The Dibra (Albania) earthquake of November 30, 1967

On November 30, 1967, a strong earthquake of magnitude M = 6.6 struck the Dibra region, eastern Albania, causing considerable loss of human life and grave material damage both in the territory of Albania and that of Yugoslavia.The object of this study is to describe the effects of this earthquake on landscape and buildings, as well as to define its macroseismic field. The study further deals with some features of the aftershocks of M 4.0 distributed in time and space, the aftershock activity and the focal-mechanism solution of the main event.From the study of the macroseismic field of this earthquake and its fault, which extends over 10 km in a 40° northeasterly direction, from the distribution of aftershocks in space and the focal-mechanism solution of this earthquake, the conclusion has been reached that this event is connected with the Vlora—Dibra seismogenic belt.The authors have mentioned the existence of this traverse belt as early as 1969 (Sulstarova and Koçiaj, 1969). The existence of this belt is also shown by the chronological and geographical distribution of some strong earthquakes in Albania in the period 1800–1967 (their macroseismic field and the position of their epicentres), and by the focal-mechanism solutions of some of these earthquakes. The Vlora—Elbasan—Dibra transverse seismogenic belt continues for several hundred kilometres northeast and southwest beyond the territory of Albania.     

The February 11, 2004 Dead Sea earthquake ML = 5.2 in Jordan and its tectonic implication

A moderate-sized (M_w  5.3) earthquake occurred in the Dead Sea basin on February 11, 2004. A rigorous seismological analysis of the main shock and numerous aftershocks suggests that seismogenic structure was a secondary, antithetic fault within the Dead Sea fault system. The main shock is well located using all available regional seismic stations, and 43 aftershocks were precisely located relative to the main shock using a double difference algorithm. The first motion, focal mechanism for this earthquake demonstrates NNW–SSE and ENE–WSW striking nodal planes, and the aftershocks distribution is consistent with the latter — indicating a right-lateral sense of displacement. This orientation and sense of shear are consistent with similarly oriented geological faults around the Dead Sea basin — these structures are likely antithetic faults within the transform system. Although moderate in size, earthquakes that occur very close to the large Dead Sea fault system warrant consideration in the earthquake hazard assessment of the region: For example, owing to the proximity to the main fault, moderate earthquakes such as this may produce static changes in Coulomb stress along the main fault.     

A seismotectonic study of the 1908 Messina earthquake

A major earthquake occurred in the Straits of Messina in Southern Italy on December 28, 1908. The shock became known in literature as the “Messina earthquake”. The present paper deals mainly with a re-interpretation of the source mechanism of this shock using modern interpretation techniques. The following parameters are discussed: Epicentre, hypocentre, origin-time, macroseismic intensity, body and surface wave magnitudes, fault-plane solution, seismic moments derived from body and surface waves, residual displacements and tsunami values.The parameters are compared with the tectonic setting of Southern Italy. As a result of the large magnitude (M = 7) and the 30 km long fault extension of this shock, the Messina earthquake reflects the large scale tectonics of Southern Italy more significantly than any other earthquake from which seismograms exist. The focal mechanism studies show a good agreement between the orientation of the shear-plane of the earthquake and the tectonic features of a fault-line which is known from geological data, the so-called Comiso-Catania-Messina-S. Eufemia fault. The rupture of the shallow earthquake was associated with normal faulting. According to the normal faulting mechanism, the earthquake resulted from tensional forces acting approximately perpendicular to the strike direction of the Straits of Messina.Geodetic measurements which were performed shortly before and after the earthquake indicate an apparent asymmetry in the volumes of uplift and subsidence. It is suggestive that there exists a strong net subsidence of material displaced with the earthquake faulting. The normal faulting mechanism of the Messina earthquake is in tectonic accordance with the uprise of olivine basalt in the volcanism observed at Etna. However, the normal faulting is contrary to the postulation of a subducting oceanic plate giving rise to the Calabrian-Sicilian arc-like feature, as this hypothesis would require mainly a compressional zone in the region of the Straits of Messina.     

鲁甸地震(Ms6.5)临震预测、中期预测及中地壳流变结构

2014年8月3日16时30分, 在云南省昭通市鲁甸县(27.1°N, 103.3°E)发生M_s6.5地震, 震源深度10 km, 死亡617人, 失踪112人, 受伤3 143人, 受灾人口108.84万人.根据月亮赤纬角、太阳黑子极值年等周期变化及两者的叠加效应, 总结出2013—2014年是云南强震高危期, 具备M_s7地震的发生条件.次年, 利用基础SW前兆仪的临震预测指纹法信息, 制定了2014年底211号地震预测表, 预测了2014年8月四川(26.18°N, 105.33°E)将发生M_s5.3地震发生.2014年8月3日云南鲁甸M_s6.5地震表明: 这次地震的指纹法预测时间相差1天, 震中相差226 km, 震级误差M_s1.2.通过构造背景、地壳速度结构和震源机制研究, NW向的包谷垴-小河左旋走滑断裂是鲁甸地震的发震断裂.中下地壳低速(高导)体与包谷垴-小河断裂交接部位是流变界面能量释放的位置, 即本次地震的震源位置, 为板内地震三层次构造模式提供了一个新的案例.      

Quaternary faulting along the Caribbean-North American plate boundary in Central America

Recent detailed mapping along the Motagua fault zone and reconnaissance along the Chixoy—Polochic and Jocotán—Chamelecón fault zones provide new information regarding the nature of Quaternary deformation along the Caribbean—North American plate boundary in Central America.The southern boundary of the Motagua fault zone is defined by a major active left-slip fault that ruptured during the February 4, 1976 Guatemala earthquake. The recurrent nature of slip along the fault is dramatically demonstrated where stream terraces of the Río El Tambor show progressive left-slip and vertical (up-to-the-north) slip. Left-slip increases from 23.7 m (youngest mappable terrace) to 58.3 m (oldest mappable terrace) and vertical slip increases from 0.6 m to 2.5 m. The oldest mappable terrace crossed by the fault appears to be younger than 40,000 years and older than 10,000 years.Reconnaissance along the Chixoy—Polochic fault zone between Chiantla and Lago de Izabal has located the traces of a previously unmapped major active left-slip fault. Geomorphic features along this fault are similar to those observed along the active trace of the Motagua fault zone. Consistent and significant features suggestive of left-slip have so far not been observed along the Guatemala section of the Jocotán—Chamelecón fault zone.In Central America, the active Caribbean—North American plate boundary is comprised of the Motagua, Chixoy—Polochic, and probably the Jocotán—Chamelecón fault zones, with each accommodating part of the slip produced at the mid-Cayman spreading center. Similarities in geomorphic expression, apparent amount of left-slip, and frequency and magnitude of historical and instrumentally recorded earthquakes between the active traces of the Motagua and Chixoy—Polochic fault zones suggest a comparable degree of activity during Quaternary time; the sense and amount of Quaternary slip on the Jocotán—Chamelecón fault zone remain uncertain, although it appears to be an active earthquake source. Uplift of major mountain ranges on the north side of each fault zone reflects the small but consistent up-to-the-north vertical component (up to 5% of the lateral component) of slip along the plate boundary. Preliminary findings, based on offset stream terraces, indicate a late Quaternary slip rate along the Caribbean—North American plate boundary of between 0.45 and 1.8 cm/yr. Age dating of offset Quaternary terraces in Guatemala will allow refinement of this rate.     

Recent crustal movements in The Central Sierra Nevada—Walker lane region of California—Nevada: Part iii, The Olinghouse fault zone

The Olinghouse fault zone is one of several NE—ENE-trending fault zones and lineaments, including the Midas Trench and the Carson—Carson Sink Lineament, which exhibit left-lateral transcurrent movement conjugate to the Walker Lane in western Nevada. The active portion of this fault zone extends for approximately 23 km, from 16 km east of Reno, Nevada, to the southern extent of Pyramid Lake. The fault can be traced for most of its length from its geomorphic expression in the hilly terrain, and it is hidden only where overlain by recent alluvial sediments. Numerous features characteristic of strike-slip faulting can be observed along the fault, including: scarps, vegetation lines, sidehill and shutter ridges, sag ponds, offset stream channels and stone stripes, enclosed rhombohedral and wedge-shaped depressions, and en-echelon fractures.A shear zone having a maximum observable width of 1.3 km is defined principally by Riedel shears and their symmetrical P-shears, with secondary definition by deformed conjugate Riedel shears. Several continuous horizontal shears, or principal displacement shears, occupy the axial portion of the shear zone. The existence of P-shears and principal displacement shears suggests evolution of movement along the fault zone analogous to the “Post-Peak” or “Pre-Residual Structure” stage.Historic activity (1869) has established the seismic potential of this zone. Maximum intensities and plots of the isoseismals indicate the 1869 Olinghouse earthquake had a magnitude of 6.7. Field study indicates the active length of the fault zone is at least 23 km and the maximum 1869 displacement was 3.65 m of left-slip. From maximum fault length and maximum fault displacement to earthquake magnitude relations, this corresponds to an earthquake of about magnitude 7.     

Observations of the performance of buildings during the 1985 Mexico earthquake,and structural design implications

Summary The high amplification of the 1985 Mexico City earthquake is explained by the large number of strong and nearly continuous cycles of 2 s period motion lasting for more than 30 s. The type of damage caused by the earthquake—particularly to engineered multi-storey buildings of high flexibility is described, and methods of adding damping and stiffness elements to reduce and resist earthquake demand forces are discussed.     

The Investigation Results of the April 12, 2014, <Emphasis Type="Italic">M</Emphasis> = 4.5 Primorye Earthquake (Far Eastern Russia)

Primorye is a region with quite moderate shallow seismicity which has been insufficiently investigated so far in this respect. Based on the obtained instrumental data of regional seismic networks and macroseismic data collected in southwestern Primorye on the crustal earthquake with M = 4.5 occurred on April 12, 2014, we have first succeeded in determining the hypocenter parameters and the focal mechanism of the mainshock of this shallow earthquake and estimating the hypocenter parameters of the following aftershock.     

Focal mechanism solution of the Himalayan earthquake of February 14, 1977

Through a closely spaced local network of seismic stations in Himachal Pradesh, India, supplemented by worldwide P-wave first-motion data, the source mechanism of the February 14, 1977 earthquake which occurred very close to the Rawalpindi area in Pakistan has been determined. The fault-plane solution as reported earlier for this event by Seeber and Armbruster (1979) showed thrust faulting. The reliability of their solution has been tested using more P-wave first-motion data from near Indian stations within the epicentral distance of 4°–7°, as well as from distant stations. The inclusion of data from these stations completely changed the type of faulting from thrust to normal type. The new solution parameters have been briefly discussed in relation to the local geological faults/thrusts.     

The earthquake in the Swabian Jura of 16 November 1911 and present concepts of seismotectonics

Beginning with the Swabian Jura earthquake in 1911 the seismic activity in Central Europe is concentrated to this area. A comparison with other events of the same epicentral region shows that the largest earthquake in Germany has the character of a left-lateral horizontal strike slip striking N — NNE. The focal parameters can be assumed within the following intervalls: Seismic moment M_o = 1…8·10¹⁷ Nm; focal area F_o = 18…53 km²; average dislocation d_o = 20…53 cm and stress drop Δp_o = 13…19 bar.     

Seismicity of the Tanzania region

The seismicity of the East African Rift system within the region bounded by latitudes 2°N and 12°S and longitudes 28°E and 40°E has been studied as far as all available instrumentally based material permits. An earthquake catalogue is presented and the data contained therein are used for tectonophysical investigations, including frequency—magnitude relations and time and space distribution of the seismicity within the region. In addition, earthquake engineering aspects are discussed.     

Method of anthropoecological stabilization of landscape and its interpretation

The study deals with the theoretical approach to anthropoecological stabilization of landscape (ASL). It describes a method consisting of four stages including detailed differentiation from the viewpoint of aim, objectives of investigation, and means of evaluation and processing. Application of the method requires to provide: the preparatory, analytical ground — I. stage (analytical part), the structural — functional evaluation of the territory under solution — II. stage (analytical-synthetical part), the solution of ecooptimization relations and bonds by way of material and energy flows — III. stage (regulative part), the monitoring and signalling activities, determination of all-system biogeoindications — IV. stage (ensuring part).The results are exemplified by application to model territories in South Bohemia region.     

The earthquake of September 6, 1975 in Lice (eastern Turkey)

The mechanism of faulting for the Lice earthquake of September 6, 1975 is thrust fault, the compressional axis is horizontal and perpendicular to the Taurus mountains with 180° azimuth and 2° plunge. This corresponds to northward movement of Arabia. The T-axis is nearly vertical. The slip vector has 15° azimuth and 65° slip angle for the fault plane which is simistral and has N72°E azimuth and dips 45° NW. The intensity distribution pattern, the location of the main aftershock epicentres, the geological aspect of the region, and the limiting boundaries of different zones indicate the predominence of the east—west direction and are in good agreement with our focal-mechanism solution.     

Seismotectonics of the Papua New Guinea—Solomon Islands region

Earthquakes for the period 1964–1973 are relocated by the method of Joint Hypocenter Determination in order better to resolve the configuration and the structure of the New Guinea—New Britain—Solomon Islands region. Focal mechanism solutions are integrated with the seismicity and interpreted closely with it. A zone of subduction exists beneath New Britain and the Solomon Islands, a zone of left-lateral strike-slip movement extends from New Ireland to New Guinea. The zone of seismicity in northern New Guinea has developed as a result of a continent—island-arc collision in late Oligocene—Miocene times and does not exhibit a well-developed inclined seismic zone. It is proposed that plate tectonics theory does not apply rigorously, but slip-line field theory allows the presentation of a new geodynamic model for this region.     

Fault location and fault activity assessment by analysis of historic level line data, oil-well data and groundwater data, Hollywood area, California

Transecting the Los Angeles metropolitan area in a general E-W direction are major north-dipping reverse faults comprising the Santa Monica—Raymond Hill fault zone, a segment of the frontal fault system separating the Transverse Ranges from the Peninsular Ranges geomorphic provinces of southern California. Pleistocene or Holocene movement is evident along some segments of these faults, but urban development precludes accurate location and assessment of Quaternary movement by conventional mapping techniques. At present no conclusive evidence of Holocene surface rupture has been found onshore west of the Raymond Hill segment of the fault zone, but the geologic conditions and urban development in the area are such that the possibility of Holocene movement cannot be excluded at this time. Groundwater barriers in Pleistocene sediments are indicative of Quaternary faulting on the Santa Monica fault segment west of the Newport—Inglewood fault zone. Most literature indicates that movement along the Beverly Hills—Hollywood segment east of the Newport—Inglewood fault zone terminated in Late Miocene or Pliocene time, and there is no general agreement on the location of faults in this segment. However, recent work by the Division of Mines and Geology, by Geotechnical Consultants, Inc., and others suggests that the Santa Monica fault transecting the Hollywood area is associated with a zone of differential subsidence that varies from 100 to 400 m wide, depending on the resolution of repeated leveling survey data and with a groundwater barrier determined from analysis of oil-well and water-well data. Additional exploration is essential to test our present geologic model and to evaluate the earthquake hazard and seismic risk of faults in the area.     

On the assessment of maximum earthquakes in the alps and adjacent areas

Strong tectonic earthquakes within the crust always occur on already existing faults, and they have the property of a shear rupture. Such earthquakes with surface-wave magnitudes M < 7 obviously have a geometric similarity. Because of this similarity and the validity of the Gutenberg and Richter's energy—magnitude relation, the expression M = 2 log₁₀ L + const., with L = focal length, is valid.The expression L_maxL^* for the maximum focal length, is also valid if L^* is the length of the rectilinear extent of the seismic line on which the maximum earthquake occurs. The bounds of L^* may be given by sharp bends and/or by traversing deep faults. Thus the maximum imaginable earthquake on a seismic line with the length L^* has the magnitude M_max = 2 log₁₀ L^* + const.For the investigated region — the Alps and adjacent areas — from the data of recent and historical strong earthquakes, it follows that M_max = 2 log₁₀ L^* + 1.7, if L^* is measured in kilometres. These limiting values lie in the centre-field of the magnitude range for maximum earthquakes, published by Shebalin in 1970. By the aid of this equation it is also possible to assess the upper limiting value of the accompanying maximum scale intensity.     

Evidence of dislocations on the southern slope of the nebrodi-madonie mountains (northern Sicily, Italy): Their neotectonics implications

The investigated area is located on the southern slope of the NebrodiMadonie Mts. (northern Sicily, Italy). It was studied in order to obtain neotectonic evidence by means of fracture measurements, morphotectonic and hydrographical patterns, aerial photographs and satellite analysis. The results were compared with the well-known geological structures.This area could be considered an outstanding crustal part of Sicily, as here we find alignments of earthquake foci and a deep gradient of gravity anomalies, testifying to an important isostatic imbalance. This analysis confirms the observed structural picture of surface tectonics. Rose diagrams elaborated from fieldwork and aerial lineations show distinctive E—W trends which conform to the directions of the main faults.From a chronological viewpoint faults breaks, aerial photographs and satellite lineations seem to indicate that the E—W trend is the less dislocated and, therefore, the most recent.     

Seismic hazard assessments for two test areas — ‘Southern Italy’ and ‘Belgium—The Netherlands—Germany’

Within the activity of the ESC Subcommission 8 Engineering Seismology, Project TERESA, seismic hazard calculations have been performed for two areas of a different earthquake activity. Fundamental seismological data (earthquake catalogues, macroseismic observations and maps) and some additional geological information were analyzed and processed to prepare inputs for hazard computations. Great attention has been paid to verifying the reliability of the input data. Seismic hazards obtained for five sites of the region of high seismic activity (Sannio-Matese, southern Italy) and six sites of the region of low seismic activity (Brabant Massif and northern Rhine, Belgium—The Netherlands—Germany) are presented and discussed.     

Stability of earthquake moment tensor inversions: effect of the double-couple constraint

We show that spurious large non-double-couple components can be obtained in inversions for the full deviatoric moment tensor for shallow crustal earthquakes due to inaccurate Earth models. The traditional “best double-couple” solution does not in general provide an optimal estimate of a double-couple mechanism, and is only reliable when the non-double-couple component of the full deviatoric solution is small. The inverse problem for the moment tensors of the 1998 Antarctic Plate and 2000 Wharton Basin strike-slip earthquakes is shown in each case to have two well-fitting minima in the misfit function of pure double-couple solutions. Such pairs of solutions are most likely to exist for earthquakes which are close either to vertical strike-slip or to dip-slip on a fault plane dipping at 45°. It is shown theoretically that these pairs of solutions arise from the combination of the pure double-couple constraint and the instability of two elements of the moment tensor. No significant non-double-couple component is found for the shallow thrusting 1996 Biak, Indonesia earthquake.     

The stress field near the sites of the Meckering (1968) and Calingiri (1970) earthquakes, Western Australia

A comparison of three methods of stress determination using overcoring tests, earthquake focal-mechanism solutions, and fault-displacement analysis, was carried out near the epicentres of the 1968 Meckering and the 1970 Calingiri earthquakes, Western Australia. Shallow overcoring measurements (3–10 m) were made at seven sites in competent granite, along a 200-km north—south traverse through the location of the Meckering earthquake. The in situ measurements indicate a high regional compressive stress, acting about N77°E. This compares with the direction of the P-axes from the Meckering and Calingiri earthquakes of N91°E and N102°E, respectively, and east-west orientation of major principal stress deduced from observations of surface faulting. The highest maximum principal stress, 23 MPa, was measured at the site farthest north from the Meckering epicentre (~ 90 km), and the lowest, 4 MPa, was measured near the epicentre. The magnitude of the stress increases with distance away from the epicentral area at about 0.2 kPa/m. The results were corrected for drilling water temperature, thermal rock stresses, and suction pore pressure. The total correction was less than 2 MPa at most sites.Estimates of shear stress release from the fault-scarp displacements for Meckering and Calingiri were of similar magnitude (~10 MPa) to the difference between observed shear stress at sites close to and sites remote from the Meckering earthquake.As a cause of the earthquake it is proposed that the fault plane is progressively weakened by alteration or weathering, and that a small long-term fluctuation of head of ground water was the trigger.The high stress at shallow depths, the growing evidence of east—west major principal stress in most of the Australian continent, and the existence of horizontal stress higher than gravity lithostatic stress may have a common explanation, in terms of the driving forces of plate tectonics. The Australian results do not agree with the north—south orientation suggested by crude plate-drift theories in which the major stress is in the direction of the drift, and do not appear to fit with orientations from other continents, in the Richardson et al. (1976) interacting plate model which assumes a velocity-dependent plate driving force. An analysis of driving forces at diverging plate boundaries was carried out and suggests no dominant force-velocity relationship, thus forces independent of plate velocity may control the stress orientation in the plate.