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1.
沙纹微地形普遍存在于海底,沙纹的消长能改变底部应力进而影响泥沙的运移。以往研究较多侧重于波致沙纹,并已应用于波浪模式的底摩擦计算,而较少考虑波流联合效应产生的沙纹,也未将其应用于综合的水动力模式和沉积物输运模式。本文在POM水动力模式中嵌入新南威尔士大学泥沙模式,通过耦合波流共同作用的微地形模型与波流相互作用底边界层模型,发展了波浪-海流-微地形(沙纹)耦合的沉积动力模式。本文将该模式应用于澳大利亚Jervis湾,针对波主导和波流联合主导沙纹两种类型,分别进行了沙纹发展状态、几何形态的分布及悬浮泥沙的模拟。结果表明:波致沙纹比波流联合作用的沙波具有更大的波高和波长,因此当波主导时沙纹对悬浮泥沙起着关键作用。通过考虑随沙纹变化的粗糙度,相比于以往模式设置均一的粗糙度,该模型能对悬浮物浓度的骤升过程进行更精细的预测。  相似文献   

2.
研究了波致底切应力和二维辐射应力对悬沙的作用.首先对东山湾的水动力进行了数值模拟并与实测资料进行了对比检验,然后对东山湾悬浮泥沙进行了考虑波浪和不考虑波浪两种情况下的数值模拟并与实测资料进行了相关对比分析.在模式建立过程中,依据东山湾独特的窄口型半封闭河口海湾的特点,基于ECOMSED模式(2002)建立了东山湾三维水动力模型,并通过第三代海浪模式MASNUM加入了波浪对底切应力及辐射应力的影响,通过ECOMSED中的底边界层模型考虑了波浪增强底摩擦的作用,综合分析了东山湾的水动力及泥沙状况.结果表明在东山湾数值模拟中,该模式能较好地模拟这类海域的水动力及泥沙输运状况.在东山湾模拟计算中,潮流的作用强于波浪的作用,但考虑波浪因素后,泥沙模拟结果更好.在波浪的作用中,底切应力相比于二维辐射应力占有绝对的优势,两者相差2个量级以上,因此可以不考虑二维辐射应力的影响.  相似文献   

3.
浪、潮、风暴潮联合作用下的底应力效应   总被引:7,自引:1,他引:6  
运用建立的二维非线性浪,潮和风暴耦全模式分析了波流相互作用下的底应力及其对耦合波浪场和流场的影响。由渤海的两次强寒潮过程的数值实验表明,在波流相互作用下,底应力明显增大,增大的底应力对波浪场影响甚微,但将明显改变水位和流速的大小,这种影响在近岸浅水区更加显著。  相似文献   

4.
近岸区域波流耦合作用的数学模型   总被引:5,自引:0,他引:5  
本文提出了一个讨论近岸波浪和波生流耦合作用的二维数学模型。在波浪场中运用波数矢量无旋和波作用量守恒方程求解波浪在波生流作用下的折射、绕射变形,以辐射应力作为波生流场的驱动力,考虑地转柯氏力和海底底摩擦的作用。文中采用Dingemans(1987)的地形对波流耦合作用进行了分析。数值计算结果表明波流耦合作用对近岸波浪场和波生流场的影响比较显著,在工程实际上应当综合考虑波流耦合问题。  相似文献   

5.
结合椭圆型缓坡方程模拟近岸波流场   总被引:6,自引:3,他引:6  
波浪向近岸传播的过程中,由波浪破碎效应所产生的近岸波流场是近岸海域关键的水动力学因素之一.结合近岸波浪场的椭圆型缓坡方程和近岸波流场数学模型对近岸波浪场及由斜向入射波浪破碎后所形成的近岸波流场进行了数值模拟.计算中考虑到波浪向近岸传播中由于波浪的折射、绕射、反射等效应使局部复杂区域波向不易确定,采用结合椭圆型缓坡方程所给出的波浪辐射应力公式来计算波浪产生的辐射应力,在此基础上耦合椭圆型缓坡方程和近岸波流场数学模型对近岸波流场进行数值模拟,从而使模型综合考虑了波浪的折射、绕射、反射等效应且避免了对波向角的直接求解,可以应用于相对较复杂区域的近岸波流场模拟.  相似文献   

6.
联合第三代浅水海浪模式SWAN和三维海流模式POM,建立考虑海浪影响的三维风暴潮模式,利用该模式,在渤黄海区域,对温带气旋830315诱发的风暴潮进行数值模拟,从海表风应力、辐射应力、底应力三方面入手,对海浪对风暴潮的影响进行了数值研究.研究表明:海浪通过风应力对风暴潮水位的影响最为显著,而波致辐射应力与依赖波流相互作用的底应力的影响只在渤海和北黄海相对明显;考虑海浪影响的风暴潮水住过程曲线模拟结果,比不考虑海浪影响的纯风暴潮模拟结果与实测水位曲线吻合的更好,尤其是在减水极值处,其相对误差不超过5.57%.  相似文献   

7.
联合第三代浅水海浪模式SWAN和三维海流模式POM,建立考虑海浪影响的三维风暴潮模式,利用该模式,在渤黄海区域,对温带气旋830315诱发的风暴潮进行数值模拟,从海表风应力、辐射应力、底应力三方面入手,对海浪对风暴潮的影响进行了数值研究.研究表明海浪通过风应力对风暴潮水位的影响最为显著,而波致辐射应力与依赖波流相互作用的底应力的影响只在渤海和北黄海相对明显;考虑海浪影响的风暴潮水住过程曲线模拟结果,比不考虑海浪影响的纯风暴潮模拟结果与实测水位曲线吻合的更好,尤其是在减水极值处,其相对误差不超过5.57%.  相似文献   

8.
珠江口磨刀门月际尺度地貌演变研究   总被引:1,自引:1,他引:0  
本文基于二维波流耦合泥沙数学模型对磨刀门河口月际尺度地貌演变进行了模拟研究。结果表明:(1)枯季,无波浪作用下,磨刀门河口总体呈淤积状态;波流耦合后,磨刀门河口整体由淤积转为以冲刷为主。洪季,无波浪作用下,磨刀门河口除西汊外均呈淤积状态;波流耦合后,拦门沙内坡与中心区转为冲刷状态,整体仍以淤积为主,但总淤积量减少;(2)月际尺度上,地貌变化幅度为厘米级,洪枯季具有明显差异。不考虑波浪作用下,磨刀门河口洪、枯季均以淤积为主,但洪季淤积幅度更大;波流耦合后,磨刀门河口呈洪淤枯冲的格局;(3)空间上,拦门沙外坡洪淤枯冲,拦门沙顶洪季淤积、枯季变化不大,内坡洪枯季均为冲刷。此外,拦门沙内坡以径潮流作用产生的底切应力为主,外坡以波浪作用引起的底切应力为主。  相似文献   

9.
针对整个渤海海域悬浮泥沙季节变化及其影响机制的数值研究相对缺乏且机制尚不清晰,基于ROMS三维海洋模型对渤海海域水动力环境与悬沙分布开展数值模拟。模拟结果显示,渤海海峡环流终年“北进南出”,夏季环流明显强于冬季,并呈现外围逆时针环、内部顺时针环的“双环”结构。渤海中部海域在夏季存在明显的温跃层现象,其强度分布与等深线较为一致,温跃层在4月开始形成,7月最强。渤海表层悬沙分布具有显著的季节变化,冬季悬沙浓度最大,秋季次之,春季再次之,夏季最小。控制悬沙浓度的波流底切应力在秋冬季节较大,春夏相对较小,且流致切应力始终在波流切应力中占主导地位。秦皇岛海域悬沙浓度常年偏低的主要原因是位于M2无潮点附近,属于弱潮流区,底层流速相对较小,底部沉积物发生再悬浮概率较小。夏季温跃层的存在在一定程度上减小了底边界层流速,增大了流速的垂向梯度,对底部悬浮泥沙的向上扩散有明显的抑制作用。因此,温跃层的存在是造成夏季表层悬沙浓度最低的重要原因。  相似文献   

10.
为准确把握新鹤海湾的演变特征和水动力条件,采用现场观测和GIS技术对其地形变化、冲淤分布和冲淤量进行探讨,并利用数值模拟分析波浪、潮流和泥沙共同作用对海湾演变的影响。结果表明:海湾演变对连续台风的响应不同,表现为先冲后淤,其中苏拉作用下的冲刷量为台风过境后全年的2倍左右;受东南季风的影响,春夏冲淤幅度较大,海湾冲淤分布为南冲北淤,波高分布不均与涨潮流入湾时的向北偏转是其主要原因;波流共同作用下的底床切应力约为潮流单独作用时的10倍,波浪是导致海湾冲刷的主要因素,常浪下底床切应力小于临界冲刷应力,泥沙不易起动,因此海湾冲刷主要是由极端天气时的大浪所导致的。  相似文献   

11.
A sediment numerical model was embedded into a wave-tide-circulation coupled model to simulate the transport processes of the Yellow River-derived sediment considering the wave-induced vertical mixing (Bv) and the wave-current coupled bottom shear stress (BSS). Numerical results show that the main stream of the Yellow River-derived sediment moves first eastward off the northern Shandong Peninsula and then southward into the South Yellow Sea all year round. In spring, the sediment moves northeastward in the Bohai Sea. In summer, there is a northeastward branch of sediment in the Bohai Sea off the west coast of the Liaodong Peninsula, while the main part goes eastward to the Yellow Sea. The Yellow River-derived sediment transport from the Bohai Sea to the North Yellow Sea across the Bohai Strait is mainly limited to the top 10 m, and with a maximum centered at 37.9°N in summer. The transport from the North Yellow Sea to the South Yellow Sea across the transect of 37°N is mainly in the 0–30 m layer with a maximum around 123.7°E in autumn. The simulated Yellow River-discharged sediment deposits along the Shandong Peninsula and between 20 and 30 m isobaths in the Yellow Sea, which is consistent with observation. If surface waves are not considered in the model, the sediment deposits westward to the nearshore area in the South Yellow Sea. The sediment would deposit further southward in the numerical experiment results without wind influence. In the numerical experiment of no tide, there is hardly any sediment deposited on the Yellow Sea floor, while in the Bohai Sea most of the sediment is transported southward and northwestward around the river mouth instead of eastward as in the Control Run, indicating the tides play a key role in forming the deposition pattern.  相似文献   

12.
A three-dimensional wave radiation stress is introduced into the hydrodynamic sediment coupled model COHERENS-SED, which has been developed through introducing wave-enhanced bottom shear stress, wave dependent surface drag coefficient, wave-induced surface mixing, SWAN, damping function of sediment on turbulence, sediment model and depth-dependent wave radiation stress to COHERENS. The COHERENS-SED is adopted to study the effects induced by wave-induced three-dimensional longshore current on suspended sediment spreading of the Huanghe River (Yellow River) mouth. Several different cases divided by setting different wave parameters of inputting boundary waves are carried out. The modeling results agree with measurement data. In terms of simulation results, it is easy to know that three-dimensional wave radiation stress plays an obvious role when inputting boundary wave height is stronger than 3 m. Moreover, wave direction also affects the sediment spreading rules of the mouth strongly too.  相似文献   

13.
A three-dimensional wave radiation stress is introduced into the hydrodynamic sediment coupled model COHERENS-SED,which has been developed through introducing wave-enhanced bottom shear stress,wave dependent surface drag coefficient,wave-induced surface mixing,SWAN,damping function of sediment on turbulence,sediment model and depth-dependent wave radiation stress to COHERENS.The COHERENS-SED is adopted to study the effects induced by wave-induced three-dimensional longshore current on suspended sediment spreading of the Huanghe River (Yellow River) mouth.Several different cases divided by setting different wave parameters of inputting boundary waves are carried out.The modeling results agree with measurement data.In terms of simulation results,it is easy to know that three-dimensional wave radiation stress plays an obvious role when inputting boundary wave height is stronger than 3 m.Moreover,wave direction also affects the sediment spreading rules of the mouth strongly too.  相似文献   

14.
海洋动力作用下,河口海岸地区海床通常处于动态变化之中。作为地质环境的控制因素,海床沉积物侵蚀再悬浮过程的研究具有重要意义。为阐明胶州湾海域水动力条件对海床侵蚀再悬浮的作用,本文利用海底原位观测三脚架进行了现场观测。观测结果显示:通常条件下,潮流导致的最大海床剪应力可达0.35 N/m2,高于波浪引起的剪应力。涨潮期间,海床发生侵蚀;退潮期间,海床发生淤积。风速达到5 m/s时,波浪引起的剪应力近似等于流致剪应力。风速达到7 m/s时,有效波高为26 cm,波浪对海床侵蚀再悬浮过程起主要作用;此时也会导致海水浊度显著上升,高于通常条件下的2-8倍。分析表明:通常条件下,周期性海流影响海床侵蚀再悬浮过程;而大幅度沉积物再悬浮过程由偶发的波浪事件控制。针对胶州湾沉积物动力学机制的深入研究仍待进一步开展。  相似文献   

15.
In order to study the mechanism of flow-sediment movement, it is essential to obtain measured data of water hydrodynamic and sediment concentration process with high spatial and temporal resolution in the bottom boundary layer (BBL). Field observations were carried out in the northwest Caofeidian sea area in the Bohai Bay. Near 2 m isobath (under the lowest tidal level), a tripod system was installed with AWAC (Acoustic Wave And Current), ADCP (Acoustic Doppler Current Profilers), OBS-3A (Optical Backscatter Point Sensor), ADV (Acoustic Doppler Velocimeters), etc. The accurate measurement of the bottom boundary layer during a single tidal period was carried out, together with a long-term sediment concentration measurement under different hydrological conditions. All the measured data were used to analyze the characteristics of wave-current-sediment movement and the BBL. Analysis was performed on flow structure, shear stress, roughness, eddy viscosity and other parameters of the BBL. Two major findings were made. Firstly, from the measured data, the three-layer distribution model of the velocity profiles and eddy viscosities in the wave-current BBL are proposed in the observed sea area; secondly, the sediment movement is related closely to wind-waves in the muddy coast area where sediment is clayey silt: 1) The observed suspended sediment concentration under light wind conditions is very low, with the peak value generally smaller than 0.1 kg/m3 and the average value being 0.03 kg/m3; 2) The sediment concentration increases continuously under the gales over 6-7 in Beaufort scale, under a sustained wind action. The measured peak sediment concentration at 0.4 m above the seabed is 0.15-0.32 kg/m3, and the average sediment concentration during wind-wave action is 0.08-0.18 kg/m3, which is about 3-6 times the value under light wind conditions. The critical wave height signaling remarkable changes of sediment concentration is 0.5 m. The results show that the suspended load sediment concentration is mainly influenced by wave-induced sediment suspension.  相似文献   

16.
为给寒区海域的波浪能估算提供科学依据,提出一种合理推算冰水共存海域波浪条件及波能流密度的方法,该方法将海冰模型与水动力学模型耦合模拟得到的冰浓度以线性修正函数的方式纳入波浪模型的海面摩阻风速方程中,并基于MCT (model coupling toolkit)耦合器将海冰模型、水动力学模型与波浪模型进行实时耦合。基于该方法模拟了渤海冬季寒潮大风期间的海冰以及波能流密度的演化。模拟结果表明,在2012年2月5~8日寒潮大风期间,结冰区域占到渤海总面积的1/3,约有76%的渤海海域的平均波能流密度受海冰影响减小,其中辽东湾近岸的波能流密度平均受冰影响最多减小了100%,而渤海湾和莱州湾近岸受冰影响最多分别减小了60%和50%。即使是无冰覆盖的老铁山水道,其波能流密度的最大值也受冰影响减少了14%。耦合模拟可以更为准确地对渤海冬季的波能流密度分布进行评估,为波浪能发电厂选址提供依据。  相似文献   

17.
In order to study the mechanism of flow-sediment movement, it is essential to obtain measured data of water hydrodynamic and sediment concentration process with high spatial and temporal resolution in the bottom boundary layer (BBL). Field observations were carried out in the northwest Caofeidian sea area in the Bohai Bay. Near 2 m isobath (under the lowest tidal level), a tripod system was installed with AWAC (Acoustic Wave And Current), ADCP (Acoustic Doppler Current Profilers), OBS-3A (Optical Backscatter Point Sensor), ADV (Acoustic Doppler Velocimeters), etc. The accurate measurement of the bottom boundary layer during a single tidal period was carried out, together with a long-term sediment concentration measurement under different hydrological conditions. All the measured data were used to analyze the characteristics of wave-current-sediment movement and the BBL. Analysis was performed on flow structure, shear stress, roughness, eddy viscosity and other parameters of the BBL. Two major findings were made. Firstly, from the measured data, the three-layer distribution model of the velocity profiles and eddy viscosities in the wave-current BBL are proposed in the observed sea area; secondly, the sediment movement is related closely to wind-waves in the muddy coast area where sediment is clayey silt: 1) The observed suspended sediment concentration under light wind conditions is very low, with the peak value generally smaller than 0.1 kg/m^3 and the average value being 0.03 kg/m^3; 2) The sediment concentration increases continuously under the gales over 6-7 in Beaufort scale, under a sustained wind action. The measured peak sediment concentration at 0.4 m above the seabed is 0.15-0.32 kg/m^3, and the average sediment concentration during wind-wave action is 0.08-0.18 kg/m^3, which is about 3-6 times the value under light wind conditions. The critical wave height signaling remarkable changes of sediment concentration is 0.5 m. The results show that the suspended load sediment concentration is mainly influenced by wave-induced sediment suspension.  相似文献   

18.
渤海海峡沉积物输运的参数化计算   总被引:1,自引:1,他引:0  
本文以2018年冬季渤海海峡两个站位的定点连续观测数据为基础,使用一维参数化方案,计算了观测站位底边界层内的水平悬浮物输运通量以及推移质输运量。在参数化方案中,简化的一维对流扩散方程被用于计算底边界层内的垂向悬浮物浓度。为了验证参数化方案的可靠性,本文基于观测数据对比了两种底剪切应力计算模型、四种临界起动剪切应力计算方法和两种一维对流扩散方程解法。对比结果表明:(1)不同模型计算的底剪切应力结果相近;(2)临界起动剪切应力受到颗粒间黏性作用的影响;(3)一维对流扩散方程的求解过程需要考虑沉积物浓度的分层效应和不同粒级颗粒临界起动剪切应力的差异。基于上述对比结果确定的最优参数化方案,进一步计算了观测站位的沉积物输运量:(1)在有再悬浮的时段,距底5 m内的水平悬浮物通量占全水深悬浮物通量的比例(T01站约为21%,T02站约为17%)显著高于相同层位水通量的占比;(2)依据参数化方案估算的冬季平均的悬浮物通量比忽略底边界层悬浮物浓度垂向变化的传统方法结果高约16%;(3)推移质输运量比悬移质输运量约低两个数量级。  相似文献   

19.
通过大尺度水槽波浪引起泥沙悬移的动床模型实验,研究了沙坝海岸破波带内水底悬沙浓度形成机理,通过比较时间平均水底悬沙浓度与时间平均水底波浪水质点动能或时间平均水底湍动能之间的相关性,论证了利用时间平均湍动能比利用时间平均波浪水质点动能计算时间平均水底悬沙浓度更为适用,并提出了以上时间平均水底悬沙浓度与水底湍动能之间的关系也可以用来近似表达时间变化的水底悬沙浓度与时间变化的水底湍动能之间的关系。研究针对规则波、波群和不规则波3种波浪形态进行,并分别对破波带内的爬坡区、内破波区和沙坝区3个区域实验结果进行讨论。  相似文献   

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