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本文对 1 999年 1月至 2 0 0 0年 1 2月福建数字地震台网测定的台湾地区ML≥ 5 .0级地震 (9.2 1地震序列取ML≥ 5 .5级地震 )测定了Ms震级 ,并将福建台网测定的ML、Ms震级与中国地震局分析预报中心测定的大震速报Ms震级进行了比较。 相似文献
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76 3长周期地震仪 1 997年起取代基式仪 ,承担我国一类合网对国内外地震的监测和对外观测资料交换任务。本文介绍了我台 76 3长周期地震仪的震相记录特征 ,有利于台站对震相的分析 ,提高对外资料交换和大震速报水平。 相似文献
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目前,人们对辅助数据与数字图象分析的复合普遍关注。其中,一个重要的辅助数据类型是数字高程模型(简称DEMs),以及由此派生的数据集合。然而,在现行图象分析系统中要求使用这些数据的软件却不多见。 这篇文章概述了DEMs在遥感数据数字分析中的作用,阐述了遥感应用中使用和处理DEMs的运算软件包(PRODEM)。这个软件包的一个重要特性是它包含了数据操作和格式转换模型。并允许直接同图象分析系统接口。 相似文献
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秦岭——大别造山带与江南造山带的差异隆升过程:来自江汉盆地中新生代沉积记录的证据 总被引:2,自引:6,他引:2
江汉叠合盆地地处扬子地区中部,夹持于秦岭——大别造山带与江南造山带中段之间,是中生代中期以来在扬子浅海台地基础上发育起来的典型海陆交互相-陆相叠合盆地,其中充填了厚逾10000m的中三叠世-新近纪陆源碎屑岩系。据印支期以来的造山活动历程与成盆演化特点,将盆山耦合过程划分为造山前期、主造山期、造山后期与非造山期4个阶段,将盆地充填层序划分为陆架边缘、前陆、断陷和坳陷4个(盆地世代)超层序。依据盆内沉积物碎屑组份分析,发现中三叠世江南造山带进入强造山活动期,白垩纪末进入造山带坍塌后的活动平静期;秦岭——大别造山带的主造山活动阶段为晚三叠-早侏罗世,古近纪末处于非造山活动相对平静阶段。盆区整体呈现东部造山活动早,山带隆升早,持续时间长,剥露地层较快较早进入变质岩层段;西部造山活动时间晚,隆升时间相对较晚,剥露地层在早侏罗世初期才依次切入变质岩层段;盆地南、北缘山带总体呈现多幕式差异隆升过程。 相似文献
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本文对 1 998年至 2 0 0 2年福建数字台网中心测定的台湾南投地震、台湾花莲地震、福建本省部分地震的观测结果永春台震级与台网平均震级进行分析。并计算出永春台的台基校正值 相似文献
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井下钻探结果和地震资料表明四川盆地北部上二叠统长兴组生物礁发育,通过对典型井长兴组岩性与电性资料的分析,明确了生物礁的岩性与储层发育特征。根据井下生物礁及围岩岩性与电性资料并结合过井地震剖面反射波的几何特征,建立台地边缘生物礁的地震正演数值模型,通过对比生物礁模型地震正演记录与实际生物礁地震剖面,建立针对研究区台地边缘生物礁的地震响应特征模式。依据生物礁的地震响应特征对该地区连片二、三维地震测线开展地震相分析,通过已有钻井地震相与沉积相对应关系分析,指出了长兴组生物礁在该地区的分布规律。四川北部地区地震相与沉积相带具有良好的对应关系,存在环台棚-海盆相的台地前缘斜坡-台地边缘生物礁相-开阔台地相沉积体系,地震剖面上生物礁的外部形态呈丘状或透镜状,内部为杂乱反射特征;礁盖白云岩具有亮点反射特征,生物礁底界面出现上凸或者下凹反射现象,生物礁的上部地层具有披覆反射结构,四川盆地北部地区长兴组台地边缘生物礁相在台棚-海盆相东、西两侧沿北西向呈条带状展布,分布面积大于2000km~2,生物礁气藏勘探潜力巨大。 相似文献
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Social vulnerability and seismic risk perception. Case study: the historic center of the Bucharest Municipality/Romania 总被引:1,自引:2,他引:1
Iuliana Armaş 《Natural Hazards》2008,47(3):397-410
Social vulnerability is as much a part of risk as building damage, hazard magnitude, and economic loss. Social vulnerability refers to the capacity of a human community exposed during the impact of a natural hazard event (in this case, an earthquake)
to resist, cope with, and recover from that impact. In the perspective of the 3rd millennium, we come to understand that the
most efficient and accessible way to reduce the pressure of natural risks is to reduce the vulnerability level of the human
communities exposed to that certain hazard. This study aims to test, in an exposed and vulnerable area, the relationship between
social vulnerability and the perception of the seismic risk. The research focuses only on the first level of social vulnerability,
defined as the ability of an individual within a household to recover from a natural hazard impact (Dwyer et al. 2004). A prevailing assumption was that social vulnerability influences the level of perception of the seismic risk, in an exposed, vulnerable area. To this end, two samples were used, different under the aspect of social vulnerability, in the context of the same residential
area. Social vulnerability was computed as a normalized composed index that includes the poverty ratio and the demographic
vulnerability ratio (depending on the age, gender, and education level indicators). The statistical processing has indicated
a significant difference in the high perception level for the two samples that were compared, in the sense that in the context
of an increased level of social vulnerability, people generally better acknowledge the seismic risk.
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Iuliana ArmaşEmail: |
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K. Kuroda T. Irifune T. Inoue N. Nishiyama M. Miyashita K. Funakoshi W. Utsumi 《Physics and Chemistry of Minerals》2000,27(8):523-532
Determination of the phase boundary between ilmenite and perovskite structures in MgSiO3 has been made at pressures between 18 and 24 GPa and temperatures up to 2000 °C by in situ X-ray diffraction measurements
using synchrotron radiation and quench experiments. It was difficult to precisely define the phase boundary by the present
in situ X-ray observations, because the grain growth of ilmenite hindered the estimation of relative abundances of these phases.
Moreover, the slow reaction kinetics between these two phases made it difficult to determine the phase boundary by changing
pressure and temperature conditions during in situ X-ray diffraction measurements. Nevertheless, the phase boundary was well
constrained by quench method with a pressure calibration based on the spinel-postspinel boundary of Mg2SiO4 determined by in situ X-ray experiments. This yielded the ilmenite-perovskite phase boundary of P (GPa) = 25.0 (±0.2) – 0.003
T (°C) for a temperature range of 1200–1800 °C, which is generally consistent with the results of the present in situ X-ray
diffraction measurements within the uncertainty of ∼±0.5 GPa. The phase boundary thus determined between ilmenite and perovskite
phases in MgSiO3 is slightly (∼0.5 GPa) lower than that of the spinel-postspinel transformation in Mg2SiO4.
Received: 19 May 1999 / Accepted: 21 March 2000 相似文献