应宏伟, 郑贝贝. 砂土中刚性挡墙不同主动变位模式任意位移土压力计算[J]. 工程力学, 2012, 29(11): 243-249. DOI: 10.6052/j.issn.1000-4750.2011.04.0214
引用本文: 应宏伟, 郑贝贝. 砂土中刚性挡墙不同主动变位模式任意位移土压力计算[J]. 工程力学, 2012, 29(11): 243-249. DOI: 10.6052/j.issn.1000-4750.2011.04.0214
YING Hong-wei, ZHENG Bei-bei. EARTH PRESSURES ON RIGID RETAINING WALLS IN SANDY SOIL WITH DIFFERENT ACTIVE MOVEMENT MODES UNDER ARBITRARRY DEFORMATION[J]. Engineering Mechanics, 2012, 29(11): 243-249. DOI: 10.6052/j.issn.1000-4750.2011.04.0214
Citation: YING Hong-wei, ZHENG Bei-bei. EARTH PRESSURES ON RIGID RETAINING WALLS IN SANDY SOIL WITH DIFFERENT ACTIVE MOVEMENT MODES UNDER ARBITRARRY DEFORMATION[J]. Engineering Mechanics, 2012, 29(11): 243-249. DOI: 10.6052/j.issn.1000-4750.2011.04.0214

砂土中刚性挡墙不同主动变位模式任意位移土压力计算

EARTH PRESSURES ON RIGID RETAINING WALLS IN SANDY SOIL WITH DIFFERENT ACTIVE MOVEMENT MODES UNDER ARBITRARRY DEFORMATION

  • 摘要: 已有模型实验及现场实测表明,刚性挡墙随着变位模式和位移量的变化,主动土压力合力和分布均发生改变,有时甚至与经典理论的线性分布有很大不同。采用中间状态系数定义非极限状态,提出了砂土中刚性挡墙不同主动位移模式下非极限状态土压力合力系数的计算公式;将墙后土体简化为连续非线性弹簧和刚塑性体的组合体作用在挡墙上,得到了不同位移模式任意位移的土压力分布和合力作用点高度。与已有理论方法和实验结果对比表明,该文方法在三种典型位移模式下与实验数据吻合更好。研究还发现,平动模式土压力呈线性分布,其合力随挡墙位移量的增大易趋于稳定并到达极限状态;绕墙底和绕墙顶转动模式下土压力合力随着位移增大只能接近极限状态且呈非线性分布。绕底转动时,土压力分布曲线逐渐向上凹,合力作用点高度趋于降低;绕顶转动时,分布曲线则逐渐向上凸,合力作用点高度趋于升高,墙顶附近表现出明显的土拱效应。

     

    Abstract: Previous experimental and monitored results on earth pressures had shown that the resultant and distribution of active earth pressures on rigid retaining walls varied with modes and magnitudes of wall movement. The distribution of earth pressures sometimes differed obviously from a linear distribution according to classical earth pressure theories. A middle-state coefficient was adopted to define the non-limit state, and the formulae of the coefficients of the resultant earth pressures on rigid retaining walls in sandy backfills at a non-limit state with different deformations were proposed. The soil behind the wall was simplified as the combination of nonlinear springs and a rigid plasticity object which applied on the wall, and the unit active pressure and the heights of points of application of pressures were obtained. The comparisons among the proposed formulae, previous methods and the experimental observations showed that the proposed equations could predict the earth pressures with the three typical modes of wall movement more satisfactorily. It was also shown that the resultant earth pressures decreased gradually with the increase of translation of the wall and trended toward a certain value quickly and the distribution of the pressures kept linear all the while. However, the resultants of pressures could only be close to but not reached an active limit state and the distributions were nonlinear with a rotation mode. The distribution curves of the earth pressures were concave upward and the heights of the points of application decreased when a wall rotated about the base, while the curves were convex upward and the heights increased when the wall rotated about the top due to the soil arching.

     

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