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851.
Nature and origin of cone-forming volcanic breccias in the Te Herenga Formation, Ruapehu, New Zealand 总被引:1,自引:1,他引:0
Volcanic breccias form large parts of composite volcanoes and are commonly viewed as containing pyroclastic fragments emplaced
by pyroclastic processes or redistributed as laharic deposits. Field study of cone-forming breccias of the andesitic middle
Pleistocene Te Herenga Formation on Ruapehu volcano, New Zealand, was complemented by paleomagnetic laboratory investigation
permitting estimation of emplacement temperatures of constituent breccia clasts. The observations and data collected suggest
that most breccias are autoclastic deposits. Five breccia types and subordinate, coherent lava-flow cores constitute nine,
unconformity-bounded constructional units. Two types of breccia are gradational with lava-flow cores. Red breccias gradational
with irregularly shaped lava-flow cores were emplaced at temperatures in excess of 580 °C and are interpreted as aa flow
breccias. Clasts in gray breccia gradational with tabular lava-flow cores, and in some places forming down-slope-dipping avalanche
bedding beneath flows, were emplaced at varying temperatures between 200 and 550 °C and are interpreted as forming part of
block lava flows. Three textural types of breccia are found in less intimate association with lava-flow cores. Matrix-poor,
well-sorted breccia can be traced upslope to lava-flow cores encased in autoclastic breccia. Unsorted boulder breccia comprises
constructional units lacking significant exposed lava-flow cores. Clasts in both of these breccia types have paleomagnetic
properties generally similar to those of the gray breccias gradational with lava-flow cores; they indicate reorientation after
acquisition of some, or all, magnetization and ultimate emplacement over a range of temperatures between 100 and 550 °C.
These breccias are interpreted as autoclastic breccias associated with block lava flows. Matrix-poor, well-sorted breccia
formed by disintegration of lava flows on steep slopes and unsorted boulder breccia is interpreted to represent channel-floor
and levee breccias for block lava flows that continued down slope. Less common, matrix-rich, stratified tuff breccias consisting
of angular blocks, minor scoria, and a conspicuously well-sorted ash matrix were generally emplaced at ambient temperature,
although some deposits contain clasts possibly emplaced at temperatures as high as 525 °C. These breccias are interpreted
as debris-flow and sheetwash deposits with a dominant pyroclastic matrix and containing clasts likely of mixed autoclastic
and pyroclastic origin. Pyroclastic deposits have limited preservation potential on the steep, proximal slopes of composite
volcanoes. Likewise, these steep slopes are more likely sites of erosion and transport by channeled or unconfined runoff rather
than depositional sites for reworked volcaniclastic debris. Autoclastic breccias need not be intimately associated with coherent
lava flows in single outcrops, and fine matrix can be of autoclastic rather than pyroclastic origin. In these cases, and likely
many other cases, the alternation of coherent lava flows and fragmental deposits defining composite volcanoes is better described
as interlayered lava-flow cores and cogenetic autoclastic breccias, rather than as interlayered lava flows and pyroclastic
beds. Reworked deposits are probably insignificant components of most proximal cone-forming sequences.
Received: 1 October 1998 / Accepted: 28 December 1998 相似文献
852.
STUDY OF THE LAVA FLOW HAZARD ZONING BASED ON THE KINEMATIC THERMO-RHEOLOGICAL MODEL:EXAMPLE STUDY FOR THE ASHIKULE VOLCANO,XINJIANG 下载免费PDF全文
The lava flow hazard is an important and frequent disaster for residents in the volcanic area. In this paper, we focus on the lava flow inundation hazard zoning based on the example case of the Ashikule volcano in Xinjiang, China. Firstly, the parameters of magma such as density, viscosity and temperature are calculated by the empirical formula of magma utilizing results of previous field geological survey and petrology analysis. Then, using the kinematic thermo-rheological model, we simulated the inundation area of lava flow from Ashi volcano at the effusion rates of 200m3/s and 500m3/s. The simulation results of Ashi volcano well coincide to the geological map and verify that the method and parameters are valid. Then the applied simulations were carried out to calculate the lava flow inundation area in future eruption at Ashi, Wuluke and Daheishan crater with different effusion rates. At last, according to the analysis of the applied simulation results and drawing lessons from the foreign disaster zoning method, the four-level hazard zoning was built and set with different colors. The first level with red color is the extra-dangerous zone that is always inundated in any eruption but only distributes near the lava spillway of the crater. The second level with orange color is the dangerous zone that is inundated in the medium scale eruption. The third level with yellow color is the sub-dangerous zone that is corresponding to the large eruption. The fourth level with blue color is the potential dangerous zone that is only inundated in the extra-large eruption. In addition, we put forward the suggestion to respond to and avoid the disaster in future. Although China has not been affected by the lava flow for nearly three hundred years, the prospective study in this paper will lay the foundation for the study of related disasters, and provide the reference for the major construction projects in the volcanic area. 相似文献
853.
PRELIMINARY VOLCANIC HAZARD ZONATION IN JINLONGDINGZI VOLCANO,LONGANG VOLCANO AREA,JILIN PROVINCE,CHINA 下载免费PDF全文
Longgang volcano cluster is 150km away from the Tianchi volcano, located in Jingyu and Huinan Counties, Jilin Province, China. It had a long active history and produced hundreds of volcanoes. The latest and largest eruption occurred between 1 500 and 1 600 years ago by Jinlongdingzi(JLDZ)volcano which had several eruptions in the history. This paper discusses the volcanic hazard types, and using the numerical simulations of lava flow obtained with the Volcflow model, proposes the hazard zonation of JLDZ volcano area. JLDZ volcano eruption type is sub-plinian, which produced a great mass of tephra fallout, covering an area of 260km2. The major types of volcanic hazards in JLDZ area are lava flow, tephra fallout and spatter deposits. Volcflow is developed by Kelfoun for the simulation of volcanic flows. The result of Volcflow shows that the flows are on the both sides of the previous lava flows which are low-lying areas now. According to the physical parameters of historical eruption and Volcflow, we propose the preliminary volcanic hazard zonation in JLDZ area. The air fall deposits are the most dangerous product in JLDZ. The highly dangerous region of spatter deposits is limited to a radius of about 2km around the volcano. The high risk area of tephra fallout is between 2km to 9km around the volcano, and between 9km to 14km is the moderate risk area. Out of 14km, it is the low risk area. Lava flow is controlled by topography. From Jinchuan Town to Houhe Village near the volcano is the low-lying area. If the volcano erupts, these areas will be in danger. 相似文献
854.
介绍了2018年12月22日发生的巽他海峡喀拉喀托火山喷发的过程及其火山监测情况,并提取了欧空局哨兵1A遥感卫星在火山喷发前后的遥感影像,通过遥感影像的对比分析获得了火山锥体的坍塌范围;使用3DAnalyst软件模块对坍塌部分的DEM影像进行分析,计算出海平面以上火山锥体的坍塌体积约为54000000m3,海面以下崩塌锥体体积更加巨大,崩塌导致火山周围水体发生激荡形成海浪,海浪相干传播至周边海岸附近引发了巽他海峡海啸;海啸灾害主要发生在印尼万丹省西冷县和板底兰县西部沿海,与根据火山喷发引发海啸的传播路径推测的受灾地区基本一致。 相似文献
855.
长白山天池火山是中国最具潜在喷发危险的多成因复式火山,在近2000年来,曾经发生过世界上最大规模的喷发。为了进一步研究长白山天池火山的潜在危险,有必要研究火山的岩浆囊位置和分布。为此,在长白山天池火山开展了一条南北方向的重力剖面测量。结合前人工作,如地震勘探P波速度反演和大地电磁测深(MT)电阻率反演,以及地质信息,采用人机交互的形式,建立了一条长约150km的密度模型。从建模结果图中可以发现:(1)长白山天池下方存在地壳岩浆囊;(2)长白山天池北坡地壳存在一个高阻、低密度体,深度在7~15km,距离天池2~10km,可能是富含气体的岩浆囊;(3)在南坡和北坡大约3km深度处普遍存在一个岩浆岩层;(4)在天池下存在一个已经塌陷堵塞的火山颈。 相似文献
856.
为了探索北大西洋涛动形成的大尺度大气物理场背景条件和外部强迫因子,通过对比分析、相关分析和环流系统温压场垂直结构分析得到:(1)强火山活动指数距平与冰岛低压和亚速尔高压海平面气压场(SLP)距平总体相关函数符号相反,强火山活动指数与冰岛低压SLP为反相关,与亚速尔高压SLP为正相关,就是说火山活动指数异常引起了高纬度冰岛低压和中低纬度亚速尔高压海平面气压场相反的变化趋势,形成高低纬之间海平面气压场反相振荡;(2)夏季7月亚速尔高压对流层中下层至海平面,温度距平中心和位势高度距平中心距平符号大致正正相对负负相对,说明夏季亚速尔高压为深厚暖性系统,低层温度升高亚速尔高压加强,低层温度降低亚速尔高压减弱,所以火山活动指数与亚速尔高压SLP均呈反相关关系;冬季1月对流层中下层至海平面,温度距平和位势高度距平符号大致正负相对,说明冬季亚速尔高压为浅薄系统,低层温度升高亚速尔高压减弱,低层温度降低亚速尔高压加强,所以火山活动指数与亚速尔高压SLP均呈正相关关系;(3)冬季1月冰岛低压对流层中下层至海平面,温度距平中心和位势高度距平中心距平符号大致正正相对负负相对,说明冬季冰岛低压为深厚冷性系统,低层温度升高冰岛低压减弱,低层温度降低冰岛低压加深,所以火山活动指数与冰岛低压SLP均呈反相关关系;夏季7月对流层中下层至海平面,温度距平和位势高度距平符号大致正负相对,说明夏季冰岛低压为浅薄系统,低层温度升高冰岛低压减弱,低层温度降低冰岛低压加深,所以火山活动指数与冰岛低压SLP均呈正相关关系;(4).由于对流层中下层至海平面冰岛低压和亚速尔高压冬、夏季温压场结构特点基本相反,火山活动指数异常在两个环流系统中引起了相反响应,导致高低纬之间海平面气压场反相振荡,形成了影响广泛的著名的北大西洋涛动现象。 相似文献