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序号发震时间地震位置月日时分秒北纬东经地点震级(ML)深度(km)精度1110161859.542°01′122°49′辽宁省新民3.212Ⅰ2122203158.548°10′130°34′黑龙江省罗北3.210Ⅱ3123074112.937°41′119°38′渤海3.6Ⅱ4124202243.751°49′122°56′黑龙江省大兴安岭呼中5.18Ⅱ5126110105.639°22′122°13′辽宁省普兰店3.211Ⅰ6128140731.739°40′123°45′北黄海3.2Ⅱ729183204.640°41′122°41′辽宁省海城3.09Ⅰ8223161241.147°41′124°42′黑龙江省富裕4.24Ⅰ932065156.251°32′123°04′黑龙江省大兴安岭呼中3.07Ⅱ东北地区2005年第… 相似文献
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The earthquakes(ML≥3·0)catalogue of Second quarter in northeastern area,2005序号发震时间地震位置月日时分秒北纬东经地点震级(ML)深度(km)精度1 4 4 20 18 29·1 42°02′123°10′辽宁新民3·1 7Ⅰ2 4 15 14 34 11·6 41°50′128°03′吉林抚松4Ⅰ3 5 5 10 11 16·0 39°05′121°28′金州湾3·3Ⅱ4 5 27 01 18 24·6 40°38′122°52′辽宁海城3·3 13Ⅰ5 6 25 11 13 47·0 47°40′130°32′黑龙江萝北3·2 5Ⅱ6 6 27 19 18 23·8 39°14′122°15′里长山海峡3Ⅱ东北地区2005年第二季度M_L≥3·0地震目录@梁灿
@温岩
… 相似文献
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The earthquakes(ML≥3.0)catalogue of fouth quarter in northeastern area,2006.序号发震时间地震位置震级(ML)深度(km)精度月日时分秒北纬东经地点1 11 2 06 54 54.5 44°42′124°16′吉林乾安3.6Ⅰ2 11 7 11 55 25.6 37°54′120°16′渤海3Ⅱ5 11 25 23 28 53.7 47°28′122°40′黑龙江龙江3 5Ⅱ6 12 16 09 58 02.4 37°53′123°14′黄海4Ⅱ3 11 8 23 09 18.4 44°38′124°01′吉林前郭3.2Ⅰ4 11 11 22 11 05.6 41°49′127°59′吉林抚松3.2Ⅱ东北地区2006年第四季度M_L≥3.0地震目录@梁灿
@张洪艳
@郝永梅~~… 相似文献
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序号 发 震 时 间地 震 位 置月日时 分 秒北 纬东 经地 点震级(ML)深度(km) 精度1 42 0 2 0 70 0 0 45°1 9′ 1 2 4°5 5′吉林省松原 3 0Ⅰ2 441 85 0 2 9 63 9°43′ 1 2 1°46′辽宁省瓦房店 3 0 1 1Ⅱ3 491 0 2 40 6 7 3 8°3 8′ 1 2 0°3 6′渤海 3 2Ⅱ45 71 93 41 1 1 3 7°43′ 1 2 1°5 3′渤海 3 3Ⅱ5 5 82 2 0 40 0 0 45°1 8′ 1 2 4°3 5′吉林省松原 3 0Ⅰ65 90 0 460 0 0 45°1 4′ 1 2 4°41′吉林省松原 3 5Ⅰ75 3 0 0 60 42 6 1 40°3 1′ 1 2 3°0 4′辽宁省岫岩 3 0 1 0Ⅰ861 41 83 3 43 6… 相似文献
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The earthquakes(ML≥3.0)catalogue of first quarter in northeastern area,2007序号月日发震时时间分秒北纬东地震经位置地点震(M级L)深(km度)1 2 10 14 33 09.7 40°43′122°35′辽宁大石桥3.2 114 3 22 20 28 13.8 45°14′131°10′黑龙江鸡东4.4 42 3 1 14 24 33.9 38°49′120°09′渤海3.1资料来源辽宁省地震局黑龙江省地震局辽宁省地震局精度ⅠⅡⅢ3 3 11 04 44 46.5 38°55′120°01′渤海3.8Ⅱ辽宁省地震局东北地区2007年第一季度M_L≥3.0地震目录@梁灿
@张洪艳
@江锦华~~… 相似文献
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Theearthquakes (ML≥ 3 0 )catalogueoffirstquarterinnortheasternarea ,2 0 0 3序号发 震 时 间地 震 位 置月日时 分 秒北 纬东 经地 点震级(ML)深度(km)精度11914 -3 9-19 63 7°48′ 12 4°49′黄海 3 6Ⅱ2 1916-3 3 -16 63 7°41′ 12 4°2 8′黄海 4 2Ⅱ3 114 19-2 9-0 8 746°3 9′ 13 2°3 6′黑龙江省宝清 3 0Ⅰ42 2 13 -4 7-0 2 3 40°3 8′ 12 2°3 7′辽宁省海城 3 113Ⅰ5 2 5 11-3 2 -11 942°3 7′ 12 5°3 9′吉林省东丰 3 0 3 3Ⅰ62 14 15 -4 2 -3 7 2 3 7°3 9′ 12 4°3 4′黄海 3 4Ⅱ72 2 … 相似文献
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Theearthquakes (ML≥ 3 0 )catalogueofFouthquarterinnortheasternarea ,2 0 0 2序号发 震 时 间地 震 位 置月日时 分 秒北 纬东 经地 点震级(ML)深度(km)精度110 90 9-3 8-3 4 0 48°48′ 13 0°2 9′黑龙江嘉荫 3 9822 10 12 13 -5 1-4 7 7 3 9°2 3′ 12 2°13′辽宁省普兰店 3 0 1113 10 2 5 0 5 -12 -0 5 5 40°3 6′ 12 2°5 2′辽宁省海城 3 6814 10 2 5 18-3 4-2 5 83 8°3 3′ 12 0°15′渤海 3 7 25 112 19-2 2 -3 2 5 3 8°2 2′ 12 0°2 6′黄海 3 5 26112 5 12 -2 0 -5 0 93 8°5 6′ 12 1… 相似文献
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Theearthquakes (ML≥3 0 )catalogueofFouthquarterinnortheasternarea ,2 0 0 3序号发震时间地 震 位 置月日时 分 秒北纬东经地 点震级(ML)深度(km) 精度1 1 0 92 3 5 3 3 5 5 41°3 6′1 2 5°40′吉林省通化市3 9Ⅰ2 1 0 1 0 2 1 3 42 9 941°3 6′1 2 5°45′吉林省通化市3 7Ⅰ3 1 0 1 3 1 71 1 5 9 2 3 6°5 8′1 2 6°0 5′黄海4 0Ⅱ41 0 1 61 2 441 1 3 41°3 5′1 2 0°2 5′辽宁省朝阳市3 2 1 1Ⅰ5 1 0 2 5 1 90 2 42 841°5 4′1 2 8°1 5′吉林省长白山3 0Ⅰ东北地区2003年第四季度M_L≥3.0地震目录$辽宁数字… 相似文献
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Shao-Xie Xu 《地震学报(英文版)》1993,6(2):517-533
The method of prediction of earthquake by using seismisity (MPES) is to make use of the message of earthquakes (including
large, middle, small) in pre-period to predict large earthquake in post-period. Some better methods are presented in this
paper which are selected among many means used in our country recent years. These methods are classified into six sets: 1.
Method of spatial pattern; 2. Method of time process; 3. Method of seismic sequence; 4. Method of earthquake correlation;
5. Method of parameters of seismic source and medium; 6. Comprehensive method. Prediction effects of each method are evaluated
with unique score. The value of each method, scoreR, are generally in a range between 0.3 and 0.6. This value only represents internal consistency, however, the ability of actual
prediction belongs to the extensional effect, which is generally lower than the value of internal consistency. If the ability
of actual prediction could be evaluated withR = 0.3, the ability of prediction of earthquake by seismicity will be stated as following: If most of earthquakes must be
predicted, the warning time needs to take seventy percent of whole time period of prediction; If half earthquakes must be
predicted, the warning time needs to take twenty percent of whole time period of prediction.
The Chinese version of this paper appeared in the Chinese edition ofActa Seismologica Sinica,15, 239–252, 1993. 相似文献
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1993年地震学期刊发文统计及引文分析 总被引:1,自引:0,他引:1
笔者统计了全国地震系统1993年度9种期刊发文量,对9种期刊的论文引文做了初步分析,内容包括;发表论文分布、引文数量、引文语种、引文类型、被引作者,论文多年产作者、引文年代及论文专题分类。 相似文献
14.
高速铁路路基动土压力测试信号的小波分析 总被引:3,自引:0,他引:3
阐述了小波分析的基本原理与方法,选用Daubechies小波对某高速铁路路基土压力的现场振动测试信号进行分析处理。由此对高速列车荷载作用下,路基动土压力产生的机理及其土压力的构成进行较深入的研究。 相似文献
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A.T. Silva 《水文科学杂志》2013,58(5):942-955
Abstract The method of fragments is applied to the generation of synthetic monthly streamflow series using streamflow data from 34 gauging stations in mainland Portugal. A generation model based on the random sampling of the log-Pearson Type III distribution was applied to each sample to generate 1200 synthetic series of annual streamflow with an equal length to that of the sample. The synthetic annual streamflow series were then disaggregated into monthly streamflows using the method of fragments, by three approaches that differed in terms of the establishment of classes and the selection of fragments. The results of the application of such approaches were compared in terms of the capacity of the method to preserve the main monthly statistical parameters of the historical samples. Editor D. Koutsoyiannis; Associate editor C. Onof Citation Silva, A.T. and Portela, M.M., 2012. Disaggregation modelling of monthly streamflows using a new approach of the method of fragments. Hydrological Sciences Journal, 57 (5), 942–955. 相似文献
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首都减灾圈,系首都减轻自然灾害预测防治圈。1991年12月20—21日在北京召开了《首都圈自然灾害及其减灾对策研讨会》。本文根据这次会议所提供的材料,在从整体上实现减灾的思想指导下,就首都减灾圈的“成灾背景”、“首都减灾圈的组成”、“首都减灾圈的灾害预测与防治状况”、“首都减灾圈的灾害关联性分析”、“首都减灾圈的减灾实效预估”和“首都减灾圈的减灾对策与实施”等六个带有共同性的问题,进行了讨论。供制定首都圈减灾方案时参考。 相似文献
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M. J. Manton 《Pure and Applied Geophysics》1977,115(3):547-559
Summary The motion of an aerosol can be described by a general force balance equation, independent of the detailed structure of the flow, provided that the interaction between the external flow field and the local flow induced by the aerosol is weak. A necessary and sufficient condition for the interaction to be weak is that the length scale of the aerosol is much less than that of the external flow. High and low Reynolds number regimes can be distinguished for the motion of an aerosol relative to the external flow. In some extreme conditions the equation of motion reduces to an algebraic equation for the aerosol velocity.After submission of this article the author was made aware of a similar treatment published inTopics of Appl. Phys., 12 (Turbulence, Chapter 7), Springer Verlag, Berlin, which at the time of the article's submission had not yet appeared in Australia. (Ed.) 相似文献
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