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1.
圆柱形沉浮式深海养殖网箱的受力分析 总被引：9，自引：0，他引：9
应用一系列力学关系，研究了深海圆柱形沉浮式养殖网箱所承受的波浪力情况。导出深海沉浮式养殖网箱的运动方程，并给出数值计算。在网箱波浪力的研究中采用绕射理论和Morison方程，讨论了在波高、波长及周期变化下水动力的变化趋势，得出网箱所受到的水平波浪力远大于竖直波浪力，波高的变化对波浪力的影响最大的结论，为深海网箱的设计校核提供1种参考方法。 相似文献
2.
单点系泊网衣构件波浪试验研究 总被引：4，自引：0，他引：4
采用四种网箱系泊方法,设计单点系泊网衣构件水槽波浪试验。试验构件由六种网衣和框架装配而成,试验工况是规则波,周期为0．7—2．0s,波高为50—250mm。构件在水槽中作来回周期性直线运动,当试验波浪周期较小时,构件的来回运动不明显,主要以波浪运动为主,水动力峰值大体上呈周期性均匀变化;而当周期较长、波高较高时,构件在水动力的作用下产生了与波向相反的长周期漂移运动,有较大振幅的位移、速度和加速度,诱发了水动力的最大值,水动力变化呈现峰值短周期不均匀变化、最大值长周期变化和零拉力周期变化的规律。试验结果显示,与波高参数类似,随着网衣特性系数d／a的增大,网衣构件的水动力也增大,而水动力最大值长周期、零拉力周期变化规律分别是减短和增长的。在周期1．21、1．41、1．61、1．82s情况下,网衣C构件单点系泊试验水动力最大值是固定系泊计算水动力最大值平均的1．706、1．826、2．125、2．236倍,最大达3．61倍,表明单点系泊在波浪条件下构件水动力有较大的增加。 相似文献
3.
依据波浪理论,分析了波浪经过网衣后的流体特性和边界条件,研究了网衣的波浪水动力、波浪透射系数与网衣尺度、特征参数、波浪参数等的关系。设计预加张力放射系泊法进行网衣构件水槽波浪试验。试验构件由10种PE网衣和HDPE框架装配而成,试验工况是规则波,周期为0·8—2·0s,波高为50—250mm。结果表明,作用在网衣上的水平波浪力变化规律与波浪基本一致,呈现周期性和不对称性变化;波浪力变化曲线呈现司托克斯二阶波形状,波峰较陡,波谷较平坦,和波面图相似;网衣水平波浪力周期峰值大约与波高的2·6次方、波长的0·8次方成比例,与网衣宽度l线性相关;随着特征参数d/a增大,网衣波浪力呈线性增加变化,透射系数减少,网衣消浪能力主要集中在网衣水表层。同时设计多层网衣组合的柔性浮式防波堤波浪试验,其消浪能力除了与网衣尺寸、特征参数等相关以外,还与网衣间隔距离有一定的关系。水槽试验时波浪最小透射系数下降到71%左右,从经济、实用角度表明,可用网衣来制作能防护渔业设施的柔性浮式防波堤。 相似文献
4.
HDPE深水网箱抗风浪流性能的海区验证试验 总被引：5，自引：0，他引：5
对HDPE深水网箱2000～2004年间的抗风浪流性能进行了海区验证试验.通过对HDPE深水网箱扶栏、框架、网具以及固泊系统受损率的统计,根据扶栏、框架、网具以及固泊系统在整个深水网系统中的重要程度,分别给予一定的权重统计出深水网箱的整体受损率,能比较客观地反映深水网箱的抗风浪流性能.海区验证试验结果表明,HDPE深水网箱抗风力达35 m/s、抗浪高6 m、抗流速1.0 m/s,与其设计参数基本相同.同时,为了增加HDPE深水网箱的抗风浪流性能,建议扶手管从110 mm改为125 mm、主浮管从250 mm改为300 mm、扶栏高度从1 m降低为0.8 m或0.6 m.风力主要影响扶栏系统,流速主要影响网具系统,而波浪对HDPE圆形浮式深水网箱的框架、网具、固泊系统以及网箱整体结构均有明显影响. 相似文献
5.
量测了在水深0.5m的情况下波浪、水流通过水平沙床所产生的床沙输移。实验波高为0.15m，周期分别为1.4和2.0s。首先量测纯波浪下的床沙输移，然后量测波流共同作用下，水流与波浪行进方向一致其稳定速度分别为0.02,0.04,0.06m/s时的床沙输移，结果表明，2个沙槽所得的总输沙率在波周期2.0s时最大，净输沙率在波周期1.4s时最大，将波叠加在速度为0.02m/s的水流上时，2种波型的净输沙率都增加约1倍，水流为0.04m/s和0.06m/s时2种波型的净输沙率分别都减少。 相似文献
6.
SWAN模型中不同风拖曳力系数对风浪模拟的影响 总被引：1，自引：1，他引：0
本文以荷兰哈灵水道海域为实验区域,通过敏感性实验,研究了在14 m/s、31.5 m/s和50 m/s（分别代表一般大风、强热带风暴和强台风的极端条件）定常风速下SWAN模型中不同风拖曳力系数对风浪模拟的影响程度。结果表明,对于近岸浅水区域（水深小于20 m）,风拖曳力系数计算方案的选择对有效波高影响较小,而且当风速增加到一定程度后,波浪破碎成为影响波高值的主要因素;对于深水区域（水深大于30 m）,一般大风条件下风拖曳力系数计算方案的选择对有效波高影响仍然较小,随着风速的继续增大,风拖曳力系数计算方案的选择对有效波高的影响逐渐显著。对于平均周期,风拖曳力系数计算方案的选择和风速的改变对其影响均较小,而由水深变浅导致的波浪破碎对其影响较为显著。根据敏感性实验结果,本文对SWAN模型中风拖曳力系数计算方案的选择做出如下建议:计算近岸浅水区域风浪场或深水区域一般大风条件风浪场时,其风拖曳力系数可以直接采用模型默认选项;而对于深水区域更大风速条件,可首先采用模型默认选项试算,然后结合当地海域实测波浪资料进行修正。 相似文献
7.
台风作用下琼州海峡海域波浪特征分析 总被引：1，自引：0，他引：1
通过在拟建琼州海峡跨海大桥西线方案主通航孔位置布置波浪测点,采集到2012年13号台风"启德"和23号台风"山神"期间波浪数据,结合两场台风期间波浪频谱和方向谱的变化,分析了该区域在台风期间的波浪特征,并进一步对风浪和涌浪进行了判别。研究结果表明:1)台风"启德"期间,海域波浪谱峰周期在3.38.0 s之间,最大谱峰值为7.92 m2/s,波浪方向为W8.0 s之间,最大谱峰值为7.92 m2/s,波浪方向为WN向,且频谱和方向谱的变化过程反映了风浪到涌浪的转变;2)台风"山神"期间,海域波浪谱峰周期在5.0N向,且频谱和方向谱的变化过程反映了风浪到涌浪的转变;2)台风"山神"期间,海域波浪谱峰周期在5.06.5 s之间,最大谱峰值为2.70 m2/s,波浪方向为E6.5 s之间,最大谱峰值为2.70 m2/s,波浪方向为EESE向,波浪以风浪为主;3)琼州海峡海域大周期波浪主要受到台风引起的涌浪影响,涌浪周期的范围大约在6.5ESE向,波浪以风浪为主;3)琼州海峡海域大周期波浪主要受到台风引起的涌浪影响,涌浪周期的范围大约在6.510.0 s之间。 相似文献
8.
通过物理模型试验研究中国《海港水文规范》(JTJ213-98)中斜坡式防波堤顶部胸墙波浪力计算公式在深水情况下的适用性.试验测量4种不同水深波浪作用下斜坡堤顶部胸墙的波浪力和作用高度.通过对胸墙迎浪面的波浪压强分布、总水平作用力和波浪作用高度的试验结果与《海港水文规范》结果的对比分析,发现胸墙迎浪面的实测波压分布不同于规范采用的均匀分布;规范计算得到的总水平力和波浪作用高度均小于实测值.本文改进规范中斜坡堤胸墙波浪力计算方法,使其更适用于深水堤顶部胸墙受力计算. 相似文献
9.
波浪力对海上风电深水导管架基础结构的稳定性和安全性至关重要。通过波浪物理模型试验对极端波浪条件下深水导管架基础结构的波浪总力进行了试验研究，试验水深包括50 m和70 m两种，在1 000 a一遇波浪条件下，分别分析了深水导管架结构所受的波浪总水平力和垂直力。研究结果表明：相同重现期极端波浪作用下，70 m水深情况下的导管架结构波浪总水平力小于50 m水深的结果，但是70 m水深的导管架结构波浪总水平力弯矩大于50 m水深的结果；相同水深、水位和波浪条件下，导管架结构受到的波浪总垂直力明显小于波浪总水平力；在相同重现期极端波浪作用下，低水位情况时70 m水深的导管架结构波浪总垂直力与50 m水深的结果差别不大，但是在高水位时，由于在70 m水深的极端波浪条件下波峰可冲击作用到上部平台底面，70 m水深的导管架结构波浪总垂直力明显大于50 m水深的结果。 相似文献
10.
透空式进海路是连接人工岛与陆岸的一种新型结构,其所受波浪力是工程设计中重点关注的问题。本文开展物理模型试验,通过改变水深、波高、桥面底高、桥面宽度等试验条件,研究透空式进海路波浪力的变化规律。试验测量透空式进海路上部结构的动水压强分布,分析得到结构的浮托力和水平波浪力。研究发现:透空式进海路上部结构波浪力的主要影响因素为桥面相对净空高度,在相对净空高度接近0时,桥面浮托力达到最大值。通过分析试验数据,并参照文献中的已有波浪力计算方法,建立透空式进海路上部结构浮托力和水平波浪力的计算公式,公式计算结果与试验结果符合较好,对透空式进海路工程设计具有重要指导意义。 相似文献
11.
The hydrodynamic force on net panels in waves plays a significant role in the wave-resistant design of net cages in the open sea. To investigate the hydrodynamic force on net panels in waves, a series of experiments about different types of net panels in waves were conducted in a wave flume. The effects of the net solidity, the net material and the knot pattern were experimentally analyzed in this study. A wave force model for the net panel was proposed based on the hydrodynamics of cylinder in waves. The experimental results indicated that the horizontal force on the net panel in waves was larger than the vertical force, and the horizontal force was heavily depended on the KC number; In addition, the horizontal force on the steel net was smaller than that on the nylon net, and the knot pattern had a negligible influence on the hydrodynamic force on the net panel in waves. The model was also compared with existing experimental measurements and previous numerical results. The comparison results indicated that the wave force model could calculate the wave force on the net panel accurately. 相似文献
12.
设计了一种新型网箱浮架系统,利用SESAM对其进行了频域水动力分析以及考虑不规则波浪、风、流载荷和系泊共同作用的时域耦合分析,并与传统双浮管网箱浮架系统进行了分析对比,得到方形网箱与圆形网箱的水动力特性的差异以及各自的优缺点,对实际中网箱的开发设计有一定的借鉴意义;通过计算,证明新型网箱浮架系统在工作海况能正常工作,在极端海况下也能满足安全性的要求;最后对4种常见系泊方式进行了时域耦合分析,得到了四种系泊方式的系泊特性,对实际工程中系泊方式的选择有一定的参考意义。 相似文献
13.
Numerical simulation of the influences of sinker weight on the deformation and load of net of gravity sea cage in uniform flow 总被引：11，自引：0，他引：11
1IntroductionThe fish farming and aquaculture industry areexpanding and the demand for suitable locations forfish farms is increasing.In the future,more of thefish farms will be located offshore,as the number ofsuitable nearshore locations is limited.Futu… 相似文献
14.
物体入水时波浪的影响不可忽略,基于流体力学模型采用VOF法,并利用自定义函数,模拟了楔形体的自由入水过程;同时结合推波板原理及海绵层消波理论实现了数值水槽的造消波,完成了波浪中楔形体自由入水的模拟,计算了楔形体入水时所受的水作用力、自由液面变化及物面压强分布等,研究了不同波高、周期以及在波浪不同位置入水时对楔形体的影响。结果表明:本文建立的数值模型可很好地模拟楔形体入水造成的射流及空泡的形成发展过程,波浪对楔形体入水的影响主要由波浪内部流场变化及表面波形决定,在波浪不同位置处入水对楔形体受力及入水形态均有较大影响。 相似文献
15.
A numerical model of flatfish cage is built based on the lumped mass method and the principle of rigid body kinematics. To validate the numerical model, a series of physical model tests are conducted in the wave flume. The numerical results correspond well with the data sets from physical model test. The effect of weight of bottom frame, height of fish net and net shape on motion responses of fish cage and tension force on mooring lines is then analyzed. The results indicate that the vertical displacements of float collar and bottom frame decrease with the increase in the weight of bottom frame; the maximum tension force on mooring lines increases with the increasing weight of bottom frame. The inclination angles of float collar and bottom frame decrease with the increasing net height; the maximum tension force increases obviously with the increase of net height. 相似文献
16.
Numerical Analysis on the Effects of Submerged Depth of the Grid and Direction of Incident Wave on Gravity Cage 总被引：1，自引：0，他引：1
In this paper,the numerical model of the net cage with the grid mooring system in waves is set up by the lumped mass method and rigid kinematics theory,and then the motion equations of floating system,net system,mooring system,and floaters are solved by the Runge-Kutta fifth-order method.For the verification of the numerical model,a series of physical model tests have been carried out.According to the comparisons between the simulated and experimental results,it can be found that the simulated and experimental results agree well in each condition.Then,the effects of submerged depth of grid and direction of incident wave propagation on hydrodynamic behaviors of the net cage are analyzed.According to the simulated results,it can be found that with the increase of submerged depth of grid,the forces acting on mooring lines and bridle lines increase,while the forces on grid lines decrease;the horizontal motion amplitudes of floating collar decrease obviously,while the vertical motion amplitudes of floating collar change little.When the direction of incident wave propagation changes,forces on mooting lines and motion of net cage also change accordingly.When the propagation direction of incident wave changes from 0° to 45°,forces on the main ropes and bridle ropes increase,while the forces on the grid ropes decrease.With the increasing propagation direction of incident wave,the horizontal amplitude of the forces collar decreases,while the vertical amplitude of the floating collar has little variation. 相似文献
17.
Based on rigid kinematics theory and lumped mass method,a mathematical model of the two net cages of grid mooring system under waves is developed.In order to verify the numerical model,a series of physical model tests have been carried out.According to the comparisons between the simulated and the experimental results,it can be found that the simulated and the experimental results agree well in each wave condition.Then,the forces on the mooring lines and the floating collar movement are calculated under different wave conditions.Numerical results show that under the same condition,the forces on the bridle ropes are the largest,followed by forces on the main ropes and the grid ropes.The horizontal and the vertical float collar motion amplitudes increase with the increase of wave height,while the relationship of the horizontal motion amplitude and the wave period is indistinct.The vertical motion amplitude of the two cages is almost the same,while on the respect of horizontal motion amplitude,cage B(behind cage A,as shown in Fig.4) moves much farther than cage A under the same wave condition.The inclination angle of the floating system both in clockwise along y axis and the counter one enlarges a little with the increase of wave height. 相似文献
18.
波浪破碎过程产生的湍流动量和能量垂向输运对于加快海洋上混合层中垂向混合具有显著效果。采用二维实验室水槽中对波浪破碎过程进行模拟。对采集的波浪振幅时间序列采用希尔伯特变换定位破碎波位置,波浪的破碎率随有效波高的增加而增大,波浪谱分析得到的波浪基本周期与有效周期结果相似。实验中采用粒子图像测速技术(particle image velocimetry, PIV)计算波浪破碎过程中湍动能耗散率的空间分布。湍流强度与波浪的相位密切相关,波峰位置处湍流活动最为剧烈,而且波峰位置处湍流混合区内湍动能耗散率量值的垂向分布基本保持不变,即出现"湍流饱和"现象,湍流影响深度可以达到波高的70%—90%。计算湍流扩散系数的垂向分布发现,湍流扩散在混合区上部随深度的增大以指数函数的形式增加,在混合区下部趋于稳定。作为对比,在相同位置处对声学多普勒流速测量仪(acoustic Doppler velocimeter, ADV)测量的单点流速做频谱分析,发现与该位置处PIV湍动能耗散率结果量级处于同一水平,进一步验证了实验结果的准确性。 相似文献
19.
《中国海洋工程》2015,(3)
The effect of biofouling on the hydrodynamic characteristics of the net cage is of particular interest as biofouled nettings can significantly reduce flow of well-oxygenated water reaching the stocked fish. For computational efficiency, the porous-media fluid model is proposed to simulate flow through the biofouled plane net and full-scale net cage. The porous coefficients of the porous-media fluid model can be determined from the quadratic-function relationship between the hydrodynamic forces on a plane net and the flow velocity using the least squares method. In this study, drag forces on and flow fields around five plane nets with different levels of biofouling are calculated by use of the proposed model. The numerical results are compared with the experimental data of Swift et al.(2006) and the effectiveness of the numerical model is presented. On that basis, flow through full-scale net cages with the same level of biofouling as the tested plane nets are modeled. The flow fields inside and around biofouled net cages are analyzed and the drag force acting on a net cage is estimated by a control volume analysis method. According to the numerical results, empirical formulas of reduction in flow velocity and load on a net cage are derived as function of drag coefficient of the corresponding biofouled netting. 相似文献
20.
The effect of biofouling on the hydrodynamic characteristics of the net cage is of particular interest as biofouled nettings can significantly reduce flow of well-oxygenated water reaching the stocked fish. For computational efficiency, the porous-media fluid model is proposed to simulate flow through the biofouled plane net and full-scale net cage. The porous coefficients of the porous-media fluid model can be determined from the quadratic-function relationship between the hydrodynamic forces on a plane net and the flow velocity using the least squares method. In this study, drag forces on and flow fields around five plane nets with different levels of biofouling are calculated by use of the proposed model. The numerical results are compared with the experimental data of Swift et al. (2006) and the effectiveness of the numerical model is presented. On that basis, flow through full-scale net cages with the same level of biofouling as the tested plane nets are modeled. The flow fields inside and around biofouled net cages are analyzed and the drag force acting on a net cage is estimated by a control volume analysis method. According to the numerical results, empirical formulas of reduction in flow velocity and load on a net cage are derived as function of drag coefficient of the corresponding biofouled netting. 相似文献