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  • 1
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    In:  J. Geophys. Res., New York, August, vol. 92, no. 3-4, pp. 4959-4964, pp. 1610, (ISSN: 1340-4202)
    Publication Date: 1987
    Keywords: Stress ; Layers ; JGR
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  • 2
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    In:  J. Geophys. Res., New York, August, vol. 93, no. 3-4, pp. 13609-13617, pp. 1610, (ISSN: 1340-4202)
    Publication Date: 1988
    Keywords: Stress ; Elasticity ; JGR
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  • 3
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    In:  Science, Bonn, Inst. f. Theoret. Geodäsie, vol. 232, no. 1, pp. 213-216, pp. B02303, (ISSN: 1340-4202)
    Publication Date: 1986
    Keywords: Crustal deformation (cf. Earthquake precursor: deformation or strain) ; Geodesy ; Fault zone ; Volcanology
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  • 4
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    In:  Pageoph, New York, August, vol. 128, no. 3-4, pp. 295-307, pp. 1610, (ISSN: 1340-4202)
    Publication Date: 1989
    Keywords: Seismology ; Earthquake hazard ; Rock bursts (see also ERDSTOSS and GEBIRGSSCHLAG)
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  • 5
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    In:  Journal of Geophysical Research, New York, August, vol. 104, no. B2, pp. 3003-3011, pp. 1610, (ISSN: 1340-4202)
    Publication Date: 1999
    Keywords: Stress ; Seismology ; Rock mechanics ; efficiency ; seismic Moment ; pore ; pressure ; Fluids ; Hypocentral depth ; Mining geophysics ; JGR
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  • 6
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    In:  Pure and Applied Geophysics, New York, August, vol. 150, no. 3-4, pp. 381-391, pp. 1610, (ISSN: 1340-4202)
    Publication Date: 1997
    Keywords: Mining geophysics ; Rock bursts (see also ERDSTOSS and GEBIRGSSCHLAG) ; GEBIRGSSCHLAG (see also rockburst and Erdstoss) ; Physical properties of rocks ; PAG
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  • 7
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    A. A. Balkema
    In:  Bull., Polar Proj. OP-O3A4, Rockbursts and Seismicity in Mines, Rotterdam, A. A. Balkema, vol. 16, no. 4, pp. 385-396, (ISBN 0080419208)
    Publication Date: 1997
    Keywords: Induced seismicity ; Seismicity ; Rock bursts (see also ERDSTOSS and GEBIRGSSCHLAG) ; GEBIRGSSCHLAG (see also rockburst and Erdstoss) ; ERDSTOSS (see also rockburst and Gebirgsschlag) ; Coulomb ; fluid ; Review article ; Stress
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  • 8
    Publication Date: 1986-04-11
    Description: After the January 1983 earthquake swarm, the last period of notable seismicity, the rapid rate of deformation of the south moat and resurgent dome of the Long Valley caldera diminished. Frequently repeated two-color laser ranging measurements made within a geodetic network in the caldera during the interval June 1983 to November 1984 reveal that, although the deformation accumulated smoothly in time, the rate of extension of many of the baselines decreased by factors of 2 to 3 from mid-1983 to mid-1984. Areal dilatation was the dominant signal during this period, with rates of extension of several baselines reaching as high as 5 parts per million per annum during the summer of 1983. Within the south moat, shear deformation also was apparent. The cumulative deformation can be modeled as the result of injection of material into two points located beneath the resurgent dome in addition to shallow right lateral slip on a vertical fault in the south moat.〈br /〉〈span class="detail_caption"〉Notes: 〈/span〉Linker, M F -- Langbein, J O -- McGarr, A -- New York, N.Y. -- Science. 1986 Apr 11;232(4747):213-6.〈br /〉〈span class="detail_caption"〉Record origin:〈/span〉 〈a href="http://www.ncbi.nlm.nih.gov/pubmed/17780806" target="_blank"〉PubMed〈/a〉
    Print ISSN: 0036-8075
    Electronic ISSN: 1095-9203
    Topics: Biology , Chemistry and Pharmacology , Computer Science , Medicine , Natural Sciences in General , Physics
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  • 9
    Electronic Resource
    Electronic Resource
    Springer
    Pure and applied geophysics 150 (1997), S. 381-391 
    ISSN: 1420-9136
    Keywords: Key words: Wall-rock velocities, rockbursts, slab buckling.
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Physics
    Notes: Abstract. —Considerable evidence has been reported for wall-rock velocities during rockbursts in deep gold mines that are substantially greater than ground velocities associated with the primary seismic events. Whereas varied evidence suggests that slip across a fault at the source of an event generates nearby particle velocities of, at most, several m/s, numerous observations, in nearby damaged tunnels, for instance, imply wall-rock velocities of the order of 10 m/s and greater. The common observation of slab buckling or breakouts in the sidewalls of damaged excavations suggests that slab flexure may be the mechanism for causing high rock ejection velocities. Following its formation, a sidewall slab buckles, causing the flexure to increase until the stress generated by flexure reaches the limit S that can be supported by the sidewall rock. I assume here that S is the uniaxial compressive strength. Once the flexural stress exceeds S, presumably due to the additional load imposed by a nearby seismic event, the slab fractures and unflexes violently. The peak wall-rock velocity v thereby generated is given by ¶¶ v = (3 + (1 - v²)/2)½ S/(ρE)½¶¶for rock of density ρ, Young's modulus E, and Poisson's ratio ν. Typical values of these rock properties for the deep gold mines of South Africa yield v = 26 m/s and for especially strong quartzites encountered in these same mines, v 〉 50 m/s. Even though this slab buckling process leads to remarkably high ejection velocities and violent damage in excavations, the energy released during this failure is only a tiny fraction of that released in the primary seismic event, typically of magnitude 2 or greater.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    Springer
    Pure and applied geophysics 129 (1989), S. 295-307 
    ISSN: 1420-9136
    Keywords: Large mine tremors ; source parameters ; ground motion parameters ; Klerksdorp mining district ; Carletonville mining district
    Source: Springer Online Journal Archives 1860-2000
    Topics: Geosciences , Physics
    Notes: Abstract An investigation of ground motion, recorded using broad-band, wide dynamic-range digital seismographs, of large mine tremors from two South African mining districts with different geologic settings, reveals some essential differences in both seismic source and ground motion parameters. In the Klerksdorp district where the strata are offset by major throughgoing normal faults, the largest tremors, with magnitudes ranging as high as 5.2, tend to be associated with slip on these pre-existing faults. Moreover, the seismic source and ground motion parameters are quite similar to those of natural crustal earthquakes. In the Carletonville district, by contrast, where substantial faults do not exist, the large-magnitude tremors appear to result from the failure of relatively intact rock and cause seismic stress drops and ground motion parameters higher than normally observed for natural shocks. Additionally, there appears to be an upper magnitude limit of about 4 in the Carletonville district. Detailed analyses of an exceptionally large event recorded locally from each of these districts serve to highlight these contrasts.
    Type of Medium: Electronic Resource
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