Cigala Valeria, Kueppers Ulrich, Fernández Juan José Peña, Dingwell Donald B
Ludwig-Maximilians-Universität (LMU) Munich, Theresienstr 41, 80333 Munich, Germany.
Bull Volcanol. 2021;83(8):53. doi: 10.1007/s00445-021-01473-0. Epub 2021 Jul 20.
Predicting the onset, style and duration of explosive volcanic eruptions remains a great challenge. While the fundamental underlying processes are thought to be known, a clear correlation between eruptive features observable above Earth's surface and conditions and properties in the immediate subsurface is far from complete. Furthermore, the highly dynamic nature and inaccessibility of explosive events means that progress in the field investigation of such events remains slow. Scaled experimental investigations represent an opportunity to study individual volcanic processes separately and, despite their highly dynamic nature, to quantify them systematically. Here, impulsively generated vertical gas-particle jets were generated using rapid decompression shock-tube experiments. The angular deviation from the vertical, defined as the "spreading angle", has been quantified for gas and particles on both sides of the jets at different time steps using high-speed video analysis. The experimental variables investigated are 1) vent geometry, 2) tube length, 3) particle load, 4) particle size, and 5) temperature. Immediately prior to the first above-vent observations, gas expansion accommodates the initial gas overpressure. All experimental jets inevitably start with a particle-free gas phase (gas-only), which is typically clearly visible due to expansion-induced cooling and condensation. We record that the gas spreading angle is directly influenced by 1) vent geometry and 2) the duration of the initial gas-only phase. After some delay, whose length depends on the experimental conditions, the jet incorporates particles becoming a gas-particle jet. Below we quantify how our experimental conditions affect the temporal evolution of these two phases (gas-only and gas-particle) of each jet. As expected, the gas spreading angle is always at least as large as the particle spreading angle. The latter is positively correlated with particle load and negatively correlated with particle size. Such empirical experimentally derived relationships between the observable features of the gas-particle jets and known initial conditions can serve as input for the parameterisation of equivalent observations at active volcanoes, alleviating the circumstances where an a priori knowledge of magma textures and ascent rate, temperature and gas overpressure and/or the geometry of the shallow plumbing system is typically chronically lacking. The generation of experimental parameterisations raises the possibility that detailed field investigations on gas-particle jets at frequently erupting volcanoes might be used for elucidating subsurface parameters and their temporal variability, with all the implications that may have for better defining hazard assessment.
The online version contains supplementary material available at 10.1007/s00445-021-01473-0.
预测火山爆发的起始、方式和持续时间仍然是一个巨大的挑战。虽然人们认为基本的潜在过程是已知的,但地球表面以上可观测到的喷发特征与紧邻地下的条件和特性之间的明确关联还远未完善。此外,爆炸事件的高度动态性质以及难以接近性意味着对此类事件进行实地调查的进展仍然缓慢。比例缩放的实验研究为分别研究单个火山过程提供了一个机会,并且尽管这些过程具有高度动态性质,但仍能对其进行系统量化。在这里,利用快速减压激波管实验产生了脉冲式垂直气粒射流。通过高速视频分析,在不同时间步长下对射流两侧的气体和颗粒的与垂直方向的角偏差(定义为“扩展角”)进行了量化。所研究的实验变量有:1)喷口几何形状,2)管道长度,3)颗粒负载,4)颗粒大小,以及5)温度。在首次在喷口上方进行观测之前,气体膨胀以适应初始气体超压。所有实验射流不可避免地都从无颗粒的气相(仅气体)开始,由于膨胀引起的冷却和冷凝,这一阶段通常清晰可见。我们记录到气体扩展角直接受1)喷口几何形状和2)初始仅气体阶段的持续时间影响。经过一定延迟(延迟长度取决于实验条件)后,射流裹挟颗粒变成气粒射流。下面我们将量化我们的实验条件如何影响每个射流这两个阶段(仅气体和气粒)的时间演化。正如预期的那样,气体扩展角总是至少与颗粒扩展角一样大。后者与颗粒负载呈正相关,与颗粒大小呈负相关。气粒射流的可观测特征与已知初始条件之间的这种基于实验得出的经验关系可作为对活火山等效观测进行参数化的输入,缓解通常长期缺乏对岩浆纹理、上升速率、温度、气体超压和/或浅部管道系统几何形状的先验知识的情况。实验参数化的产生增加了一种可能性,即对频繁喷发火山的气粒射流进行详细的实地调查可用于阐明地下参数及其时间变化性,这可能对更好地定义灾害评估具有所有相关意义。
在线版本包含可在10.1007/s00445 - 021 - 01473 - 0获取的补充材料。