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Experimental deformation of partially melted granite revisited: implications for the continental crust

机译:重现部分熔融花岗岩的实验变形:对大陆壳的影响

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A review and reinterpretation of previous experimental data on the deformation of partially melted crustal rocks reveals that the relationship of aggregate strength to melt fraction is non-linear, even if plotted on a linear ordinate and abscissa. At melt fractions, Phi < 0.07, the dependence of aggregate strength on Phi is significantly greater than at Phi > 0.07. This melt fraction (Phi = 0.07) marks the transition from a significant increase in the proportion of melt-bearing grain boundaries up to this point to a minor increase thereafter. Therefore, we suggest that it is the increase of melt-interconnectivity that causes the dramatic strength drop between the solidus and a melt fraction of 0.07. We term this drop the 'melt connectivity transition' (MCT). A second, less-pronounced strength drop occurs at higher melt fractions and corresponds to the breakdown of the solid (crystal) framework. This is the 'solid-to-liquid transition' (SLT), corresponding to the well known 'rheologically critical melt percentage'. Although the strength drop at the SLT is about four orders of magnitude, the absolute value of this drop is small compared with the absolute strength of the unmelted aggregate, rendering the SLT invisible in a linear aggregate strength v. melt-fraction diagram. On the other hand, the more important MCT has been overlooked in previous work because experimental data usually are plotted in logarithmic strength v. melt-fraction diagrams, obscuring large strength drops at high absolute strength values. We propose that crustal-scale localization of deformation effectively coincides with the onset of melting, pre-empting attainment of the SLT in most geological settings. The SLT may be restricted to controlling flow localization within magmatic bodies, especially where melt accumulates.
机译:对先前关于部分熔融的地壳岩石变形的实验数据的回顾和重新解释表明,即使以线性纵坐标和横坐标绘制,骨料强度与熔融分数的关系也是非线性的。在熔体分数Phi <0.07时,聚集强度对Phi的依赖性显着大于Phi> 0.07时的强度。此熔体分数(Phi = 0.07)标志着从含熔体晶界比例的显着增加到此点的过渡。因此,我们认为是由于熔体相互连接性的增加导致固相线和熔体分数为0.07之间的急剧降低。我们称此为“融化连接过渡”(MCT)。第二个不那么明显的强度下降出现在较高的熔体分数下,并且对应于固体(晶体)骨架的分解。这是“固-液转变”(SLT),对应于众所周知的“流变临界熔体百分比”。尽管SLT处的强度下降约为四个数量级,但与未熔融骨料的绝对强度相比,该下降的绝对值较小,从而使SLT在线性骨料强度与熔体分数图之间不可见。另一方面,更重要的MCT在以前的工作中被忽略了,因为实验数据通常以对数强度与熔体分数图的形式绘制,从而掩盖了高绝对强度值下的大强度下降。我们提出,地壳尺度的形变局部化与融化的开始有效地相吻合,从而在大多数地质环境中抢先实现了SLT。 SLT可能仅限于控制岩浆体内的流动局部化,特别是在熔体聚集的地方。

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