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61.
62.
为厘清季冻土区临水内、外拱护墙结构冻胀平位移冻害机理,测试隔离层防冻害装置的有效性,在20101110-20110531、20131110-20140531、20171110-20180531三个观测年内,以长春某湖泊临水内、外拱护墙结构为研究对象,选择内、外拱护墙结构和设隔离层防冻害装置的试验内拱护墙结构三者相对比,用钢尺量距法观测三者寒期的平位移状态。结果表明:内拱护墙结构出现倾斜、裂缝导致的内向冻胀平位移冻害,其内向平位移曲线随气温均呈"半驼峰型",对应观测年持续降温-持续低温-持续升温-正温时段,内向冻胀平位移呈减小-增大-减小-稳定残余的位移运动,诱因是平冻胀应力的生成-增长-减弱-消失作用;外拱护墙结构出现较小的外向冻胀平位移,外向冻胀平位移曲线均呈"波浪型",无冻害发生,冰凸拱平冻胀应力推动外拱护墙结构压缩冻土凹拱形成外向冻胀平位移,冻土凹拱限制了外向冻胀平位移发展;设隔离层防冻害装置的试验内拱护墙结构未发生平位移冻害,其内向冻胀平位移较自然冻胀的内拱护墙结构减小83.92%,较外拱护墙结构减小51.74%,表明隔离层防冻害装置防治冻胀平位移冻害有效。 相似文献
63.
郑永飞 《中国地球化学学报》1994,13(4):305-316
The effect of Co2 and CH4 degassing from the mantle on the carbon isotopic composition of diamond has been quantitatively modeled in terms of the principles of Rayleigh distillation.Assuming the δ^13 C value of -5‰ for the mantle,the outgassing of CO2 can result in the large negative δ^13 C values of diamond,whereas the outgassing of CH4 can drive the δ^13C values of diamond in the positive direction.The theoretical expectations can be used to explain the full range of δ^13 C values from-34.4‰5 to 5‰ observed for natural diamonds.It is possible that diamond formation was triggered by the degassing of Co2 and/or CH4 from the mantle and the associated fractional crystallization of carbonate-bearing melt. 相似文献
64.
讨论了DPP100-3型钻机在改型设计中动力匹配,改换汽车底盘的轴荷分配,改装部分的传动装置布置等,主要以选用CA141S型汽车底盘的改型设计为例进行说明。 相似文献
65.
DX桩是在钻、冲孔灌注桩基础上发展起来的一种变截面的新桩型。由于其桩身多个扩径体(承力盘或承力岔)能承受较大的荷载,充分发挥扩径体周边土体的承载力,从而大幅度提高单桩承载力。介绍了DX多节挤扩灌注桩及在浙江软土地区某高层建筑桩基工程中的应用效果。 相似文献
66.
针对目前相关的三轴渗流试验装置缺乏高压水及负压加载功能而不能对高压水及负压加载状态下煤样瓦斯渗流规律进行研究这一问题,研制出了煤样试件出口负压可调并可对其进行高压水加载的新型三轴应力渗流试验装置。该装置主要由三轴应力加载系统、气体渗透系统、水力压裂控制系统、气体流量测试系统、传感与控制系统5部分组成,能够进行高压水及负压载荷下的各种单轴与三轴渗流试验。研究表明,该装置能够模拟抽采钻孔负压状态下煤体内的瓦斯运移规律及考察高压水对煤体的压裂效果,在实验室能完成对煤体试样负压状态下的渗流规律研究以及试件采取水力压裂措施后的增透效果考察。 相似文献
67.
介绍软土层用新型孔底工具-滚压器施工桩基的工作原理、施工工艺,滚压器基本结构及不同直径滚压器的技术特征。 相似文献
68.
数字化地震观测及技术系统建设若干问题 总被引:1,自引:0,他引:1
首先论述了数字地震台网的基本特点和优点,然后着重论述数字地震台网技术系统建设中的若干问题,包括台址的选择,拾振器,采集器,传输信道和无线数字传输设备的选择和安装,以及系统安装中的总体技术要求等。 相似文献
69.
Indira Molina Hiroyuki Kumagai Alexander García-Aristizábal Masaru Nakano Patricia Mothes 《Journal of Volcanology and Geothermal Research》2008
Renewed seismic activity of Cotopaxi, Ecuador, began in January 2001 with the increased number of long-period (LP) events, followed by a swarm of volcano-tectonic (VT) earthquakes in November 2001. In late June 2002, the activity of very-long-period (VLP) (2 s) events accompanying LP (0.5–1 s) signals began beneath the volcano. The VLP waveform was characterized by an impulsive signature, which was accompanied by the LP signal showing non-harmonic oscillations. We observed temporal changes of both the VLP and LP signals from the beginning until September 2003: The VLP signal gradually disappeared and the LP signal characterized by decaying harmonic oscillations became dominant. Assuming possible source geometries, we applied a waveform inversion method to the observed waveforms of the largest VLP event. Our inversion and particle motion analyses point to volumetric changes of a sub-vertical crack as the VLP source, which is located at a depth of 2–3 km beneath the northeastern flank. The spectral analysis of the decaying harmonic oscillations of LP events shows frequencies between 2.0 and 3.5 Hz, with quality factors significantly above 100. The increased VT activity and deformation data suggest an intrusion of magma beneath the volcano. A release of gases with small magma particles may have repetitively occurred due to the pressurization, which was caused by sustained bubble growth at the magma ceiling. The released particle-laden gases opened a crack above the magma system and triggered the resonance of the crack. We interpret the VLP and LP events as the gas-release process and the resonance of the crack, respectively. 相似文献
70.
Degassing through open paths such as bubble and/or fracture networks is considered to be the principal mode of degassing in silicic magmas. However, its detailed mechanisms remain unclear. To investigate the behavior of bubbles in a hypothetical open-system condition, we performed a series of vesiculation experiments on natural rhyolitic obsidian using a newly designed semipermeable cell, which artificially maintains a pressure difference between its inside and outside. The thick-wall cell maintains a constant volume within the sample chamber, while allowing water vapor to escape the cell during the experimental runs. The cells containing obsidian cores with ca. 0.66 wt.% initial water content were externally heated to 1000 °C for a period of 1–288 h. The run charges generally showed a zonal structure composed of two contrasting regions: a central region within which the bubbles were concentrated (bubble-rich core, BC) and a bubble-free melt region surrounding the BC (bubble-free margin, BFM). With increased heating duration, the thickness of the BFM increased via dissolution of the outermost bubbles in the BC. The water content was nearly uniform throughout the BC, whereas an outward-decreasing gradient was observed in the BFM. We found that diffusive dehydration occurred from the sample surface, and the bubbles were resorbed into the melt. Thus, the BFM–BC boundary moved inwards. These processes were modelled numerically, and the calculation results were in good agreement with the experimental data. If a “lifetime” of open paths is approximated as the relaxation time of a melt in a shallow volcanic environment, then the paths have to be pinched off quickly (1.2 h at maximum pressure difference between the open path and the melt) and thus the thickness of the bubble-free layer reaches at most ~ 0.1 mm. For the formation of bubble-free obsidian layers with a width of a few millimeters, which are often observed in natural obsidian flows, open paths should be maintained for at least a few hundred hours. 相似文献