MR阻尼器对斜拉索共振峰频率漂移的影响

本文采用Spencer提出的MR模型,对斜拉索和MR阻尼器组成的系统进行了动力分析,考察了MR阻尼器型号、安装位置、施加的电压以及斜拉索基频(张力、索长、质量)、激励荷载(类型、频率、大小)等各种因素对斜拉索共振峰频率漂移的影响。进而对钱江三桥南岸154m长的斜拉索进行了现场试验。斜拉索自由振动的衰减信号通过阶跃激励的方法获得,经小波变换、Hilbert变换识别出系统的共振峰频率,并与斜拉索在安装油阻尼器和无阻尼器两种情况进行了比较。计算了杭州湾大桥330m长的索在被动控制、半主动控制下的各阶共振峰频率。研究表明,斜拉索在安装MR阻尼器后共振峰频率略微增大。其影响程度比安装油阻尼器时要大。因此MR阻尼器的制振效果除主要来自耗能外,还有部分来自调频作用。     

斜拉索局部振动对结构地震响应的影响

以苏通长江公路大桥为研究对象,将斜拉索分成若干等长度的单元模拟斜拉索局部振动,以探讨其对结构地震响应的影响。计算结果表明:考虑斜拉索局部振动后,结构的自振频率变化较小;由于斜拉索基频与结构基频相近,斜拉索在地震动作用下,大幅振动,同时索—梁耦合振动明显,主梁和主塔内力降低,主塔根部弯矩明显减小。     

考虑斜拉索刚度、垂度、阻尼的非线性运动方程研究

随着斜拉桥跨径的快速增长,斜拉索的长度也大大增加,斜拉索是斜拉桥的主要受力构件,其在外荷载作用下经常引发大幅振动,这样就降低了斜拉索的寿命或造成拉索的破坏,因此研究斜拉索的非线性运动方程对解决振动问题具有实际工程的意义。本文在考虑斜拉索非线性静平衡曲线、抗弯刚度、粘滞阻尼影响的斜拉索平面内非线性振动的基础上,建立了斜拉索非线性运动方程。采用Galerkin法解耦了斜拉索非线性运动方程,并运用Runge-Kutta法对其自由振动和周期强迫振动两种情形进行了求解,最后,通过对该索的理论计算数据与原型仿真数据的对比分析,可知上述非线性方程比传统的线性方程更精确。本文的研究为今后斜拉索的非线性分析及其振动控制奠定了一定的理论基础。     

基于环境振动的斜拉桥拉索基频识别

斜拉索是现代斜拉桥最重要的结构构件，索力在斜拉桥的施工控制和长期监测中起着重要作用。振动测试法是斜拉桥索力测定、监测和状态评估中应用最广泛的一种方法。振动法测索力的关键在于准确地识别出索的基频。本文使用自功率谱和倒频谱方法，基于MATLAB平台，开发出了斜拉桥拉索环境振动模态分析图形用户交互(GUI)工具箱，实现了斜拉索基频的快速自动识别。应用本文的方法，对福州青洲闽江主跨605m斜拉桥拉索的环境振动实测加速度数据进行了分析处理，斜拉索基频识别方便直观，结果可靠。     

斜拉索拱与索拱体系静动力性能的对比性研究

在索拱结构的基础上添加上部斜拉系统则构成了斜拉索拱结构,因此两种结构呈现出不同的受力特性。本文基于实际的工程背景,借助ANSYS建立斜拉索拱结构与索拱结构的有限元分析模型,在四种相同荷载工况作用下,对静力性能和动力性能,进行了结构参数的比较分析,得出了两者在力学性能的异同。结果表明斜拉索拱结构的受力特性优于索拱结构。     

采用Ernst公式计算斜拉桥拉索振动特性的精度分析

斜拉桥拉索的动力特性是建立在斜拉桥的静力分析的基础上的.在静力分析中,几何非线性明显的索经常通过Ernst公式线性化成二力杆,但是,在动力分析中,很少有人研究过Ernst公式的精度.编制了基于弹性悬链线单元的斜拉索的非线性有限元分析程序,该程序可以一根索的任何一个参数值为已知条件来确定索的状态,研究了斜拉索不同张拉阶段索的频率和振型特性,并比较了Ernst公式计算拉索动力特性的精度和适用范围.     

索梁耦合振动下拉索几何非线性频率与空间运动

为研究索梁结构非线性振动过程中拉索的空间运动轨迹及其特性,进行了索梁结构模型试验。测试了索梁结构面内、外几何非线性频率,并和有限元结果对比,两者吻合良好;分别研究了索梁结构在自由振动和强迫振动时,拉索空间运动轨迹的变化过程和规律。研究表明:索梁结构面内固有频率的几何非线性效应明显,频率法测斜拉索索力应以面外固有频率为准;索梁结构在自由振动时,拉索空间振动除幅值呈指数衰减外,还具有"气圈"椭圆形状的长/短轴互换和转动方向的顺/逆时针互换两个特征;在稳态的强迫振动时,拉索空间振动"气圈"形状仅随激励频率的变化而改变。     

双排隔振屏障对振动波的阻隔作用及动力响应分析

本文采用模拟试验的方法,对分层土地基中双排隔振屏障对振动波的动力响应进行了探讨,并研究了桩长与土层分界面位置关系、激振频率对其隔振效果的影响作用,得出结论:（1）屏障前振动强度远大于屏障后振动强度,并随着振源距、激振频率、桩长的增加而下降,且屏障前出现明显振动增强现象,在激振频率80 Hz时产生振动峰值,振动强度在高频时基本稳定,继续增加激振频率,振动强度并不会发生明显变化。（2）屏障后中线左右2倍桩长范围内为整个隔振区域的薄弱区,其他区域则由包络线围成一个封闭有效隔振区。（3）屏障对中频和高频有更好的隔振效果,且桩长越大有效隔振面积越大,当桩长超过土层分界面时,有效隔振面积可达到53.25%～69.78%,但此时有效隔振面积增幅由原来的14.29%下降到11.64%,增幅降低了约3%。（4）未设屏障区振动强度较小,随激振频率小范围内浮动,在激振频率为30 Hz和80 Hz时取得振动峰值,且随着屏障布置方向减小,即靠近屏障一侧振动强度较强,远离屏障一侧振动强度较弱。     

具有弹性转动约束的斜拉桥多索-浅拱模型及其面内自由振动分析

考虑斜拉桥的初始构型,建立具有弹性转动约束的多索-浅拱模型。首先,采用Hamilton变分原理得到了索和浅拱的控制微分方程。为了保证浅拱在索-浅拱连接处满足连续条件,将浅拱分段考虑,通过索-浅拱连接处的位移连续条件和力的平衡条件以及两端支座处的边界条件,推导了求解该系统自由振动问题的基本方法。然后,以弹性转动约束双索-浅拱模型为例,对其面内特征值问题进行求解,同时,建立相应的ANSYS模型,得到该模型频率和振型的有限元解。通过与有限元方法计算结果的对比,表明本文方法的正确性和有效性。最后,选取了斜拉索的倾角、垂度,浅拱的抗弯刚度、矢跨比,以及支座的转动刚度等参数,对模型的前5阶频率进行了参数化分析。     

黏滞阻尼器对拉索参数振动的控制分析

提出采用黏滞阻尼器对拉索参数振动进行控制,建立了黏滞阻尼器控制拉索参数振动的运动方程。从频域和时域以及起振幅值等角度,研究了最优黏滞阻尼器对不同垂度拉索参数振动的控制效果;此外,还研究了最优黏滞阻尼器安装位置对拉索参数振动控制效果的影响。研究表明,黏滞阻尼器可以有效控制拉索的参数振动,控制效果与拉索的激励幅值、最优阻尼器的安装位置和斜拉索的垂度有关。激励幅值越大,控制效果一般越差;最优阻尼器的安装位置越靠近跨中,则控制效果越好;黏滞阻尼器对大垂度拉索的控制效果不及对小垂度拉索的控制效果。     

Einige geoelektrische Untersuchungen auf österreichischen Gletschern

Summary Experiments to determine the thickness of glaciers by high frequency prospecting were carried out on the Austrian glacier Hintereisferner in 1938. After the war electrohydrographical measurements on glacier rivulets were carried out in the Kaprun Valley. The resistance of the glacier water fluctuates according to the time of season. It depends on the respective composition of these waters (Fig. 2). Therefore the geologic and mineralogic properties of the glacier-water may be deducted from the electric resistance. Especially the amount of surface water may be deducted (Fig. 3). An example is shown in Fig. 4.     

Seasonal variation in water column conditions in the upper Gulf of Thailand

Seasonal variation in water column conditions in the upper Gulf of Thailand (UGoT) was analyzed by considering four major factors including surface heat flux, freshwater discharge, tidal and wind stirrings. The coincidence of surface heat loss, low river discharge and strong wind resulted in vertical well-mixing in December. Strong stratification developed in September and October due to large river discharge and moderate heat flux. Strong surface heating in April and May has a potential to generate strong stratification, although not as large as that in September and October due to low river discharge. Although no factors are prominent during January and March, and June and August, weak to moderate stratification results, because the influences of river discharge and surface heating are still larger than those of tidal and wind stirrings. The results of water column analysis based on monthly average data agree well with analyses derived from cruise data in the same months. Most analytical results correspond to the distributions of temperature and salinity from field observations. Disagreement, however, was found in December 2003 (cruise CU-2) when stratification in some small regions occurs in the distribution of water properties, but the water column analysis suggests vertical well-mixing. This phenomenon is triggered by non-uniform distribution of freshwater over UGoT, which is related to river discharge, monsoonal wind and current. Compared to a previous study regarding surface chlorophyll dynamics, water column conditions may be used to explain the occurrence of phytoplankton bloom in this region.     

Analysis of Weak Wind Stable Conditions from the Observations of the Land Surface Processes Experiment at Anand in India

The observations in weak wind stable conditions are scarce. The present study examines the observations from the Land Surface Processes Experiment (LASPEX) conducted at Anand, (Gujarat, India) during the year 1997–1998 to study the characteristics of surface layer under weak wind stable conditions. The observed surface fluxes are compared with those computed using Monin-Obukhov (M-O) similarity theory. The upper air observations and regional climatology are used to justify the persistence of weak wind conditions at Anand. The frequency of occurrence of weak wind stable conditions is observed to be around 67%. In 86% of the cases under weak wind conditions, bulk Richardson number (R_iB) is found to be larger than 0.2. The magnitude of surface fluxes computed from M-O similarity theory is shown to be smaller in comparison to those based on the observations in weak wind stable conditions. Surface fluxes computed using the empirical relations for the eddy diffusivities and drag and heat exchange coefficients are found to be comparable with those based on M-O similarity theory however these fluxes are under-predicted in comparison to the observations. The traditional M-O similarity theory is not able to simulate the observed fluxes well in weak wind stable conditions at Anand.     

井水位前驱波与气压、 风、 降雨及强震关系的分析

对山西朔州井与静乐井水位前驱波与气压、 风、 降雨及强震关系进行定量、 半定量统计分析的结果表明, 前驱波引起的井水位变幅与气压引起的井水位的水位变幅不一致, 前驱波的周期与气压、 风、 降雨周期不匹配, 出现的时间不同步, 形态差异也很大, 与短时间集中降雨也无明显的对应关系。 前驱波与强震之间存在较好的对应关系, 对应率在50%左右。 井水位前驱波现象不是气压、 风、 降雨等干扰因素的短期突变所造成的, 可能反映了大震前震源内部信息。     

基于高频高光谱近感观测量化风对蓝藻水华的影响

全球气候变化显著影响湖泊理化环境和生态系统演化,对生态系统服务造成负面影响甚至引发生态系统灾变,其中风速下降可能促使富营养化湖泊蓝藻水华的暴发和水面漂浮集聚。以往由于较低的观测频次,往往很难精细量化风对蓝藻水华的影响。利用陆基高光谱近感观测技术,基于分钟小时尺度开展周年高频观测,通过对6—10月蓝藻生长期太湖表层水体叶绿素a浓度统计分析,量化蓝藻水华高频动态变化特征,确定蓝藻水华漂浮集聚的风速阈值。研究发现,随着风速的下降,水体表层叶绿素a浓度随之增加,蓝藻水华出现概率也随之增加。概率分析显示,当近地面风速小于2.5 m/s时,湖泊表层比较容易形成明显肉眼可见的蓝藻水华,藻华发生概率为55.1%。长时间持续的低风速容易诱发蓝藻水华形成和漂浮集聚,强风浪事件后低风速出现1～2天叶绿素a往往就能恢复以往较高水平,这为管理者有效防控蓝藻水华提供了新视角。长期气象观测显示,气候变化影响下太湖地区风速呈现显著下降趋势,增加了蓝藻竞争优势和发生概率,有助于其在表面漂浮集聚。在未来的气候变化情景下,如果风速继续呈现下降趋势,在营养盐条件不变情况下湖泊表层蓝藻水华发生概率可能还会上升,增加蓝藻水华防控...     

西北太平洋热带气旋活动对大尺度环境场影响的线性回归分析

本文使用西北太平洋累积气旋能量(ACE)月尺度异常序列,对850 hPa相对涡度、地表纬向风、柱水汽含量、OLR、降水和SST等大尺度环境场变量进行时滞回归分析,讨论了月尺度TC活动对大尺度环境场的影响及其与周尺度的区别和联系.结果表明:(1)月尺度ACE回归出的纬向风无论是强度还是范围都要明显大于周尺度ACE回归结果,TC的频繁发生,尤其是强度大且持续时间长的近赤道TC,对于激发或加强TC活动区域南侧的低纬地区西风异常有一定的积极作用,持续并且强度较大的西风异常可能导致西风的爆发,而西风爆发会在很大程度上影响ENSO事件的发生和演变.(2)在月尺度上,OLR、柱水汽含量、降水和SST等物理量均呈现出较为明显的E1Nino型分布,而在周尺度上,仅SST呈现出明显的El Nino型分布,这在一定程度上反映了月尺度TC活动和太平洋ENSO信号之间存在更密切的关联.(3)在TC发生后1-2月,TC的主要生成区域柱水汽含量减少、OLR增大,这会在一定程度上降低该区域生成TC的潜能.虽然TC所引起SST降低的空间尺度很小,但其通过大气和海洋的传导会扩大到更大尺度上,由于这种反馈具有一定的滞后性,所以月尺度TC对大尺度环境场影响的信号更为显著.     

Transient upwelling in the central Baltic Sea

The paper presents a theoretical study to explain the regular occurrence of a cold water upwelling cell at the southern east coast of the Gotland island in the central Baltic Sea. While for a circular island up- and downwelling patterns would rotate around the island, the responses around the elongated Gotland island with narrow tips at its southern and northern ends are different. The study uses the example of the response of a coastal ocean to a wind band to develop an understanding of important aspects of generation of Kelvin waves and how the waves change the response patterns.     

基于MODIS数据的2000-2010年乌梁素海"黄苔"时空变化

利用2000-2010年每年5-9月MODIS数据根据比值算法提取乌梁素海湖区黄苔的面积和空间分布信息并进行统计分析,探求乌梁素海黄苔产生的时空分布规律及特征,从而为黄苔的预防和治理提供支持.结果表明:(1)黄苔面积变化的年际和月际特征方面,2000、2001、2005、2006、2008、2010年黄苔面积超过了多年平均值(24 km2).5—7月份黄苔面积较小,保持在20 km2左右;8月黄苔面积迅速增长(约28 km2),9月黄苔面积最大,达到40 km2左右.(2)黄苔发生频率方面,2001年黄苔的规模和频率最高,发生频率达到0.58;2005、2006、2010年次之,发生频率在0.25附近波动(多年年均黄苔暴发频率为0.19);其他年份黄苔的发生频率处于低于0.10的水平.黄苔发生规模较大、次数较多的月份集中在8、9月,发生频率分别达到0.27、0.52,超过多年月均黄苔暴发频率0.19;其他月份黄苔的发生频率处于低于0.10的水平.(3)黄苔出现的空间分布方面,西大滩为东大滩的北部至中部,以及乌梁素海南部明水区排干口附近的西部沿岸是黄苔出现频率较高的区域.(4)2个月前的日均温度、降雨和营养盐浓度及当月风速与黄苔的产生具有极显著相关性;营养盐含量(TN、TP)的空间分布与黄苔的空间分布表现出较好的相关性.乌梁素海黄苔面积的年际变化受人类活动特别是生态补水的影响明显.     

Wind flow and wind loads on the surface of a towershaped building: Numerical simulations and wind tunnel experiment

Flow structure and wind pressure distribution caused by obtuse obstacles are usually the focuses in Computational Wind Engineer researches (CWE). By solving the non-hydrostatical dynamic equations, PUMA model (Peking University Model of Atmospheric Environment) was developed and applied to simulating the flow structure and wind pressure distribution around a tower-shaped building. Evaluation about the wind environment and wind loads around the building was obtained through the analysis of the numerical simulation results and wind tunnel data. Comparisons between the simulation and wind tunnel study indicate that numerical simulation results agree well in the flow field and wind pressure distribution around the tower-shaped building. On the other hand, the horizontal grid interval of 2 m and the vertical grid of 3 m were still too crude to simulate the flow structure and wind pressure distribution on the building surface more exactly in detail; and the absence of suitable pressure perturbation parameterization scheme between the solid and the adjacent space also limits the accuracy of the numerical simulation. The numerical simulation model can be used to evaluate the wind environment and wind load around high buildings.     

Wind influence on surface current variability in the Ibiza Channel from HF Radar

Surface current variability is investigated using 2.5 years of continuous velocity measurements from an high frequency radar (HFR) located in the Ibiza Channel (Western Mediterranean Sea). The Ibiza Channel is identified as a key geographical feature for the exchange of water masses but still poorly documented. Operational, quality controlled, HFR derived velocities are provided by the Balearic Islands Coastal Observing and Forecasting System (SOCIB). They are assessed by performing statistical comparisons with current-meter, ADCP, and surface lagrangian drifters. HFR system does not show significant bias, and its accuracy is in accordance with previous studies performed in other areas. The main surface circulation patterns are deduced from an EOF analysis. The first three modes represent almost 70 % of the total variability. A cross-correlation analysis between zonal and meridional wind components and the temporal amplitudes of the first three modes reveal that the first two modes are mainly driven by local winds, with immediate effects of wind forcing and veering following Ekman effect. The first mode (37 % of total variability) is the response of meridional wind while the second mode (24 % of total variability) is linked primarily with zonal winds. The third and higher order modes are related to mesoscale circulation features. HFR derived surface transport presents a markedly seasonal variability being mostly southwards. Its comparison with Ekman-induced transport shows that wind contribution to the total surface transport is on average around 65 %.