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1.
震级-频度关系的修改及其对部分地震区带的应用   总被引:1,自引:1,他引:1       下载免费PDF全文
在本文中作者根据对实际资料的计算,提出将传统的震级-频度关系修改成logN=b_1+b_2M+b_3M~2的形式。用该公式对我国部分地震区带的地震资料进行了计算,结果表明,修改后的震级-频度关系的拟合精度显著提高,其残差比原关系式缩小。用修改后的公式可方便地求得地震区带的震级上限,只要有足够时间长度的观测资料,所求得的震级上限是比较合理的。  相似文献   

2.
从理论上推导了修正的古登堡-里克特模型的震级上限的确定方法, 应用常用的两种模型对我国分区域进行了震级-频度关系的修正和震级极限值的确定. 结果表明, 我国大陆存在非线性的震级-频度关系, 传统的NGR模型不能反映非线性的震级-频度关系, 而MGR模型能反映适合非线性和线性的震级-频度关系, 因此MGR模型适合我国各研究区中强以上地震的震级-频度关系. 当震级 频度关系为非线性时, 用MGR模型确定的震级极限值较准确.   相似文献   

3.
本文利用两种常用的NGR和MGR模型,对我国大陆地区1970年以来各地震带的震级-频度关系和震级上限进行了修定.结果表明,MGR模型能很好地描述非线性的震级-频度关系,因此该模型更适合于我国大陆地区各地震带ML3.0以上地震的震级-频度关系,用MGR方法拟合确定震级上限时,样本量越高拟合的结果越准确.  相似文献   

4.
最大熵原理与地震频度-震级关系   总被引:1,自引:0,他引:1       下载免费PDF全文
冯利华 《地震地质》2003,25(2):260-265
地震是一种随机事件 ,它的发生具有极大的不确定性 ,因而可以用熵来进行描述。地震以最无序的方式在各地发生 ,意味着地震熵达到了极大值。古登堡 (Gutenberg)和里克特 (Richter)根据资料和经验得出的地震频度 -震级关系式实际上是在给定的约束条件下 ,当地震熵取极大值时得到的一种负指数分布。文中从最大熵原理得出了同一形式的地震频度 -震级关系 ,使它的来源从理论上得到了解释  相似文献   

5.
震级频度关系的Gutenburg-Richter公式近年来受到了挑战,一些学者在不同条件下都发现了b值的非线性表现。本文利用自己装配的实验系统对围压下岩石破裂声发射活动的震级频度关系和时间序列特征进行了研究。实验表明AE事件的震级频度关系在某个中强震级K′之前基本符合b值规律,其b值的大小与破裂方式有关。在摩擦滑动中AE序列具有低b值的特征。从K′起震级频度关系出现明显的非线性现象。根据非线性表现的不同,可将其分为第一型和第二型两类。在AE序列中,也存在着“特征震级”的现象  相似文献   

6.
关于震级频度关系的一些讨论   总被引:1,自引:1,他引:1  
讨论了地震活动的复杂性特征与震级频度的关系.认为一般情况下地震活动系统具有多重分形特征.文中利用多重分形的观点讨论了震级频度关系的形式,分析了震级频度关系出现非线性的可能的原因.作为示例,文中概要地讨论了新西兰近年来的地震活动bq谱.   相似文献   

7.
本文介绍了表示地震的震级频度分布与古登堡-里克特关系式偏离的一种量度。以前曾认为震级频度分布遵从古登堡-里克特关系式,然而,实际分布常常与这一关系式偏离相当大。令ni,N,M0和b分别是震级为Mi-Mi+ΔM的事件数目、震极的下限以及古登堡-里克特关系式的b值。  相似文献   

8.
具有独立过程的地震序列震级——频度分布   总被引:5,自引:2,他引:5       下载免费PDF全文
孙文福  顾浩鼎 《地震学报》1992,14(3):273-280
在先前向地震学家研究震级-频度关系的基础上,我们通过12个具有独立过程的地震序列,详细研究了它们实际的震级-频度分布.注意到低震级的频度分布特征决非因地震仪漏记所致.12个地震序列归-化后的震级-频度分布是类似的.作为初级近似,它们十分接近对数正态分布.对于这些序列,G-R 关系只在分段的震级范围内成立,并不能在整个震级范围内满足.同时,我们也讨论了在计算 b 值时诸如合理选择下限震级这样一些需注意的问题.   相似文献   

9.
在前人研究震级—频度关系的基础上,我们分别通过十个具有独立过程和十个非独立过程的地震序列,详细研究了它们实际的震级一频度分布.由十个独立过程的地震序列震级—频度分布证明,低震级端的频度分布特征决非因地震仪漏记所致.无论是独立过程或是非独立过程的地震序列归一化后的震级频度分布是类似的.作为初级近似,它们十分接近对数正态分布.对于这些序列,G-R关系只在特征震级右侧除掉高震级拖尾段后的范围内成立,并不能在整个震级范围内满足.同时,我们也讨论了在计算b值时诸如合理选择下限震级这样一些需注意的问题.  相似文献   

10.
根据截断的G-R模型计算东北地震区震级上限   总被引:2,自引:0,他引:2       下载免费PDF全文
震级上限是指一个地区可能发生地震的最大震级,其概率意义为发生超过该震级地震的概率几乎为0.在有些地区,由于对其内部的地震构造研究和认识存有局限性,很难根据构造或者地质学的原则来确定震级上限.因此,根据数学模型,采用统计手段,使用地震活动性资料来计算震级上限的估计值是一种可行的方法.本文根据截断的G-R关系模型,采用最大似然计算方法,使用东北地震区的地震目录,计算了东北地震区震级上限,结果表明东北地震区的震级上限应为Mu=7.5左右.计算中我们考虑了不同震级的转换、震级误差的修正以及计算方法的影响.最终结果表明,不论采用何种方案进行计算,东北地震区的震级上限值均始终保持在7.5左右,这说明我们采用本文中方法计算得到的东北地震区的震级上限值是合理可信的,同时也说明在以往的研究中对东北地震区震级上限的估计大都是偏小的.  相似文献   

11.
The relationship between frequency and magnitude in homogeneous series of earthquakes is studied. The linear relation of Gutenberg and Richter between the logarithm of frequency and the magnitude is found to be applicable only in a restricted range of magnitudes.The plots of the cumulative number of earthquakes versus magnitude for 20 different series (the total number of events in a single series ranging from about 50 to more than 3000) clearly indicate the presence of vertical asymptotes. This fact suggests that upper and lower limits could exist for the magnitude of a single event, i.e. for the energy that can be released in an earthquake. From the position of the vertical asymptotes it is possible to obtain the upper and lower bounds of magnitude for each series of earthquakes. The empirical shape of the cumulative number-magnitude distribution can be well represented by equilateral hyperbolas. A least 2 method has been used to obtain the best-fitting hyperbolas and corresponding the minimum and maximum magnitudes for each series.The shape of the frequency-magnitude relationship is discussed in lesser detail. It is found, however, that after suitable rescaling the earthquakes in each series follow much the same law, with a comparatively small scatter.  相似文献   

12.
速度型记录设备的地震速报,一般直接使用记录到的波形数据计算震级(速度震级).编写台网观测报告,需要把速度波形仿真成位移后再计算震级(仿真震级).本文利用北京市地震台网2003年以来1 000多条记录,以全网、单台两种方式研究了上述两种震级的关系,结果表明.它们之间存在很好的线性关系,且与震中距、台基、设备等因素有关.建议在速报阶段,可用震级差和线性关系两种方法对仿真震级进行估计.  相似文献   

13.
Prediction of magnitude of the largest potentially induced seismic event   总被引:1,自引:0,他引:1  
We propose a method for determining the possible magnitude of a potentially largest induced seismic event derived from the Gutenberg–Richter law and an estimate of total released seismic moment. We emphasize that the presented relationship is valid for induced (not triggered) seismicity, as the total seismic moment of triggered seismicity is not bound by the injection. The ratio of the moment released by the largest event and weaker events is determined by the constants a and b of the Gutenberg–Richter law. We show that for a total released seismic moment, it is possible to estimate number of events greater than a given magnitude. We determine the formula for the moment magnitude of a probable largest seismic event with one occurrence within the recurrence interval (given by one volumetric change caused by mining or injecting). Finally, we compare theoretical and measured values of the moment magnitudes of the largest induced seismic events for selected geothermal and hydraulic fracturing projects.  相似文献   

14.
In the framework of a joint project of theItalian Gruppo Nazionale per la Difesadai Terremoti (GNDT) and the IstitutoNazionale di Geofisica (ING), devoted tothe reorganization of the Italianearthquake instrumental database from 1981to 1996, we approached the problem of thehomogeneous determination of localmagnitude in Italy. As a first step, webuilt a database of real Wood-Andersonamplitudes deduced from the available dataof the two instruments that were inoperation in Italy up to 1989 as well as ofsimulated Wood Anderson amplitudes computedby Very Broad Band recordings, availablesince 1990. The simultaneous computation ofthe attenuation function together with themagnitudes and the station residuals allowsus to verify that, for the Italian area,this function does not significantly differfrom the original one given by Richter. Inthe second step, the so obtained Mlmagnitudes are used as a reference data setto estimate a new empirical relation forthe duration magnitude Md using the unifiedphases database of the Italian NationalSeismic Network (RSNC) of ING and of themost important local seismic networksoperating in Italy. The same data set wasalso employed to calibrate magnitude Mabased on amplitudes coming from shortperiod vertical seismograms recorded by theRSNC automatic acquisition system. At lasta set of reasonable criteria to choose themost reliable among Ml, Md and Ma has beenformulated. The resulting set of magnitudesproved to be definitely better calibratedthan the one obtained by procedures in useat RSNC.  相似文献   

15.
Tinti  S.  Mulargia  F. 《Pure and Applied Geophysics》1985,123(2):199-220
The apparent magnitude of an earthquakey is defined as the observed magnitude value and differs from the true magnitudem because of the experimental noisen. Iff(m) is the density distribution of the magnitudem, and ifg(n) is the density distribution of the errorn, then the density distribution ofy is simply computed by convolvingf andg, i.e.h(y)=f*g.If the distinction betweeny andm is not realized, any statistical analysis based on the frequency-magnitude relation of the earthquake is bound to produce questionable results. In this paper we investigate the impact of the apparent magnitude idea on the statistical methods that study the earthquake distribution by taking into account only the largest (or extremal) earthquakes. We use two approaches: the Gumbel method based on Gumbel theory (Gumbel, 1958), and the Poisson method introduced byEpstein andLomnitz (1966). Both methods are concerned with the asymptotic properties of the magnitude distributions. Therefore, we study and compare the asymptotic behaviour of the distributionsh(y) andf(m) under suitable hypotheses on the nature of the experimental noise. We investigate in detail two dinstinct cases: first, the two-side limited symmetrical noise, i.e. the noise that is bound to assume values inside a limited region, and second, the normal noise, i.e. the noise that is distributed according to a normal symmetric distribution.We further show that disregarding the noise generally leads to biased results and that, in the framework of the apparent magnitude, the Poisson approach preserves its usefulness, while the Gumbel method gives rise to a curious paradox.  相似文献   

16.
ResearchoncharacteristicsofmagnitudestructureofearthquakesequencesPEI-QINGSUN(孙佩卿)QIN-ZULI(李钦祖)YING-HUADAI(戴英华)JUNZHAO(赵军)Se...  相似文献   

17.
CumulativefrequencybvaluewithoutupperboundmagnitudeanditsregressiondeterminationJian-WenSHEN(沈建文)(SeismologicalBureauofAnhuiP...  相似文献   

18.
在地震震级国家标准《地震震级的规定》(GB17740—2017)发布以后,收集整理鹤岗地震台2018年1月—2020年3月测定的远震面波震级M_(S(HEG)),与中国地震台网中心地震目录中给定的面波震级M_(S(CENC))进行比较,统计二者偏差值。利用统计学方法,分析震级偏差与震级、震中距和反方位角的关系。结果表明:与中国地震台网中心地震目录发布震级相比,鹤岗地震台测定的面波震级偏高,且震级偏差与震中距表现为正相关性;震中位于鹤岗地震台站西北方位,震级偏差较小,而在其他方位,震级偏差则较大。  相似文献   

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