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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 >Time scales of crystal residence and magma chamber volume from modelling of diffusion profiles in phenocrysts: Vesuvius 1944
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Time scales of crystal residence and magma chamber volume from modelling of diffusion profiles in phenocrysts: Vesuvius 1944

机译:晶体停留时间和岩浆室体积的时标,来自对隐晶的扩散剖面建模:维苏威火山(Vesuvius)1944年

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Diffusional smoothing of Fe–Mg compositional gradients in clinopyroxene crystals from the 1944 eruption of Vesuvius is used to determine the preeruption residence times of crystals at magmatic temperatures. The result is a distribution of crystal residence times from one sample that can be used to constrain magma chamber volumes. Diffusional zones between compositionally distinct cores and rims were observed by backscattered electron (BSE) imaging to vary in width from 1.6 to 11.9 m and represent storage of crystals at magmatic temperatures for periods ranging from 4.5 months up to 9 years prior to eruption. The distribution of residence times is skewed to young ages and is best explained by the open-system behaviour of an 8.0×10~7 m~3 chamber that received an input of between 3.5×10~7 and 7.0×10~7 m~3 in the final 6 months prior to eruption. The calculated inputs, compared with contemporary observations of the emitted magma volumes, implies that some 3.0×107–6.5×10~7 m~3 of magma input did not erupt but was accommodated by chamber expansion before the 1944 eruption. This would place the preeruptive chamber volume between 1.15×10~8 and 1.5×10~8 m~3. The eruption was then triggered by a further input of ~1.9×10~7 m~3 which forced the extrusion of a similar volume of relatively degassed magma as lava flows prior to the fire-fountaining episode. The backscattered electron imaging technique for residence time determination has great potential in unravelling the histories of populations of phenocrysts in many volcanic systems.
机译:1944年维苏威火山喷发引起的斜辉石晶体中Fe-Mg组分梯度的扩散平滑用于确定岩浆温度下晶体的喷发停留时间。结果是一个样品的晶体停留时间分布,可用于限制岩浆室的体积。通过背向散射电子(BSE)成像观察到成分不同的核与边缘之间的扩散区的宽度在1.6到11.9 m之间变化,代表了在岩浆温度下晶体萌发前4.5个月至9年的时间。停留时间的分布偏向年轻年龄,最好用8.0×10〜7 m〜3腔室的开放系统行为来解释,该腔室的输入在3.5×10〜7到7.0×10〜7 m〜之间。 3在爆发前的最后6个月内。计算得出的输入值,与当代对发射的岩浆量的观察结果相比,暗示着大约3.0×107–6.5×10〜7 m〜3的岩浆输入没有爆发,而是在1944年喷发之前由室膨胀所容纳。这将使术前房的容积在1.15×10〜8和1.5×10〜8 m〜3之间。然后由〜1.9×10〜7 m〜3的进一步输入触发喷发,这迫使喷火前喷出与熔岩流相似体积的相对脱气的岩浆。用于确定停留时间的反向散射电子成像技术在揭示许多火山系统中隐晶石种群的历史方面具有巨大潜力。

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