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Low-Temperature Plasticity and Dislocation Creep of Fangshan Dolomite

机译:方山白云岩的低温可塑性和脱臼蠕变

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To explore the rheology of dolomite and investigate recent findings regarding the so-called inversion of activation energy between dislocation and diffusion creep, we compressed medium-grained Fangshan dolomite (113 +/- 42 mu m) at effective confining pressures of 50-300 MPa, temperatures of 27 degrees C-900 degrees C, and strain rates of 10(-6) to 2 x 10(-4) s(-1) using a Paterson gas-medium apparatus. Two end-member deformation regimes with corresponding diagnostic flow laws and microstructures were identified. At temperatures <= 500 degrees C, low-temperature plasticity (LTP), which is characterized by microstructures of predominant abrupt undulatory extinctions and f-twins, was determined to dominate the deformation of Fangshan dolomite. The corresponding flow behavior can be described by an (epsilon) over dot = (epsilon) over dot(0) x exp(alpha x sigma) with alpha =0.0806 +/- 0.0078 and ln (epsilon) over dot(0)=-76.66 +/- 6.24 (Regime 1). At temperatures >= 800 degrees C, dislocation creep, which shows characteristic microstructures of smooth undulating extinction and new recrystallized grains, dominated the deformation of Fangshan dolomite. The corresponding flow behavior can be expressed by a power law equation, (epsilon) over dot = A sigma(n) exp(-Q/RT) with n = 4.75 +/- 0.58, Q=436 +/- 54kJ/mol, and logA=3.48 +/- 1.41(Regime 2). At temperatures between similar to 500 and 800 degrees C, a transition regime between LTP and dislocation creep was identified (Regime 3) with the dependence of flow stress on strain rate increasing gradually with increasing temperature. When extrapolated to natural conditions, our flow law of dislocation creep for dolomite in combination with that of diffusion creep reported by Davis et al. (2008) suggests that the dislocation creep regime of dolomite is limited to a relatively narrow region of high temperature and relatively high stress, whereas the diffusion creep regime dominates the deformation of dolomite in tectonic settings with low stress levels.
机译:为了探索白云石的流变学,并研究有关位错和扩散蠕变之间的所谓活化能反转的最新发现,我们在50-300 MPa的有效围压、27℃-900℃的温度下压缩中等粒度的房山白云石(113+/-42μm),使用Paterson气体介质装置,应变率为10(-6)到2 x 10(-4)s(-1)。确定了具有相应诊断流动规律和微观结构的两种端部构件变形状态。在<=500°C的温度下,低温塑性(LTP)被确定为房山白云石变形的主导因素,其特征是主要的突然波动灭绝和f孪晶的微观结构。相应的流动行为可以用点上的(ε)表示=点(0)上的(ε)x exp(αx西格玛),α=0.0806+/-0.0078,点(0)上的ln(ε)=-76.66+/-6.24(状态1)。在温度>=800℃时,方山白云石的变形主要由位错蠕变控制,位错蠕变显示出平滑起伏的消光和新的再结晶晶粒的特征显微结构。相应的流动行为可以用幂律方程(epsilon)表示,在n=4.75+/-0.58、Q=436+/-54kJ/mol和logA=3.48+/-1.41的情况下,点=aσ(n)exp(-Q/RT)。在类似于500到800℃的温度下,发现了LTP和位错蠕变之间的过渡区(区3),随着温度的升高,流变应力对应变率的依赖性逐渐增加。当外推到自然条件时,我们的白云石位错蠕变流动规律与Davis et al.(2008)报告的扩散蠕变流动规律相结合,表明白云石的位错蠕变状态仅限于相对狭窄的高温和相对高应力区域,而在低应力水平的构造环境中,白云石的变形主要由扩散蠕变机制控制。

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