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李顺才 缪协兴 陈占清 茅献彪. 破碎岩体非等温渗流的非线性动力学研究[J]. 力学学报, 2010, 42(4): 652-659. DOI: 10.6052/0459-1879-2010-4-lxxb2008-767
引用本文: 李顺才 缪协兴 陈占清 茅献彪. 破碎岩体非等温渗流的非线性动力学研究[J]. 力学学报, 2010, 42(4): 652-659. DOI: 10.6052/0459-1879-2010-4-lxxb2008-767
Miao Xiexing Zhanqing Chen Xianbiao Mao. Study on nonlinear dynamics of non-isothermal flow in broken rock[J]. Chinese Journal of Theoretical and Applied Mechanics, 2010, 42(4): 652-659. DOI: 10.6052/0459-1879-2010-4-lxxb2008-767
Citation: Miao Xiexing Zhanqing Chen Xianbiao Mao. Study on nonlinear dynamics of non-isothermal flow in broken rock[J]. Chinese Journal of Theoretical and Applied Mechanics, 2010, 42(4): 652-659. DOI: 10.6052/0459-1879-2010-4-lxxb2008-767

破碎岩体非等温渗流的非线性动力学研究

Study on nonlinear dynamics of non-isothermal flow in broken rock

  • 摘要: 分别从固体及流体导热的能量方程出发,导出破碎岩体非等温渗流的能量本构方程, 结合渗流的连续性方程、运动方程、状态方程等建立了破碎岩体非等温渗流的一维非线性动力学方程组;结合Mathcad软件计算得到了系统的无量纲化平衡态, 利用逐次亚松弛迭代法分析了对应于不同参数时平衡态的稳定性;指出非等温渗流系统存在鞍结分岔及折叠突变, 与等温渗流相比, 考虑温度场的破碎岩体渗流动力系统更容易发生渗流突变.

     

    Abstract: The special physical environment with the high groundstress, high ground temperature, high karst hydraulic pressure, and intensemining disturbance`` in deep broken rocks, determines that their mechanicsystem is a complicated nonlinear dynamical one. Given a relative stablestress field, the flow in broken rock can be considered as a non-isothermalone, and the dynamical mechanism on the instability of non-isothermal flowin broken rock is analyzed by the theory of bifurcation and catastrophe ofnonlinear science.(1) According to the energy equations of the fluid and the solid, the energyconstitutive equation on non-isothermal flow in the broken rock isdeveloped, and combining with the continuity equation, kinetic equation andthe state equation of the flow, the one-dimensional nonlinear dynamicalequations of non-isothermal flow in broken rock are established.(2) Using these equations and boundary conditions, the dimensionless steadystates of the flow system are obtained by using Mathcad software. It isindicated that the obtaining of the steady states for the non-isothermalflow system is much more difficult than that for the isothermal flow systemand there are analytical solutions of steady states in isothermal flowsystem, while for the non-isothermal flow system, its analytical solutionsof steady states can not be obtained.(3) The branch figure of the steady states of flow velocity for thenon-isothermal flow system is drawn by the numerical analysis and comparedwith the isothermal flow, both the limited equilibrium point correspondingto the non-isothermal seepage field and the parameter value when thehysteresis appears all have an offset.(4) The stability of the steady states is analyzed by the iteration methodof successive lower relaxation, and the non-isothermal flow system has asaddle-node bifurcation and a fold catastrophe. But its catastrophe positionexist a rightward deviation, and the absolute value of the limited parameterb decreases a magnitude, so the catastrophe is apt to take place in thenon-isothermal flow dynamical system , namely, even if the breakingphenomenon is not very serious, the fold catastrophe may take place possiblyin the non-isothermal flow system.

     

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