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Recycled materials and secondary processes controlled the chemical and isotopic compositions of bubbling gases discharged from two adjacent geothermal springs in the Northern Luzon Arc 回收材料和二次加工过程控制了北吕宋弧两个相邻地热泉所排放的冒泡气体的化学成分和同位素组成
IF 2.9 3区 地球科学 Q2 GEOSCIENCES, MULTIDISCIPLINARY Pub Date : 2024-05-17 DOI: 10.1016/j.jvolgeores.2024.108108
Jia-Yi Wu , Xue-Gang Chen , Mark Schmidt , Xiaohu Li , Chen-Tung Arthur Chen , Ying Ye

Gas emissions from hydrothermal systems can serve as indicators of subsurface activity. In addition to gas sources, hydrothermal gas geochemistry is strongly influenced by secondary processes that occur during/after hydrothermal circulation. Here, we observed statistically significant differences in the geochemical characteristics (except for helium isotopes) of bubbling gases discharged from two adjacent vents in the Northern Luzon Arc. Helium (3He/4He = 4.25–7.09 Ra) in both vents was controlled by mixing between mantle and crustal components, where about 74% of helium was contributed by the mantle. Differences in N2/Ar ratios (∼ 300–330) of the two neighboring springs are attributed to subducted materials and seawater mixing (contributing ∼2.5% N2 and Ar), rather than phase separation in the reaction zone. Specifically, Ar was mainly supplied by atmospheric components that dissolved in the percolated seawater with only 8%–9% contributed by the excess radiogenic 40Ar. Excess N2 relative to Ar was mainly supplied by the decomposition of subducted materials (83%–92%) of the South China Sea plate beneath the Philippine Sea Plate. The Lutao gases showed low CO2 concentrations (0.07–22.2 mmol/mol), despite the high 3He/4He ratios indicating a significant contribution of magmatic components. Magmatic CO2 may have been largely consumed by the high Ca Lutao vent fluids via carbonate precipitation in the reaction zone. Alternatively, stable carbon isotope compositions (δ13C) indicate that Lutao CO2 may be supplied by microbial oxidation of alkanes (e.g., CH4 with concentrations of 14.6–173 mmol/mol in the samples), with fractionation factor ΔCO2–CH4 ranging from −15‰ to −25‰ and conversion rates of <10%. Up to 65% of the CO2 in the 2016 samples experienced secondary calcite precipitation in the discharge zone. Our results indicate that recycled subducted materials could potentially affect the geochemical characteristics of gases discharged from arc-volcanic systems. In addition, the influence of secondary processes needs to be considered before tracing the sources of hydrothermal fluids and/or gases, especially in shallow-water hydrothermal systems.

热液系统排放的气体可以作为地下活动的指标。除了气体来源之外,热液循环过程中或之后发生的次生过程也会对热液气体地球化学产生重大影响。在这里,我们观察到北吕宋弧两个相邻喷口排出的冒泡气体的地球化学特征(氦同位素除外)存在显著的统计学差异。两个喷口中的氦(3He/4He = 4.25-7.09 Ra)受地幔和地壳成分混合的控制,其中约 74% 的氦来自地幔。两个相邻喷泉的 N2/Ar 比率(300-330)的差异归因于俯冲物质和海水的混合(N2 和 Ar 的贡献率为 2.5%),而不是反应区的相分离。具体来说,氩主要由溶解在渗流海水中的大气成分提供,只有8%-9%由过量的放射源40Ar提供。相对于 Ar 而言,过量的 N2 主要由菲律宾海板块下的南海板块俯冲物质分解提供(83%-92%)。尽管3He/4He比值较高,表明岩浆成分在其中占了很大比例,但卢陶气体显示出较低的二氧化碳浓度(0.07-22.2 mmol/mol)。岩浆中的二氧化碳可能在很大程度上被高钙的鲁陶喷口流体通过反应区的碳酸盐沉淀所消耗。另外,稳定碳同位素组成(δ13C)表明,鲁陶的二氧化碳可能是由微生物氧化烷烃(如样品中浓度为14.6-173毫摩尔/摩尔的CH4)提供的,分馏系数ΔCO2-CH4为-15‰至-25‰,转化率为<10%。2016年样本中高达65%的二氧化碳在排泄区经历了二次方解石沉淀。我们的研究结果表明,回收的俯冲物质有可能影响弧-火山系统排放气体的地球化学特征。此外,在追踪热液和/或气体的来源之前,需要考虑次生过程的影响,尤其是在浅水热液系统中。
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引用次数: 0
Internal structure of the volcanic island of Surtsey and surroundings: Constraints from a dense aeromagnetic survey 苏尔特西火山岛及其周边地区的内部结构:密集航磁勘测的制约因素
IF 2.9 3区 地球科学 Q2 GEOSCIENCES, MULTIDISCIPLINARY Pub Date : 2024-05-16 DOI: 10.1016/j.jvolgeores.2024.108096
Sara Sayyadi , Magnús T. Gudmundsson , James D.L. White , Thorsteinn Jónsson , Maxwell C. Brown , Marie D. Jackson

Surtsey, a young basaltic island off the south coast of Iceland, was built by volcanic activity in 1963–1967 from a pre-eruption oceanic seafloor depth of 130 m. An aeromagnetic survey was carried out in October 2021 over a 60 km2 area covering Surtsey and its surroundings. It aimed to explore the internal structure and the possible existence of basaltic intrusions associated with the five vents active at different times over the 3.5 years of eruptive activity. The survey line spacing was 200 m and the flying altitude was generally 90 m a.s.l. The strongest anomalies (amplitude ∼700 nT) are caused by the 30–100 m thick subaerially erupted lava field on the southern part of Surtsey, formed in two episodes of effusive activity:1964–1965 and 1966–1967. 2D spectral analysis and Euler deconvolution indicate that the causative bodies of anomalies outside the island of Surtsey are located within the uppermost 300 m of the seafloor and their horizontal dimensions are similar to or smaller than their depth. 3D forward modeling of the island and its surroundings, constrained by observations during the formation of the island and drill cores extracted in 1979 and 2017, is consistent with an absence, at all vents, of pillow lava and therefore effusive activity in their opening phases. However, the data support the existence of a 10–20 m thick pillow lava field on the seafloor, 2.5–3 km2 in area, extending about ∼1 km to the south of Surtsey. The field is considered to have been fed by magma reaching the seafloor via channelized intrusive flow through the foreset breccia constituting the submarine part of an emerging lava delta during the early stage of effusive eruption in May–July 1964. The general scarcity of significant magnetic bodies within the edifices is consistent with magma fragmentation dominating the submarine eruptions from the onset of activity. A small magnetic anomaly is observed over the submarine edifice of Surtla, built during short-lived activity over ∼10 days in 1963–1964. This anomaly is consistent with observed subaqueous weak or moderate explosive activity that may have allowed a dyke to be preserved within the submarine tephra mound. More violent Surtseyan activity was observed at other vents, however, and may have destroyed any initial dykes that, if preserved, might have been resolved magnetically. Indications of magnetized volcanic rocks of unknown age predating the Surtsey eruption are found beneath the flank of the ephemeral island of Jólnir, the southernmost of the Surtsey vents.

苏尔特西岛是冰岛南海岸外的一个年轻玄武岩岛,1963-1967 年由火山活动从火山爆发前海底 130 米深处建造而成。勘测的目的是探索内部结构,以及在 3.5 年的喷发活动中,在不同时期活跃的五个喷口可能存在的玄武岩侵入体。测量线间距为 200 米,飞行高度一般为 90 米(海拔高度)。最强烈的异常(振幅 ∼700 nT)由苏尔特西南部 30-100 米厚的近海喷发熔岩区引起,该熔岩区是在 1964-1965 年和 1966-1967 年两次喷发活动中形成的。二维频谱分析和欧拉解卷积表明,苏尔特西岛外的异常致因体位于海底最上层 300 米范围内,其水平尺寸与其深度相近或更小。根据该岛形成过程中的观测结果以及 1979 年和 2017 年提取的钻芯,对该岛及其周边地区进行了三维前向建模,结果表明所有喷口都没有枕状熔岩,因此在喷口形成阶段没有喷出活动。然而,这些数据支持在海底存在一个 10-20 米厚的枕状熔岩区,面积为 2.5-3 平方公里,延伸至苏尔特西以南约 1 公里处。据认为,在 1964 年 5 月至 7 月喷发的早期阶段,岩浆通过构成新兴熔岩三角洲海底部分的前置角砾岩,经由渠化侵入流到达海底。建筑物内普遍缺乏重要的磁性体,这与活动开始时海底喷发主要以岩浆破碎为主是一致的。在苏尔特拉海底火山口上观测到了一个小的磁异常,它是在 1963-1964 年 10 天左右的短暂活动中形成的。这种异常现象与观测到的水下微弱或中等程度的爆炸活动相吻合,这种活动可能使水下火山灰堆中的堤坝得以保存。不过,在其他喷口观察到的苏尔特塞火山活动更为剧烈,可能已经摧毁了任何最初的堤坝,如果这些堤坝被保留下来,可能会被磁化。在苏尔特西火山喷发最南端的短暂岛屿约尼尔岛的侧翼下,发现了苏尔特西火山喷发前磁化火山岩的迹象,其年代不详。
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引用次数: 0
Reconstructing episodic and multi-vent, rhyolitic eruptions: The ∼ 1314 CE Kaharoa eruption of the Tarawera Dome Complex, Okataina Caldera (New Zealand) 重建偶发性和多喷口流纹岩喷发:新西兰奥卡泰纳火山口塔拉韦拉圆顶复合体的 ~ 公元 1314 年卡哈罗亚火山爆发
IF 2.9 3区 地球科学 Q2 GEOSCIENCES, MULTIDISCIPLINARY Pub Date : 2024-05-16 DOI: 10.1016/j.jvolgeores.2024.108107
Andrea Todde, Jonathan N. Procter, Gabor Kereszturi

Detailed stratigraphic reconstructions and quantitative deposit characterisations of moderate to large-scale rhyolitic eruptions are limited. This hinders our ability to model the multiple eruptive phenomena and hazards associated with rhyolitic volcanism. To gain new perspectives on the patterns and behaviours of rhyolitic eruptions, we present a study on the explosive phases of the 1314 ± 12 CE Kaharoa eruption of Tarawera, New Zealand. The eruption occurred from multiple aligned vents within the Okataina Caldera and is the youngest rhyolitic eruption of the frequently active Taupō Volcanic Zone. We systematically quantify the deposit characteristics of the Kaharoa pyroclastic succession to provide new insights into the type of eruption sequence and eruptive style changes. Based on field evidence, stratigraphic correlations, grain size and componentry analyses, we subdivide the Kaharoa deposit into 24 units and identify 7 main deposit types, which are linked to different eruptive and depositional processes. The explosive activity was discontinuous, characterised by repeated discrete episodes of sustained magma discharge separated by short time breaks. The activity consisted mainly of repeated subplinian-type columns that gave way to fallout deposition and emplacement of numerous lapilli beds. This activity transitioned to a pyroclastic density current (PDC) dominated phase in response to lateral vent migration. Ash emission activity occurred within and towards the end of the explosive sequence, indicating declines in the eruptive intensity. Six main intra-eruption phases (A to F) of dominant eruptive styles are established to describe the temporal evolution of the eruption. Phases A, B and D are associated with the repeated subplinian-type activity. Phase C comprises the major PDC activity, while the final two Phases E and F are associated with ash emission during initiation of lava dome extrusion and to the final dome-building sequence. This study highlights the complex nature of episodic, multi-phase, and multi-vent, explosive to dome-forming rhyolitic eruptions, depicting a scenario of great relevance for future volcanic hazard studies at active rhyolitic volcanoes worldwide.

对中度至大规模流纹岩喷发的详细地层重建和定量沉积特征描述十分有限。这阻碍了我们模拟与流纹岩火山活动相关的多种喷发现象和危害的能力。为了从新的角度了解流纹岩喷发的模式和行为,我们对新西兰塔拉韦拉(Tarawera)发生于公元 1314 ± 12 年的卡哈罗亚(Kaharoa)喷发的爆炸阶段进行了研究。这次喷发发生在奥卡泰纳火山口(Okataina Caldera)内多个排列整齐的喷口,是频繁活动的陶波火山带最年轻的一次流纹岩喷发。我们系统地量化了卡哈罗亚火山碎屑岩演替的沉积特征,为了解喷发序列的类型和喷发方式的变化提供了新的视角。根据实地证据、地层关联、粒度和成分分析,我们将卡哈罗亚沉积物细分为 24 个单元,并确定了 7 种主要沉积物类型,这些类型与不同的喷发和沉积过程有关。火山爆发活动是不连续的,其特点是反复出现持续的岩浆排出,中间有短暂的间歇。这种活动主要包括反复出现的亚火成岩柱,随后是岩屑沉积和大量青石岩床的形成。随着喷口的横向迁移,这种活动过渡到以火成碎屑密度流(PDC)为主的阶段。火山灰喷发活动发生在爆炸序列内和爆炸序列末期,表明喷发强度下降。为描述喷发的时间演变,确定了六个主要的喷发内部阶段(A 至 F)。A、B和D阶段与反复的亚浆状活动有关。C 阶段包括主要的 PDC 活动,而最后两个阶段 E 和 F 则与熔岩穹隆挤压开始时的火山灰喷发以及最后的穹隆建造过程有关。这项研究突出了偶发、多阶段、多喷口、爆炸到穹顶形成流纹岩喷发的复杂性,描绘了一种对全世界流纹岩活火山未来火山灾害研究具有重要意义的情景。
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引用次数: 0
The impacts of lulls and peaks in eruption rate on lava flow propagation 喷发率的低谷和高峰对熔岩流传播的影响
IF 2.9 3区 地球科学 Q2 GEOSCIENCES, MULTIDISCIPLINARY Pub Date : 2024-05-15 DOI: 10.1016/j.jvolgeores.2024.108099
S.I. Peters , A.B. Clarke , E.L. Rader
<div><p>Variable effusion rates have been observed during the eruption and emplacement of lava flows which can complicate lava flow predictability. Conventional wisdom suggests that eruption rates decrease exponentially with time, however, this broad trend may also be subject to short-timescale fluctuations. Flow obstructions, changes in source diameter, channel or pond overflow, and changes within the magma reservoir to name a few factors can increase or decrease local flow rates repeatedly during an active eruption and impact the behavior of the flow. Analog experiments are a useful tool for investigating the role of changing effusion rates on flow propagation because they allow reasonably precise control of conditions and detailed documentation of resulting flows. In this work, we address the effects of decreasing and increasing extrusion rates (Q) on flow propagation and four emplacement modes common to lava flows: <em>resurfacing, marginal breakouts, inflation, and lava tubes</em>. We conducted 30 experiments by injecting dyed PEG wax into a chilled bath (∼ 0 °C) on a flat slope. We divided the experiments into two pulsatory extrusion rate patterns, or conditions: stepwise decrease followed by increase in extrusion rate (lull) and stepwise increase then decrease in extrusion rate (peak). We tested a range of flow conditions spanning from flows for which strong crust was favored (low wax temperature; low extrusion rates) and those for which weak crust was favored (high wax temperature; high extrusion rates). We found that a lull in extrusion rates when a strong crust was present promoted flow expansion and thickening via limited resurfacing, localized marginal breakouts, inflation, possible tube formation, with lower rates of flow expansion after the lull. In contrast, a lull and weak crust promoted flow expansion via widespread marginal breakouts, with flow advance rebounding after the lull, and inhibited flow thickening via inflation. A peak in extrusion rates with a strong crust favored flow expansion via widespread marginal breakouts, with flow-advance deceleration after the peak, and possible thickening via inflation. Conversely, a peak in extrusion rate with weak crust promoted flow expansion via widespread marginal breakouts, with flow-advance deceleration after the peak, and inhibited flow thickening via resurfacing and inflation. Our results have implications for pahoehoe flow emplacement and have been used to assess the most appropriate parameters to be used in a probabilistic flow propagation model, MrLavaLoba.</p></div><div><h3>Plain Language Summary</h3><p>Variable effusion rates have been observed during the eruption of lava flows which can complicate lava flow forecasts. In general, lava flow effusion rates decrease with time exponentially although there may be fluctuations in flow rate on short timescales. Flow rates can wax or wane for a variety of reasons, such as flow obstructions, changes in the shape of the erupting sourc
在熔岩流的喷发和安置过程中观察到了不同的喷出率,这可能会使熔岩流的可预测性变得复杂。传统观点认为,喷发率会随着时间的推移呈指数式下降,但这种大趋势也可能受到短时间波动的影响。流体阻塞、源直径变化、通道或池塘溢流以及岩浆库内的变化等因素都会在活跃的喷发过程中反复增加或减少局部流速,并影响流体的行为。模拟实验是研究不断变化的喷出率对岩流传播的作用的有用工具,因为模拟实验可以合理精确地控制条件,并详细记录所产生的岩流。在这项工作中,我们研究了降低和提高挤出率(Q)对熔岩流传播的影响,以及熔岩流常见的四种置换模式:重现、边缘断裂、膨胀和熔岩管。我们进行了 30 次实验,将染色的 PEG 蜡注入平坡上的冷槽(0 °C~)中。我们将实验分为两种脉动挤出速率模式或条件:挤出速率先逐步下降后上升(静止)和挤出速率先逐步上升后下降(峰值)。我们测试了一系列流动条件,包括有利于强结壳的流动(低蜡温;低挤出率)和有利于弱结壳的流动(高蜡温;高挤出率)。我们发现,在强结壳时,挤压速率的停顿会通过有限的复面、局部边缘断裂、膨胀和可能的管状形成促进流体扩张和增厚,而停顿后流体扩张的速率会降低。与此相反,平静期和弱地壳会通过广泛的边缘断裂促进水流扩张,平静期后水流推进会反弹,并通过膨胀抑制水流增厚。地壳坚固时,挤压速率达到峰值,有利于通过广泛的边缘断裂实现流体扩张,峰值后流体前进速度减慢,并可能通过膨胀实现流体增厚。相反,地壳薄弱的挤出率峰值通过广泛的边缘断裂促进流体扩张,峰值后流体推进减速,并通过重铺和膨胀抑制流体增厚。我们的研究结果对帕霍霍熔岩流的喷发有影响,并被用于评估概率熔岩流传播模型--MrLavaLoba--中最合适的参数。一般来说,熔岩流的喷出率会随着时间的推移呈指数式下降,但在短时间内可能会出现波动。流速的增减有多种原因,如流动障碍、喷发源形状的变化或从地下释放出更多岩浆。使用蜡等表现为熔岩的材料进行实验,可用于研究喷出率和后续流速的变化如何影响岩流置放。在这项工作中,我们研究了挤出率的暂时低谷和峰值对流动传播的影响。我们重点研究了熔岩流常见的四种喷出模式:重现、边缘断裂、膨胀和熔岩管。我们在平坡上将染色蜡注入冷浴(0 °C)中,进行了 30 次实验。我们将实验分为两种挤出速率模式或条件:低谷(挤出速率暂时下降)和高峰(挤出速率暂时上升)。我们测试了一系列流动条件--从强地壳流动到弱地壳流动。我们发现,在结壳较强的情况下,挤出率的低谷期会通过有限的复位和膨胀促进流体增厚,并通过局部边缘断裂、可能的管状形成和低谷期后较低的流体膨胀率促进流体扩张。与此相反,冷流和弱结壳会通过大范围的边缘断裂促进流体扩张,冷流后流体推进反弹。地壳坚固时,挤压率达到峰值,有利于通过广泛的边缘断裂实现流体扩张,并通过回升和膨胀实现流体增厚,峰值后流体前进速度减慢。相反,地壳薄弱时的挤出率峰值有利于通过广泛的边缘断裂实现流动扩张,并导致峰值后流动推进减速。这些实验可以帮助我们了解褶皱流是如何增长和增厚的,其结果可与数值模型一起用于改进流动预测。
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引用次数: 0
A lower bound on the rheological evolution of magma in the 2021 Fagradalsfjall Fires 2021 年法格拉德尔斯菲亚尔大火岩浆流变演变的下限
IF 2.9 3区 地球科学 Q2 GEOSCIENCES, MULTIDISCIPLINARY Pub Date : 2024-05-14 DOI: 10.1016/j.jvolgeores.2024.108098
Arianna Soldati , Donald B. Dingwell , Thorvaldur Thordarson , Ármann Höskuldsson , Ingibjörg Jónsdóttir , William M. Moreland , Jóna S. Pálmadóttir , Catherine R. Gallagher , Helga K. Torfadóttir , Jacqueline Grech Licari , Iðunn Kara Valdimarsdóttir , Lilja B. Pétursdóttir , Robert A. Askew

As magma temperature and composition drift and change, respectively, throughout an eruption, so does its rheology. These changes may span orders of magnitude in magma viscosity and result in orders of magnitude flow velocity changes, as well as transitions in eruptive style. In this study, we present a systematic high precision quantification of the rheological variations that occurred during the 2021 Fagradalsfjall Fires. In the field, we collected a suite of 22 representative samples emplaced between day 2 and 183 of the 2021 eruption. In the laboratory, we measured the melt viscosity of each sample in a concentric cylinder viscometer. Temperatures were initially raised to 1392 °C, and then lowered stepwise to eruptive temperatures as determined through syn-eruptive radiometric measurements. The resulting dataset is analyzed as a time series. An overall trend of viscosity decrease emerges. As the eruption progressed, melt viscosity decreased by 25%, from 40 Pa s to 30 Pa s at a constant temperature of 1200 °C. However, this trend is not monotonous. At least 3 positive spikes in viscosity can be identified, at day 80, 120, and 138 of the eruption. This trend tracks with geochemical variations.

在整个喷发过程中,岩浆温度和成分分别发生漂移和变化,其流变性也随之变化。这些变化可能跨越岩浆粘度的数量级,导致流速的数量级变化以及喷发方式的转变。在本研究中,我们对 2021 年法格拉斯菲亚尔大火期间发生的流变变化进行了系统的高精度量化。在野外,我们采集了 2021 年火山喷发第 2 天至第 183 天期间喷发的 22 个代表性样本。在实验室中,我们使用同心圆粘度计测量了每个样本的熔体粘度。温度最初升至1392 °C,然后逐步降低到通过同步喷发辐射测量确定的喷发温度。所得数据集作为时间序列进行分析。粘度总体呈下降趋势。随着喷发的进行,熔体粘度降低了 25%,在 1200 °C 的恒温条件下从 40 Pa s 降至 30 Pa s。然而,这一趋势并不单调。在喷发的第 80 天、第 120 天和第 138 天,至少可以发现三个粘度正峰值。这一趋势与地球化学变化一致。
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引用次数: 0
Time scales of olivine storage and transport as revealed by diffusion chronometry at Waitomokia Volcanic Complex, Auckland Volcanic Field, New Zealand 新西兰奥克兰火山场怀托莫基亚火山群扩散计时法揭示的橄榄石储存和迁移时间尺度
IF 2.9 3区 地球科学 Q2 GEOSCIENCES, MULTIDISCIPLINARY Pub Date : 2024-05-12 DOI: 10.1016/j.jvolgeores.2024.108094
Rosa Didonna , Heather Handley , Helena Albert , Fidel Costa

Detailed knowledge of the pre-eruptive time scales associated with magma storage and transport is vital to improve volcanic hazard forecasting in active volcanic regions. However, quantification of the timescales of volcanic processes at mafic volcanic centres in continental intraplate settings is challenging, despite them being a source of significant hazards for human populations and infrastructure due to their limited predictability in space and time. We conducted a detailed petrological study to investigate the time scales of olivine storage and transfer throughout the eruption sequence of Waitomokia Volcanic Complex, a tuff ring and scoria cone complex in the Auckland Volcanic Field. Olivine crystal textures and compositions were determined from stratigraphically-constrained samples of the volcanic complex, from the initial phreatomagmatic phase to the final magmatic phase. Olivine crystals are typically <300 μm in length and characterised by skeletal morphologies, displaying chemical zoning in forsterite (Fo = 100*Mg/[Mg + Fe]; mol%), CaO, MnO and NiO wt% contents. We classified olivine into three major groups based on their Fo core compositions: (1) normally zoned crystals with high Fo content (Fo > 85), (2) crystals with intermediate Fo contents (84–81), and (3) reversely zoned crystals with lower Fo core content (<80). Olivine chemical zoning (diffusion) profiles were modelled in the context of a specific magmatic environment linked with changes in thermodynamic variables during storage (temperature, pressure, and oxygen fugacity). We propose that the normally zoned olivine crystals grew in one magmatic environment (ME1), which subsequently intruded into a more evolved (lower MgO) environment (ME2), where they interacted and were stored for up to 135 days before their eruption. During magma ascent to the surface, a second magma mixing event occurred between ME2 and magma within a third magmatic environment (ME3), forming reversely-zoned olivine crystals yielding notably shorter ascent times of approximately a few days. The rocks from the opening phreatomagmatic phase of the eruption show a larger range in olivine group types compared to the final magmatic phase, where those from the deeper ME1 are more abundant. The short time scales of magma transport obtained in our study, on the order of days to months, should be informative of the warning times that may be encountered between the onset of volcanic unrest and an eruption in the Auckland Volcanic Field.

详细了解与岩浆储存和运输相关的爆发前时间尺度,对于改进活火山地区的火山灾害预报至关重要。然而,对大陆板块内环境中的岩浆火山中心的火山过程时间尺度进行量化具有挑战性,尽管由于其在空间和时间上的可预测性有限,它们是对人类和基础设施造成重大危害的根源。我们开展了一项详细的岩石学研究,以调查奥克兰火山场怀托莫基亚火山群(一个凝灰岩环和灼热锥复合体)整个喷发序列中橄榄石储存和转移的时间尺度。从最初的喷气岩浆阶段到最后的岩浆阶段,对火山群的地层限制样本进行了橄榄石晶体纹理和成分测定。橄榄石晶体的长度通常为 300 微米,具有骨架状形态,并显示出沸石(Fo = 100*Mg/[Mg + Fe]; mol%)、氧化钙、氧化锰和氧化镍重量百分比含量的化学分区。我们根据橄榄石的 Fo 核心成分将其分为三大类:(1) Fo 含量高(Fo > 85)的正常分带晶体;(2) Fo 含量居中(84-81)的晶体;(3) Fo 核心含量较低(<80)的反向分带晶体。橄榄石化学分带(扩散)剖面是在特定岩浆环境下,结合贮存期间热力学变量(温度、压力和氧富集度)的变化而建立的模型。我们认为,正常分带的橄榄石晶体生长在一个岩浆环境(ME1)中,随后侵入到一个更进化(氧化镁含量更低)的环境(ME2)中,在那里它们相互作用,并在喷发前储存了长达 135 天。在岩浆上升到地表的过程中,ME2 和第三个岩浆环境(ME3)中的岩浆发生了第二次岩浆混合,形成了反向分带的橄榄石晶体,使上升时间明显缩短,约为几天。与最后岩浆阶段相比,喷发初期的岩浆阶段的岩石显示出更大范围的橄榄石组类型,而在最后岩浆阶段,来自更深的 ME1 的橄榄石组类型更为丰富。我们的研究获得的岩浆迁移时间尺度很短,大约为几天到几个月,这应该能够说明奥克兰火山区从火山动荡开始到火山爆发之间的预警时间。
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引用次数: 0
The spatial distribution and evolution of volcanic vents in monogenetic fields in active extensional tectonic setting: Examples from the northern Main Ethiopian Rift (Ethiopia) 活动伸展构造背景下单源区火山喷口的空间分布和演变:埃塞俄比亚主裂谷北部(埃塞俄比亚)的实例
IF 2.9 3区 地球科学 Q2 GEOSCIENCES, MULTIDISCIPLINARY Pub Date : 2024-05-12 DOI: 10.1016/j.jvolgeores.2024.108093
Francesco Mazzarini, Ilaria Isola

Monogenetic volcanic fields are present in different geo-tectonic settings (subduction, divergence and intraplate settings) consisting of tens to hundreds of volcanic constructs (cones, maars, fissures, small shields) that are the physical expression of distributed volcanism.

Notably, the spatial distribution of the volcanic constructs in volcanic fields often shows a spatial clustering that is thought to be linked to shallow (i.e., crustal strain, structural inheritance) and deep processes (i.e., magma input, composition and rheology). Noteworthy, the spatial distribution of vents (cones, maars, fissures, small shields) is the final frame of the history of the volcanic field and does not provide information about its time-evolution.

Consequently, when a vent spatial clustering is assessed for a particular volcanic field two questions remain unanswered: i) have the vents always been clustered during the life of the volcanic field? ii) If not, when did the clustering of vents begin? To answer these questions, the spatial distributions of vents along with their morphologic classification have been applied to volcanic fields located in an active tectonic and volcanic area. The northern Main Ethiopian Rift, being its geo-tectonic setting and its geologic evolution well known, is the locale where the time evolution of vent spatial clustering can be investigated. Spatial distribution and morphometric analysis of vents have been applied to three well known monogenetic volcanic fields (Debre Zeyt, Wonji and Kone) in the northern Main Ethiopian Rift. Vent clustering initiated when about 60% of the vents formed within each of the above mentioned fields. The Kone volcanic field show vent clustering since the beginning suggesting that, within a specific tectonic setting, vent clustering is favoured by crustal strain partitioning and associated volcanic activity.

单生火山岩场存在于不同的地质构造环境中(俯冲、分异和板块内环境),由数十至数百个火山构造物(火山锥、火山口、裂隙、小盾)组成,是分布式火山活动的物理表现、值得注意的是,火山岩田中火山构造的空间分布往往显示出空间聚类,这被认为与浅层(即地壳应变、结构继承)和深层过程(即岩浆输入、成分和流变)有关。值得注意的是,喷口(圆锥、火山口、裂缝、小盾形火山口)的空间分布是火山区历史的最终定格,并不提供有关其时间演变的信息。因此,当对特定火山区的喷口空间聚类进行评估时,有两个问题仍未回答:i) 在火山区的生命周期中,喷口是否总是聚类的? ii) 如果不是,喷口聚类始于何时?为了回答这些问题,我们将喷口的空间分布及其形态分类应用于位于活跃构造和火山地区的火山区。埃塞俄比亚大裂谷北部的地质构造背景及其地质演变众所周知,因此是研究喷口空间集群时间演变的理想地点。喷口的空间分布和形态计量分析已应用于埃塞俄比亚主裂谷北部三个著名的单源火山区(Debre Zeyt、Wonji 和 Kone)。当上述每个火山带内约 60% 的喷口形成时,喷口集群就开始了。科内火山区从一开始就显示出喷口聚集现象,这表明在特定的构造环境中,地壳应变分区和相关的火山活动有利于喷口聚集。
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引用次数: 0
Near-real-time multiparametric seismic and visual monitoring of explosive activity at Sabancaya volcano, Peru 秘鲁萨班卡亚火山爆炸活动的近实时多参数地震和视觉监测
IF 2.9 3区 地球科学 Q2 GEOSCIENCES, MULTIDISCIPLINARY Pub Date : 2024-05-11 DOI: 10.1016/j.jvolgeores.2024.108097
Riky Centeno , Valeria Gómez-Salcedo , Ivonne Lazarte , Javier Vilca-Nina , Soledad Osores , Efraín Mayhua-Lopez

This study presents the development of a multiparametric system that utilizes artificial intelligence techniques to identify and analyze volcanic explosions in near real-time. The study analyzed 1343 explosions recorded between 2019 and 2021, along with seismic, meteorological, and visible image data from the Sabancaya volcano. Deep learning algorithms like the U-Net convolutional neural network were used to segment and measure volcanic plumes in images, while boosting-based machine learning ensembles were used to classify seismic events related to ash plumes. The findings demonstrate that these approaches effectively handle large amounts of data generated during seismic and eruptive crises. The U-Net network achieved precise segmentation of volcanic plumes with over 98% accuracy and the ability to generalize to new data. The CatBoost classifier achieved an average accuracy of 94.5% in classifying seismic events. These approaches enable the real-time estimation of eruptive parameters without human intervention, contributing to the development of early warning systems for volcanic hazards. In conclusion, this study highlights the feasibility of using seismic signals and images to detect and characterize volcanic explosions in near real-time, making a significant contribution to the field of volcanic monitoring.

本研究介绍了多参数系统的开发情况,该系统利用人工智能技术近乎实时地识别和分析火山爆炸。该研究分析了 2019 年至 2021 年期间记录的 1343 次爆炸,以及来自萨班卡亚火山的地震、气象和可见光图像数据。U-Net 卷积神经网络等深度学习算法被用来分割和测量图像中的火山羽流,而基于提升的机器学习集合被用来对与火山灰羽流相关的地震事件进行分类。研究结果表明,这些方法能有效处理地震和火山爆发危机期间产生的大量数据。U-Net 网络实现了对火山羽流的精确分割,准确率超过 98%,并且能够泛化到新数据。CatBoost 分类器对地震事件分类的平均准确率达到 94.5%。这些方法能够在没有人工干预的情况下实时估计火山爆发参数,有助于开发火山灾害预警系统。总之,这项研究强调了利用地震信号和图像近实时检测火山爆发并描述其特征的可行性,为火山监测领域做出了重大贡献。
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引用次数: 0
Estimating emission flux of H2S from fumarolic fields using vertical sensor array system 利用垂直传感器阵列系统估算沼气田的 H2S 排放通量
IF 2.9 3区 地球科学 Q2 GEOSCIENCES, MULTIDISCIPLINARY Pub Date : 2024-05-03 DOI: 10.1016/j.jvolgeores.2024.108090
Yutaka Miyagi , Urumu Tsunogai , Kohei Watanabe , Masanori Ito , Fumiko Nakagawa , Ryunosuke Kazahaya
<div><p>The emission flux of volatiles from each fumarolic field in volcanic and geothermal areas can be used to evaluate the current state of magmatic activity and predict its future trends. The emission flux of <span><math><mi>S</mi><msub><mi>O</mi><mn>2</mn></msub></math></span> has been quantified in many fumarolic fields using remote sensing techniques, such as differential optical absorption spectroscopy (DOAS). However, most of these remote sensing techniques are inapplicable to fumarolic fields emitting volatiles depleted in <span><math><mi>S</mi><msub><mi>O</mi><mn>2</mn></msub></math></span> to which most of the geothermal fields are classified. In this study, we developed a vertical sensor array system to quantify the emission flux of <span><math><msub><mi>H</mi><mn>2</mn></msub><mi>S</mi></math></span> from each fumarolic field by integrating the cross-sectional distributions of <span><math><msub><mi>H</mi><mn>2</mn></msub><mi>S</mi></math></span> concentrations in the volcanic plume using the vertical sensor array system. In Iwo-yama of the Kirishima volcanic complex, the cross-sectional distribution of <span><math><msub><mi>H</mi><mn>2</mn></msub><mi>S</mi></math></span> concentrations was determined using the walking traverse method by moving the vertical sensor array system in the plume perpendicular to the direction of plume transport. The emission flux of <span><math><mi>S</mi><msub><mi>O</mi><mn>2</mn></msub></math></span> (2.2 ± 0.4 ton <span><math><mi>S</mi><msub><mi>O</mi><mn>2</mn></msub></math></span>/day) was estimated from that of <span><math><msub><mi>H</mi><mn>2</mn></msub><mi>S</mi></math></span> using the walking traverse method (2.6 ± 0.5 ton <span><math><msub><mi>H</mi><mn>2</mn></msub><mi>S</mi></math></span>/day) and the molar ratio of the plume (<span><math><mi>S</mi><msub><mi>O</mi><mn>2</mn></msub></math></span>/<span><math><msub><mi>H</mi><mn>2</mn></msub><mi>S</mi><mo>=</mo><mn>0</mn><mo>.</mo><mn>45</mn></math></span>) corresponds well with that estimated optically by JMA. We concluded that the emission flux quantified using the vertical sensor array system was reliable. In the Oyunuma pond in the Kuttara volcano, the emission flux of <span><math><msub><mi>H</mi><mn>2</mn></msub><mi>S</mi></math></span> was quantified as 2.0 ton <span><math><msub><mi>H</mi><mn>2</mn></msub><mi>S</mi></math></span>/day through the fixed point method, wherein the vertical sensor array system was fixed in one point, whereas the cross sectional distribution of <span><math><msub><mi>H</mi><mn>2</mn></msub><mi>S</mi></math></span> in the plume was estimated using the natural variation in wind direction. The topography is often irregular and wind direction is variable in most fumarolic fields; thus, in general, the fixed point method should be more suitable to determine the emission flux of <span><math><msub><mi>H</mi><mn>2</mn></msub><mi>S</mi></math></span> from fumarolic fields, wherein <span><math><msub><mi>H</mi><mn>2</mn></m
火山区和地热区每个火成岩场的挥发物排放通量可用于评估岩浆活动的现状并预测其未来趋势。目前已利用遥感技术,如差分光学吸收光谱(DOAS),对许多火成岩区的二氧化硫排放通量进行了量化。然而,这些遥感技术大多不适用于排放二氧化硫贫乏挥发物的火成岩场,而大多数地热田都属于此类。在这项研究中,我们开发了一个垂直传感器阵列系统,利用垂直传感器阵列系统对火山羽流中 H2S 浓度的横截面分布进行整合,从而量化每个火成岩场的 H2S 排放通量。在雾岛火山群的硫磺山,使用行走横移法确定了 H2S 浓度的横截面分布,方法是在垂直于羽流传输方向的羽流中移动垂直传感器阵列系统。根据行走横移法估算出的 H2S 排放通量(2.6 ± 0.5 吨 H2S/天)估算出了 SO2 排放通量(2.2 ± 0.4 吨 SO2/天),烟羽的摩尔比(SO2/H2S=0.45)与 JMA 的光学估算值十分吻合。我们的结论是,利用垂直传感器阵列系统量化的排放通量是可靠的。在库塔拉火山的 Oyunuma 池塘,通过定点法,即把垂直传感器阵列系统固定在一个点上,H2S 的排放通量被量化为每天 2.0 吨 H2S,而羽流中 H2S 的横截面分布则是利用风向的自然变化估算的。大多数火成岩区的地形往往不规则,风向也不固定;因此,一般来说,定点法更适合确定火成岩区的 H2S 排放通量,因为 H2S 在硫排放总量中占主要部分。
{"title":"Estimating emission flux of H2S from fumarolic fields using vertical sensor array system","authors":"Yutaka Miyagi ,&nbsp;Urumu Tsunogai ,&nbsp;Kohei Watanabe ,&nbsp;Masanori Ito ,&nbsp;Fumiko Nakagawa ,&nbsp;Ryunosuke Kazahaya","doi":"10.1016/j.jvolgeores.2024.108090","DOIUrl":"https://doi.org/10.1016/j.jvolgeores.2024.108090","url":null,"abstract":"&lt;div&gt;&lt;p&gt;The emission flux of volatiles from each fumarolic field in volcanic and geothermal areas can be used to evaluate the current state of magmatic activity and predict its future trends. The emission flux of &lt;span&gt;&lt;math&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;msub&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; has been quantified in many fumarolic fields using remote sensing techniques, such as differential optical absorption spectroscopy (DOAS). However, most of these remote sensing techniques are inapplicable to fumarolic fields emitting volatiles depleted in &lt;span&gt;&lt;math&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;msub&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; to which most of the geothermal fields are classified. In this study, we developed a vertical sensor array system to quantify the emission flux of &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mi&gt;H&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; from each fumarolic field by integrating the cross-sectional distributions of &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mi&gt;H&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; concentrations in the volcanic plume using the vertical sensor array system. In Iwo-yama of the Kirishima volcanic complex, the cross-sectional distribution of &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mi&gt;H&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; concentrations was determined using the walking traverse method by moving the vertical sensor array system in the plume perpendicular to the direction of plume transport. The emission flux of &lt;span&gt;&lt;math&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;msub&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt; (2.2 ± 0.4 ton &lt;span&gt;&lt;math&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;msub&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;/day) was estimated from that of &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mi&gt;H&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; using the walking traverse method (2.6 ± 0.5 ton &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mi&gt;H&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;/day) and the molar ratio of the plume (&lt;span&gt;&lt;math&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;msub&gt;&lt;mi&gt;O&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;/math&gt;&lt;/span&gt;/&lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mi&gt;H&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;mo&gt;=&lt;/mo&gt;&lt;mn&gt;0&lt;/mn&gt;&lt;mo&gt;.&lt;/mo&gt;&lt;mn&gt;45&lt;/mn&gt;&lt;/math&gt;&lt;/span&gt;) corresponds well with that estimated optically by JMA. We concluded that the emission flux quantified using the vertical sensor array system was reliable. In the Oyunuma pond in the Kuttara volcano, the emission flux of &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mi&gt;H&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; was quantified as 2.0 ton &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mi&gt;H&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt;/day through the fixed point method, wherein the vertical sensor array system was fixed in one point, whereas the cross sectional distribution of &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mi&gt;H&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; in the plume was estimated using the natural variation in wind direction. The topography is often irregular and wind direction is variable in most fumarolic fields; thus, in general, the fixed point method should be more suitable to determine the emission flux of &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mi&gt;H&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/msub&gt;&lt;mi&gt;S&lt;/mi&gt;&lt;/math&gt;&lt;/span&gt; from fumarolic fields, wherein &lt;span&gt;&lt;math&gt;&lt;msub&gt;&lt;mi&gt;H&lt;/mi&gt;&lt;mn&gt;2&lt;/mn&gt;&lt;/m","PeriodicalId":54753,"journal":{"name":"Journal of Volcanology and Geothermal Research","volume":"450 ","pages":"Article 108090"},"PeriodicalIF":2.9,"publicationDate":"2024-05-03","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.sciencedirect.com/science/article/pii/S0377027324000829/pdfft?md5=912fda4ba00404380669d349488a7cd2&pid=1-s2.0-S0377027324000829-main.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"140843415","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
The Nieve volcanic cluster: A Pliocene - Pleistocene lava dome cluster in the Michoacán-Guanajuato volcanic field (México) 尼韦火山群:米却肯-瓜纳华托火山区(墨西哥)的上新世-更新世熔岩穹丘群
IF 2.9 3区 地球科学 Q2 GEOSCIENCES, MULTIDISCIPLINARY Pub Date : 2024-05-03 DOI: 10.1016/j.jvolgeores.2024.108091
Denis-Ramón Avellán , Silvestre Cardona-Melchor , Martha Gabriela Gómez-Vasconcelos , José Luis Macías , Paul William Layer , Giovanni Sosa-Ceballos , María-Camila Ruíz , Jeff Benowitz , Guillermo Cisneros-Máximo , Hugo Murcia , Mathieu Perton , Gabriela Reyes-Agustín , Felipe García-Tenorio

The Nieve monogenetic volcanic cluster is located in the central–eastern region of the Michoacán–Guanajuato volcanic field, along the Huiramba fault zone, a relay ramp in the Morelia–Acambay fault system produced by oblique north-northwest transtension. This volcanic cluster includes at least 17 middle Pliocene to late Pleistocene lava domes, two small shield volcanoes, and two scoria cones. Between 4 and 3.8 Ma, two effusive eruptions built two small shield volcanoes overlying one another, with a magma volume of 3.93 km3. Between 2.9 Ma and 21.4 ka, 17 lava domes and two scoria cones were emplaced on the flanks of these volcanoes. The entire cluster resulted in a total erupted volume of 17 km3, covering an area of  326 km2 and reaching a thickness of emplaced volcanic material of 1200 m, resulting in a magma eruption rate equivalent to 0.004 km3/ka. All the rocks associated with this cluster are within a relatively restricted range in composition, between 53.9 and 64.2 wt% SiO₂, from andesite enriched in silica to basaltic andesite. The presence of intrusive-rock xenoliths and xenocrysts with dissolution textures reveals that assimilation processes modified the magmas. Based on the regional geological record, we suggest that the establishment of the Nieve volcanic cluster has been controlled by tectonic structures and the basement of the region, which has allowed the chemical evolution of these magma batches that probably had sources in at least two deep reservoirs as reflected by the Nb/Th versus Ta/U ratio.

尼韦单源火山群位于米却肯-瓜纳华托火山区的中东部地区,沿着惠兰巴断层带,这是莫雷利亚-阿坎贝断层系统中的一个中继斜坡,由西北-北向斜张力产生。该火山群包括至少 17 个中新世到晚更新世熔岩穹丘、两个小型盾状火山和两个焦岩锥。在公元前 4 至 3.8 年间,两次喷发建造了两座相互覆盖的小型盾状火山,岩浆体积为 3.93 立方公里。在 2.9 Ma 到 21.4 ka 之间,在这些火山的侧面形成了 17 个熔岩穹丘和两个灼热锥。整个火山群的总喷发量为 17 千立方米,覆盖面积 326 平方千米,喷发的火山物质厚度达 1200 米,岩浆喷发率相当于 0.004 千立方米/千卡。与该火山群相关的所有岩石的成分范围相对有限,在 53.9 至 64.2 wt% SiO₂之间,既有富含二氧化硅的安山岩,也有玄武安山岩。侵入岩异长岩和具有溶蚀纹理的异长晶的存在表明,同化过程改变了岩浆。根据该地区的地质记录,我们认为尼韦火山群的形成受到了该地区构造结构和基底的控制,这使得这些岩浆批次的化学演变成为可能,正如 Nb/Th 与 Ta/U 的比率所反映的那样,这些岩浆的来源可能至少有两个深层储层。
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Journal of Volcanology and Geothermal Research
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