共查询到20条相似文献,搜索用时 78 毫秒
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《振动与冲击》2016,(23)
为研究大跨度混凝土斜拉桥在爆炸荷载下的动力响应和损伤模式。建立全桥实体模型和跨中主梁局部模型,并开展不同炸药条件下的斜拉索应力分析和结构动力响应分析。结果表明:(1)斜拉索在爆炸荷载下直接破坏的风险较低,只有偏载作用时近爆点斜拉索有断索风险;(2)斜拉桥混凝土主梁的局部破坏模式与爆炸位置和TNT当量均有关系;爆炸位置相同时,随着TNT当量增大,破坏模式由弯曲破坏转变为直剪破坏;(3)梁体纵向加劲肋在中小爆炸荷载作用下能有效提高梁体的抗爆能力,其与箱梁顶板形成具有相对强弱刚度的熔断体系,有效限制梁体横向破坏面的扩展,降低破坏程度,甚至可改变梁体的破坏模式;(4)箱梁结构破坏时冲击波在箱室内传播存在明显的约束效应并引起更严重破坏。 相似文献
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冷却塔定向爆破拆除及爆破效果有限元数值模拟 总被引:2,自引:1,他引:1
介绍了3000m2冷却塔的爆破拆除实例,采用动力有限元分析软件ANSYS/LS-DYNA建立了冷却塔爆破拆除三维有限元模型,对爆破倒塌效果进行了模拟.模拟结果与真实情形在倾倒过程与倒塌效果方面有很大相似性.冷却塔结构上窄下宽,重心较低,失稳后重心不容易移出,但由于本身体积和重量都比较大,而塔壁较薄,爆破缺口形成后发生塑... 相似文献
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分阶段施工实际上是斜拉桥结构体系与作用于结构上的荷载不断变化的过程。施工工序的变化引起荷载的变化,结构上荷载的变化改变着斜拉索的索力,斜拉索的主动调索表面上是改变着斜拉索的索力,而本质上是改变了斜拉索的无应力长度。按照无应力状态控制法最终结构的内力和线形与施工过程无关的基本原理,可以实现斜拉桥施工中斜拉索调索与其他工序同步并行作业。 相似文献
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根据建筑物拆除爆破失稳原理,对桥礅柱定向倒塌控制爆破拆除试爆时产生后坐进行力学分析,得出试爆产生后坐的主要原因是保留支撑截面瞬间强度不够,调整主爆相关参数,使主爆达到预期效果。 相似文献
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大跨度钢索和CFRP索斜拉桥车桥耦合振动研究 总被引:5,自引:0,他引:5
以跨度600m~1400m的大跨度斜拉桥为对象,应用考虑拉索侧向振动影响的车桥耦合振动分析方法研究了钢索和CFRP索斜拉桥的交通振动响应,比较了车辆计算模型、行车速度对计算结果的影响,并分析了斜拉桥的动力冲击系数。研究结果表明,大跨度斜拉桥主梁的振动响应以静位移和长周期振动成分为主,拉索局部侧向振动不明显,车辆计算模型对结构振动响应的影响十分有限,行车速度的提高增加了结构的动力系数,两种拉索材料对斜拉桥在车辆荷载下的振动响应影响很小,斜拉桥的动力系数离散性大且与构件类型有关。 相似文献
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《工程爆破》2022,(1)
针对贵阳发电厂内冷却塔是由钢筋混凝土构成的薄壁双曲型圆筒,具有底部直径大,垂直高度高,塔壁外部没有施工条件且周边环境较为复杂的特点,采用预拆除技术,以确保冷却塔爆破拆除顺利实施并取得良好的效果。预拆除技术主要由3个部分组成:冷却塔内部支撑、倒塌方向薄壁的减荷槽以及倒塌反向的泄压窗。通过理论计算设计出正梯形爆破切口的参数,在人字形柱上同时采用开设减荷槽(13个)的方法,来保证冷却塔筒壁在倒塌过程中的屈服破碎效果,为了进一步减小爆炸冲击波对冷却塔筒壁的破坏作用,在倒塌方向的反方向开出一个2m×4m的矩形泄压窗。根据现场实验结果和冷却塔整体爆破效果,预拆除技术对薄壁双曲型冷却塔爆破起到了良好的作用,达到了冷却塔整体失稳倒塌,精确定向以及整体不下坐的效果。 相似文献
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Zh. Tomilo P. Molchan S. Ustinovich V. Finskaya N. Prytkova L. Kurochkin 《Journal of Low Temperature Physics》1999,117(5-6):1635-1639
Superconducting yttrium borocarbides were synthesized by different methods. A two-step method was found to be advantageous. Influence of the annealing time on superconducting properties is investigated. The superconducting temperature of YNi
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B
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C single crystal is 15 K. 相似文献
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Gangan Prathap 《Scientometrics》2014,101(3):1781-1787
In this paper, we look at the issue of the high-end of research performance which is captured in the tail of a citation distribution. As the mean is insufficient to capture the skewness of such distributions, a consistency or concentration measure is the additional parameter needed. We show that the h-index is only approximately a heuristic mock of a composite indicator built from three primary indicators which are the number, mean and consistency term. The z-index is able to sense the change in consistency in the distribution due to the outliers in the tail of the distribution. 相似文献
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Geraldine L. C. Paulus Qing Hua Wang Zachary W. Ulissi Thomas P. McNicholas Aravind Vijayaraghavan Chih‐Jen Shih Zhong Jin Michael S. Strano 《Small (Weinheim an der Bergstrasse, Germany)》2013,9(11):1954-1963
Junctions between a single walled carbon nanotube (SWNT) and a monolayer of graphene are fabricated and studied for the first time. A single layer graphene (SLG) sheet grown by chemical vapor deposition (CVD) is transferred onto a SiO2/Si wafer with aligned CVD‐grown SWNTs. Raman spectroscopy is used to identify metallic‐SWNT/SLG junctions, and a method for spectroscopic deconvolution of the overlapping G peaks of the SWNT and the SLG is reported, making use of the polarization dependence of the SWNT. A comparison of the Raman peak positions and intensities of the individual SWNT and graphene to those of the SWNT‐graphene junction indicates an electron transfer of 1.12 × 1013 cm?2 from the SWNT to the graphene. This direction of charge transfer is in agreement with the work functions of the SWNT and graphene. The compression of the SWNT by the graphene increases the broadening of the radial breathing mode (RBM) peak from 3.6 ± 0.3 to 4.6 ± 0.5 cm?1 and of the G peak from 13 ± 1 to 18 ± 1 cm?1, in reasonable agreement with molecular dynamics simulations. However, the RBM and G peak position shifts are primarily due to charge transfer with minimal contributions from strain. With this method, the ability to dope graphene with nanometer resolution is demonstrated. 相似文献
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In this work, a gamma ray Compton backscatter technique is used for imaging defects and thickness variations in insulated pipes and metal plates containing depressions of various diameters and at various depths from one side of the object. The scattered radiation was measured by a scintillation detector that scans the object using a two-dimensional mechanical scanning system. The gamma spectrum was displayed with a multichannel analyzer (MCA), and the energy window width was selected so that only Compton single scatter counts were measured. Images were constructed using the LabVIEW computer program. Successful images of defects on the outer surface of the object under the insulation were obtained, and the system was found to be able to detect wall thickness changes in large pipes with walls more than 15 mm thick. Low activity sources of 108 Bq (a few mCi) were used, and the dose rate near the surface is four orders of magnitude lower than conventional industrial radiography sources, permitting it to be much safer. 相似文献
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A single bubble trapped at an antinode of an acoustic standing wave field in water can emit 50ps-140ps light pulses, called "single bubble sonoluminescence" (SBSL). It arouses much interest in physical acoustics because of its highly non-linear characteristics, high concentration of energy, and stable cavitation behavior. In this paper, bubble stability, the dynamic behavior of bubbles, non-invasive measurement of driving acoustic pressure and Mie scattering method are introduced. 相似文献
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Single electron tunneling (SET) technology offers the ability to control the transport of individual electrons. In this paper, we investigate single electron encoded logic (SEEL) memory circuits, in which the Boolean logic values are encoded as zero or one electron charges. More specifically, we focus on the implementation of SEEL latches and flip-flops. All proposed circuits are verified by means of simulation using the SIMulation Of Nanostructures package. We first present a generic SEEL linear threshold gate implementation, from which we derive a family of Boolean logic gates. Second, we propose Boolean gate-based implementations of the RS latch, the D latch, and D flip-flop. Third, we propose threshold gate-based implementations of the same memory elements. Finally, we discuss the estimated area, delay, and power consumption of the Boolean gate-based and threshold gate-based implementations, and compare them with other SET-based memory elements. 相似文献
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