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Dislocation creep of polycrystalline dolomite

机译:多晶白云石的位错蠕变

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The field of dislocation creep and rheological parameters for coarse-grained (d=240μm) natural dolomite has been determined through experiments performed at temperatures of 700-1000°C, effective pressures of 300-900MPa and strain rates of 10~(-4)/s to 10~(-7)/s. At low strain (<7%), dolomite aggregates deform homogeneously and define a power law between strain rate and differential stress with a stress exponent of 3.0+/-0.1, but at higher strains, through-going, fine-grained (<10μm) shear zones develop in the dolomite aggregates concomitant with strain weakening. Recrystallization is limited at low strain and microstructures observed in the low strain samples include undulatory extinction, twins, grain boundary bulging, limited recrystallization along twins and fluid inclusion trails. These same microstructures are present outside of the narrow, through-going shear zones in high strain samples; however, within the shear zones the grain size is small (<10μm) with some larger porphyroclasts (20-50μm). Shear zones nucleate at fine-grained zones formed at twin boundaries, twin-twin intersections and fluid inclusion trails and is likely due to a switch in deformation mechanism due to the large strength contrast between the fine-grained zones deforming by diffusion creep and the coarse-grained protolith. The activation energy (Q) for creep of coarse-grained dolomite at low strain is 145kJ/mol. In contrast to other activation energies for dislocation and diffusion creep of minerals, Q for dislocation creep of dolomite is considerably less than that for diffusion creep (248kJ/mol). The results of this study indicate that coarse-grained dolomite will initially deform by dislocation creep at natural strain rates and temperatures between 200 and 550°C, but due to limited recovery mechanisms, fine-grained shear zones will nucleate and diffusion creep may control the rheology of these fine-grained shear zones in nature at temperatures above ~300°C.
机译:通过在700-1000°C的温度,300-900MPa的有效压力和10〜(-4)的应变速率下进行的实验确定了粗粒(d =240μm)天然白云石的位错蠕变场和流变参数。 / s至10〜(-7)/ s。在低应变(<7%)时,白云石聚集体均匀变形,并在应变速率和差应力之间定义幂律,应力指数为3.0 +/- 0.1,但在较高应变下,贯穿的细粒度(<10μm )剪切带在白云岩聚集体中形成,并伴随着应变减弱。在低应变下再结晶受到限制,并且在低应变样品中观察到的微观结构包括起伏消光,孪晶,晶界凸起,沿孪晶的有限再结晶和流体包裹体痕迹。这些相同的微观结构存在于高应变样品中狭窄的,贯穿的剪切区域之外。但是,在剪切区内,晶粒尺寸较小(<10μm),而较大的卟啉弹性体(20-50μm)。剪切区在双边界,双孪生相交和流体包裹体轨迹处形成的细颗粒区成核,这很可能是由于变形机理的转换所致,这是由于细颗粒区域因扩散蠕变和粗糙而产生的大强度反差所致。颗粒的原石。低应变下粗粒白云岩蠕变的活化能(Q)为145kJ / mol。与矿物的位错和扩散蠕变的其他活化能相反,白云石的位错蠕变的Q明显小于扩散蠕变的(248kJ / mol)。这项研究的结果表明,在自然应变率和200至550°C的温度下,粗粒白云石会首先因位错蠕变而变形,但由于有限的恢复机制,细粒剪切带将成核,而扩散蠕变可能会控制蠕变。自然界中这些细颗粒剪切区的流变学温度高于〜300°C。

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