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Wave propagation in a concrete filled steel tubular column due to transient impact load

机译:瞬态冲击载荷在钢管混凝土柱中的波传播

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This study aims to present a three dimensional finite element model to investigate the wave propagation in a concrete filled steel tubular column (CFSC) due to transient impact load. Both the concrete and steel are regarded as linear elastic material. The impact load is simulated by a semi sinusoidal impulse. Besides the CFSC models, a concrete column (CC) model is established for comparing under the same loading condition. The propagation characteristics of the transient waves in CFSC are analyzed in detail. The results show that at the intial stage of the wave propagation, the velocity waves in CFSC are almost the same as those in CC before they arrive at the steel tube. When the waves reach the column side, the velocity responses of CFSC are different from those of CC and the difference is more and more obvious as the waves travel down along the column shaft. The travel distance of the wave front in CFSC is farther than that in CC at the same time. For different wave speeds in steel and concrete material, the wave front in CFSC presents an arch shape, the apex of which locates at the center of the column. Differently, the wave front in CC presents a plane surface. Three dimensional effects on top of CFSC are obvious, therefore, the peak value and arrival time of incident wave crests have great difference at different locations in the radial direction. High-frequency waves on the waveforms are observed. The time difference between incident and reflected wave peaks decreases significantly with r/R when r/R < 0.6, however, it almost keeps constant when r/R >= 0.6. The time duration between incident and reflected waves calculated by 3D FEM is approximately equal to that calculated by 1D wave theory when r/R is about 2/3.
机译:这项研究的目的是提出一个三维有限元模型,以研究由于瞬态冲击载荷引起的钢管混凝土柱(CFSC)中的波传播。混凝土和钢都被视为线性弹性材料。冲击载荷由半正弦脉冲模拟。除了CFSC模型外,还建立了混凝土柱(CC)模型以在相同载荷条件下进行比较。详细分析了CFSC中瞬态波的传播特性。结果表明,在波传播的初始阶段,CFSC中的速度波在到达钢管之前与CC中的速度波几乎相同。当波到达柱侧时,CFSC的速度响应不同于CC的速度响应,并且随着波沿着柱轴向下传播,这种差异越来越明显。同时,CFSC中波前的行进距离比CC中的波前行进距离远。对于钢和混凝土材料中不同的波速,CFSC中的波前呈弓形,其顶点位于圆柱的中心。不同的是,CC中的波前呈现出一个平面。 CFSC顶部的三维效应是明显的,因此,入射波峰的峰值和到达时间在径向的不同位置有很大差异。观察到波形上的高频波。当r / R <0.6时,入射波峰和反射波峰之间的时间差随r / R显着减小,但是,当r / R> = 0.6时,它几乎保持恒定。当r / R约为2/3时,通过3D FEM计算的入射波和反射波之间的持续时间大约等于通过1D波理论计算的时间。

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