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1.
V. E. Levin V. F. Bakhtiarov V. M. Pavlov N. N. Titkov S. S. Serovetnikov 《Journal of Volcanology and Seismology》2010,4(3):193-202
This paper presents results from an analysis of GPS observations made by the Kamchatka regional GPS network (KAMNET) in relation
to the Olyutorskii earthquake and plate interaction. The coseismic changes were interpreted for the Olyutorskii earthquake
and its largest aftershock (May 22, 2006, M
W
= 6.6) within the framework of a dislocation source in an elastic half-space. 相似文献
2.
对湖北省阳新县网湖所采得的862尾似刺鳊鮈的年龄与生长的研究表明,其年轮特征主要为切割型和碎裂型。其体长与鳞径呈直线相关:L=5.6784+4.3056R;体长与体重呈幂函数的增长关系:W=2.8026×10~(-2)L~(2.8754)。应用Van Bertalanffy生长方程拟合该鱼的一般生长规律,其生长参数为:L_∞=25.0143cm,W_∞=277.8876g,K=0.4668,t_0=-1.3886,拐点年龄t_i=1龄,拐点体长L_i=16.42cm,拐点体重W_i=82.82g。 相似文献
3.
Summary The integral mean values of gravity on the surface W=W
0
, obtained from satellite observations with the use of harmonic coefficients[3, 7] and from terrestrial gravity measurements[12], are compared. The squares and products of the harmonic coefficients were neglected, with the exception of [J
2
(0)
]
2
, which was taken into account. The Potsdam correction and the geocentric constant are being discussed. The paper ties up with[13–15] and the symbols used are the same. The given problem was treated, e.g., in[2, 4, 6, 8–10]; in the present paper the values of gravity are compared directly. 相似文献
4.
5.
The Caribou Lake gabbro, part of the Blachford Lake Intrusive Suite accurately dated at –2186±10 mA, has a predominantNW–/SE+ magnetization with a mean, irrespective of sign, ofD=119°,I=50°, 95=5° and a palaeopole 14°N, 064°W,A
95=5°; it has not proved possible to determine if the magnetization is primary. The Easter Island dyke, less well-dated in the range –2200 to –2500 Ma, has a predominantWNW+ magnetization, whose mean, when corrected for an 8° tilt, isD=288°,I=46°, 95=5 and palaeopole is 32°S, 2°W,A
95=5°; the magnetization is probably primary. A vertical magnetization (D), not significantly different from the present field, occurs sporadically in both units and is considered to be Late Phanerozoic in age. Palaeopoles from the Caribou Lake gabbro and the Easter Island dyke, together with those already known from Early Proterozoic intrusives of the Archaean Slave Structural Province, roughly define a swath (the Slave Track) which maps the motion of the Slave Province relative to the geomagnetic axis during this interval. The corresponding array of palaeopoles (the Superior Track) from the Superior Structural Province does not fall in the same place. Hence it would appear that Slave and Superior were not in their present relative positions in the Early Proterozoic in disagreement with arguments that have been made for a fixed supercontinent during much of the Proterozoic. Mid-Proterozoic paleomagnetic signatures indicate that Slave and Superior had assumed their present relative position by about –1750 mA. These Early Proterozoic relative motions are the earliest for which there is palaeomagnetic evidence.Earth Physics Branch Contribution No. 1111. 相似文献
6.
We study the October 18, M
W = 7.1, 1992 Atrato earthquake, and its foreshocks and aftershocks, which occurred in the Atrato valley, northwestern Colombia. The main shock was preceded by several foreshocksof which the M
W = 6.6, October 17 earthquacke was the largest. Inparticular, we examine foreshocks and aftershocks performing joint-hypocenter relocations using high quality Pn and Sn wave readingsfrom permanent regional networks. We observed a few hours prior to the main shock a sudden increase of foreshocks. Maybe this could be used as a predictor since foreshocks have been known for other major events in the region. Our locations align for 90 km with a trend of 5° ±4° in agreement with the Harvard CMT solution showing the faultplane trending 9° to be the plane of rupture. In relation to theepicenter of the main shock, maximum intensities were located to thesouth, consistent with a rupture that traveled from north to south witha larger energy release in the south as suggested by an empirical Green'sfunction study (Li and Toksöz, 1993; Ammon et al., 1994). The boundarybetween the Panama and North Andes blocks has been placed close to thePanama-Colombia border as either a sharp boundary or a diffuse zone. TheAtrato earthquake, however, shows that the plate boundary between thePanama and North Andes microblocks is a diffuse deformation zone. Thiszone has a width of at least 2° stretching from 78°W to 76°W. Quantification of earthquake moment release (during the past30 years) in this zone shows a similar amount of moment release in thewestern and eastern parts of this zone. 相似文献
7.
Burša Milan Kouba Jan Kumar Muneendra Müller Achim Raděj Karel True Scott A. Vatrt Viliam Vojtíšková Marie 《Studia Geophysica et Geodaetica》1999,43(4):327-337
The geoidal geopotential value of W
0
= 62 636 856.0 ± 0.5m
2
s
–2
, determined from the 1993 –1998 TOPEX/POSEIDON altimeter data, can be used to practically define and realize the World Height System. The W
0
-value can also uniquely define the geoidal surface and is required for a number of applications, including General Relativity in precise time keeping and time definitions. Furthermore, the W
0
-value provides a scale parameter for the Earth that is independent of the tidal reference system. All of the above qualities make the geoidal potential W
0
ideally suited for official adoption as one of the fundamental constants, replacing the currently adopted semi-major axis a of the mean Earth ellipsoid. Vertical shifts of the Local Vertical Datum (LVD) origins can easily be determined with respect to the World Height System (defined by W
0
), in using the recent EGM96 gravity model and ellipsoidal height observations (e.g. GPS) at levelling points. Using this methodology the LVD vertical displacements for the NAVD88 (North American Vertical Datum 88), NAP (Normaal Amsterdams Peil), AMD (Australian Height Datum), KHD (Kronstadt Height Datum), and N60 (Finnish Height Datum) were determined with respect to the proposed World Height System as follows: –55.1 cm, –11.0 cm, +42.4 cm, –11.1 cm and +1.8 cm, respectively. 相似文献
8.
This work deals with the preliminary relationship between strain path and strain partitioning pattern in a sinistral transpressional zone,Lancangjiang shear zone,located to the southeast of Tibet.Various ductile rocks provide an opportunity to investigate quantitative finite strain(Rs),kinematic vorticity values(Wm),and proportions of simple and pure shear components.The mean kinematic vorticity values(Wm) were evaluated based on three methods,such as Rs-θ,prophyroclast hyperbolic distribution method(PHD),a... 相似文献
9.
高邮湖、南四湖和东平湖作为南水北调东线枢纽湖泊,其水质状况对保障调水安全起到关键性作用本文运用三维荧光光谱平行因子分析法(EEMs-PARAFAC)分析了3个湖泊在不同水文情景下有色可溶性有机物(CDOM)吸收、荧光光谱特征以及荧光组分与主要水质参数的相关性,以探究3个湖泊CDOM来源组成特征结果表明,平行因子分析法解析CDOM三维荧光图谱,得到陆源类腐殖质C1、类色氨酸C2和类酪氨酸C3不同水文情景对高邮湖CDOM来源与结构组成影响较明显,丰水期其类腐殖质荧光强度显著大于枯水期(t-test,P0.01),并且与a(254)呈正相关(R~2=0.85,P0.01),表明类腐殖质是CDOM主要部分,该荧光组分贡献率可达50%[F_(max)C1/(F_(max)C1+F_(max)C2+F_(max)C3)×100%],高邮湖受到入湖河流来水的影响较大,丰水期入湖口附近荧光强度明显高于其他水域东平湖和南四湖CDOM来源组成特征相似,丰水期东平湖和南四湖组分C2和C3显著低于枯水期(t-test,P0.01),两湖泊枯水期工农业等人为污染源影响较大相关性分析表明高邮湖中类腐殖质荧光特征在一定程度是能反演DOC浓度,并且类腐殖质的输入会增加湖泊总磷、总氮和叶绿素a浓度而东平湖和南四湖CDOM荧光特征与主要水质参数的相关性较差,这与高邮湖水体存在较大差异. 相似文献
10.
2016年8月24日意大利中部发生MW6.0地震,2个月之后,震中附近相继发生MW5.5、MW5.9、MW6.5地震。研究这几次较大地震间的相互触发作用及机制十分必要,然而在大地震之后传统地震目录通常缺失很多余震事件,缺失的余震事件包含着早期余震时空分布和迁移规律的信息,为完善余震目录本文利用匹配滤波方法对MW6.0地震后80天内的连续数据进行余震检测,得到了数十倍于模板数量的新检测事件,检测事件与模板事件组成的新余震目录完备震级为1.0,提高了地震目录的完备性。依据新余震目录进行余震时空分布研究,结果显示MW6.0、MW5.9、MW6.5地震的早期余震迁移规律不同。MW6.0地震的早期余震沿着断裂走向同时朝两侧迁移;而MW5.9、MW6.5地震的早期余震向南、北迁移表示出不对称的特征。通过拟合余震迁移前端发现,MW6.0、MW5.5地震的早期余震朝着随后较大地震的方向迁移,且较符合lgt的特征,表明余震迁移可能与慢滑动有关。 相似文献
11.
Summary Using the geocentric constant GM=398 601.3 × 10
9
m
3s
–2
, the known value of the angular velocity of the Earth's rotation , Stokes' constants J
n
(k)
and S
n
(k)
upto n=21 (zonal), n=16 (tesseral and sectorial) [2], the geocentric co-ordinates and heights above sea-level of SAO satellite stations [2], the following will be derived: the potential on the geoid Wo, the scale factor for lengths Ro=GM/Wo, the radius-vector of the surface W=Wo, the parameters of the best-fitting Earth tri-axial ellipsoid, and the components of the deflections of the vertical with respect to the geocentric rotational IAG ellipsoid (Lucerne 1967), as well as to the best-fitting geocentric tri-axial ellipsoid. Some of the differences in the structure of the gravity field over the Northern and Southern Hemispheres will be given, and the mean values of gravity over the equatorial zone, determined from the dynamics of satellite orbits, on the one hand, and from terrestrial gravity data, on the other, will be compared.Presented at the Fifteenth IUGG General Assembly, Moscow, July 30 — August 14, 1971. 相似文献
12.
Fault dimensions,displacements and growth 总被引：15，自引：0，他引：15
Juan Watterson 《Pure and Applied Geophysics》1986,124(1-2):365-373
Maximum total displacement (D) is plotted against fault or thrust width(W) for 65 faults, thrusts, and groups of faults from a variety of geological environments. Displacements range from 0.4 m to 40 km and widths from 150 m to 630 km, and there is a near linear relationship betweenD andW
2. The required compatibility strains (e
s) in rocks adjacent to these faults increases linearly withW and with
and ranges frome
s=2×10–4 toe
s=3×10–1. These are permanent ductile strains, which compare with values ofe
s=2×10–5 for the elastic strains imposed during single slip earthquake events, which are characterised by a linear relationship between slip (u) andW.The data are consisten with a simple growth model for faults and thrusts, in which the slip in successive events increases by increments of constant size, and which predicts a relationship between displacement and width of the formD=cW
2. Incorporation of constant ductile strain rate into the model shows that the repreat time for slip events remains constant throughout the life of a fault, while the displacement rate increases with time. An internally consistent model withe
s=2×10–5, giving repeat times of 160 years and instantaneous displacement rates of 0.02 cm/yr, 0.2 cm/yr, and 2.0 cm/yr when total displacement is 1 m, 100 m, and 10 km, and slip increasing by 0.5 mm with each event, gives a good approximation of the data. The model is also applicable to stable sliding, the slip rate varying with ductile strain rate and withW
2. 相似文献
13.
Seismic anisotropy of shales 总被引：3，自引：0，他引：3
C.M. Sayers 《Geophysical Prospecting》2005,53(5):667-676
Shales are a major component of sedimentary basins, and they play a decisive role in fluid flow and seismic‐wave propagation because of their low permeability and anisotropic microstructure. Shale anisotropy needs to be quantified to obtain reliable information on reservoir fluid, lithology and pore pressure from seismic data, and to understand time‐to‐depth conversion errors and non‐hyperbolic moveout. A single anisotropy parameter, Thomsen's δ parameter, is sufficient to explain the difference between the small‐offset normal‐moveout velocity and vertical velocity, and to interpret the small‐offset AVO response. The sign of this parameter is poorly understood, with both positive and negative values having been reported in the literature. δ is sensitive to the compliance of the contact regions between clay particles and to the degree of disorder in the orientation of clay particles. If the ratio of the normal to shear compliance of the contact regions exceeds a critical value, the presence of these regions acts to increase δ, and a change in the sign of δ, from the negative values characteristic of clay minerals to the positive values commonly reported for shales, may occur. Misalignment of the clay particles can also lead to a positive value of δ. For transverse isotropy, the elastic anisotropy parameters can be written in terms of the coefficients W200 and W400 in an expansion of the clay‐particle orientation distribution function in generalized Legendre functions. For a given value of W200, decreasing W400 leads to an increase in δ, while for fixed W400, δ increases with increasing W200. Perfect alignment of clay particles with normals along the symmetry axis corresponds to the maximum values of W200 and W400, given by and . A comparison of the predictions of the theory with laboratory measurements shows that most shales lie in a region of the (W200, W400)‐plane defined by W400/W200≤Wmax400/Wmax200 . 相似文献
14.
大型浅水湖泊与大气之间的动量和水热交换系数——以太湖为例 总被引：5，自引：1，他引：4
湖泊水面与大气之间垂直方向的动量、水汽和热量通量与风速、湿度和温度梯度之间存在比例关系,因此在湖泊水-气相互作用研究中,这比例系数(交换系数)是关键因子.在以往的研究中,交换系数通常直接采用水面梯度观测法或海洋大气近地层的参数化方案进行计算.本文采用涡度相关系统和小气候系统仪器在太湖平台上直接观测的通量和气象要素,对上述交换系数(最小均方差原则)进行优化,结果为:动量交换系数CD10N=1.52×10-3、水汽交换系数CE10N=0.82×10-3、热量交换系数CH10N=1.02×10-3,与其他内陆湖泊涡度相关观测数据的推导结果一致.本文的研究结果表明:与海洋参数化方案相比,在相同的风速条件下,湖面的空气动力学粗糙度比海洋高,这可能是由于受到水深的影响;如果采用海洋参数化方案,会导致湖泊年蒸发量的估算值偏大40%.太湖的动量、水汽和热量交换系数可以视为常数,可以不考虑稳定度和风速的影响.这是因为本文中83%的数据为近中性条件.敏感性分析表明:如果考虑稳定度的影响,LE模拟值的平均误差降低了0.5 W/m2,H的平均误差降低了0.4 W/m2,u*的计算值没有变化;如果考虑风速的影响,u*模拟值的平均误差降低了0.004 m/s,LE的平均误差升高了1.3 W/m2,H的模拟结果几乎不受影响.这一结果能为湖气相互作用研究提供参考. 相似文献
15.
AbstractIn discrete water quality surveys, riverine fluxes are associated with unknown uncertainties (biases and imprecisions). Annual flux errors have been determined from the generation of discrete surveys by Monte Carlo sorting for monthly sampling, from 10 years of daily records (120 records). Eight calculation methods were tested for suspended particulate matter, dissolved solids and dissolved and total nutrients in medium to large basins (103 to 106 km2) covering a wide range of hydrological conditions and riverine biogeochemistry. The performance of each method was analysed first by type of riverine material, which appeared to be much less pertinent than the flux variability matrix. The latter combines the river flow duration in two percent of time (W2%) and the truncated exponent (b50sup) defining the relationship of concentration vs discharge (C–Q) at higher flows (C = aQb50sup). As flux variability increases (high W2% and/or high b50sup), averaging and rating curve methods become less efficient compared to hydrograph separation methods. Flux biases and imprecisions were plotted in the [W2%, b50sup] matrix for discrete monthly surveys.Editor Z. W. KundzewiczCitation Raymond, S., Moatar, F., Meybeck, M., and Bustillo, V., 2013. Choosing methods for estimating dissolved and particulate riverine fluxes from monthly sampling. Hydrological Sciences Journal, 58 (6), 1326–1339. 相似文献
16.
17.
18.
Jennifer L. Lewicki George E. Hilley Laura Dobeck Bruno D. V. Marino 《Bulletin of Volcanology》2012,74(1):135-141
Use of eddy covariance (EC) techniques to map the spatial distribution of diffuse volcanic CO2 fluxes and quantify CO2 emission rate was tested at the Horseshoe Lake tree-kill area on Mammoth Mountain, California, USA. EC measurements of CO2 flux were made during September–October 2010 and ranged from 85 to 1,766 g m−2 day−1. Comparative maps of soil CO2 flux were simulated and CO2 emission rates estimated from three accumulation chamber (AC) CO2 flux surveys. Least-squares inversion of measured eddy covariance CO2 fluxes and corresponding modeled source weight functions recovered 58–77% of the CO2 emission rates estimated based on simulated AC soil CO2 fluxes. Spatial distributions of modeled surface CO2 fluxes based on EC and AC observations showed moderate to good correspondence (R
2 = 0.36 to 0.70). Results provide a framework for automated monitoring of volcanic CO2 emissions over relatively large areas. 相似文献
19.
G. S. Steinberg 《Bulletin of Volcanology》1976,40(2):116-120
The determination of the energy and depth of powerful volcanic explosions using direct geophysical and geological methods is rarely successful. In most of cases investigators have to solve the problem of estimating the energy of an explosion, its depth, the mass and the amount of thrown-out materials from the dimensions of the funnel (crater, maar) and from geological data. Experiments with big throw-out blasts have allowed us to determine the energy and depth of explosions by giving us relations which determine the radius of the explosion funnel as a function of the energy of explosion and of the depth of its center (1) $$R_o = F(E,W)$$ whereR o is the radius of the funnel,E is the energy,W is the depth of the explosion center. The inverse problem — to determineE andW from a knownR o — has an ambiguous solution and it is solved parametrically relative toE andW. In order to obtain an unambiguous solution, some more or less arbitrary conditions must be assumed. When the problem of volcanic explosions is examined from the outer ballistic point of view the following equation is obtained whereR t is the throw-out distance of explosion fragments. (2) $$R_1 = F(E,W)$$ Equations (1) and (2) give us an unambiguous determination of the energy of explosionE and of the depth of the centerW. There is a good correlation between these results and the data from direct geophysical observations. 相似文献
20.
A large earthquake (M
W=7.6) occurred in Jiji (Chi-Chi), Taiwan, China on September 20, 1999, and was followed by many moderate-size shocks in the
following days. Two of the largest aftershocks with the magnitudes of M
W=6.1 and M
W=6.2, respectively, were used as empirical Green’s functions (EGFs) to obtain the source time functions (STFs) of the main
shock from long-period waveform data of the Global Digital Seismograph Network (GDSN) including IRIS, GEOSCOPE and CDSN. For
the M
W=6.1 aftershock of September 22, there were 97 pairs of phases clear enough from 78 recordings of 26 stations; for the M
W=6.2 aftershock of September 25, there were 81 pairs of phases clear enough from 72 recordings of 24 stations. For each station,
2 types of STFs were retrieved, which are called P-STF and S-STF due to being from P and S phases, respectively. Totally,
178 STF individuals were obtained for source-process analysis of the main shock. It was noticed that, in general, STFs from
most of the stations had similarities except that those in special azimuths looked different or odd due to the mechanism difference
between the main shock and the aftershocks; and in detail, the shapes of the STFs varied with azimuth. Both of them reflected
the stability and reliability of the retrieved STFs. The comprehensive analysis of those STFs suggested that this event consisted
of two sub-events, the total duration time was about 26 s, and on the average, the second event was about 7 s later than the
first one, and the moment-rate amplitude of the first event was about 15% larger than that of the second one.
Foundation item: State Natural Science Foundation of China (49904004) and IPGP of France.
Contribution No. 02FE2007, Institute of Geophysics, China Seismological Bureau. 相似文献