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1)  Main stress arching circle
主应力拱形圈
2)  principal stress arching
主应力拱
1.
Based on Coulomb’s earth pressure theory,assuming the trace of the principal stress arching in the back of rigid retaining wall as parabola,the theory formulae are obtained including the lateral coefficients of active and passive earth pressures and the friction coefficients of horizontal differential elements;then improved formulae of active and passive earth pressures are presented.
基于库仑土压力理论,假定刚性挡墙后主应力拱迹线为抛物线,推导了主、被侧土压力系数和水平微分单元间摩擦系数的理论公式,得到改进的主、被动土压力计算公式。
3)  major principal stress arch
大主应力拱
1.
The major principal stress arch is studied in the backfill in passive critical state.
研究土体被动极限状态时的大主应力拱,给出大主应力拱的曲线方程和被动土压力系数;利用水平层分析法,分析被动土压力的分布规律。
2.
The direct earth pressure should be calculated by analysis of minor principal stress arch while the indirect earth pressure by analysis of major principal stress arch.
可用小主应力拱应力分析计算直接土压力 ,用大主应力拱应力分析计算间接土压力。
4)  minor principal stress arch
小主应力拱
1.
The direct earth pressure should be calculated by analysis of minor principal stress arch while the indirect earth pressure by analysis of major principal stress arch.
可用小主应力拱应力分析计算直接土压力 ,用大主应力拱应力分析计算间接土压力。
5)  main arch ring
主拱圈
1.
Construction technology with support of the long span main arch ring of the reinforced concrete arch bridge;
大跨钢筋混凝土拱桥主拱圈有支架施工技术
2.
Demolishing scheme of main arch ring in deck-type reinforced concrete trussed arch bridge;
上承式钢筋混凝土桁架拱桥主拱圈拆除方案
3.
For the old road widening and rebuilding discussion is made on the design and the construction technology of stone arch bridge especially in its foundation, main arch ring, roadway pavement, sidewall and fills.
针对旧路加宽改造路段,本着考虑新旧路段结构受力体系一致、变形协调及外观统一的原则,从基础、主拱圈、桥面铺装、侧墙及填料等几个方面论述了石拱桥的加宽设计与施工的要点。
6)  main arch circle
主拱圈
1.
Some diseases were presented in the main arch circle and the architecture above the arch of Wanche ArchBridge.
万车双曲拱桥主拱圈和拱上建筑出现病害破坏,采取对主拱圈增加拱肋和按梁板体系重新实施拱上建筑的方式进行加固维修,效果较好。
补充资料:主应力


主应力
principal stress

  zhuyingli主应力(prineipal stress)没有切应力作用的截面上的法向应力。经数学证明,金属塑性加工时于变形物体内某一点的应力状态可用下式所表示的二次曲面来确定: A“一‘X“十乞丁2+氏Z“+2场叉丫 +2殊yZ十2屯Z尤(1)式中A为任意常数,几、丐、么和rx.、,、几分别为作用在通过该点所引三个相互垂直坐标面上的正应力和切应力,X、Y、Z为此二次曲面上某点的坐标。当所取坐标轴的位置发生变化时,即用新的坐标来表示该曲面时,式中各项的系数将发生变化。这样,通过上述确定应力状态的点总可以引出这样三个相互垂直的平面(与坐标面平行),在其上仅有正应力而无切应力。主应力符号的脚标分别用l、2、3表示,以分别代替正应力的脚标x、y、z。这样,所得到的三个主应力应为。1、。2、a:,分别作用在三个坐标面上。
  
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