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H2O diffusion in dacitic and andesitic melts

机译:H2O扩散到大山和安山岩熔体中

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The diffusion of water in dacitic and andesitic melts was investigated at temperatures of 1458 to 1858 K and pressures between 0.5 and 1.5 GPa using the diffusion couple technique. Pairs of nominally dry glasses and hydrous glasses containing between 1.5 and 6.3 wt.% dissolved H2O were heated for 60 to 480s in a pis on cylinder apparatus. Concentration profiles of hydrous species (OH groups and H2O molecules) and total water (C-H2O = sum of OH and H2O) were measured along the cylindrical axis of the diffusion sample using IR microspectroscopy. Electron microprobe traverses show no significant change in relative proportions of anhydrous components along H2O profiles, indicating that our data can be treated as effective binary interdiffusion between H2O and the rest of the silicate melt. Bulk water diffusivity (D-H2Ot) was derived from profiles of total water using a modified Boltzmann-Matano method as well as using fittings assuming a functional relationship between D, C, and In dacitic melts D-H2Ot is proportional to C-H2Ot up to 6 wt.%. In andesitic melts the dependence of D-H2Ot on C-H2Ot is less pronounced. A pressure effect on water diffusivity could not be resolved for either dacitic or andesitic melt in the range 0.5 to 1.5 GPa. Combining our results with previous studies on water diffusion in rhyolite and basalt show that for a given water content D-H2Ot increases monotonically with increasing melt depolymerization at temperatures >1500 K. Assuming an Arrhenian behavior in the whole compositional range, the following formulation was derived to estimate D-H2Ot (m(2)/s) at 1 wt.% H2Ot in melts with rhyolitic to andesitic composition as a function of T(K) P(MPa) and S(wt.% SiO2):log D-H2Ot = (-0.757-0.0868 (.) S) + (-14.785 + 131.7 (.) S)/T + (3.079-0.0490 (.) S) (.) P/TThe experimental data (69 in total. covering 803 to 1848 K and 0.1 to 1500 MPa) are. reproduced by this relationship with a standard error of 0.12 too units. Using proportionality between water content and bulk water diffusivity. the above equation can also be used to estimate D-H2Ot in rhyolite to dacite containing up to 2 wt.% H2Ot at magmatic temperatures. For andesitic melts the functional relationship between D-H2Ot and C-H2Ot is not known at magmatic temperatures and. hence, application of our model remains uncertain for such conditions. As the activation energy for water diffusion increases from rhyolite to andesite, the diffusivities become similar at intermediate temperatures. Below 1000 K (depending on H2O content and pressure), water diffusion may be faster in rhyolite than in dacite than in andesite. Copyright (C) 2004 Elsevier Ltd.
机译:使用扩散耦合技术在1458至1858 K的温度和0.5至1.5 GPa的压力下研究了水在Datictic和Andestic熔体中的扩散。将成对的干燥玻璃和含水玻璃溶解在1.5至6.3 wt。%之间的水在pis on cylinder设备上加热60至480s。使用红外显微技术沿着扩散样品的圆柱轴测量含水物(OH基和H2O分子)和总水(C-H2O = OH和H2O之和)的浓度分布。电子探针横移显示无水组分沿H2O分布的相对比例无明显变化,表明我们的数据可被视为H2O与其余硅酸盐熔体之间的有效二元互扩散。散水扩散率(D-H2Ot)是使用改良的Boltzmann-Matano方法以及假设D,C和C的函数关系从拟合中从总水的分布中得出的.D-H2Ot与C-H2Ot成正比至6重量%。在安山岩熔体中,D-H2Ot对C-H2Ot的依赖性不太明显。在0.5至1.5 GPa的范围内,无论是Datic还是Andestic熔体,都无法解决对水扩散系数的压力影响。将我们的结果与先前在流纹岩和玄武岩中水扩散的研究相结合,表明对于给定的水含量,D-H2Ot在> 1500 K的温度下随着熔体解聚的增加而单调增加。假定在整个组成范围内有阿雷尼行为,则得出以下公式估算熔体中流延至安山岩成分的熔体中H-Ot为1%(重量)时的D-H2Ot(m(2)/ s):T(K)P(MPa)和S(wt。%SiO2):log D- H2Ot =(-0.757-0.0868(。)S)+(-14.785 + 131.7(。)S)/ T +(3.079-0.0490(。)S)(。)P / T实验数据(总共69个,覆盖803个)至1848 K和0.1至1500 MPa)。通过这种关系复制的标准误差也为0.12个单位。使用水含量与散水扩散率之间的比例关系。上式还可以用来估算在岩浆温度下流纹岩至方晶石中的D-H2Ot含量高达2 wt。%H2Ot。对于安山型熔体,D-H2Ot和C-H2Ot之间的功能关系在岩浆温度下未知。因此,在这种情况下我们模型的应用仍然不确定。随着水扩散的活化能从流纹岩到安山岩的增加,在中等温度下扩散率变得相似。低于1000 K(取决于H2O含量和压力),流纹岩中的水扩散速度可能比榴辉岩中的水扩散快于安山岩中的水扩散。版权所有(C)2004 Elsevier Ltd.

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