大陆溢流玄武岩(CFB)以两种特征熔岩形态为主。第一种类型被称为“复合型”或“丘状 pāhoehoe”,具有枕状熔岩流瓣,横截面约为 0.5-2 m,冷边缘较薄。第二种类型被称为“简单”或“片瓣”,保留了更巨大的膨胀流动内部,这些内部在数百米到公里的尺度上横向连续。先前的假设表明,有两个因素可能导致地层形态从“复合”到“简单”的变化:1)喷发持续时间增加或2)挤出速率增加。我们测试了这样的假设:挤压速率的大幅增加将导致流动形态从多个小波瓣转变为膨胀的片状波瓣,这是由于流动传播从内流表面重修主导到边缘突破主导的转变。我们使用将聚乙二醇 (PEG) 蜡挤出到直径 130 厘米的圆形水箱中,进行了比以前的研究更大、更复杂的实验。我们的工作模拟了更复杂的熔岩场,熔岩场随着距喷发口的距离而改变流动形态,这是循环流化床的特征。之前的 PEG 研究将挤出速率与近源表面形态联系起来,而我们的实验评估了流动传播机制如何随着挤出速率和距源距离的变化而变化。确定了两种流动传播方式:1)重铺,其中熔融物质突破流动表面并覆盖较旧的地壳;2)边缘突破,其中熔融物质在流动的活动远端边缘延伸到地壳之外。发现通过边缘突破传播的流动具有较低比例的重新表面区域,反之亦然。我们表明,需要进行大量的表面重整,以保留流动内的内部冷却边界和低挤压率的表面形态,而边缘突破主导的流动往往会使枕状表面形态膨胀,从而在距通风口很远的地方保留大量的内部。更高且更稳定的挤出速率往往会降低表面重修的程度,并增加源与保留的低挤出速率表面形态之间的距离。我们发现,挤出速率的增加相当于挤出速率比例因子 Ψ 值从 < 1 到 > 5 的跳跃,这对于确保从表面重修主导的叶状形态转变为边缘突破主导的传播方式是必要的。假设喷口几何形状没有变化,这相当于裂隙喷发的渗出率增加了 125 倍,点源喷发的喷发率增加了 625 倍。这相当于 1987-1990 年基拉韦厄火山喷发记录的 0.2 m 3 /s 的喷出率,增加到 125 m 3/s,通常在 2014 年冰岛 Holuhraun 喷发和 2018 年夏威夷 Leilani Estates 喷发期间测量。因此,我们认为大陆溢流玄武岩不需要异常大的喷发率,而是比小体积喷发活动的时间更长、更一致。
"点击查看英文标题和摘要"
Morphological transitions between lobate resurfacing and distal breakout lava flows in flood basalts: insights from analog experiments
Continental flood basalts (CFBs) are dominated by two characteristic lava morphologies. The first type, referred to as ‘compound’ or ‘hummocky pāhoehoe,’ exhibits pillow-like lava flow lobes with cross-sections of ~ 0.5–2 m and thin chilled margins. The second type, referred to as ‘simple’ or ‘sheet lobes’ preserves more massive, inflated flow interiors that are laterally continuous on scales of 100s of meters to kilometers. Previous hypotheses suggest that two factors may contribute to stratigraphic changes in morphology from ‘compound’ to ‘simple’: 1) increased eruption duration or 2) increased extrusion rate. We test the hypothesis that a large increase in extrusion rate would result in flow morphology transitioning from multiple small lobes to inflated sheet lobes due to a shift in flow propagation from intraflow resurfacing-dominated to marginal breakout-dominated. Using polyethylene glycol (PEG) wax extruded into a circular water-filled tank 130 cm in diameter, we produced larger, more complex experiments than previous studies. Our efforts simulated more complex lava fields which change flow morphology with distance from the eruptive vent, characteristic of CFBs. Whereas previous PEG studies linked extrusion rate to near-source surface morphologies, our experiments evaluated how flow propagation mechanisms change with variable extrusion rate and distance from the source. Two flow propagation styles were identified: 1) resurfacing, in which molten material breaks through the surface of a flow and covers the older crust and 2) marginal breakouts, in which molten material extends beyond the crust at the active distal margin of the flow. Flows that propagated via marginal breakouts were found to have lower proportions of resurfaced area and vice versa. We show that significant resurfacing is needed to preserve internal chilled boundaries within a flow and a low-extrusion-rate surface morphology, whereas marginal breakout-dominated flows tend to inflate the pillow-like surface morphology preserving a massive interior at great distances from the vent. Higher and more steady extrusion rates tend to decrease the extent of resurfacing and increase the distance between the source and preserved low-extrusion-rate surface morphologies. We find that an extrusion rate increase equivalent to a jump in the extrusion rate scaling factor, Ψ value, from < 1 to > 5 would be necessary to ensure a switch from resurfacing-dominated lobate morphologies to marginal breakout-dominated propagation style. This amounts to a factor of 125 increase in effusion rate for fissure eruptions and a factor of 625 for point source eruptions, assuming no change in vent geometry. This would be equivalent to an effusion rate of 0.2 m3/s, as documented in 1987–1990 Kīlauea eruptions, increasing to 125 m3/s, which was commonly measured during the 2014 Holuhraun eruption in Iceland and the 2018 eruption at Leilani Estates in Hawai‘i. Thus, we propose that continental flood basalts do not require unusually large effusion rates, but instead were active for a longer and more consistent time period than smaller-volume eruptions.