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不规则波作用下岸基式振荡水柱波能装置的水动力性能研究

傅磊 宁德志 王荣泉 RobertMayon

傅磊,宁德志,王荣泉,等. 不规则波作用下岸基式振荡水柱波能装置的水动力性能研究[J]. 海洋学报,2024,46(1):101–110 doi: 10.12284/hyxb2024005
引用本文: 傅磊,宁德志,王荣泉,等. 不规则波作用下岸基式振荡水柱波能装置的水动力性能研究[J]. 海洋学报,2024,46(1):101–110 doi: 10.12284/hyxb2024005
Fu Lei,Ning Dezhi,Wang Rongquan, et al. Hydrodynamic performance study of a land-based OWC under the action of irregular wave[J]. Haiyang Xuebao,2024, 46(1):101–110 doi: 10.12284/hyxb2024005
Citation: Fu Lei,Ning Dezhi,Wang Rongquan, et al. Hydrodynamic performance study of a land-based OWC under the action of irregular wave[J]. Haiyang Xuebao,2024, 46(1):101–110 doi: 10.12284/hyxb2024005

不规则波作用下岸基式振荡水柱波能装置的水动力性能研究

doi: 10.12284/hyxb2024005
基金项目: 国家自然科学基金项目(52271260, 52001054);辽宁省兴辽英才计划项目(XLYC2002033);中央高校基本科研业务费资助项目(DUT23RC(3)017)。
详细信息
    作者简介:

    傅磊(1999—),男,江苏省镇江市人,从事波浪能高效利用研究。E-mail:fulei@mail.dlut.edu.cn

    通讯作者:

    王荣泉(1989—),男,湖南省邵阳市人,主要从事波浪能开发与利用研究。E-mail: rqwang@dlut.edu.cn

  • 中图分类号: P731.22

Hydrodynamic performance study of a land-based OWC under the action of irregular wave

  • 摘要: 为了研究真实海域中振荡水柱(OWC)波能转换装置的水动力性能,本文基于势流理论和高阶边界元方法,建立了不规则波与岸基式OWC波能装置相互作用的二维非线性数值模型,不规则波基于JONSWAP谱生成。为了考虑由于水体黏性引起的能量耗散,在气室内水面边界条件中引入人工黏性阻尼。并在大连理工大学波流水槽中开展了物理模型试验,对数值模型的有效性进行了验证。研究发现,在不规则波作用下,OWC波能装置的水动力效率相较于规则波作用下有所降低,特别是在低频波区域效率差值最大。与规则波相比,不规则波浪作用下装置峰值效率对应的频率变大。气室内的相对水面高程随着有效波高的增加而降低,而气室内相对气压则随有效波高的增加而增大。OWC波能装置的水动力效率受有效波高的影响较小,其峰值效率对应的频率不受波浪非线性的影响。本文可以为OWC波能装置的设计提供参考。
  • 图  1  数值水槽示意图

    Fig.  1  Sketch of the numerical flume

    图  2  水槽试验模型布置

    Fig.  2  The OWC device and the sketch of experimental set-up

    图  3  自由液面(a)和气体压强(b)的试验数据重复性对比

    Fig.  3  Comparison of experimental repeatability of free surface (a) and air pressure (b)

    图  4  数值水槽网格划分示意图

    Fig.  4  Sketch of the meshes of the numerical wave flume

    图  5  预测的转换效率和试验结果对比

    Fig.  5  Comparison of predicted hydrodynamic efficiency and experimental results

    图  6  数值预测与试验中波能谱(a)和压强谱(b)对比

    Fig.  6  Comparison of the wave energy spectrums (a) and the air pressure spectrums (b) between numerical with experiments

    图  7  不同峰值周期下气室内液面高程(a)和气体压强(b)的时域曲线

    Fig.  7  Time-domain series of the surface elevation (a) and air pressure (b) for different peak periods

    图  8  气室内液面高程(a)和气体压强(b)随kph的特征统计值变化

    Fig.  8  Variations of the surface elevation (a) and air pressure (b) with kph for characteristic statistics

    图  9  规则波和不规则波场景下OWC装置效率的比较

    Fig.  9  Comparison of hydrodynamic efficiency of the OWC under regular and irregular wave scenarios

    图  10  入射波、气室外侧和气室中点波面的波能谱

    Fig.  10  The wave energy spectrums of incident wave, surface elevation at outside and mid-point of the chamber

    图  11  不同有效波高下自由表面高程(a)和气体压强(b)随kph的变化

    Fig.  11  Variations of the free-surface elevations (a) and air pressures (b) with kph for different significant wave heights

    图  12  Tp = 1.9 s时气室内液面的谱分析

    Fig.  12  Spectral analysis of surface inside the chamber at Tp = 1.9 s

    图  13  不同有效波高下OWC效率随kph的变化

    Fig.  13  Variations of the OWC efficiency with kph for different significant wave heights

    表  1  物理装置的具体设计参数

    Tab.  1  The specific design dimensions of the physical devices

    结构参数尺寸/m
    前墙吃水d0.125
    气室宽度b0.7
    前墙厚度w0.05
    圆孔直径 D0.067
    气室高度ha0.2
    下载: 导出CSV

    表  2  规则波与不规则波的波浪条件

    Tab.  2  Wave conditions of regular and irregular waves

    规则波 与规则波同波浪
    参数的不规则波1
    与规则波同单宽波
    功率的不规则波2
    T/s H/m Tp/s Hs/m Tp/s Hs/m
    1.4 0.06 1.4 0.06 1.4 0.087 2
    1.5 0.06 1.5 0.06 1.5 0.087 5
    1.6 0.06 1.6 0.06 1.6 0.087 7
    1.7 0.06 1.7 0.06 1.7 0.087 9
    1.8 0.06 1.8 0.06 1.8 0.088 0
    1.9 0.06 1.9 0.06 1.9 0.088 0
    2.0 0.06 2.0 0.06 2.0 0.087 9
    2.1 0.06 2.1 0.06 2.1 0.087 8
    下载: 导出CSV
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出版历程
  • 收稿日期:  2023-10-18
  • 修回日期:  2023-12-21
  • 网络出版日期:  2024-04-15
  • 刊出日期:  2024-01-01

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