Jambon A, Zhang Y, Stolper E M
Laboratoire MAGIE, Université Pierre et Marie Curie, Paris, France.
Geochim Cosmochim Acta. 1992;56:2931-5. doi: 10.1016/0016-7037(92)90369-t.
Water diffusion experiments were carried out by dehydrating rhyolitic obsidian from Valles Caldera (New Mexico, USA) at 510-980 degrees C. The starting glass wafers contained approximately 0.114 wt% total water, lower than any glasses previously investigated for water diffusion. Weight loss due to dehydration was measured as a function of experiment duration, which permits determination of mean bulk water diffusivity, mean Dw. These diffusivities are in the range of 2.6 to 18 X 10(-14) m2/s and can be fit with the following Arrhenius equation: ln mean Dw (m2/s) = -(25.10 +/- 1.29) - (46,480 +/- 11,400) (J/mol) / RT, except for two replicate runs at 510 degrees C which give mean Dw values much lower than that defined by the above equation. When interpreted according to a model of water speciation in which molecular H2O is the diffusing species with concentration-independent diffusivity while OH units do not contribute to the transport but react to provide H2O, the data (except for the 510 degrees C data) are in agreement with extrapolation from previous results and hence extend the previous data base and provide a test of the applicability of the model to very low water contents. Mean bulk water diffusivities are about two orders of magnitude less than molecular H2O diffusivities because the fraction of molecular H2O out of total water is very small at 0.114 wt% total water and less. The 510 degrees C experimental results can be interpreted as due to slow kinetics of OH to H2O interconversion at low temperatures.
通过在510 - 980摄氏度下对来自美国新墨西哥州瓦莱斯卡尔德拉的流纹质黑曜岩进行脱水处理来开展水扩散实验。起始玻璃薄片的总含水量约为0.114 wt%,低于之前用于水扩散研究的任何玻璃。测量脱水导致的重量损失作为实验持续时间的函数,这使得能够确定平均体相水扩散率,即平均Dw。这些扩散率在2.6至18×10⁻¹⁴ m²/s范围内,并且可以用以下阿伦尼乌斯方程拟合:ln平均Dw(m²/s)= -(25.10 ± 1.29) - (46,480 ± 11,400) (J/mol)/ RT,但在510摄氏度下的两次重复实验给出的平均Dw值远低于上述方程所定义的值。当根据水的形态模型进行解释时,其中分子H₂O是具有与浓度无关的扩散率的扩散物种,而OH单元不参与传输但反应以提供H₂O,这些数据(除了510摄氏度的数据)与先前结果的外推一致,因此扩展了先前的数据库,并对该模型在极低含水量下的适用性进行了测试。平均体相水扩散率比分子H₂O扩散率小约两个数量级,因为在总含水量为0.114 wt%及更低时,分子H₂O占总水的比例非常小。510摄氏度的实验结果可以解释为是由于低温下OH向H₂O相互转化的动力学缓慢所致。