大气边界层湍流温度序列的信息熵分析   总被引：2，自引：0，他引：2  

汪景烨  付遵涛  张霖  刘式达 《高原气象》2005,24(1):38-42

利用大气边界层内近地面的大气湍流温度时间序列，运用功率谱分析、信息熵分析等方法，分析了大气边界层内近地面的大气湍流特点，并对稳定层和不稳定层的大气湍流进行了对比。结果表明，信息熵和功率谱指数是区别稳定层结和不稳定层结大气边界层湍流特征的指标，对造成两者之间的差别做出了对应的解释。  相似文献   

黑龙江气候变暖的时空变化特征   总被引：15，自引：0，他引：15  

潘华盛  张桂华 《黑龙江气象》2002,(3):3-6,11

进入80年代以来，黑龙江气温明显变暖，近120年来年平均气温上升1.4℃，春季次之，气温突变在1990年前后，从年、各季平均气温变化趋势与全国北半球及全球气温变化进行比较，年及冬季我国增暖中心在黑龙江，春季增暖中心在内蒙古北部及黑龙江省；夏秋增暖不明显，但仍有上升趋势，近50年来，50～70年代黑龙江省及全国各大区域普遍增暖不明显，80年代开始黑龙江省增暖明显，三北地区次之，90年代黑龙江增暖更加明显，而全国及其他区域上升已达到80年代北方增温幅度，这里从黑龙江变暖的事实，突变时间，与全球、北半球、全国区域的气温及雪盖海温变化关系来揭示黑龙江气候变化的时空特点。  相似文献   

显式自由表面模型时间分裂格式的一个积分方案   总被引：5，自引：0，他引：5  

Zhou Weidong 《大气科学进展》2002,19(2):255-265

讨论了有关显式自由表面模型的时间分裂格式中的分裂误差。在传统的积分方案中，由于采用蛙跳格式，斜压动量方程具有三层的时间离散结构，但是，正压动量方程在相应的时间层上只有二层的离散结构。因此，正压方程与斜压方程的时间离散结构是不相容的。分析结果表明，这是导致分裂误差的原因。本提出一种能保持时间离散结构相容的正压和斜压方程的时间积分方案。该积分方案的分裂误差很小因此特别适合于需要长期积分的气候研究。该方案在北太平洋的一个自由表面模型中得到了应用。  相似文献   

Electrical aerosol spectrometer of Tartu University     

H. Tammet  A. Mirme  E. Tamm   《Atmospheric Research》2002,62(3-4)

The electrical aerosol spectrometer (EAS) of the parallel measuring principle at Tartu University is an efficient instrument for rapid measurement of the unstable size spectrum of aerosol particles. The measuring range from 10 nm to 10 μm is achieved by simultaneously using a pair of differential mobility analyzers with two different particle chargers. The particle spectrum is calculated and measurement errors are estimated in real time by using a least-squares method. Experimental calibration ensures reliability of measurement. The instrument is well suited for continuous monitoring of atmospheric aerosol.  相似文献   

Study on effects of damping in laminated rubber bearings on seismic responses for a ⅛ scale isolated test structure     

Bong Yoo  Yang‐Hann Kim 《地震工程与结构动力学》2002,31(10):1777-1792

The effects of damping in various laminated rubber bearings (LRB) on the seismic response of a ?‐scale isolated test structure are investigated by shaking table tests and seismic response analyses. A series of shaking table tests of the structure were performed for a fixed base design and for a base isolation design. Two different types of LRB were used: natural rubber bearings (NRB) and lead rubber bearings (LLRB). Three different designs for the LLRB were tested; each design had a different diameter of lead plug, and thus, different damping values. Artificial time histories of peak ground acceleration 0.4g were used in both the tests and the analyses. In both shaking table tests and analyses, as expected, the acceleration responses of the seismically isolated test structure were considerably reduced. However, the shear displacement at the isolators was increased. To reduce the shear displacement in the isolators, the diameter of the lead plug in the LLRB had to be enlarged to increase isolator damping by more than 24%. This caused the isolator stiffness to increase, and resulted in amplifying the floor acceleration response spectra of the isolated test structure in the higher frequency ranges with a monotonic reduction of isolator shear displacement. Copyright © 2002 John Wiley & Sons, Ltd.  相似文献   

Numerical Analysis of Space–Time Finite Element Formulations for Miscible Displacements     

Rigoberto G. Sanabria Castro  Sandra M. C. Malta  Abimael F. D. Loula  Luiz Landau 《Computational Geosciences》2002,5(4):301-330

A finite element formulation is proposed to approximate a nonlinear system of partial differential equations, composed by an elliptic subsystem for the pressure–velocity and a transport equation (convection–diffusion) for the concentration, which models the incompressible miscible displacement of one fluid by another in a rigid porous media. The pressure is approximated by the classical Galerkin method and the velocity is calculated by a post-processing technique. Then, the concentration is obtained by a Galerkin/least-squares space–time (GLS/ST) finite element method. A numerical analysis is developed for the concentration approximation. Then, stability, convergence and numerical results are presented confirming the a priori error estimates.  相似文献   

震源时间函数与震源破裂过程   总被引：2，自引：0，他引：2  

许力生  陈运泰 《地震地磁观测与研究》2002,23(6):1-8

简要介绍了现代数字地震学的两个重要概念。一个是震源时间函数，另一个是地震震源的时空破裂过程。首先，从地震断层位移表示定量出发，介绍震源时间函数和震源破裂过程的基本概念。然后，分别介绍两种从远场地震记录中提取震源时间函数和获取有限断层面上时空破裂过程图像的反演方法。  相似文献   

Most likely locations of large earthquakes in the Kanto and Tokai areas, Japan, based on the local recurrence times     

Max Wyss  Shozo Matsumura 《Physics of the Earth and Planetary Interiors》2002,131(2):173-184

We examined the hypothesis that minima in local recurrence time, T_L, or equivalently maxima in local probability, P_L, may map asperities in the Kanto and Tokai areas of Japan, where the earthquake catalog of the National Research Institute for Earth Science and Disaster Prevention (NIED) is complete at the M=1.5 (M1.5) level. We mapped T_L (P_L) based on the a- and b-values of the nearest earthquakes within 20 km of every node of a grid spaced 0.01° for M7 target events. Only earthquakes within the top 33 km were used. The b-values increase strongly with depth, in several areas. Therefore, some of the T_L (P_L) anomalies are not revealed if data from the entire crustal seismogenic zone are mixed. Thus, we mapped T_L (P_L) separately for the top 15 km and the rest of the depth range, as well as for the entire seismogenic crust. The resulting T_L- and P_L-maps show that approximately 12% of the total area shows anomalously short recurrence times. Out of six shallow target events with M≥6.5 and which occurred since 1890, five are located within the anomalous areas with T_L <450 years. We interpret this to mean that areas with anomalously short T_L map asperities, which are more likely than other areas to generate future target events. The probability that this result is due to chance is vanishingly small. The great Kanto rupture of 1923 appears to have initiated in the most significant asperity we mapped in the study area. One anomaly is located in the northeastern part of the area of the proposed future rupture of the Tokai earthquake, and another one at its southwestern corner. The absolute values of T_L calculated are uncertain because they depend on the size of the volume used for the calculation.  相似文献   

2001年1月2 6日印度古杰拉特(Gujarat)Ｍem>Ssub>7.8地震时空破裂过程   总被引：4，自引：2，他引：4       下载免费PDF全文

许力生  陈运泰  高孟潭 《地震学报》2002,24(5):447-461

从全球数字地震台网的长周期记录中，选择了震中距小于90的27个台站的54个P波震相和44个S波震相资料．首先，用波形反演方法确定了2001年1月26日印度古杰拉特(Gujarat)ＭS7.8地震的地震矩张量、震源机制、震源时间函数和时空破裂过程等震源参数．通过矩张量反演，并根据Kutch Mainland断层的走向、地震烈度的空间分布、余震震源的空间分布和震害的空间分布，确认2001年1月26日印度古杰拉特ＭS7.8地震的发震断层的走向为92、倾角为58、滑动角为62，即一走向近东-西向、断层面向南倾斜、以逆冲为主的左旋-逆断层．这次地震所释放的地震矩为3.51020 Nm，矩震级ＭW＝7.6．然后，借助合成地震图，采用频率域求谱商的方法，得到了依赖于台站方位的27个P波震源时间函数、22个S波震源时间函数以及平均的P波震源时间函数和S波震源时间函数．对震源时间函数的分析表明，这次地震是一次连续的破裂事件，开始比较急遽，但结束比较迟缓，总持续时间约19 s．最后，以所提取的P波和S波震源时间函数为资料，采用时间域的反演技术得到了断层面上滑动的时空分布．滑动量在断层面上的静态分布表明，断层面上的最大滑动量约为7 m．断层面上的最大应力降约为30 MPa，平均应力降约为7 MPa．滑动量大于0.5 m的区域在走向方向长85 km，在断层面倾斜方向宽约60 km(相应地，在深度方向约51 km)．破裂向东扩展约50 km，向西扩展约35 km．滑动量大于0.5 m的区域的主要部分呈椭圆形，其长轴取向与断层滑动方向一致．表明此区域破裂扩展的方向即是断层错动的方向．这种现象对于走滑断层情形是多见的，但对逆冲断层情形却少见．断层面上初始破裂点以东、以上部分面积大于初始破裂点以西、以下部分的面积，这是破裂非对称性的表现，表明破裂具有自西向东、自下向上单侧破裂的特征．从滑动率随时空变化的快照可以看出，滑动率在第4 s达到最大值，此时滑动率约为0.2 m/s，滑动基本上发生在破裂起始点及其周围．从第6 s开始，起始点的破裂基本结束，破裂开始向外围扩展．破裂向西的扩展速度明显小于向东的扩展速度．在第15 s，这种环形的扩展基本结束．自16 s以后，主要是一些零星的破裂点分布在破裂区的外围．从滑动量随时空变化的快照看，破裂自起始点开始后，逐渐向四周扩展．主要的破裂(滑动量大于5 m的区域)在6～10 s，具有明显的自西向东、向上的单侧破裂特征．在第11～13 s，破裂的西端向西、向下有所扩展．整个破裂过程持续约19 s．在整个破裂过程中的平均破裂速度约为3.3 km/s．   相似文献   

Nonlinear earthquake response analysis and energy calculation for seismic slit shear wall structures     

蒋欢军  吕西林 《地震工程与工程振动(英文版)》2002,1(2):227-237

Based on the concept of structural passive control, a new type of slit shear wall, with improved seismic performance when compared to an ordinary solid shear wall, was proposed by the authors in 1996. The idea has been verified by a series of pseudo-static and dynamic tests. In this paper a macro numerical model is developed for the wall element and the energy dissipation device. Then, nonlinear time history analysis is carried out for a 10-story slit shear wall model tested on a shaking table. Furthermore, the seismic input energy and the individual energy dissipated by the components are calculated by a method based on Newmark-β assumptions for this shear wall model, and the advantages of this shear wall are further demonstrated by the calculation results from the viewpoint of energy. Finally, according to the seismic damage criterion on the basis of plastic accumulative energy and maximum response, the optimal analysis is carried out to select design parameters for the energy dissipation device.  相似文献