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Basic dynamic characteristics and seismic design of anchorage system
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作者 段建 言志信 +1 位作者 任志华 赵红亮 《Journal of Central South University》 SCIE EI CAS 2014年第8期3275-3283,共9页
Based on some assumptions,the dynamic governing equation of anchorage system is established.The calculation formula of natural frequency and the corresponding vibration mode are deduced.Besides,the feasibility of the ... Based on some assumptions,the dynamic governing equation of anchorage system is established.The calculation formula of natural frequency and the corresponding vibration mode are deduced.Besides,the feasibility of the theoretical method is verified by using a specific example combined with other methods.It is found that the low-order natural frequency corresponds to the first mode of vibration,and the high-order natural frequency corresponds to the second mode of vibration,while the third mode happens only when the physical and mechanical parameters of anchorage system meet certain conditions.With the increasing of the order of natural frequency,the influence on the dynamic mechanical response of anchorage system decreases gradually.Additionally,a calculating method,which can find the dangerous area of anchorage engineering in different construction sites and avoid the unreasonable design of anchor that may cause resonance,is proposed to meet the seismic precautionary requirements.This method is verified to be feasible and effective by being applied to an actual project.The study of basic dynamic features of anchorage system can provide a theoretical guidance for anchor seismic design and fast evaluation of anchor design scheme. 展开更多
关键词 anchorage system natural frequency vibration mode dangerous region resonance line seismic precautionary
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Na_2高位振动态与Ar,N_2碰撞中模温度的变化
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作者 刘静 封丽 +1 位作者 戴康 沈异凡 《原子与分子物理学报》 CAS CSCD 北大核心 2015年第4期611-615,共5页
利用受激发射泵浦激发Na2分子,使Na2[X1∑+g(ν″=33,J″=11)]得到布居,研究了高振动激发态Na*2与Ar和N2的碰撞弛豫过程.由激光诱导荧光得到Na2(ν≤33)各振动能级的时间分辨布居分布,从而得到Boltzmann振动温度和转动温度随时间的变化... 利用受激发射泵浦激发Na2分子,使Na2[X1∑+g(ν″=33,J″=11)]得到布居,研究了高振动激发态Na*2与Ar和N2的碰撞弛豫过程.由激光诱导荧光得到Na2(ν≤33)各振动能级的时间分辨布居分布,从而得到Boltzmann振动温度和转动温度随时间的变化.对于Na*2与Ar碰撞,在泵浦-探测延迟时间tD=8μs前,振动温度Tvib减小很慢;在8-12μs间,Tvib迅速下降并达到平衡.而转动温度Trot和平移温度Ttran在Tvib迅速下降时才开始缓慢增加.对于Na*2与N2碰撞,Tvib存在三个变化阶段,先是迅速下降,然后下降减缓,最后减小很慢并达到平衡.而在整个过程中,Trot和Ttran一直是很缓慢地增加.实验数据说明了弛豫过程是分阶段进行的,单一速率系数不能正确解释复杂的弛豫过程,并会丢失平衡过程中的关键特点. 展开更多
关键词 平衡过程 模温度 受激发射泵浦 Na2高位振动态 激光诱导荧光
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