The 18th historic eruption of Hekla started on 26 February, 2000. It was a short-lived but intense event, emitting basaltic
andesitic (55.5 wt% SiO2) pyroclastic fragments and lava. During the course of the eruption, monitoring was done by both instruments and direct observations,
together providing unique insight into the current activity of Hekla. During the 12-day eruption, a total of 0.189 km3 DRE of magma was emitted. The eruptive fissure split into five segments. The segments at the highest altitude were active
during the first hours, while the segments at lower altitude continued throughout the eruption. The eruption started in a
highly explosive manner giving rise to a Subplinian eruptive column and consequent basaltic pyroclastic flows fed by column
collapses. After the explosive phase reached its maximum, the eruption went through three more phases, namely fire-fountaining,
Strombolian bursts and lava effusion. In this paper, we describe the course of events of the eruption of Hekla and the origin
of its magma, and then show that the discharge rate can be linked to different style of eruptive activity, which are controlled
by fissure geometry. We also show that the eruption phases observed at Hekla can be linked with inferred magma chamber overpressure
prior to the eruption. 相似文献
Proximal (<3 km) deposits from episodes II and III of the 60-h-long Novarupta 1912 eruption exhibit a very complex stratigraphy, the result of at least four transport regimes and diverse depositional mechanisms. They contrast with the relatively simple stratigraphy (and inferred emplacement mechanisms) for the previously documented, better known, medial–distal fall deposits and the Valley of Ten Thousand Smokes ignimbrite. The proximal products include alternations and mixtures of both locally and regionally dispersed fall ejecta, and numerous thin complex deposits of pyroclastic density currents (PDCs) with no regional analogs. The locally dispersed component of the fall deposits forms sector-confined wedges of material whose thicknesses halve radially from and concentrically about the vent over distances of 100–300 m (cf. several kilometers for the medial–distal fall deposits). This locally dispersed fall material (and many of the associated PDC deposits) is rich in andesitic and banded pumices and richer in shallow-derived wall-rock lithics in comparison with the coeval medial fall units of almost entirely dacitic composition. There are no marked contrasts in grain size in the near-vent deposits, however, between locally and widely dispersed beds, and all samples of the proximal fall deposits plot as a simple continuation of grain size trends for medial–distal samples. Associated PDC deposits form a spectrum of facies from fines-poor, avalanched beds through thin-bedded, landscape-mantling beds to channelized lobes of pumice-block-rich ignimbrite. The origins of the Novarupta near-vent deposits are considered within a spectrum of four transport regimes: (1) sustained buoyant plume, (2) fountaining with co-current flow, (3) fountaining with counter-current flow, and (4) direct lateral ejection. The Novarupta deposits suggest a model where buoyant, stable, regime-1 plumes characterized most of episodes II and III, but were accompanied by transient and variable partitioning of clasts into the other three regimes. Only one short period of vent blockage and cessation of the Plinian plume occurred, separating episodes II and III, which was followed by a single PDC interpreted as an overpressured "blast" involving direct lateral ejection. In contrast, regimes 2 and 3 were reflected by spasmodic sedimentation from the margins of the jet and perhaps lower plume, which were being strongly affected by short-lived instabilities. These instabilities in turn are inferred to be associated with heterogeneities in the mixture of gas and pyroclasts emerging from the vent. Of the parameters that control explosive eruptive behavior, only such sudden and asymmetrical changes in the particle concentration could operate on time scales sufficiently short to explain the rapid changes in the proximal 1912 products.Editorial responsibility: R. Cioni 相似文献
Thermochemical plumes form at the base of the lower mantle as a consequence of heat flow from the outer core and the presence of local chemical doping that decreases the melting temperature. Theoretical and experimental modelling of thermochemical plumes show that the diameter of a plume conduit remains practically constant during plume ascent. However, when the top of a plume reaches a refractory layer, whose melting temperature is higher than the melt temperature in the plume conduit, a mushroom-shaped plume head develops. Main parameters (melt viscosity, ascent time, ascent velocity, temperature differences in the plume conduit, and thermal power) are presented for a thermochemical plume ascending from the core–mantle boundary. In addition, the following relationships are developed: the pressure distribution in the plume conduit during the ascent of a plume, conditions for eruption-conduit formation, the effect of the P–T conditions and controls on the shape and size of a plume top, heat transfer between a thermochemical plume and the lithosphere (when the plume reaches the bottom of a refractory layer in the lithosphere), and eruption volume versus the time interval t1 between plume formation and eruption. These relationships are used to determine thermal power and time t1 for the Tunguska syneclise and the Siberian traps as a whole.
The Siberian and other trap provinces are characterized by giant volumes of lavas and sills formed a very short time period. Data permit a model for superplumes with three stages of formation: early (variable picrites and alkali basalts), main (tholeiite plateau basalts), and final (ultrabasic and alkaline lavas and intrusions). These stages reflect the evolution of a superplume from the ascent of one or several independent plumes, through the formation of thick lenses of mantle melts underplating the lithosphere and, finally, intrusion and extrusion of differentiated mantle melts. Synchronous syenite–granite intrusions and bimodal volcanism abundant in the margins of the Siberian traps are the result of melting of the lower crust at depths of 65–70 km under the effect of plume melts. 相似文献
Numerous tephra dispersion and sedimentation models rely on some abstraction of the volcanic plume to simplify forecasts of
tephra accumulation as a function of the distance from the volcano. Here we present solutions to the commonly used advection–dispersion
equation using a variety of source shapes: a point, horizontal and vertical lines, and a circular disk. These may be related
to some volcanic plume structure, such as a strong plume (vertical line), umbrella cloud (circular disk), or co-ignimbrite
plume (horizontal line), or can be used to build a more complex plume structure such as a series of circular disks to represent
a buoyant weak plume. Basing parameters upon eruption data, we find that depositions for the horizontal source shapes are
very similar but differ from the vertical line source deposition. We also compare the deposition from a series of stacked
circular disk sources of increasing radius above the volcanic vent with that from a vertical line source. 相似文献
In situ measurement of volcanic eruption velocities is one of the great challenges left in geophysical volcanology. In this
paper we report on a new radar Doppler technique for monitoring volcanic eruption velocities. In comparison with techniques
employed previously (e.g., photographic methods or acoustic Doppler measurements), this method allows continuous recordings
of volcanic eruptions even during poor visibility. Also, radar Doppler instruments are usually light weight and energy efficient,
which makes them superior to other Doppler techniques based on laser light or sound. The proposed new technique was successfully
tested at Stromboli Volcano in late 1996 during a period of low activity. The recorded data allow a clear distinction between
particles rising from the vent and particles falling back towards the vent. The mean eruption velocity was approximately 10 m/s.
Most of the eruptions recorded by radar were correlated to seismic recordings. The correlation between the magnitude of the
volcanic shocks and the eruption force index defined in the paper may provide new insights into magma transport in the conduit.
Received: 15 May 1998 / Accepted: 15 December 1998 相似文献
3 ) erupted from circumferential vents near the summit. These flows are nearly an order of magnitude smaller in volume than
the predominantly aa flows erupted from radial eruptive fissures near the break in slope (0.06–0.1 km3). The differences in volume and flow morphology with altitude are due to slower eruption rates from summit vents than from
flank vents, which, in turn, are attributable to the different heights the magmas must ascend from shallow reservoirs. These
observations support the contention that the steep upper flanks were constructed by the buildup of short lava flows rather
than by the structural deformation of originally gently dipping flanks. In addition to the higher eruption rates, a subdued
lower flank geometry is promoted by the deposition of lava deltas onto the shallow Galápagos platform on the western, northern,
and eastern flanks of the volcano. 40Ar/39Ar geochronology and volume estimates show that, despite their morphologic differences, the growth of the western Galápagos
shields has been nearly synchronous, precluding an evolutionary model for their development. The wide variations in elevation,
volume, area, and the distribution of slope angles among the western volcanoes can be linked instead to different long-term
eruption rates and, to a lesser degree, the position of each volcano relative to the edge of the Galápagos platform.
Received: 24 September 1998 / Accepted: 7 August 1999 相似文献
Numerous volcanoes in the Afar Triangle and adjacent Ethiopian Rift Valley have erupted during the Quaternary, depositing volcanic ash (tephra) horizons that have provided crucial chronology for archaeological sites in eastern Africa. However, late Pleistocene and Holocene tephras have hitherto been largely unstudied and the more recent volcanic history of Ethiopia remains poorly constrained. Here, we use sediments from lakes Ashenge and Hayk (Ethiopian Highlands) to construct the first <17 cal ka BP tephrostratigraphy for the Afar Triangle. The tephra record reveals 21 visible and crypto-tephra layers, and our new database of major and trace element glass compositions will aid the future identification of these tephra layers from proximal to distal locations. Tephra compositions include comendites, pantellerites and minor peraluminous and metaluminous rhyolites. Variable and distinct glass compositions of the tephra layers indicate they may have been erupted from as many as seven volcanoes, most likely located in the Afar Triangle. Between 15.3−1.6 cal. ka BP, explosive eruptions occurred at a return period of <1000 years. The majority of tephras are dated at 7.5−1.6 cal. ka BP, possibly reflecting a peak in regional volcanic activity. These findings demonstrate the potential and necessity for further study to construct a comprehensive tephra framework. Such tephrostratigraphic work will support the understanding of volcanic hazards in this rapidly developing region. 相似文献
The vesiculation of magma during the 1983 eruption of Miyakejima Volcano, Japan, is discussed based on systematic investigations
of water content, vesicularity, and bubble size distribution for the products. The eruption is characterized by simultaneous
lava effusion and explosive sub-plinian (‘dry’) eruptions with phreatomagmatic (‘wet’) explosions. The magmas are homogeneous
in composition (basaltic andesite) and in initial water content (H2O = 3.9±0.9 wt%), and residual groundmass water contents for all eruption styles are low (H2O <0.4 wt%) suggestive of extensive dehydration of magma.
For the scoria erupted during simultaneous ‘dry’ and ‘wet’ explosive eruptions, inverse correlation was observed between vesicularity
and residual water content. This relation can be explained by equilibrium exsolution and expansion of ca. 0.3 wt% H2O at shallow level with different times of quenching, and suggests that each scoria with different vesicularity, which was
quenched at a different time, provides a snapshot of the vesiculation process near the point of fragmentation. The bubble
size distribution (BSD) varies systematically with vesicularity, and total bubble number density reaches a maximum value at
vesicularity Φ ∼ 0.5. At Φ ∼ 0.5, a large number of bubbles are connected with each other, and the average thickness of bubble
walls reaches the minimum value below which they would rupture. These facts suggest that vesiculation advanced by nucleation
and growth of bubbles when Φ < 0.5, and then by expansion of large bubbles with coalescence of small ones for Φ > 0.5, when
bubble connection becomes effective.
Low vesicularity and low residual water content of lava and spatter (Φ < 0.1, H2O < 0.1 wt%), and systematic decrease in bubble number density from scoria through spatter to lava with decrease in vesicularity
suggest that effusive eruption is a consequence of complete degassing by bubble coalescence and separation from magma at shallow
levels when magma ascent rate is slow.