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煤矿矿震应力窗口效应 总被引：5，自引：0，他引：5
对煤矿矿震活动特征,震源机制解,与天然地震的相关性以及特殊的环境条件等进行了研究,认为煤矿矿震的孕育和发生受控于区域应力场,具有区域应力变化的灵敏窗口效应,可视为探索天然地震前兆和区域应力场变化的应力窗口。 相似文献
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对京西门头沟的近１０万条矿震记录,进行了整理和研究,结果表明,矿山地震具有天然地震的特征,并与近邻区域的较大天然地震存在一定的关系,特别是对１９８９年１０月１８日山西大同－－阳高６．１级地震及１９９８年１月１０日河北张北６．２级地震有较好的前兆反映,认为,该矿之矿震可作为地震活动中尺度监测的一种方法及监视区域应力场变化的一个天然“窗口”, 相似文献
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矿震及其深井水位的异常响应车服务态度 总被引：1，自引：0，他引：1
简要介绍了山东省陶庄煤矿的二次矿震及其井水位的同震效应与震前异常。结果表明，矿震活动与天然地震活动在时间上有同步性，并且二次矿震的井水位同震效应形态与震前异常持续时间有差异，而这种差异主要同震源体的破坏特征有关。 相似文献
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矿震识别及成因研究进展 总被引：2，自引：0，他引：2
矿震主要受开采活动、矿山所处构造环境及区域构造应力场的影响。本文首先回顾了矿震的识别研究进展,然后从矿震震源机制、矿震与构造关系、矿震与瓦斯溢出、矿震与开采进程关系、矿震成因力学机制理论与实验研究等角度对矿震的成因研究进行了阐述,最后给出矿震识别及成因研究的进一步建议。矿震成因研究深化了对天然地震的认识。在研究矿震发生机理时,必须针对具体条件进行深入讨论与分析,应更多采用有关数学和力学手段,结合具体的生产地质条件和科学实验研究,有针对性地开展研究工作。可利用层析成像技术详细了解矿震演变过程,深化对地壳介质在应力作用下发生破裂或位错过程的认识,进而对矿震发震成因进行深入研究。 相似文献
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用小波包识别地震和矿震 总被引：6，自引：0，他引：6
在能检测到天然地震和矿震的区域，这两类地震的快速识别无论对于区域台网和矿区台网都具有现实意义。这两类震动都是非稳态信号，用传统的Fourier变换不能提取出信号的特征信息，小波包分析方法却能很好提取出信号的特征信息。本文提供了一种基于非参数识别算法，即把信号变换到频域，然后再用奇异值分解作为统计工具，提取出信号的特征信息，作为识别天然地震和矿震的识别因子。以辽宁抚顺2001年1月1日到2003年6月30的18个矿震和16个天然地震，以及北京门头沟2001年1月1日到2002年12月31日的15个矿震和14个天然地震为样本，提取出识别因子。最后，用其它的天然地震和矿震资料检验了识别因子的识别率。 相似文献
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非火山震颤是在远离火山地区观测到的一种具有较长持续时间,没有明显体波到时的地震波信号,与振幅相似的小震相比,非火山震颤的高频成分几乎没有。非火山震颤常在环太平洋俯冲带以及转换断层的板块交界面被探测到,并且有些非火山震颤伴随着慢地震,还能被远震面波诱发,但对于诱发非火山震颤所必需的环境尚不明确。中国是地震频发的国家,具有东南沿海俯冲带以及多个大断层构造环境,这就给国内非火山震颤的研究提供了非常充分的研究环境。本文对非火山震颤的研究历史进行了梳理,并综述其定义、识别、定位、成因以及研究现状。 相似文献
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在中国地震台网的宽频数字地震计和倾斜、重力仪的观测中,记录到来自西太平洋热带气旋（热带风暴、台风）引起的震颤波.通过对2006年来自西太平洋的全部热带气旋的分析,以及所观测到的震颤波与气旋运动过程中强度的变化、运动路径、观测点与其之间的距离变化等方面的分析研究得到以下结论：震颤信号的持续时间与热带气旋的生命过程基本相符,其中出现强震颤的时间大多为2～3天,特征为信号的包络线呈纺锤状叠加在观测背景上,震颤波的主要频率范围为0.13～0.33 Hz（周期：3～7 s）.我国内陆大部分区域内的宽频地震计、重力仪、倾斜仪等都能清晰记录到这类由热带气旋引起的震颤波.震颤波的强度主要与热带气旋的强度、运动路径以及气旋中心到地震观测台站的距离这几个因素直接相关;而震颤波的变化过程与热带气旋的运动和变化过程密切相关,其中强震颤波的出现时间与气旋过大陆板块边界进入大陆架的时间一致.经对热带气旋的结构、运动规律及动力学特点的了解分析,初步分析认为其主要源于热带气旋运动过程中与浅海区大陆架及陆地表面的摩擦、气压载荷变化以及由此产生的海浪对地壳板块的冲击,及板块边界断层对气旋扰动的响应.此外,我们对北印度洋孟加拉湾生成并在缅甸登陆的热带气旋也进行了实例分析.结果表明：与西太平洋相比,北印度洋热带气旋引起的震颤波对我国大陆的地震观测而言信号较弱. 相似文献
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在地震与固体潮台站的日常监测中,常发现有一些异常"脉动"信号叠加在固体潮曲线上.这些异常"脉动"与宽频带数字地震计的观测在时间上同步、一致,其中的一部分由发生在西太平洋上的热带气旋引起,而其他的则大多与强地震相伴随,统称为震颤异常波.本文介绍了华中科技大学的地震与固体潮观测台站(HUST)的概况,报道了该台应用 DZW重力仪和VS-1倾斜仪观测记录到的大量震颤异常波事例.大量观测事实表明:中国固体潮台站记录的震颤异常波,绝大多数只在DZW重力仪和VS-1倾斜仪的低通滤波1 通道(LP1)出现,而在其低通滤波2通道(LP2)和其他固体潮仪器中则罕有发现;震颤异常波的包络线大多呈"纺锤状"或"尾巴状",持续时间多为1~3天. 通过对震颤异常波和固体潮观测仪器的分析研究,得到以下结论:震颤异常波实际上就是一种来源复杂的地球脉动信号,响应范围广泛,可被宽频带数字地震计和固体潮仪器记录.由西太平洋上的热带气旋引起的震颤异常波的主要周期在3~7 s范围,而强震前的震颤异常波则除此外,还包含10~60 s及更长周期的信号.固体潮仪器对震颤异常波响应的差异是因为仪器的传递函数不同和特性所致. DZW重力仪和VS-1倾斜仪分钟值采样数据中的震颤异常波,只是真实信号的一种"混叠"或映射.强震前的震颤异常波是否与地震有关？是否是震兆？尚需做更深入细致的分析和研究. 相似文献
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Mt. Veniaminof, Alaska Peninsula, is a stratovolcano with a summit ice-filled caldera containing a small intracaldera cone
and active vent. From January 2 to February 21, 2005, Mt. Veniaminof erupted. The eruption was characterized by numerous small
ash emissions (VEI 0 to 1) and accompanied by low-frequency earthquake activity and volcanic tremor. We have performed spectral
analyses of the seismic signals in order to characterize them and to constrain their source. Continuous tremor has durations
of minutes to hours with dominant energy in the band 0.5–4.0 Hz, and spectra characterized by narrow peaks either irregularly
(non-harmonic tremor) or regularly spaced (harmonic tremor). The spectra of non-harmonic tremor resemble those of low-frequency
events recorded simultaneously with surface ash explosions, suggesting that the source mechanisms might be similar or related.
We propose that non-harmonic tremor at Mt. Veniaminof results from the coalescence of gas bubbles while low-frequency events
are related to the disruption of large gas pockets within the conduit. Harmonic tremor, characterized by regular and quasi-sinusoidal
waveforms, has duration of hours. Spectra containing up to five harmonics suggest the presence of a resonating source volume
that vibrates in a longitudinal acoustic mode. An interesting feature of harmonic tremor is that frequency is observed to
change over time; spectral lines move towards higher or lower values while the harmonic nature of the spectra is maintained.
Factors controlling the variable characteristics of harmonic tremor include changes in acoustic velocity at the source and
variations of the effective size of the resonator. 相似文献
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Stephen R. McNutt 《Pure and Applied Geophysics》1987,125(6):1051-1077
In thirteen years (1973–1986) of seismic monitoring of Pavlof Volcano, 488 episodes of volcanic tremor have been recorded, only 26 of which have been previously described in the literature. This paper tabulates and describes all the tremor episodes and reports on the results of all analyses to date. Pavlof tremor durations range from 2 minutes to greater than 1 week; episodes accompanying magmatic eruptions have durations greater than 1 hour, and sustained amplitudes of greater than 6 mmP-P (=54 nanometers at 1.5 Hz) on station PVV, 8.5 km from the vent. Digital data provide much better amplitude resolution than helicorders do. Helicorders, however, provide continuous coverage, whereas digital data are intermittent. Correlations of tremor with visual eruption observations shows that tremor amplitudes are roughly correlated with heights of lava fountains, but the correlation of tremor amplitudes with plume heights is more problematic. Fast Fourier Transform (FFT) spectra show that Pavlof tremor is quite statinary for the entire time period, 1973–1983. All principal spectral peaks lie between 0.8 and 3.0 Hz, and may be caused by resonance of magma and gas, and resonance of the volcanic pile. Preliminary analysis of 2-and 3-component data shows thatP, S, PL, and Rayleigh waves may be present in Pavlof volcanic tremor. Other waveforms can be misidentified as tremor, most commonly those caused by storms orS-waves of regional earthquakes. A strategy is proposed to distinguish tremor from noise using automatic seismic data acquisition and analysis systems. Pavlof's volcanic tremor is briefly compared with a preliminary sample of over 1100 cases of tremor from 84 volcanoes worldwide. Finally, several recommendations for monitoring and reporting volcanic tremor are discussed. 相似文献
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R. R. Dibble 《Bulletin of Volcanology》1966,29(1):761-762
Volcanic vibrations from Ruapehu volcano which is situated in the centre of the North Island of New Zealand have been recorded on high magnification slow motion tape seismographs and drum seismographs at the Chateau Volcanological Observatory since December, 1960. In 1964, volcanic microtremor with a dominant frequency of 2 c/s commenced late in March, and reached a peak seismic power level of 100 KW for short periods in May. During the maximum phase, the tremor completely ceased for up to 20 minutes, and recommenced with an explosion or burst of strong tremor. The sequence and timing were very similar to the sequence of ash discharge-stoppage-explosion-ash discharge observed during the 1945 eruption of Ruapehu. In 1964 it is thought that the eruption of ash clouds was prevented by the Crater Lake, so that visible activity was limited to a few fumaroles, steam rising from the lake, and turbulence in the water. The lake temperature increased from about 25°C (a normal temperature) on 20 March to 50°C on 26 May. The corresponding rates of heat loss from the lake are 200 and 700 MW respectively, and an additional 150 MW or more was required to heat up the lake, giving a total average heat output of 850 MW for about 4 weeks. The corresponding average seismic power was about 3 KW, which is 0.0005 per cent of the thermal power. If this relationship is constant, the peak thermal power over a period of 6 minutes was of the order of 20,000 MW. The explosions initiating the tremor were mostly identical except in amplitude, and their magnitudes ranged up to 2.3, corresponding to 1014 erg. This was slightly greater than the energy conserved during the preceding stoppage of tremor. The dominant tremor frequency was normally 2.2 c/s and sometimes 1.2 c/s. Individual bands of frequency within the spectrum varied in power, but coherent migrations of frequency bands occurred on a few occasions. Near the end of the maximum phase, the entire spectrum migrated downwards by half an octave and the tremor power decreased to zero. Tremor power and frequency increased again, and a violent period of explosions and tremor of changing frequency occurred. Quite frequently the explosions initiating the tremor were multiple, and a few explosions occurred which were followed by tremor lasting only a matter of seconds. Explosions apparently unrelated to tremor were very rare and minor. The explosions were located by temporary installation of portable slow motion tape recorders around the volcano. The epicentre is very close to Crater Lake, but the depth cannot be determined from the data. Graphs of tremor power against time covering the active period from April to September, and graphs of cumulative energy against time, and frequency spectrum against time, for explosions and tremor are presented, and slow motion tape recordings will be played many times faster than the recording speed so that the tremor and explosion vibrations can be heard as audible noises. 相似文献
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Volcanic tremor at the Hekla volcano is directly related to eruptive activity. It starts simultaneously with the eruptions and dies down at the end of them. No tremor at Hekla has been observed during non-eruptive times. The 1991 Hekla eruption began on 17 January, after a short warning time. Local seismograph stations recorded small premonitory earthquakes from 16:30 GMT on. At 17:02 GMT, low-frequency volcanic tremor became visible on the seismograph records, marking the onset of the eruption. The initial plinian phase of the eruption was short-lived. During the first day several fissures were active but, by the second day, the activity was already limited to a segment of one principal fissure. The eruption lasted almost 53 days. At the end of it, during the early hours of 11 March, volcanic tremor disappeared under the detection threshold and was followed by a swarm of small earthquakes. At the start of the eruption, the tremor amplitude rose rapidly and reached a maximum in only 10 min. The tremor was most vigorous during the first hour and started to decline sharply during the next hour, and later on more gently. During the eruption as a whole, the tremor had a continuous declining trend, with occasional increases lasting up to about 2 days. Spectral analysis of the tremor during the first 7 h of the eruption shows that it settled quickly, within a couple of minutes, to its characteristic frequency band, 0.5–1.5 Hz. The spectrum had typically one dominant peak at 0.7–0.9 Hz, and a few subdominant peaks. Hekla tremor likely has a shallow source. Particle motion plots suggest that it contains a significant component of surface waves. The tremor started first when the connection of the magma conduit with the atmosphere was reached, suggesting that degassing may contribute to its generation. 相似文献
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2001年11月14日的昆仑山Ms8.1级地震前几天,中国地震台网多个台站都观测到了持续数天的低频震颤波信号.由于这些震颤波发生在强震前,所以备受关注.多年来研究人员对该震颤波的产生原因进行过多方探讨,但没有定论.该震颤波信号是否源自强震区的慢地震?是否是地震前兆?或为其它因素?为了回答这些问题,我们从多方面分析和研究了昆仑山强震前中国大陆宽频地震仪所观测的震颤波信号的特征、持续时间、震颤波强度变化与大规模大气运动的关系、信号强度随观测空间的衰减变化特征.结果表明:中国大陆宽频地震仪在昆仑山强震前观测到的震颤波由两个信号组成,其中11月10日开始出现,主要频率范围0.15~0.22 Hz (周期约4~7 s)、持续时间在10-13日的震颤波,主要由同时间段内发生在西太平洋的强台风玲玲(Ling Ling)引发;而11月11日开始出现,主要频率范围0.1~0.13 Hz (周期7~10 s)、持续时间在11-12日的震颤波,不是来自昆仑山强震区的慢地震,而是由来自欧洲北部及欧亚大陆的强温带气旋引发. 相似文献
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E.J. Delahaye J. Townend M.E. Reyners G. Rogers 《Earth and Planetary Science Letters》2009,277(1-2):21-28
Geodetically-detected episodes of slow slip appear in several subduction zones to be accompanied by bursts of low-frequency coherent noise known as seismic tremor, but whether a single physical process governs this association or even whether slow slip is invariably accompanied by tremor remains unresolved. Detailed analysis of broadband seismic data spanning a slow slip episode in the Hikurangi subduction zone, New Zealand, reveals that slow slip was accompanied by distinct reverse-faulting microearthquakes, rather than tremor. The timing, location, and faulting style of these earthquakes are consistent with stress triggering down-dip of the slow slip patch, either on the subduction interface or just below it. These results indicate that tremor is not ubiquitous during subduction zone slow slip, and that slow slip in subduction zone environments is capable of triggering high-frequency earthquakes near the base of the locked subduction thrust. In this and other locations (Hawaii, Boso Peninsula) where slow slip is accompanied by triggered microseismicity, the estimated upper extent of the slow slip is shallower (less than ~ 20 km) than in those locations from which tremor has been reported. This suggests that ambient temperature- or pressure-dependent factors govern the character of the seismic response to slow slip on subduction thrusts and other large faults, with rheological or lithological conditions at shallow depths triggering high-frequency microearthquakes and those at greater depths triggering seismic tremor. 相似文献
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Harmonic tremor is widely studied and modelled in a very narrow frequency band (1–5 Hz) which represents the eigenfrequencies of a resonator assumed as the source of the phenomenon. Minimal effort was dedicated towards understanding its behaviour in larger temporal scales. Here we characterise the dynamic behaviour of volcanic tremor while evaluating the complete spectrum of the generalised dimension of the phase space. The starting time series constitutes the tremor amplitude picked every 10 minutes. The choice of this lag time is made on the basis of a qualitative analysis of the properties of the tremor. The results show intermittent behaviour of the dynamics which requires an 8-dimensional map to be completely described. An interesting result is that the maximum clustering of point density in phase space occurs in a monodimensional space which implies a periodicity sometimes observed experimentally. An appropriate predictive model needs more constraints on the nature of the eight variables involved in the process. 相似文献