<th id="5nh9l"></th><strike id="5nh9l"></strike><th id="5nh9l"><noframes id="5nh9l"><th id="5nh9l"></th><strike id="5nh9l"></strike>
<progress id="5nh9l"><noframes id="5nh9l"><th id="5nh9l"><noframes id="5nh9l">
<th id="5nh9l"></th> <strike id="5nh9l"><noframes id="5nh9l"><span id="5nh9l"></span>
<progress id="5nh9l"><noframes id="5nh9l"><span id="5nh9l"><noframes id="5nh9l"><span id="5nh9l"></span><strike id="5nh9l"><noframes id="5nh9l"><strike id="5nh9l"></strike>
<span id="5nh9l"><noframes id="5nh9l">
<span id="5nh9l"><noframes id="5nh9l">
<span id="5nh9l"></span><span id="5nh9l"><video id="5nh9l"></video></span>
<th id="5nh9l"><noframes id="5nh9l"><th id="5nh9l"></th>
<progress id="5nh9l"><noframes id="5nh9l">

動載下層狀復合巖石能量耗散及斷裂特征研究

Energy dissipation and fracture characteristics of composite layered rock under dynamic load

  • 摘要: 利用砂巖、大理巖、花崗巖制作6種不同組合方式的層狀復合巖石,采用分離式霍普金森壓桿試驗系統,對不同組合方式的層狀巖石進行動態沖擊試驗,利用高速相機記錄其破壞形態,分析復合巖石材料的動態斷裂模式、波阻抗效應以及能量耗散規律,探究不同復合巖石試件的動能及斷裂能關系. 利用離散格子彈簧模型模擬復合巖石試件的動態斷裂過程,分析復合試件的應力波傳播特性及應力、損傷演化規律. 研究結果表明:復合巖石材料的動態斷裂特征與上下層材料具有相關性,當下層材料動態起裂韌度較低時,裂紋從起裂至擴展到巖石膠結面歷時較短. 上層材料對于復合巖石的應力傳導作用具有較大的相關性,上層材料密度越大,更有利于透射波傳遞,應力傳導效果越好,而下層材料與上層材料密度相差越大,膠結面上下端應力差越大;受波阻抗效應影響,復合巖石試件應力波的傳播行為具有明顯差異,波阻抗越大應力波傳播速度越快,透射系數越大,產生更多的透射能;復合巖石試件的耗散能時密度、動能及斷裂能與上下層巖石材料的密度有關,下層材料不變,上層材料密度越大時,耗散能時密度及斷裂能更小,試件完全斷裂時獲得較大的動能.

     

    Abstract: Six combinations of layered composite rocks were prepared using sandstone, dali rock, and granite. The composite rock specimens underwent a dynamic impact test using the separated Hopkinson pressure rod test system, and the failure patterns of the specimens were recorded using high-speed cameras. The dynamic fracture mode, wave impedance effect, and energy dissipation nature of these composite rock specimens were analyzed, and the relationship between their kinetic energy and fracture energy was explored. The discrete lattice spring model was used to simulate the dynamic fracture process of the composite rock specimens, and the stress wave propagation characteristics and stress and damage evolution nature of the composite specimens were analyzed. The results show that the dynamic fracture characteristics of composite rock materials are strongly influenced by the uppermost and lowermost layer materials. When the dynamic cracking toughness of the material in the lower layer is low, the crack can maintain a high propagation speed and requires a short time from initiation to expansion to the rock cemented surface. The upper layer material has a greater influence on the stress conduction of the composite rock specimen. The overall transmission capacity depends on the upper layer material such that the greater its density, the more conducive it is to wave transmission and the better the stress conduction. The greater the difference in the densities of the lower and upper layer materials, the greater the difference between the stresses at the upper and lower ends of the rock cemented surface. Wave impedance has a significant effect on the propagation behavior of the stress wave. The propagation speed of the stress wave in the composite specimen is influenced by the porosity and density of the material. The larger the wave impedance, the faster the propagation speed of the stress wave, the larger the transmission coefficient, and the higher the energy transmitted. When energy is dissipated, the density, kinetic energy, and fracture energy of the composite rock specimen are influenced by the densities of the materials in the upper and lower layers. If the lower layer material is unchanged, a higher density of the upper layer material results in a smaller density and fracture energy when the energy is dissipated, yielding more kinetic energy when the specimen is completely fractured. When the upper layer material remains unchanged and the density of the lower material is increased, the cutting tip is more likely to crack, and the density and fracture energy are smaller when the energy is dissipated.

     

/

返回文章
返回
<th id="5nh9l"></th><strike id="5nh9l"></strike><th id="5nh9l"><noframes id="5nh9l"><th id="5nh9l"></th><strike id="5nh9l"></strike>
<progress id="5nh9l"><noframes id="5nh9l"><th id="5nh9l"><noframes id="5nh9l">
<th id="5nh9l"></th> <strike id="5nh9l"><noframes id="5nh9l"><span id="5nh9l"></span>
<progress id="5nh9l"><noframes id="5nh9l"><span id="5nh9l"><noframes id="5nh9l"><span id="5nh9l"></span><strike id="5nh9l"><noframes id="5nh9l"><strike id="5nh9l"></strike>
<span id="5nh9l"><noframes id="5nh9l">
<span id="5nh9l"><noframes id="5nh9l">
<span id="5nh9l"></span><span id="5nh9l"><video id="5nh9l"></video></span>
<th id="5nh9l"><noframes id="5nh9l"><th id="5nh9l"></th>
<progress id="5nh9l"><noframes id="5nh9l">
259luxu-164