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471.
大直径超长桩压浆后承载性能的试验研究及有限元分析 总被引:11,自引:1,他引:10
结合大直径超长桩试桩得到的试验资料,应用有限元方法分析了压浆对大直径超长钻孔灌注桩承载性能的影响。根据反分析计算结果可知,桩周摩阻力、桩端加固体变形模量及桩周土的变形模量均有不同程度的提高,桩周土在整个桩长范围内变形模量提高幅度为33 %~67 %,平均侧阻力提高幅度为30 %~40 %,与实测结果相基本一致。 相似文献
472.
确定大直径扩底桩承载力的最直接的方法是静力载荷试验。但由于加载的困难和试验费用高等原因,静力载荷试验往往不可行。目前进行大直径扩底桩设计时通常借用建筑桩基技术规范的经验参数法,对大直径灌注桩端阻力值和侧阻力值折减确定,容易造成大直径扩底灌注桩的承载能力得不到充分发挥。结合大直径扩底桩的规范编写,对收集的完整试桩资料进行统计分析,并参考《建筑桩基技术规范》及北京、天津、浙江、福建、广东等地方给出的经验值,最终按不同扩底直径给出了端阻承载力特征值和侧阻承载力特征值的经验值表,并与各试桩的承载力实测值以及按桩基规范确定的承载力特征值进行比较,结果表明,本文建议的大直径扩底桩端阻力特征值和侧阻力特征值具有一定的可靠性和较大的适用性。 相似文献
473.
为了揭示植物地上部分枝条防风抗蚀生物力学响应机制、筛选合适的防风树种,以内蒙古准格尔露天煤矿排土场6种常见植物枝条为对象,进行室内瞬时极限拉伸试验,研究枝条极限抗拉强度以及不同加载速度、枝径和枝条水分变化对极限抗拉强度的影响及其变化规律。结果表明:测试植物枝径0~3 mm范围枝条平均极限抗拉强度随加载速度的增加而增加、随直径增加呈降低趋势,极限抗拉强度大小顺序为柠条(50.13 MPa)>沙棘(37.27 MPa)>紫花苜蓿(30.25 MPa)>沙打旺(22.74 MPa)>草木樨(22.22 MPa);枝条水分变化对其极限抗拉强度的影响表现为枝条越细,对水分变化的敏感程度也越高,继而对极限抗拉强度的影响越大,即直径相同情况下水分损失率越大则平均极限抗拉强度越大。几种植物枝条在不同加载速度、不同直径、不同枝条水分变化影响下的抗拉生物力学特性既存在相同规律,又有差别,其内在原因还需要进一步的研究。 相似文献
474.
富水性斜坡易产生滑坡进而形成泥石流,斜坡排水是防止地质灾害的重要手段。虹吸排水具有实时性和免动力等优势,但因斜坡排水涉及高扬程,在虹吸管内的低压环境中流动液体会发生强烈的空化现象,从而产生气液两相流。在间歇性虹吸排水过程中,如果不及时将析离的气泡带走,气泡会积聚在虹吸管顶点附近,最终破坏虹吸过程。通过对管内两相流型分析,发现只有形成完整的弹状流,才能将气泡带走,保证虹吸的长期有效。采用流体数值计算软件FLUENT的VOF模型,分别对管径为4、5、6、8 mm的虹吸管内气液两相流型进行模拟。结果表明:管径小于5 mm的条件下,表面张力起主要作用,形成完整弹状流;管径大于6 mm的条件下,形成附壁弹状流。该结论通过物理模型试验也得到证明。 相似文献
475.
传统单管法旋喷桩径一般在300~800mm,桩材强度、桩径、水泥用量等参数变化很不稳定。而采用异型喷头工艺技术,单管法旋喷的桩径可有效增大,其成桩工效及质量明显提高,也降低了施工成本。 相似文献
476.
介绍了煤矿坑道大直径水平长钻孔的工业性试验情况。试验中使用定向钻进技术施工了4个钻孔,两个钻孔长度达到80 0m以上,试验钻孔最深86 5m,其中85 5m保持在煤层中连续延伸,孔径15 3mm,最高时效达到2 8m/h。文中还对试验中遇到的问题提出了自己的见解。 相似文献
477.
The measurement of instantaneous sediment concentration remains a challenging task. In this study, a three-step procedure is proposed to estimate instantaneous sediment concentration using acoustic backscatter from Acoustic Doppler Velocimeter (ADV). The influences of acoustic noise and particle diameter on an ADV's performance was first tested in the laboratory, then the three-step procedure was verified based on field measurements in the Zhongxian and Fengjie reaches in the Three Gorges Reservoir. The first step involves reconstructing the backscatter signal time series. Due to contamination from both the noise floor and spurious spikes, the denoising-despiking method was applied instead of the traditional velocity-despiking methods, and this approach performed well based on spectrum ana-lysis. The second step involves calibrating the sediment concentration against the backscatter signal. A linear relation, whose slope and intercept were calibrated to be dependent on particle diameter, is proposed in double logarithmic coordinates. The third step involves calculating the instantaneous sediment concentration using reconstructed instantaneous backscatter based on the proposed relation. The accuracy of the proposed method was evaluated through consideration of the concentration spec-trum and sediment flux, indicating that the proposed three-step procedure is effective for the mea-surement of instantaneous sediment concentration. 相似文献
478.
In aeolian saltation, the sand bed is a mixture of sand particle with a wide range of particle sizes. Generally, the particle size distribution (PSD) of saltating particles is ignored by previous aeolian transport models, which will result in differences between predictions and observations. To better understand the saltation process, a prediction method of the PSD of saltating particles was proposed in this article. The probability of contact between incident sand and bed sand was introduced into the particle-bed collision process. An artificial PSD of the incident saltating particles was set as the initial condition. A stochastic particle-bed collision model considering contact probability was then used in each iteration step to calculate a new PSD of saltating particles. Finally, the PSD of saltating particles can be determined when aeolian saltation reaches a steady state (saltation is in a steady state when its primary characteristics, such as horizontal mass flux and the concentration of saltating particles, remain approximately constant over time and distance). Meanwhile, according to the experimental results, a calculation formula for the contact parameter n is given, which characterizes the shielding effect of particles on each other. That is, if soil PSD and friction velocity were given, the PSD of saltating particles can be determined. Our results do not depend on the initial conditions, and the predicted results are consistent with the experimental results. It indicated that our method can be used to determine the PSD of saltating particles. © 2020 John Wiley & Sons, Ltd. 相似文献
479.
AbstractThis study established a Couple Eulerian–Lagrange model to simulate monopile vibratory penetration for the investigation of soil plugging effect during high-frequency penetration of monopiles for wind turbine. Simulation analysis is focused particularly on soil plugging effect of a large diameter monopile during vibratory penetration into sand, clay, or layered soil. The results of the numerical simulation show that soil plugging effect is unlikely to occur during monopile penetration into the clay soil, while partial soil plugging may occur during the sand penetration. Penetration resistance at the pile toe is transferred to the radial stress around the pile wall. At a critical point penetration process, internal shaft friction becomes larger than external shaft friction. Moreover, radial pressure factors increase during partial soil plugging effect. For layered soil, the topsoil not only has great influence on the soil plugging effect, but also affects shaft friction in the subsoil during monopile penetration. 相似文献
480.