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An extended displacement discontinuity method for analysis of stress wave propagation in viscoelastic rock mass
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作者 L.F.Fan F.Ren g.w.ma 《Journal of Rock Mechanics and Geotechnical Engineering》 SCIE 2011年第1期73-81,共9页
An extended displacement discontinuity method(EDDM)is proposed to analyze the stress wave propagation in jointed viscoelastic rock mass(VRM).The discontinuities in a rock mass are divided into two groups.The primary g... An extended displacement discontinuity method(EDDM)is proposed to analyze the stress wave propagation in jointed viscoelastic rock mass(VRM).The discontinuities in a rock mass are divided into two groups.The primary group with an average geometrical size larger than or in the same order of magnitude of wavelength of a concerned stress wave is defined as'macro-joints',while the secondary group with a high density and relatively small geometrical size compared to the wavelength is known as'micro-defects'.The rock mass with micro-defects is modeled as an equivalent viscoelastic medium while the macro-joints in the rock mass are modeled explicitly as physical discontinuities.Viscoelastic properties of a micro-defected sedimentary rock are obtained by longitudinally impacting a cored long sedimentary rod with a pendulum.Wave propagation coefficient and dynamic viscoelastic modulus are measured.The EDDM is then successfully employed to analyze the wave propagation across macro-joint in VRM.The effect of the rock viscosity on the stress wave propagation is evaluated by comparing the results of VRM from the presented EDDM with those of an elastic rock mass(ERM)from the conventional displacement discontinuity method(CDDM).The CDDM is a special case of the EDDM under the condition that the rock viscosity is ignored.Comparison of the reflected and transmitted waves shows that the essential rock viscosity has a significant effect on stress wave attenuation.When a short propagation distance of a stress wave is considered,the results obtained from the CDDM approximate to the EDDM solutions,however,when the propagation distance is sufficiently long relative to the wavelength,the effect of rock viscosity on the stress wave propagation cannot be ignored. 展开更多
关键词 stress wave propagation extended displacement discontinuity method(EDDM) viscoelastic rock mass(VRM) micro-defect macro-joint
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Simulations of explosion-induced damage to underground rock chambers
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作者 g.w.ma H.Hao F.Wang 《Journal of Rock Mechanics and Geotechnical Engineering》 SCIE 2011年第1期19-29,共11页
A numerical approach is presented to study the explosion-induced pressure load on an underground rock chamber wall and its resultant damage to the rock chamber.Numerical simulations are carried out by using a modified... A numerical approach is presented to study the explosion-induced pressure load on an underground rock chamber wall and its resultant damage to the rock chamber.Numerical simulations are carried out by using a modified version of the commercial software AUTODYN.Three different criteria,i.e.a peak particle velocity(PPV)criterion,an effective strain(ES)criterion,and a damage criterion,are employed to examine the explosion-induced damaged zones of the underground rock chamber.The results show that the charge chamber geometry,coupling condition and charge configuration affect significantly the dynamic pressure exerted on the rock chamber wall.Thus the chamber is damaged.An inaccurate approximation of pressure boundary ignoring the influences of these factors would result in an erroneous prediction of damaged area and damage intensity of the charge chamber.The PPV criterion yields the largest damaged zone while the ES criterion gives the smallest one.The presented numerical simulation method is superior in consideration of the chamber geometry,loading density,coupling condition and rock quality.The predicted damage intensity of rock mass can be categorized quantitatively by an isotropic damage scalar.Safe separation distance of adjacent chambers for a specific charge weight is also estimated. 展开更多
关键词 underground explosion rock damage numerical simulation safe separation distance
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