首页|基于全阶法的柔性光伏支架颤振性能分析

基于全阶法的柔性光伏支架颤振性能分析

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以某三索柔性光伏支架作为研究对象,建立有限元模型.采用全阶颤振分析方法,计算了0°倾角柔性光伏支架的颤振临界风速和颤振频率,计算结果与风洞试验数据吻合良好.进一步分析研究了承重索和稳定索预拉力对柔性光伏支架自振频率和颤振临界风速的影响.研究结果表明:增加承重索预拉力可显著提高结构前4阶自振频率;当承重索预拉力从22 kN增加到102 kN时,颤振临界风速从17.1 m/s增加至21.6 m/s;与承重索相比,稳定索预拉力对柔性光伏支架的自振频率和颤振临界风速影响较小;当稳定索预拉力从22 kN增加到102 kN时,颤振临界风速从17.1 m/s增加至17.7 m/s.对于柔性光伏支架的抗风设计,建议优先增加承重索预拉力以提高结构颤振性能.
Analysis on flutter performance of flexible photovoltaic support based on full-order method
Taking a three-cable flexible photovoltaic(PV)support structure as the research subject,a finite element model was established.Utilizing a full-order flutter analysis method,the flutter critical wind speed and flutter frequency of the flexible PV support structure at a tilt angle of 0° were calculated.The results showed good agreement with wind tunnel test data.Further analysis examined the pretension effects in the load-bearing and stabilizing cables on the natural frequency and flutter critical wind speed of the flexible PV support structure.The research findings indicate increasing the pretension in the load-bearing cables significantly raises the natural frequencies of the first four modes.Specifically,as the pretension in the load-bearing cables increases from 22 to 102 kN,the flutter critical wind speed rises from 17.1 to 21.6 m/s.By contrast,the pretension in the stabilizing cable has a smaller effect on the natural frequency and flutter critical wind speed of the flexible PV support structure.When the pretension in the stabilizing cable increased from 22 to 102 kN,the flutter critical wind speed increased from 17.1 to 17.7 m/s.For wind-resistant design of flexible PV support structures,it is recommended to prioritize increasing the pretension in the load-bearing cables to enhance the structural flutter performance.

flexible photovoltaic supportflutter critical wind speedfull-order methodfinite element model

周锐、王浩、徐梓栋

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东南大学混凝土及预应力混凝土结构教育部重点实验室,南京 211189

柔性光伏支架 颤振临界风速 全阶法 有限元模型

2024

东南大学学报(英文版)
东南大学

东南大学学报(英文版)

影响因子:0.211
ISSN:1003-7985
年,卷(期):2024.40(3)