...
首页> 外文期刊>Journal of Volcanology and Geothermal Research2012V243-244NOCT,15 >Non-eruptive ice melt driven by internal heat at glaciated stratovolcanoes
【24h】

Non-eruptive ice melt driven by internal heat at glaciated stratovolcanoes

机译:冰川平流层火山内部热量驱动的非火山喷发冰融化

获取原文
获取原文并翻译 | 示例

摘要

Mudflows, floods and lahars from rapid snow and ice melting present potentially devastating hazards to populations surrounding glacial stratovolcanoes. Most ice-melt induced lahars have resulted from eruptive processes. However, there is evidence for non-eruptive hydrothermal volcanic unrest generating rapid and hazardous glacial melt. Here, we use TOUGH2 numerical fluid flow simulations to explore ice melt potential associated with hydrothermal perturbation. Our simulations are loosely based on Cotopaxi Volcano, Ecuadorian Andes. We show that dynamic permeability has a strong control on ice melt response to perturbation. In the absence of concurrent permeability increases, the delay time between onset of a deep hydrothermal perturbation and a response in surface heat flow is on the order of many 10s of years. When increased hot fluid influx at depth is combined with permeability enhancement, the surface heat flow response can be immediate. However, our results suggest that melt rates resulting from such hydrothermal perturbation are still orders of magnitude lower than those induced by eruptive processes; potentially hazardous melt volumes take many months to accumulate, compared to minutes for eruption induced melting. Additional mechanisms, such as glacier destabilisation, meltwater impounding and hydrothermal outburst, may be required to generate volumes of water similar to those associated with catastrophic eruption initiated ice-melt lahars. (C) 2016 Published by Elsevier B.V.
机译:快速冰雪融化造成的泥流,洪水和拉哈尔河对冰川平流火山周围的居民构成潜在的破坏性危害。大多数由冰融化引起的拉哈尔是由喷发过程造成的。但是,有证据表明非火山爆发的热液火山爆发会产生快速而危险的冰川融化。在这里,我们使用TOUGH2数值流体模拟来探索与水热扰动有关的冰融化潜力。我们的模拟大致基于厄瓜多尔安第斯山脉的科托帕希火山。我们显示动态渗透率对冰融化对扰动的响应有很强的控制力。在没有同时渗透率增加的情况下,深部热液扰动开始与表面热流响应之间的延迟时间约为数十年。当深处增加的热流体涌入与渗透率增强相结合时,表面热流响应会立即发生。然而,我们的结果表明,由这种水热扰动引起的熔体速率仍比喷发过程引起的熔体速率低几个数量级。潜在危险的熔体体积需要花费数月的时间才能积聚,而喷发诱导的熔体则需要数分钟。可能需要其他机制,例如冰川破坏,融水蓄积和热液喷发,以产生类似于与灾难性喷发引发的冰融融哈拉相关的水量。 (C)2016由Elsevier B.V.发布

著录项

相似文献

  • 外文文献
  • 中文文献
  • 专利
获取原文

客服邮箱:kefu@zhangqiaokeyan.com

京公网安备:11010802029741号 ICP备案号:京ICP备15016152号-6 六维联合信息科技 (北京) 有限公司©版权所有
  • 客服微信

  • 服务号