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延安大学建筑工程学院,陕西 延安 716000
Received:27 February 2025,
Revised:2025-06-03,
Published:28 April 2026
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程麦理,郭少恒,拓鹏鹏等.复杂地形下碎屑流冲击混凝土桥墩的损伤机理研究[J].防灾减灾工程学报,2026,46(02):400-408.
CHENG Maili,GUO Shaoheng,TA Pengpeng,et al.Study on Damage Mechanisms of Concrete Piers Impacted by Debris Flow in Complex Terrain[J].Journal of Disaster Prevention and Mitigation Engineering,2026,46(02):400-408.
程麦理,郭少恒,拓鹏鹏等.复杂地形下碎屑流冲击混凝土桥墩的损伤机理研究[J].防灾减灾工程学报,2026,46(02):400-408. DOI: 10.13409/j.cnki.jdpme.20250227002.
CHENG Maili,GUO Shaoheng,TA Pengpeng,et al.Study on Damage Mechanisms of Concrete Piers Impacted by Debris Flow in Complex Terrain[J].Journal of Disaster Prevention and Mitigation Engineering,2026,46(02):400-408. DOI: 10.13409/j.cnki.jdpme.20250227002.
为探究艰险山区复杂地形下碎屑流对混凝土桥墩的冲击致灾机理,利用离散元软件PFC
3D
开展了凸型、直线型及凹型三种斜坡滑槽仿真模拟试验,分析了碎屑流的运动规律及堆积特征,深入研究了混凝土桥墩在碎屑流动力冲击作用下的损伤演化规律。结果表明:凹型斜坡碎屑流启动阶段速度最大且峰值平均速度最高(6.38 m/s),但运动时间最短,凸型斜坡碎屑流启动阶段速度最小且峰值平均速度最低(2.53 m/s),但运动时间最长;凸型斜坡碎屑流堆积最为分散、致灾范围最广、桥墩前堆积高度最高,凹型斜坡碎屑流堆积规律则相反;凸型斜坡碎屑流对桥墩的峰值冲击力在
X
向、
Z
向均最大,墩顶位移响应最显著(5.0 mm),凹型斜坡碎屑流对桥墩冲击力峰值在三向均最小,且墩顶位移最小仅1.07 mm;凸型斜坡场地下桥墩损伤最严重,损伤高度范围最大(距墩底0.27~1.32 m),直线型斜坡次之,凹型斜坡下桥墩损伤高度范围最小(0.06~0.31 m);桥墩损伤率与主冲击方向(
X
向)峰值冲击力排序相同,即凸型斜坡
>
直线型斜坡
>
凹型斜坡。研究结果可为艰险山区桥梁碎屑流冲击灾害防治提供参考。
To investigate the disaster-causing mechanisms of debris flow impact on concrete piers in complex terrain within hazardous mountainous areas
simulation tests were conducted using discrete element software PFC3D on three types of slope flumes: convex
linear
and concave. The movement patterns and accumulation characteristics of the debris flow were analyzed
and the damage evolution patterns of concrete piers under dynamic impact of debris flow were deeply studied. The results indicated that the debris flow on the concave slope exhibited the largest start-up velocity and the highest peak average velocity (6.38 m/s)
but the shortest movement duration. In contrast
the debris flow on the convex slope showed the smallest start-up velocity and the lowest peak average velocity (2.53 m/s)
but the longest movement duration. The debris flow accumulation on the convex slope was the most dispersed
covered the widest disaster area
and resulted in the greatest accumulation height in front of the pier
while the accumulation patterns on the concave slope exhibited the opposite trend. The peak impact force of the debris flow on the pier under the convex slope condition was the largest in both the X and Z directions
and the displacement response at the pier top was the most significant (5.0 mm). Under the concave slope condition
the peak impact force of the debris flow on the pier was the smallest in all three directions
and the pier-top displacement was minimal at only 1.07 mm. The pier damage was the most severe under the convex slope terrain
with the largest damage height range (0.27 m to 1.32m from the bottom of the pier)
followed by the linear slope
while the concave slope exhibited the smallest damage height range (0.06 m to 0.31 m). The pier damage rate followed the same ranking as the peak impact force in the main impact direction (X-direction): convex slope > linear slope > concave slope. The research findings can provide a reference for the prevention and mitigation of debris flow impact disasters on bridges in hazardous mountainous areas.
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