首页> 外文期刊>Journal of geophysical research. Solid earth: JGR >Viscous constitutive relations of solid-liquid compositesin terms of grain boundary contiguity: 2. Compositional model for small melt fractions
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Viscous constitutive relations of solid-liquid compositesin terms of grain boundary contiguity: 2. Compositional model for small melt fractions

机译:固液复合材料的粘固本构关系,以晶界连续性表示:2.小熔体分数的组成模型

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We develop a compositional model for the grain boundary (GB) diffusion creep ofmelt-bearing polycrystalline aggregates. This model is an extension of the GB diffusioncontrol model by taking into account the effects of finite liquid diffusivity and finitereaction rates, which are important at small melt fractions (0). For shear viscosity 7/, thereexists a critical melt fraction 07,/ below which the rate-limiting process changes fromdiffusion through GB to diffusion through the liquid, and for bulk viscosity e, there existsa critical melt fraction c& below which the rate-limiting process changes from diffusionthrough GB to reaction at the pore surface. The implication of the model results is thatdifferent processes may limit the kinetics of bulk and shear viscosities at small 0. Themodel also predicts that stress can cause compositional and hence volumetric asymmetryin pores. As melt fraction increases from zero to the critical melt fractions, rapid decreasesoccur in n, from 77, to 0.277, and in e, from Do to 0.476, where n, represents I/ for Coblecreep. In the GB diffusion control model, these decreases occur discontinuously at zeromelt fraction, but this singularity is removed in the compositional model. For a typicalgrain size in the mantle (3 mm), the critical melt fractions are estimated semiquantitativelyas 0'2. = 10-4 and < 6 x 10-8, demonstrating the significant effect of very small amountof melt on the viscosities in the mantle.
机译:我们开发了含熔多晶聚集体的晶界(GB)扩散蠕变的成分模型。通过考虑有限的液体扩散率和有限的反应速率的影响,该模型是GB扩散控制模型的扩展,这对于小熔体分数(0)而言很重要。对于剪切粘度7 /,存在临界熔体分数07 /,低于该极限熔体分数c&,对于本体粘度e,存在一个临界熔体分数c&,低于该极限熔体极限c从GB扩散到孔表面反应。该模型结果的含义是,不同的过程可能会限制体积小和剪切粘度为0时的动力学。该模型还预测应力会导致孔隙中的成分和体积不对称。随着熔体分数从零增加到临界熔体分数,n迅速下降,n从77降低到0.277,e e从Do升高到0.476,其中n代表Coblecreep的I /。在GB扩散控制模型中,这些降低在零熔体分数下不连续发生,但是在组成模型中消除了这种奇异性。对于地幔中的典型晶粒尺寸(3毫米),临界熔体分数半定量估算为0'2。 = 10-4且<6 x 10-8,表明极少量的熔体对地幔粘度具有显着影响。

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