火山通道岩浆流动动力学模型在天池火山喷发过程中的应用

魏海泉 Melnik O 刘永顺 Barmin A Sparks RSJ. 火山通道岩浆流动动力学模型在天池火山喷发过程中的应用[J]. 岩石学报, 2006, 22(12): 3007-3013.
引用本文: 魏海泉 Melnik O 刘永顺 Barmin A Sparks RSJ. 火山通道岩浆流动动力学模型在天池火山喷发过程中的应用[J]. 岩石学报, 2006, 22(12): 3007-3013.
WEI HaiQuan, Melnik O, LIU YongShun, Barmin A, Sparks RSJ. Conduit modeling of magma flow dynamics: a case study on the eruptive process at the Tianchi volcano[J]. Acta Petrologica Sinica, 2006, 22(12): 3007-3013.
Citation: WEI HaiQuan, Melnik O, LIU YongShun, Barmin A, Sparks RSJ. Conduit modeling of magma flow dynamics: a case study on the eruptive process at the Tianchi volcano[J]. Acta Petrologica Sinica, 2006, 22(12): 3007-3013.

火山通道岩浆流动动力学模型在天池火山喷发过程中的应用

  • 基金项目:

    本项目得到了自然科学基金项目(40172033)、科技部火山预警项目(2002DIA20009-20)以及人事部优秀回国人员基金的经费支持. 致谢本文系多年来中外作者合作研究天池火山的成果之一,研究过程中得到了国家自然科学基金,科技部攻关项目与火山预警项目的支持.野外工作得到了吉林省地震局、吉林省地矿局有关领导与同事的大力支持.特别要感谢的是吉林省地震局郑雅琴局长、吉林省地矿局金伯禄高工的大力支持与合作.

Conduit modeling of magma flow dynamics: a case study on the eruptive process at the Tianchi volcano

  • 在圆柱形火山通道的下部,岩浆上升速度与岩浆粘度、密度及压力有关。这时的流体动力学过程可以应用一般的牛顿流体模型。火山通道中部气泡化岩浆上升时,液相和气相的转化符合质量守恒方程,混合相总体符合动量守恒方程。其中气泡形成与生长过程符合达西定律与数密度方程。在火山通道靠上部的碎屑化带里,不同组分符合质量守恒方程,混合相总体符合动量守恒方程。天池火山千年大喷发时,通道直径是62m。岩浆房内的岩浆舍有约3%体积百分数的气泡,气泡体积在65%时岩浆破碎,颗粒离开通道时的速度是145ms^-1,而气体离开通道时的速度是170ms^-1。气体颗粒分散相出口压力是12.2MPa。在破火山口塌陷之前,岩浆房内气泡体积可高达30%-40%。与此同时,碎屑化发生时岩浆的孔隙度也增加到70%-75%左右。这时的出口压力降低至7—8MPa,出口气体速度增加到180ms^-1。气象站碱流质寄生火山喷发对应的喷发通道直径是40m,喷发以气体出口速度15-25ms^-1的弱爆破性喷发和侵出式喷发为特征。这时浮岩的孔隙度比千年大喷发的孔隙度低,为48%~61%,而浮岩密度高,为1.01~1.35gcm^-3。在侵出相喷发时最高释放率可以达到42m^3s^-1(致密岩石当量DRE),孔隙度变化范围是70%-80%。
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出版历程
收稿日期:  2005-10-16
修回日期:  2006-11-20
刊出日期:  2006-12-31

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