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首页> 外文期刊>Earth and Planetary Science Letters: A Letter Journal Devoted to the Development in Time of the Earth and Planetary System >Homogenization processes in silicic magma chambers by stirring and mushification (latent heat buffering)
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Homogenization processes in silicic magma chambers by stirring and mushification (latent heat buffering)

机译:通过搅拌和乳化(潜热缓冲)使硅质岩浆室内的均质化过程

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Heterogeneities in crustal magma chambers are generated by incomplete mixing of different batches of magmas, precipitation or remelting of solids similar to 10-20% denser than surrounding liquids at cooling/heating boundaries, and by liquid extraction from more dense crystalline residues. Volcanic eruptions commonly sample that heterogeneity as many deposits from large explosive events show gradients in composition, crystallinity and temperature. However, some of the most viscous of all magmas - crystal-rich rhyolites-dacites and large silicic plutons - are, in contrast. strikingly homogeneous. This observation is in stark contradiction to the common assumption that the main homogenizing process in magma chambers is mechanical mixing by convection. The timescale for convective stirring is governed by flow velocities. The faster the convective currents, the more rapidly mixing occurs. However, it is the total amount of strain that determines whether homogeneity can be attained. Here, we show that convectiving magma body needs 5-10 overturns following the introduction of heterogeneities to be homogenized to lengthscales at which diffusion is effective, irrespective of the vigor of the convection. For heterogeneities that are discrete in time and space and mechanically passive (such as patches of magmas with slightly different characteristics), the threshold of 5-10 overturns can potentially be reached if enough time is allowed for the system to convect. For heterogeneities that are continuously re-established or introduced by the convective process itself (such as density instabilities generated by crystallization at the cooling boundaries of magma chambers), convective stirring is unable to produce complete homogeneity. Therefore, to explain the low variability in major element whole-rock composition in crystal-rich dacitic/rhyolitic ignimbrites and silicic plutons, we propose that another mechanism of homogenization acts to decrease thermal, and related crystallinity variability at high crystal fraction (>50 vol.%). It is induced by latent heat buffering of silicic magmas close to the haplogranitic eutectic, and leads to the rapid equilibration of temperature (and crystal fraction) throughout the magma reservoir. As this process drives the magma body towards a uniformly high crystallinity ("crystal mush"), we refer to it as "mushification". Nevertheless, the homogeneity of both large crystal-rich silicic ignimbrites and granites also require (I) incremental growth dominated by addition of magma batches that are compositionally similar to reach the observed large sizes without inducing unmixable chemical heterogeneities and (2) some late convective stirring at high crystallinity to explain the dispersal of externally derived crystalline material, e.g. xenocrysts and antecrysts. Late mechanical mixing mostly occurs at high crystallinity (similar to 30-50 vol.% crystals) following the intrusion of hotter magmas (and gas) from below, triggering whole-reservoir convective overturn without introducing new significant gradients.
机译:地壳岩浆室内的非均质性是由于不同批次岩浆的不完全混合,在冷却/加热边界处比周围液体的密度比周围液体密度高10-20%的固体沉淀或重熔,以及从更稠密的结晶残余物中提取液体而产生的。火山喷发通常会采样为异质性,因为来自大型爆炸事件的许多沉积物在成分,结晶度和温度方面均表现出梯度。然而,相比之下,所有岩浆中最粘稠的部分是富含晶体的流纹岩-达克石和大型硅质岩体。惊人地同质。这种观察与岩浆室内主要均质化过程是对流机械混合这一普遍假设完全相反。对流搅拌的时间尺度取决于流速。对流越快,混合发生得越快。但是,应变的总量决定了是否可以实现均匀性。在这里,我们表明,对流岩浆体在引入非均质性之后需要5-10翻转,才能均匀化到有效扩散的长度尺度,而与对流的活力无关。对于在时间和空间上不连续且在机械方面无源的异质性(例如岩浆斑块的特性略有不同),如果有足够的时间让系统对流,则可能会达到5-10个翻转的阈值。对于通过对流过程本身不断重新建立或引入的非均质性(例如在岩浆室冷却边界处因结晶产生的密度不稳定性),对流搅拌无法产生完全的均质性。因此,为解释富含晶体的达格/流纹石火成岩和硅质岩体中主要元素全岩成分的低变异性,我们提出了均质化的另一种作用是降低热和相关的高结晶度(> 50 vol)下的结晶度变异性。 。%)。它是由硅质岩浆接近热成岩共晶的潜热缓冲引起的,并导致整个岩浆储层的温度(和晶体分数)迅速平衡。由于该过程将岩浆体带向统一的高结晶度(“结晶糊状物”),因此我们将其称为“糊化”。然而,富含晶体的大型硅质火成岩和花岗岩的均质性也需要(I)通过增加岩浆批料(以在观察到的大尺寸下达到观察到的大尺寸而不会引起不可混合的化学异质性)为主导的增量生长,以及(2)一些对流后期搅拌以高结晶度来解释外部衍生晶体材料的扩散,例如异晶和前晶。从下方侵入较热的岩浆(和气体)之后,后期机械混合主要发生在高结晶度(类似于30-50 vol。%的晶体)时,触发整个储层对流翻转,而不会引入新的明显梯度。

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