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      KCI등재 SCIE SCOPUS

      Dynamic Performance and Stress Wave Propagation Characteristics of Parallel Jointed Rock Mass Using the SHPB Technique

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      https://www.riss.kr/link?id=A108570753

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      다국어 초록 (Multilingual Abstract)

      To investigate the effects of joint number on dynamic compressive strength, crushing effect, stress wave propagation, stress wave conversion, and energy evolution of rock masses, SHPB and LS-DYNA were used to conduct impact experiments and numerical simulations, respectively. The results demonstrate that the dynamic strength of a multi-jointed (two- and three-jointed) rock are 11.1 and 25.1% lower, respectively, compared with that of a single-jointed rock. The weak surface near the joint causes the rock mass to crack first. The rock cracking time advances significantly as the joints number increases. The reflection coefficient falls as the number of joints increases, because the wave impedance of the joint differs from that of the rock. The transmission coefficient, however, is exactly the reverse. When the P wave strikes the specimen, the vibration direction of the particles is deflected at the joint, resulting in a shear wave. P waves are reflected and superimposed between joints, increasing the strength of shear waves and resulting in more transverse cracks in multi-jointed rock masses under dynamic loading. Meanwhile, the total energy consumed by a bedrock under dynamic loading is obviously larger than that of joints. However, the total energy absorbed by joints exceeds that of the bedrock when the joints number increases. The results further enrich the dynamic basis of jointed rock masses.
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      To investigate the effects of joint number on dynamic compressive strength, crushing effect, stress wave propagation, stress wave conversion, and energy evolution of rock masses, SHPB and LS-DYNA were used to conduct impact experiments and numerical s...

      To investigate the effects of joint number on dynamic compressive strength, crushing effect, stress wave propagation, stress wave conversion, and energy evolution of rock masses, SHPB and LS-DYNA were used to conduct impact experiments and numerical simulations, respectively. The results demonstrate that the dynamic strength of a multi-jointed (two- and three-jointed) rock are 11.1 and 25.1% lower, respectively, compared with that of a single-jointed rock. The weak surface near the joint causes the rock mass to crack first. The rock cracking time advances significantly as the joints number increases. The reflection coefficient falls as the number of joints increases, because the wave impedance of the joint differs from that of the rock. The transmission coefficient, however, is exactly the reverse. When the P wave strikes the specimen, the vibration direction of the particles is deflected at the joint, resulting in a shear wave. P waves are reflected and superimposed between joints, increasing the strength of shear waves and resulting in more transverse cracks in multi-jointed rock masses under dynamic loading. Meanwhile, the total energy consumed by a bedrock under dynamic loading is obviously larger than that of joints. However, the total energy absorbed by joints exceeds that of the bedrock when the joints number increases. The results further enrich the dynamic basis of jointed rock masses.

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      참고문헌 (Reference)

      1 Zhang YM, "Strong discontinuity embedded approach with standard SOS formulation : Element formulation, energy-based crack-tracking strategy, and validations" 287 : 335-366, 2015

      2 Xiong F, "Strength and fracture behaviors of sandstone samples containing intersect fissures under uniaxial compression" 42 (42): 886-895, 2017

      3 Liu HY, "Similar material test study of dynamic failure of jointed rock mass with SHPB" 35 (35): 659-665, 2014

      4 Ma QY, "SHPB experimental study on dynamic characteristics and failure behaviors of sandstone containing weakly filled joints with various angles in deep roadways" 39 (39): 1104-1116, 2020

      5 Zhang YM, "Predicting the porePressure and temperature of fire-loaded concrete by a hybrid neural network" 2142011-, 2022

      6 Zhou SW, "Phase-field modeling of fluiddriven dynamic cracking in porous media" 350 : 169-198, 2019

      7 Zhuang XY, "On the hydraulic fracturing in naturally-layered porous media using the phase field method" 266 : 105306-, 2021

      8 Zhang YM, "On the crack opening and energy dissipation in a continuum based disconnected crack model" 170 : 103333-, 2019

      9 Zhang ML, "Numerical simulation of mechanical properties of rock specimens with cross-crack under different confining pressure" 16 (16): 758-769, 2020

      10 Li C, "Numerical experiment of failure process of jointed rock mass under dynamic loading" 36 : 655-664, 2015

      1 Zhang YM, "Strong discontinuity embedded approach with standard SOS formulation : Element formulation, energy-based crack-tracking strategy, and validations" 287 : 335-366, 2015

      2 Xiong F, "Strength and fracture behaviors of sandstone samples containing intersect fissures under uniaxial compression" 42 (42): 886-895, 2017

      3 Liu HY, "Similar material test study of dynamic failure of jointed rock mass with SHPB" 35 (35): 659-665, 2014

      4 Ma QY, "SHPB experimental study on dynamic characteristics and failure behaviors of sandstone containing weakly filled joints with various angles in deep roadways" 39 (39): 1104-1116, 2020

      5 Zhang YM, "Predicting the porePressure and temperature of fire-loaded concrete by a hybrid neural network" 2142011-, 2022

      6 Zhou SW, "Phase-field modeling of fluiddriven dynamic cracking in porous media" 350 : 169-198, 2019

      7 Zhuang XY, "On the hydraulic fracturing in naturally-layered porous media using the phase field method" 266 : 105306-, 2021

      8 Zhang YM, "On the crack opening and energy dissipation in a continuum based disconnected crack model" 170 : 103333-, 2019

      9 Zhang ML, "Numerical simulation of mechanical properties of rock specimens with cross-crack under different confining pressure" 16 (16): 758-769, 2020

      10 Li C, "Numerical experiment of failure process of jointed rock mass under dynamic loading" 36 : 655-664, 2015

      11 Ban LR, "Modified 2D roughness parameters for rock joints at two different scales and their correlation with JRC" 2020 : 104549-, 2020

      12 Zhang YM, "Image representations of numerical simulations for training neural networks" 134 : 821-833, 2022

      13 Zhang YM, "Global cracking elements : A novel tool for Galerkin-based approaches simulating quasi-brittle fracture" 121 : 2462-2480, 2020

      14 Bandis SC, "Fundamentals of rock joint deformation" 20 (20): 249-268, 1983

      15 Wang ZL, "Finite element analyses of constitutive models performance in the simulation of blast-induced rock cracks" 135 : 104172-, 2021

      16 Yan YT, "Experimental study on the influence of joint roughness and matching state on dynamic compression characteristics of rock masses" 40 (40): 1132-1144, 2020

      17 Yan YT, "Experimental study on the influence of joint roughness and matching state on dynamic compression characteristics of rock masses" 40 (40): 1132-1144, 2021

      18 Li JC, "Experimental study of stress wave propagation across a filled rock join" 46 (46): 471-478, 2009

      19 Deng ZD, "Equivalent elastic model and strength properties for cross-jointed rock mass containing persistent and non-persistent joints" 43 (43): 3098-3106, 2018

      20 Xie HZ, "Energy dissipation and fractal characteristics of basalt fiber reinforced concrete under impact loading" 46 : 654-663, 2022

      21 Zhao J, "Dynamic model of fracture normal behaviour and application to prediction of stress wave attenuation across fractures" 41 (41): 671-693, 2008

      22 Rabczuk T, "Cracking particles : A simplified meshfree method for arbitrary evolving cracks" 61 : 2316-2343, 2004

      23 Zhang YM, "Cracking elements method with a dissipation-based arc-length approach" 195 : 103573-, 2021

      24 Zhang YM, "Cracking elements method for dynamic brittle fracture" 102 : 1-9, 2019

      25 Zhang YM, "Cracking elements : A self-propagating strong discontinuity embedded approach for quasi-brittle fracture" 287 : 335-366, 2018

      26 Pyark-Nolte LJ, "Anisotropy inseismic velocities and amplitudes from multiple parallel fractures" 95 (95): 345-358, 1990

      27 Zare S, "Analysis and determination of the behavioral mechanism of rock bridges using experimental and numerical modeling of non-persistent rock joints" 141 (141): 104714-, 2021

      28 Kolsky H, "An investigation of the mechanical properties of materials at very high rates of loading" 62 (62): 676-, 1949

      29 Li JC, "An equivalent 1D dynamic continuum model for rock mass with parallel joints" 29 (29): 4063-4067, 2010

      30 Chen W, "A split Hopkinson bar technique for low-impedance materia" 39 (39): 81-85, 1999

      31 Rabczuk T, "A simple and robust three-dimensional cracking-particle method without enrichment" 199 : 2437-2455, 2010

      32 Wang TT, "A constitutive model for the deformation of a rock mass containing sets of ubiquitous joints" 46 (46): 521-530, 2009

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