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1.
收集、整理四川省地震台网2013年5月至2017年9月产出的震相观测报告数据,采用单台多震和达法,重点分析2017年8月8日九寨沟MS 7.0强震前龙门山断裂带中北段地区波速比变化特征。结果表明：龙门山断裂带中段西侧的茂县地震台,在发震前2年左右,波速比出现一次持续时间约一年半的下降异常;发震前半年左右,波速比出现明显回返特征,波速比回返至均值上下时即发生九寨沟MS 7.0地震;震源区周边其他6个地震台波速比在发震前变化较平稳。茂县地震台波速比低值异常对判定九寨沟MS 7.0强震前龙门山断裂带中北段可能存在孕震体具有重要参考价值。 相似文献
2.
P. Mandal Jainendra S. Joshi Sudesh Kumar Rajendra Bhunia B. K. Rastogi 《Pure and Applied Geophysics》2004,161(8):1635-1654
On 26 January, 2001 (03:46:55,UT) a devastating intraplate earthquake of Mw 7.7 occurred in a region about 5 km NW of Bhachau, Gujarat (23.42°N, 70.23°E). The epicentral distribution of aftershocks defines a marked concentration along an E-W trending and southerly dipping (45°) zone covering an area of (60 × 40) km2. The presence of high seismicity including two earthquakes of magnitudes exceeding 7.7 in the 200 years is presumed to have caused a higher level of shallow crustal heterogeneity in the Kutch area; a site lying in the seismic zone V (zone of the highest seismicity for potentially M8 earthquakes) on the seismic zoning map of India. Attenuation property of the medium around the epicentral area of the Bhuj earthquake covering a circular area of 61,500 km2 with a radius of 140 km is studied by estimating the coda-Qc from 200 local earthquakes of magnitudes varying from 3.0–4.6. The estimated Q0 values at locations in the aftershock zone (high seismicity) are found to be low in comparison to areas at a distance from it. This can be attributed to the fact that seismic waves are highly scattered for paths through the seismically active and fractured zone but they are well behaved outside the aftershock zone. Distribution of Q0 values suggests that the local variation in Q0 values is probably controlled by local geology. The estimated Q0 values at different stations suggest a low value of Q=(102 ± 0.80)*f(0.98 ± 0.02) indicating an attenuative crust beneath the entire region. The frequency-dependent relation indicates a relatively low Qc at lower frequencies (1–3 Hz) that can be attributed to the loss of energy due to scattering attenuation associated with heterogeneities and/or intrinsic attenuation due to fluid movement in the fault zone and fluid-filled cracks. The large Qc at higher frequencies may be related to the propagation of backscattered body waves through deeper parts of the lithosphere where less heterogeneity is expected. Based on the attenuation curve estimated for Q0=102, the ground acceleration at 240 km distance is 13% of 1 g i.e., 0.13 g agreeing well with the ground acceleration recorded by an accelerograph at Ahmedabad (0.11 g). Hence, it is inferred that the Q0 value obtained from this study seems to be apt for prediction of ground motion for the region. 相似文献
3.
In this paper we study the variation of Vp/Vs and Poisson's ratio (δ) in the Yellowstone National Park region, using earthquakes which were well recorded by a local seismic network. We find that the average Vp/Vs value within the geothermally active Yellowstone caldera is about 7% lower than in the area outside the caldera. Within the caldera itself there may be a further 2–7% reduction of Vp/Vs in the hydrothermally active Norris Geyser Basin, the Upper and Lower Geyser Basins, and the Yellowstone Lake and Mud Volcano regions. After considering various possible causes for Vp/Vs changes, such as geologic and structural differences, thermal effects, partial melting, and hydrothermal activity, we conclude that the most plausible explanation for the observed Vp/Vs reduction is the presence of hot-water at temperatures and pore-pressures near the water steam transition in the caldera geothermal reservoirs. 相似文献
4.
A tomographic study of the V
p and V
p/V
s structures in the crust and upper mantle beneath the Taiwan region of China is conducted by simultaneous inversion of P and
S arrival times. Compared with the previous tomographic results, the spherical finite difference technique is suitable for
the strong heterogeneous velocity structure, and may improve the accuracy in the travel time and three-dimensional ray tracing
calculations. The V
p and V
p/V
s structures derived from joint inversion and the relocated earthquakes can provide better constraints for analyzing the lateral
heterogeneity and deep tectonic characters in the crust and upper mantle. Our tomographic results reveal significant relations
between the seismic wavespeed structure and the tectonic characters. In the shallow depth, sedimentary basins and orogen show
distinct wavespeed anomalies, with low V
p, high V
p/V
s in basins and high V
p, low V
p/V
s in orogen. As the suture zone of Eurasian Plate and Philippine Sea Plate, Longitudinal Valley is characterized by a significant
high V
p/V
s anomaly extending to the middle-lower crust and upper mantle, which reflects the impact of rock cracking, partial melting,
and the presence of fluids. In the northeast Taiwan, the V
p, V
p/V
s anomalies and relocated earthquakes depict the subducting Philippine Sea Plate under the Eurasian Plate. The high V
p of oceanic plate and the low V
p, high V
p/V
s atop the subducted oceanic plate extend to 80 km depth. Along the east-west profiles, the thickness of crust reaches 60 km
at the east of Central Range with eastward dipping trend, which reveals the eastward subduction of the thickened and deformed
crust of the Eurasian continental plate.
Supported by Knowledge Innovation Program of the Chinese Academy of Sciences (Grant No. KZCX3-SW-234-2), National Basic Research
Program of China (Grant No. 2007CB411701), National High Technology Research and Development Program of China (Grant No. 2006AA09A101-0201)
and National Natural Science Foundation of China (Grant Nos. 40804016, 40704013) 相似文献
5.
Shanxi Graben is in the middle part of the North China Craton, from south to north. With the teleseismic data recorded by Regional Seismograph Networks and the temporary ZBnet-W Seismic Array around east part of Shanxi Graben, we measured the crustal thickness and vP/vS ratio beneath each station using the H-κ stack of receiver functions. The observed crustal thickness shows obvious lateral variation, increasing gradually from east to west in the Shanxi Graben. Beneath the Shanxi Graben the crust is relatively thicker than both sides of the south and the north. In addition, the vP/vS ratio in the north of study zone is higher than that in the south. The highest vP/vS ratio exists in the crust of the Xinding basin and the Datong basin. Our study also suggests that high velocity ratio might result from the strong activities of the magmation and volcanism. 相似文献
6.
7.
Ultrasonic compressional wave velocity Vp and quality factor Qp have been measured in alkali basalt, olivine basalt and basic andesite melts in the frequency range of 3.4–22 MHz and in the temperature range of 1100–1400°C. Velocity and attenuation of the melts depend on frequency and temperature, showing that there are relaxation mechanisms in the melts. Complex moduli are calculated from the ultrasonic data. The results fit well a complex modulus of Arrhenius temperature dependence with log-normal Gaussian distribution in relaxation times of attenuation. The analysis yields average relaxation time, its activation energy, relaxed modulus, unrelaxed modulus and width of Gaussian distribution in relaxation times. Relaxed modulus is smaller (17.5 GPa) for basic andesite melt of high silica and high alumina contents than for the other two basalt melts (18.1–18.4 GPa). The most probable relaxation times decrease from ～ 3 × 10?10 s for basic andesite to ～ 10?11 s for alkali basalt at 1400°C. Activation energies of attenuation, ranging from 270 to 340 kJ mol?1 in the three melts, are highest in basic andesite. Longitudinal viscosity values and their temperature dependences are also calculated from Vp and Qp data. The volume viscosity values are estimated from the data using the shear viscosity values. Longitudinal, volume and shear viscosities and their activation energies are highest in the basic andesite melt of the most polymerized structure. 相似文献
8.
利用布设于兴蒙造山带诺敏河火山群地区的宽频带流动地震台站资料,基于接收函数方法,获取了该地区的地壳厚度与波速比值.研究结果显示,该地区的地壳厚度介于32~38 km,莫霍面深度在空间上分布特征与五大连池为中心的火山带分布具有较好的一致性：沿着火山带延展方向地壳较薄.该地区的波速比介于1.74~1.84,波速比在空间上与地壳厚度变化具有一致性：高波速比主要集中于靠近五大连池火山带地区,向诺敏河火山和小古里河火山延展.研究认为：诺敏河火山与五大连池火山带可能具有相同的岩浆来源,可能与富钾岩石圈地幔拆沉作用造成的地幔热物质上涌有关.研究区地壳厚度与波速比呈现负相关关系,暗示该地区可能发生过岩浆底侵作用. 相似文献
9.
《Physics of the Earth and Planetary Interiors》1979,18(4):309-318
On November 7, 1976, an earthquake of the strike-slip fault type, and of magnitude 6.7, occurred at two mountainous localities, Yanyuan and Ninglang, in the border region of the Szechuan and Yunnan Provinces, China. One year before the earthquake, a prediction was made as to the magnitude and location of the impending earthquake by the present authors, on the basis of the results of a general survey of an area of about 20,000 km2 for Vp/Vs ratio variations. The prediction of time of occurrence was made afterwards by the combined analysis of results of observations of some other precursory phenomena. The actual occurrence of the event was generally considered as being in agreement with the prediction.The present study may be taken as a new example for the detection of Vp/Vs ratio variations prior to an earthquake of the strike-slip fault type. By considering the difference between the shear rupture and stick-slip motion and the anisotropy induced by dilatancy, a preliminary discussion is made concerning the related results. 相似文献
10.
收集整理了四川省地震台网1990—2012年产出的地震直达波震相数据, 利用单台多震和达法对2008年汶川MS8.0地震前后四川地区的波速比变化特征进行了分析研究(共筛选出13个数据量较为丰富、 连续性较好的台站). 结果显示: 其中位于龙门山断裂中北段西侧的4个台站, 震前出现长达7年左右的中长期波速比低值异常; 其它9个台站的波速比震前变化基本稳定. 震前波速比出现异常的4个台站的分布与汶川MS8.0地震孕震区范围大体一致, 从而为研究汶川MS8.0地震前是否存在地壳介质特性的时间变化过程, 提供了有力的判定依据. 相似文献
11.
Abstract Petrogenetic grids for ultrahigh-pressure (UHP) metamorphism were calculated at different Xco2 conditions in the model system CaO-MgO-SiO2-CO2-H2O involving coesite (Co), diopside (Di), dolomite (Do), enstatite (En), forsterite (Fo), magnesite (Ms), quartz (Qz), talc (Tc), tremolite (Tr) using a published internally consistent thermodynamic data set. Two P-T grids at Xco2= 0.01 and 0.5 are described. In the calculated P-T grid at Xco2= 0.01, four out of 10 stable invariant points, Co-En-Ms-Tc, Co-Di-En-Tc-Tr, Co-Di-Ms-Tc-Tr and Di-En-Ms-Tc-Tr lie within the stability field of coesite. If the fluid phase has Xco2= 0.5, no invariant point is stable under UHP conditions. Some magnesite-bearing assemblages are stabilized by the following three reactions: Di + Ms = Do + Fo + CO2, Ms + Tr = Do + Fo + CO2+ H2O and Ms + Tc = Fo+ CO2+ H2O at Xco2= 0.01 and by reaction Ms + Tc = Fo + CO2+ H2O together with these three at Xco2= 0.5. Ten possible UHP assemblages for mafic and ultramafic compositions at very low Xco2 conditions include the following: Co-Do-Ms, Co-Di-Ms, Co-Di-Tc, Di-Ms-Tc, Di-En-Tc-, Di-En-Ms, Co-Di-En, Di-En-Fo, Di-Fo-Ms, Di-Do-Fo. Among them, talc-bearing assemblages are restricted to Xco2 < 0.02 and their high-P limit is 31.7 kb (749°C) at Xco2= 0.01. Dolomite-magnesite-silica assemblages have large P-T stability fields even if Xco2 is as low as 0.1, and could occur in cold subduction zones with very low geothermal gradients. Reported UHP coesite-dolomite assemblage is restricted only to a calc-silicate rock interlayered with marble where Xco2 is relatively higher; no such assemblage appears for mafic and ultramafic rocks with low Xco2 evidenced by the occurrence of diopside (or omphacite) at the expense of dolomite + coesite. The effect of Xco2 on the stability of coesite-dolomite-magnesite, diopside-enstatite-magnesite, diopside-talc assemblages is examined and the occurrence of coesite-dolomite, magnesite-bearing and talc-bearing assemblages in the Dabie UHP rocks are interpreted by employing the calculated P-T grids. 相似文献
12.
Lin-Gun Liu 《Earth and Planetary Science Letters》1975,26(3):425-433
Two synthetic end-members and two natural solid solutions of the system Mg3Al2Si3O12-Fe3Al2Si3O12 have been found to display successive phase transformations at increasingly high pressures when they were compressed in a diamond-anvil cell and heated with a YAG laser to temperatures of approximately 1400–1800°C. X-ray diffraction studies of the quenched samples show that the iron-rich garnets apparently first transform to a garnet-related high-pressure phase, then disproportionate into a mixture of magnesiowüstite plus an unknown phase(s). The latter phase(s) may further transform to a still denser unknown phase(s). The ultimate high-pressure phase may be a perovskite-like structure as was previously found for the magnesium-rich garnets. One of the unknown phases may be the high-pressure phase of Al2O3 · nSiO2 compounds. Magnesium-rich garnets display similar phase transformations as do the iron-rich garnets with the exception of the garnet-related high-pressure phase. These results disagree with a previous interpretation for the high-pressure phase of iron-silicate garnets recovered in shock-wave experiments reported by Ahrens and Graham (1972). 相似文献
13.
Data from 753 earthquakes are used to determine a relationship between surface-wave magnitude (M
s) and bodywave magnitude (m
b), and from 541 earthquakes to determine a relationship between surface-wave magnitude (M
s) and local magnitude (M
L) for China and vicinity: M
s=0.9883 m
b-0.0420, M
s=0.9919 M
L-0.1773. The relationship of M
s
versus m
b is obtained for 292 events occurred in the Chinese mainland in the time period from 1964 to 1996, 291 events occurred in
Taiwan in the time period from 1964 to 1995 and 170 events occurred in the surrounding area. Standard deviation of the fitting
is 0.445. Relationship of M
s
versus M
L is obtained for 36 events occurred in the Chinese mainland, 293 events occurred in Taiwan, China and 212 events occurred
in the surrounding area. The total amount is 541 events. Standard deviation of the fitting is 0.4673.
The uncertainties of the converted M
s in different magnitude intervals can be estimated using complementary cumulative distribution function (CCDF). In the relationship
of M
s
versus m
b, taking ±0.25 as a range of uncertainties, in magnitude interval m
b 4.0–4.9, the probabilities for the converted M
s taken value less than (M
s-0.25) and more than (M
s+0.25) are 17% and 27% respectively. Similarly, we have probabilities for m
b 5.0–5.9 are 34% and 20% and that for m
b 6.0–6.9 are 11% and 47%.
In the relationship of M
s
versus M
L, if the range of uncertainties is still taken as ±0.25, the corresponding probabilities for magnitude interval M
L 4.0–4.9 are 22% and 38%, for M
L 5.0–5.9 are 20% and 15% and for magnitude interval M
L 6.0–6.9, are 15% and 29%, respectively.
The relationships developed in this paper can be used for the conversion of one magnitude scale into another magnitude scales
conveniently. The estimation of uncertainties described in this paper is more accurate and more objective than the usual estimation
expressed by deviation. The estimations described in this paper indicate various dispersions in different magnitude intervals
of original data. The estimations of uncertainties described by probabilities can be well connected with the total estimations
of uncertainties in seismic hazard assessment. 相似文献
14.
Pyroxene-garnet solid-solution equilibria have been studied in the pressure range 41–200 kbar and over the temperature range 850–1,450°C for the system Mg4Si4O12Mg3Al2Si3O12, and in the pressure range 30–105 kbar and over the temperature range 1,000–1,300°C for the system Fe4Si4O12Fe3Al2Si3O12. At 1,000°C, the solid solubility of enstatite (MgSiO3) in pyrope (Mg3Al2Si3O12) increases gradually to 140 kbar and then increases suddenly in the pressure range 140–175 kbar, resulting in the formation of a homogeneous garnet with composition Mg3(Al0.8Mg0.6Si0.6)Si3O12. In the MgSiO3-rich field, the three-phase assemblage of β- or γ-Mg2SiO4, stishovite and a garnet solid solution is stable at pressures above 175 kbar at 1,000°C. The system Fe4Si4O12Fe3Al2Si3O12 shows a similar trend of high-pressure transformations: the maximum solubility of ferrosilite (FeSiO3) in almandine (Fe3Al2Si3O12) forming a homogeneous garnet solid solution is 40 mol% at 93 kbar and 1,000°C.If a pyrolite mantle is assumed, from the present results, the following transformation scheme is suggested for the pyroxene-garnet assemblage in the mantle. Pyroxenes begin to react with the already present pyrope-rich garnet at depths around 150 km. Although the pyroxene-garnet transformation is spread over more than 400 km in depth, the most effective transition to a complex garnet solid solution takes place at depths between 450 and 540 km. The complex garnet solid solution is expected to be stable at depths between 540 and 590 km. At greater depths, it will decompose to a mixture of modified spinel or spinel, stishovite and garnet solid solutions with smaller amounts of a pyroxene component in solution. 相似文献
15.
Bian Yin-ju 《地震学报(英文版)》2005,18(4):441-450
We try to give a quantitative and global discrimination function by studying m
b/M
S data using Fisher method that is a kind of pattern recognition methods. The reliability of the function is also analyzed.
The results show that this criterion works well and has a global feature, which can be used as first-level filtering criterions
in event identification. The quantitative and linear discrimination function makes it possible to identify events automatically
and achieve the goal to react the events quickly and effectively.
Contribution No.05FE3018, Institute of Geophysics, China Earthquake Administrtion. 相似文献
16.
17.
210Pb/226Ra and 210Po/210Pb disequilibria in seawater and suspended particulate matter 总被引：1，自引：0，他引：1
The distribution of210Po and210Po in dissolved (<0.4 μm) and particulate (>0.4 μm) phases has been measured at ten stations in the tropical and eastern North Atlantic and at two stations in the Pacific. Both radionuclides occur principally in the dissolved phase. Unsupported210Pb activities, maintained by flux from the atmosphere, are present in the surface mixed layer and penetrate into the thermocline to depths of about 500 m. Dissolved210Po is ordinarily present in the mixed layer at less than equilibrium concentrations, suggesting rapid biological removal of this nuclide. Particulate matter is enriched in210Po, with210Po/210Pb activity ratios greater than 1.0, similar to those reported for phytoplankton. Box-model calculations yield a 2.5-year residence time for210Pb and a 0.6-year residence time for210Po in the mixed layer. These residence times are considerably longer than the time calculated for turnover of particles in the mixed layer (about 0.1 year). At depths of 100–300 m,210Po maxima occur and unsupported210Po is frequently present. Calculations indicate that at least 50% of the210Po removed from the mixed layer is recycled within the thermocline. Similar calculations for210Pb suggest much lower recycling efficiencies.Comparison of the210Pb distribution with the reported distribution of226Ra at nearby GEOSECS stations has confirmed the widespread existence of a210Pb/226Ra disequilibrium in the deep sea. Vertical profiles of particulate210Pb were used to test the hypothesis that210Pb is removed from deep water by in-situ scavenging. With the exception of one profile taken near the Mid-Atlantic Ridge, significant vertical gradients in particulate210Pb concentration were not observed, and it is necessary to invoke exceptionally high particle sinking velocities to account for the inferred210Pb flux. It is proposed instead that an additional sink for210Pb in the deep sea must be sought. Estimates of the dissolved210Pb/226Ra activity ratio at depths greater than 1000 m range from 0.2 to 0.8 and reveal a systematic increase, in both vertical and horizontal directions, with increasing distance from the sea floor. This observation implies rapid scavenging of210Pb at the sediment-water interface and is consistent with a horizontal eddy diffusivity of 3?6 × 107 cm2/sec. The more reactive element Po, on the other hand, shows evidence of rapid in-situ scavenging. In filtered seawater,210Po is deficient, on the average, by ca. 10% relative to210Pb; a corresponding enrichment is found in the particulate phase. Total inventories of210Pb and210Po over the entire water column, however, show no significant departure from secular equilibrium. 相似文献
18.
基于首都圈数字地震台网的宽频带资料,首先采用CAP方法确定了永清MS4.3地震和廊坊MS3.0地震的震源机制解:永清地震节面Ⅰ的走向、倾角和滑动角分别为52°,62°和?140°,节面Ⅱ的走向、倾角和滑动角分别为300°,55°和?35°;廊坊地震节面I的走向、倾角和滑动角分别为48°,57°和?147°,节面Ⅱ的走向、倾角和滑动角分别为299°,63°和?38°。两次地震的震源机制解较为一致,推测它们可能具有相同的发震断层。利用近震转换波获得两次地震的震源深度,分别为19 km和13 km。利用双差法对两次地震的主余震进行重新定位,结果显示:两个地震序列的震中均呈NE向分布,余震震源深度均浅于主震震源深度,震源深度分别集中在17—20 km和12—13 km范围内,两个序列的短轴剖面揭示了震源分布均呈现倾向SE,倾角陡立的特点。将地震序列的分布与震源机制解的结果进行对比,认为两个序列的水平展布方向与其对应的主震震源机制解中节面Ⅰ的走向比较接近,深度分布的高倾角特征也与节面Ⅰ比较相似,因此认为发震断层面均为节面Ⅰ。通过将震源机制解中节面Ⅰ的参数和地震序列的分布与区域活动断层的产状性质进行比较,取得了一些关于发震构造和地震成因的重要认识:① 永清MS4.3地震和廊坊MS3.0地震的发震构造不是上地壳的先存正断裂?河西务断裂,不排除与中下地壳的新生构造或深大断裂有关;② 永清、廊坊地震发生在13—19 km深度上,结合地壳结构、断裂构造以及区域流变结构等资料,推测该深度范围可能是廊固凹陷的壳内脆性?韧性转换区域,是地震孕育和发生的有利构造部位。 相似文献
19.
铜绿微囊藻和四尾栅藻光合利用碳酸氢盐探讨 总被引：2，自引：0，他引：2
为了探讨羹类光合过程对碳酸氧盐的利用,研究不同pH值下铜绿微囊藻和四尾栅藻的净光合速率,并着重研究这两株藻的碳酸氢盐摄取速率.结果表明,从弱酸性到弱碱性,四尾栅藻的净光合速率都比铜绿微囊藻高.由pH值超过pH转折点后的无机碳摄取速率计算得到的碳酸氢盐摄取速率对铜绿微囊藻和四尾栅藻分别为142.14和314.08μmo1DIC/(g·h,FW),故这两株藻都可利用碳酸氢盐作为碳源进行光合,且均为强碳酸氧盐利用者;但是,四尾栅藻对碳酸氲盐的利用能力强于铜绿微囊藻.另外,与四尾栅藻相比,铜绿微囊藻的碳酸氧盐摄取速率更易受抑制剂的抑制. 相似文献
20.
动态追踪了云南地区第4 强震活跃期6 .3 级以上强震前波速比异常图像,显示出明显的南北差异:滇西南的1988 年11 月6 日澜沧- 耿马7 .6 、7 . 2 级和1993 年1 月27 日普洱6 .3 级强震发生在低波速比异常区内; 中缅边境上的1992 年4 月23 日6 .7 、6 .8 级和1995 年7 月12 日孟连西7 .2 级强震发生在低波速比异常区边缘;而滇西北的1996 年2 月3 日丽江7 .0 级、1976 年11 月7 日、12 月14 日宁蒗6 .7 、6 .4 级和滇东的1995 年10 月24 日武定6 .5 级强震却都发生在高波速比异常区内.强震前近震震级 ML 与持续时间震级 MD 的震级差的南北差异也进一步证实了波速比异常的差别. 相似文献