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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 >Experimental constraints on bubble interactions in rhyolite melts: implications for vesicle size distributions
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Experimental constraints on bubble interactions in rhyolite melts: implications for vesicle size distributions

机译:流纹岩熔体中气泡相互作用的实验约束:对囊泡大小分布的影响。

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We have studied interactions between bubbles of two distinct size classes in rhyolite melts experimentally decompressed between 200 and 80 MPa. The first set of 'decompression' bubbles has a size range (R_(dec)) of 1-11 μm and is formed from nucleation and growth upon isothermal decompression of the melt. The larger populations of 'hydration' bubbles are on average 30-40 μm in the radius (R_(hyd)) and are formed from pore spaces present that were filled with water vapor during the saturation runs prior to the decompression experiments. The first type of interaction results in the elongation of decompression bubbles oriented radially around the larger hydration bubbles. The degree of elongation increases both as a function of distance and with increasing ratio of hydration to decompression bubble size (R_(hyd)/R_(dec)). The second type of interaction studied results in a reduction of the size of decompression bubbles located within a range of distances from 10 to 65 μm from a hydration bubble surface, relative to the modal size of the unaffected bubbles in the same sample. In addition, within an average distance of 10 μm, melt next to the hydration bubble surface is depleted in decompression bubbles. Our results indicate that concentration gradients in the melt are probably responsible for bubble size reduction and the depleted zones, because the predicted time scales for Ostwald ripening are much longer than those of the experiments. These effects persist even to the lowest ending pressures studied 80 MPa), which indicates that size distributions of small bubbles may be affected by concentration gradients in the depleted melt shell surrounding large bubbles. Large bubbles present in an ascending magma, prior to a subsequent nucleation event, could therefore affect the growth of the smaller bubble population occurring within the depleted melt shell of the larger bubbles, and produce a bimodal vesicle size distribution. Elongated decompression bubbles may be strained as a result of melt flowing away from the much larger hydration bubbles as they grow. Estimates of capillary number (Ca) plotted against deformation (D_f) indicate that bubbles in water-rich rhyolite melts are deformable, even at small sizes (1 250L蘭) and small values of Ca. Our results show a different trend of D_f with Ca than previous studies in non-geological systems predict, indicating that viscosity effects may be important. The preservation of deformation textures depends strongly on relaxation time, explaining the lack of deformation textures in less viscous natural lavas.
机译:我们研究了流纹岩熔体中两种不同尺寸类别的气泡之间的相互作用,这些气泡在200至80 MPa的压力下进行了实验性减压。第一组“减压”气泡的尺寸范围(R_(dec))为1-11μm,由熔体等温减压后的成核和生长形成。较大的“水化”气泡总体半径为(R_(hyd)),平均为30-40μm,由存在的孔隙空间形成,这些孔隙空间在减压实验之前的饱和运行期间充满了水蒸气。第一种相互作用导致径向围绕较大的水合气泡定向的减压气泡的伸长。伸长度随距离而变,并且随水合度与减压气泡尺寸的比率(R_(hyd)/ R_(dec))的增加而增加。相对于同一样品中未受影响的气泡的模态尺寸,所研究的第二种相互作用类型导致距水化气泡表面10至65μm距离内的减压气泡的尺寸减小。另外,在10μm的平均距离内,水合气泡表面附近的熔体被减压气泡消耗。我们的结果表明,熔体中的浓度梯度可能是气泡尺寸减小和贫化区域的原因,因为奥斯特瓦尔德熟化的预计时间尺度比实验时间长得多。这些影响甚至持续到研究的最低最终压力(80 MPa),这表明小气泡的尺寸分布可能会受到围绕大气泡的贫化熔体壳中浓度梯度的影响。因此,在随后的成核事件之前,存在于上升的岩浆中的大气泡可能会影响在较大气泡的贫化熔壳内发生的较小气泡种群的增长,并产生双峰囊泡尺寸分布。伸长的减压气泡可能会因熔体从长大的水化气泡生长而流失而变形。相对于变形(D_f)绘制的毛细管数(Ca)的估计值表明,即使在小尺寸(1×250L兰)和小Ca值的情况下,富水流纹岩熔体中的气泡也是可变形的。我们的结果表明,Ca的D_f趋势与非地质系统先前的研究预测的趋势不同,这表明粘度效应可能很重要。变形纹理的保存在很大程度上取决于松弛时间,这解释了在粘性较小的天然熔岩中缺乏变形纹理。

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