散粒体滑坡涌浪运动特征与能量转化规律研究

王佳佳, 陈浩, 肖莉丽, 李枝强, 许昕, 向宇恒, 车思璐. 散粒体滑坡涌浪运动特征与能量转化规律研究[J]. 水文地质工程地质, 2023, 50(4): 160-172. doi: 10.16030/j.cnki.issn.1000-3665.202207022
引用本文: 王佳佳, 陈浩, 肖莉丽, 李枝强, 许昕, 向宇恒, 车思璐. 散粒体滑坡涌浪运动特征与能量转化规律研究[J]. 水文地质工程地质, 2023, 50(4): 160-172. doi: 10.16030/j.cnki.issn.1000-3665.202207022
WANG Jiajia, CHEN Hao, XIAO Lili, LI Zhiqiang, XU Xin, XIANG Yuheng, CHE Silu. A study of the kinematic characteristics and energy conversion of waves generated by granular landslide[J]. Hydrogeology & Engineering Geology, 2023, 50(4): 160-172. doi: 10.16030/j.cnki.issn.1000-3665.202207022
Citation: WANG Jiajia, CHEN Hao, XIAO Lili, LI Zhiqiang, XU Xin, XIANG Yuheng, CHE Silu. A study of the kinematic characteristics and energy conversion of waves generated by granular landslide[J]. Hydrogeology & Engineering Geology, 2023, 50(4): 160-172. doi: 10.16030/j.cnki.issn.1000-3665.202207022

散粒体滑坡涌浪运动特征与能量转化规律研究

  • 基金项目: 国家自然科学基金项目(41907237;41907234);国家重点研发计划项目(2019YFB1600702;2021YFB1600302);云南省交通厅科技项目(云交科2018-12)
详细信息
    作者简介: 王佳佳(1988-),男,博士,副教授,主要从事地质灾害动力学研究。E-mail: jwang@chd.edu.cn
    通讯作者: 肖莉丽(1985-),女,博士,副教授,主要从事滑坡涌浪灾害动力学研究。E-mail: llxiao@chd.edu.cn
  • 中图分类号: P642.22

A study of the kinematic characteristics and energy conversion of waves generated by granular landslide

More Information
  • 滑坡涌浪灾害造成的伤亡和损失一般远超滑坡灾害本身,已引起广泛关注。针对该类灾害的预测评价一直是研究的难点,精细刻画滑坡涌浪运动特征和能量转化规律是解决问题的关键和前提。因此,以天然碎石模拟散粒体滑坡,建立缩尺的矩形水槽滑坡涌浪三维物理试验模型,研究滑坡体积、速度和水深对堆积体形态和涌浪特征的影响以及滑体与水体能量转化规律。研究结论包括:(1)滑体通过冲击、挤压和抬升水体形成涌浪的特征受滑体规模和形态影响显著;厚度大且速度快的滑体趋向产生非线性过渡波,厚度小且速度低的滑体一般产生非线性震荡波;(2)基于试验提出的体积效应和速度效应揭示了一定水深的涌浪规模与滑坡体积和速度呈正相关规律,水深效应则解释了一定波能的涌浪在波形和速度上的分布差异,结果表明浅水比深水工况涌浪高度平均高出67%、波速平均高出51.17%;(3)基于试验的数值反演总结了滑体势能与波能转化率为1.00%~3.07%,由于三维试验中滑体与水体在水平和环向的扩散造成更多能量耗散,相较二维试验转化率较低。通过探讨散粒体滑坡运动过程和首浪产生、传播及爬高特征,揭示滑体-水体能量转化基本规律,研究成果对滑坡涌浪防灾减灾工作具有一定的理论价值和意义。

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  • 图 1  滑坡涌浪试验模型尺寸示意图(单位:cm)

    Figure 1. 

    图 2  滑坡涌浪物理试验模型实景图

    Figure 2. 

    图 3  水/土相互作用正面、侧面图

    Figure 3. 

    图 4  散粒体堆积展布形态及WG1波高变化

    Figure 4. 

    图 5  散粒体滑坡涌浪两种典型波形及K2V2W1工况WG1—WG6位置波形曲线

    Figure 5. 

    图 6  不同下滑速度(V1、V2、V3)下首浪高度传播衰减曲线

    Figure 6. 

    图 7  不同下滑速度(V1、V2、V3)下沿纵剖面Z波速变化曲线

    Figure 7. 

    图 8  不同滑坡体积(K1、K2、K3)下首浪高度传播衰减曲线

    Figure 8. 

    图 9  不同滑体体积(K1、K2、K3)沿纵剖面Z波速变化曲线

    Figure 9. 

    图 10  试验工况波形简图

    Figure 10. 

    图 11  K2V2W1试验工况能量转化图

    Figure 11. 

    表 1  W1水位工况下的能量转化率

    Table 1.  Energy conversion rate at W1 water level

    工况 最大总波能/J 滑体势能/J 能量转化率/%
    K1V1W1 7.32 238.64 3.07
    K1V2W1 10.76 364.88 2.95
    K1V3W1 10.83 455.81 2.38
    K2V1W1 13.04 510.06 2.56
    K2V2W1 14.31 759.51 1.88
    K2V3W1 9.37 940.57 1.00
    K3V1W1 23.97 1179.35 2.03
    K3V2W1 23.25 1608.39 1.45
    K3V3W1 60.82 2083.75 2.92
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出版历程
收稿日期:  2022-07-22
修回日期:  2022-10-28
录用日期:  2022-12-08
刊出日期:  2023-07-15

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