分布较为适合本海域实测波高分布和波周期分布。波谱特性方面,本海域双峰谱占到总数的62.5%,且低频谱峰值普遍高于高频谱峰值,其中低频谱峰出现在0.04 Hz左右,高频谱峰则出现在0.15~0.20 Hz之间,分别为本海域涌浪和风浪所集中的频率区间。采用回归分析方法进一步分析了各特征波要素之间以及各波谱参数之间的关系,发现多数波参数之间存在显著的相关性,但受波浪浅水变形影响,各参数之间的比值与理论深水关系有所区别。本文的研究成果可为沿海建筑物的设计以及防灾减灾提供参考和依据。  相似文献   

19.
LI  Yucheng 《中国海洋工程》2002,16(1):79-87
Regular wave deformation and breaking on very gende slopes is calculated by Mixed-Eulerian-Lagrangian procedure. The velocity potentials and their normal derivatives on the boundary are calculated through the mixed 0-1 boundary element method. The wave elevation and the potentials of time-stepping integration are detertnined by the 2nd-order Taylor expansion at the nodes of free surface boundary elements. During calculation the x-coordinates of the free surface element nodes are supposed to remain unchanged, i.e. the partial derivatives of wave elevation and potentials with respect to x are considered as zero. The numerical results of asymmetric parameters of breaking waves are verified by experimental study. It is shown that when the wave asymmetry is weak, the maximum horizontal velocity of water particales occurs at the wave peak and, the average ratio of this maximum velocity to wave celerity is 0.96. However, when the wave asymmetry is strong, the maximum horizontal velocity of water particles occu  相似文献   

20.
浙江中部三门湾波浪特征统计分析   总被引:2,自引:0,他引:2  
为了研究浙江中部三门湾海域的波浪特征,本文基于AWAC波浪观测仪在该海域进行了连续1年的观测,对观测得到的波浪参数进行了统计分析、线性回归分析,同时研究分析了三门湾海域受台风影响时,波浪参数和波浪谱的变化情况,探讨了波浪变化的原因。研究表明,三门湾海域常浪向和强浪向均为E向,地形是主导因素;显著波高绝大部分在0.8 m以下,期间的最大波高为2.71 m;该海域的波浪特征分布是一个比较典型的瑞利分布;台风“泰利”期间波能谱以双峰为主,外海涌浪和研究海域风区内的风浪形成混合浪,其中0.08 Hz左右的低频涌浪成分占比很大,而0.25 Hz左右的高频风浪成分占比较小。本文的研究工作为沿海海洋工程结构物的设计建造以及防灾减灾提供重要参考依据。  相似文献   

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