台湾集集大地震及其余震的长周期地震动特性

用丰富的高质量数字强震记录对台湾集集大地震及余震的长周期地震动特性进行了研究. 本文主要研究了长周期地震动的强度随震级、距离及场地条件的变化情况;同时对近断层的长周期地震动特性进行了分析. 结果表明,集集大地震及余震的长周期地震动反应谱的形状主要受场地条件和震级控制（D+E类场地的反应谱要比B+C类的宽,震级大的反应谱要比震级小的宽）,而受距离影响并不显著;近断层长周期地震动明显受断层活动特性影响:上盘的长周期地震动比下盘的强,北部的比南部的强.      

区域性中心城市辐射力及其评价--以郑州市为例

文章以郑州市为例,主要研究了区域性中心城市辐射力指标体系,采用层次分析法对所研究指标进行了赋值。以此为基础,用裂点法对郑州与周边相邻、相关城市的不同城市要素相互作用的范围进行了分析。找出了郑州作为区域性中心城市的影响区域、发展优势和不足,并就提高郑州辐射力的途径、措施进行了研究。     

长春市强冰雪冻害天气系统及物理量特征

应用1971~2000年长春气象站10月至次年3月的逐日降水量、气温资料以及相应的NCEP/NCAR再分析资料,通过对资料的统计分析,给出了确定长春市发生强冰雪冻害天气的标准;根据对36个历史个例的高低空环流形势的分析,建立了4种强冰雪冻害的天气概念模型:冷涡型、深槽型、浅槽型、锋区平直型;进一步分析了长春市冰雪冻害天气的物理量场、要素场的特征。     

THE ‘NEW IMPLICIT METHOD’ FOR TUNNEL ANALYSIS

Tunnel excavation is a coupled three-dimensional problem dealing with two different structures: lining and rockmass. For a simple application it is useful to develop simplified methods by treating the problem as plane strain. If the problem of tunnel face advance presents an axisymmetric geometry, then we show that the major parameter governing the ground–interface–lining interaction is the convergence of the tunnel U₀ at the moment of the lining installation. The ‘New Implicit Method’ (NIM) presented in this paper makes use of principles similar to those of the ‘convergence–confinement’ method, but it provides a better appreciation of the coupled behaviour of rockmass and lining. For independent time constitutive laws (elasticity and plasticity), we point out that the convergence U₀ depends not only on the mechanical behaviour of the rockmass and on the distance from the tunnel face, as predicted by the ‘convergence–confinement’ method, but also on the stiffness of the lining previously set. We present the ‘NIM’ for elastic and perfect elastoplastic rockmasses without dilatancy for many criteria. The development of this new method is based on the results of tunnel calculations with an axisymmetric FEM numerical model that takes into account the three-dimensional aspect of the problem. Using this method is simple and its results agree well with the FEM numerical results. Its accuracy is highly satisfactory for a geotechnical study.     

应用核磁共振成像(NMRI)技术研究复合剂驱油特征

本文应用核磁共振成像技术,在均值、非均值模型中研究了复合剂驱油动态实验过程。观察及分析了复合剂驱油特征和效果,对复合剂驱油段塞前缘进行了实时跟踪,得到了复合剂驱油段塞前缘油墙的形成及剩余油分布与运移的二维图像,给出了复合剂驱油后,剩余油的饱和度分布曲线。实验表明:在层状非均值地层中,若渗透率差异大,复合剂段塞主要进入高渗层,而波及不到低渗层,即复合剂波及效率低。若渗透率差异小,复合剂段塞大部分进入高渗层,有少部分进入低渗层,即复合剂波及效率较高。     

GE VCT-高图像质量和低剂量的和谐

在本文中讨论了实现图像质量和X射线剂量的和谐和同一的重要性,介绍了GELightSpeedVCT在硬件,软件和临床应用上降低病人剂量的方法。VCT在实现各向同性高分辨率的同时努力提高X射线的有效利用率,降低病人剂量,真正实现了高图像质量和低剂量的和谐。     

医用PET系统技术概述

PET(正电子发射成像)是当今高层次的核医学技术。它综合了核技术、核电子学、计算机、数据处理等领域中的尖端技术,是当前医学界最先进的大型医疗诊断成像设备之一,在肿瘤、心血管疾病和神经系统疾病的临床诊断中发挥着越来越重要的作用。本文以国产32环高档临床PET为例,较详细地介绍了PET设备的工作原理、总体基本结构及各子系统基本功能,对PET整机性能及其临床应用也做了简述。     

热带西太平洋海温距平与Rossby波传播对1993和1994年东亚夏季风异常影响的差异

利用NCEP/NCAR再分析资料、Hadley中心海温资料与降水资料,分析了1993和1994年东亚夏季风异常的天气气候特征以及大气环流的差异.分析结果表明: 1993年东亚夏季风弱,副热带西风急流和副热带高压位置偏南,来自于孟加拉湾和南海的水汽仅输送到35°N以南地区.东亚地区出现低温凉夏天气.1994年东亚夏季风强,副热带西风急流和副热带高压位置偏北,7～8月副高持续偏强并控制日本,水汽可以输送到45°N以北的较高纬度,东亚发生破纪录的热浪干旱.对1993和1994年东亚夏季风异常物理过程差异的研究发现,副热带西风急流中静止Rossby波的传播和热带西太平洋暖池海温距平激发出来的PJ型遥相关波列作用的叠加引起1994和1993年东亚夏季风异常差异.     

基于MultiGen Creator/Vega的虚拟图书馆设计研究

以虚拟图书馆为研究对象,利用MuhiGen Creator和Vega进行建模和系统设计。本文论述了在图书馆模型建立过程中层次结构模型、细节层次结构、实例技术和纹理贴图等技术的实现,以及使用Vega及其提供的API函数的系统开发方法。研究证明,采用MuhiGen Creator和Vega将虚拟现实技术与数字图书馆结合的方案可行．并具有较大的开发空间。     

Chromium(VI) reduction by sulphur(IV) in aqueous solutions

The rates of the reduction of Cr(VI) with S(IV) were measured in deaerated NaCl solution as a function of pH, temperature and ionic strength. The rates of the reaction were found to be first order with respect to Cr(VI) and second order with respect to S(IV), in agreement with previous results obtained at concentrations two order higher than the present study. The reaction also showed a first-order dependence of the rates on the concentration of the proton and a small influence of temperature with an apparent energy of activation ΔH_app of 22.8 ± 3.4 kJ/mol. The rates were independent of ionic strength from 0.01 to 1 M. The rate of Cr(VI) reduction is described by the general expression

−d[Cr(VI)]/dt=k[Cr(VI)][S(IV)]²