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41.
42.
Thor H. Hansteen Andreas Klügel Hans-Ulrich Schmincke 《Contributions to Mineralogy and Petrology》1998,132(1):48-64
Gabbroic and ultramafic xenoliths and olivine and clinopyroxene phenocrysts in basaltic rocks from Gran Canaria, La Palma,
El Hierro, Lanzarote and La Gomera (Canary Islands) contain abundant CO2-dominated fluid inclusions. Inclusion densities are strikingly similar on a regional scale. Histogram maxima correspond to
one or more of the following pressures: (1) minimum 0.55 to 1.0 GPa (within the upper mantle); (2) between 0.2 and 0.4 GPa
(the Moho or the lower crust); (3) at about 0.1 GPa (upper crust). Fluid inclusions in several rocks show a bimodal density
distribution, the lower-density maximum comprising both texturally early and late inclusions. This is taken as evidence for
an incomplete resetting of inclusion densities, and simultaneous formation of young inclusions, at well-defined magma stagnation
levels. For Gran Canaria, pressure estimates for early inclusions in harzburgite and dunite xenoliths and olivine phenocrysts
in the host basanites overlap at 0.9 to 1.0 GPa, indicating that such magma reservoir depths coincide with levels of xenolith
entrainment into the magmas. Magma chamber pressures within the mantle, inferred to represent levels of mantle xenolith entrainment,
are 0.65–0.95 GPa for El Hierro, 0.60–0.68 GPa for La Palma, and 0.55–0.75 GPa for Lanzarote. The highest-density fluid inclusions
in many Canary Island mantle xenoliths have probably survived in-situ near-isobaric heating at the depth of xenolith entrainment.
Inclusion data from all islands indicate ponding of basaltic magmas at Moho or lower crustal depths, and possibly at an additional
higher level, strongly suggestive of two main crustal accumulation levels beneath each island. We emphasize that repeated
magmatic underplating of primitive magmas, and therefore intrusive accretion, are important growth mechanisms for the Canary
Islands, and by analogy, for other ocean islands. Comparable fluid inclusion data from primitive rocks in other tectonic settings,
including Iceland, Etna and continental rift systems (Hungary, South Norway), indicate that magma accumulation close to Moho
depths shortly before eruption is not, however, restricted to oceanic intraplate volcanoes. Lower crustal ponding and crystallization
prior to eruption may be the rule rather than the exception, independent of the tectonic setting.
Received: 30 May 1997 / Accepted: 6 February 1998 相似文献
43.
S?mundur?A.?HalldórssonEmail author Enik??Bali Margaret?E.?Hartley David?A.?Neave David?W.?Peate Guemundur?H.?Guefinnsson Ilya?Bindeman Martin?J.?Whitehouse Morten?S.?Riishuus Gro?B.?M.?Pedersen Sigureur?Jakobsson Rob?Askew Catherine?R.?Gallagher Esther?R.?Guemundsdóttir Jónas?Gudnason William?M.?Moreland Birgir?V.?óskarsson Paavo?Nikkola Hannah?I.?Reynolds Johanne?Schmith Thorvaldur?Thordarson 《Contributions to Mineralogy and Petrology》2018,173(8):64
The 2014–2015 Holuhraun fissure eruption provided a rare opportunity to study in detail the magmatic processes and magma plumbing system dynamics during a 6-month-long, moderate- to large-volume basaltic fissure eruption. In this contribution, we present a comprehensive dataset, including major and trace elements of whole-rock and glassy tephra samples, mineral chemistry, and radiogenic and oxygen isotope analyses from an extensive set of samples (n?=?62) that were collected systematically in several field campaigns throughout the entire eruptive period. We also present the first detailed chemical and isotopic characterization of magmatic sulfides from Iceland. In conjunction with a unique set of geophysical data, our approach provides a detailed temporal and spatial resolution of magmatic processes before and during this eruption. The 2014–2015 Holuhraun magma is compositionally indistinguishable from recent basalts erupted from the Bárðarbunga volcanic system, consistent with seismic observations for magma ascent close to the Bárðarbunga central volcano, followed by dyke propagation to the Holuhraun eruption site. Whole-rock elemental and isotopic compositions are remarkably constant throughout the eruption. Moreover, the inferred depth of the magma reservoir tapped during the eruption is consistently 8?±?5 km, in agreement with geodetic observations and melt inclusion entrapment pressures, but inconsistent with vertically extensive multi-tiered magma storage prior to eruption. The near constancy in the chemical and isotopic composition of the lava is consistent with the efficient homogenization of mantle-derived compositional variability. In contrast, occurrence of different mineral populations, including sulfide globules, which display significant compositional variability, requires a more complex earlier magmatic history. This may include sampling of heterogeneous mantle melts that mixed, crystallized and finally homogenized at mid- to lower-crustal conditions. 相似文献
44.
Tephra dispersal and eruption dynamics of wet and dry phases of the 1875 eruption of Askja Volcano, Iceland 总被引:1,自引:1,他引:0
The 1875 rhyolitic eruption of Askja volcano in Iceland was a complex but well-documented silicic explosive eruption. Eyewitness
chronologies, coupled with examination of very proximal exposures and historical records of distal deposit thickness, provide
an unusual opportunity for study of Plinian and phreatoplinian eruption and plume dynamics. The ∼ 17 hour-long main eruption
was characterized by abrupt and reversible shifts in eruption style, e.g., from ‘wet’ to ‘dry’ eruption conditions, and transitions
from fall to flow activity. The main eruption began with a ‘dry’ subplinian phase (B), followed by a shift to a very powerful
phreatoplinian ‘wet’ eruptive phase (C1). A shift from sustained ‘wet’ activity to the formation of ‘wet’ pyroclastic density
currents followed with the C2 pyroclastic density currents, which became dryer with time. Severe ground shaking accompanied
a migration in vent position and the onset of the intense ‘dry’ Plinian phase (D). Each of the fall units can be modeled using
the segmented exponential thinning method (Bonadonna et al. 1998), and three to five segments have been recognized on a semilog plot of thickness vs. area1/2. The availability of very proximal and far-distal thickness data in addition to detailed observations taken during this eruption
has enabled calculations of eruption parameters such as volumes, intensities and eruption column heights. This comprehensive
dataset has been used here to assess the bias of volume calculations when proximal and distal data are missing, and to evaluate
power-law and segmented exponential thinning methods using limited datasets. 相似文献
45.
L. Gurioli D. Andronico P. Bachelery H. Balcone-Boissard J. Battaglia G. Boudon A. Burgisser M. R. Burton K. Cashman S. Cichy R. Cioni A. Di Muro L. Dominguez C. D’Oriano T. Druitt A. J. L. Harris M. Hort K. Kelfoun J. C. Komorowski U. Kueppers J. L. Le Pennec T. Menand R. Paris L. Pioli M. Pistolesi M. Polacci M. Pompilio M. Ripepe O. Roche E. Rose-Koga A. Rust F. Schiavi L. Scharff R. Sulpizio J. Taddeucci T. Thordarson 《Bulletin of Volcanology》2015,77(6):1-33
46.
Geraint A. Tarling Thor Klevjer Sophie Fielding Jon Watkins Angus Atkinson Eugene Murphy Rebecca Korb Mick Whitehouse Russell Leaper 《Deep Sea Research Part I: Oceanographic Research Papers》2009,56(11):1994-2012
Swarming is a fundamental part of the life of Euphausia superba, yet we still know very little about what drives the considerable variability in swarm shape, size and biomass. We examined swarms across the Scotia Sea in January and February 2003 using a Simrad EK60 (38 and 120 kHz) echosounder, concurrent with net sampling. The acoustic data were analysed through applying a swarm-identification algorithm and then filtering out all non-krill targets. The area, length, height, depth, packing-concentration and inter-swarm distance of 4525 swarms was derived by this method. Hierarchical clustering revealed 2 principal swarm types, which differed in both their dimensions and packing-concentrations. Type 1 swarms were generally small (<50 m long) and were not very tightly packed (<10 ind. m−3), whereas type 2 swarms were an order of magnitude larger and had packing concentrations up to 10 times greater. Further sub-divisions of these types identified small and standard swarms within the type 1 group and large and superswarms within the type 2 group. A minor group (swarm type 3) was also found, containing swarms that were isolated (>100 km away from the next swarm). The distribution of swarm types over the survey grid was examined with respect to a number of potential explanatory variables describing both the environment and the internal-state of krill (namely maturity, body length, body condition). Most variables were spatially averaged over scales of 100 km and so mainly had a mesoscale perspective. The exception was the level of light (photosynthetically active radiation (PAR)) for which measurements were specific to each swarm. A binary logistic model was constructed from four variables found to have significant explanatory power (P<0.05): surface fluorescence, PAR, krill maturity and krill body length. Larger (type 2) swarms were more commonly found during nighttime or when it was overcast during the day, when surface fluorescence was low, and when the krill were small and immature. A strong pattern of diel vertical migration was not observed although the larger and denser swarms tended to occur more often at night than during the day. The vast majority of krill were contained within a minor fraction of the total number of swarms. These krill-rich swarms were more common in areas dominated by small and immature krill. We propose that, at the mesoscale level, the structure of swarms switches from being predominantly large and tightly packed to smaller and more diffuse as krill grow and mature. This pattern is further modulated according to feeding conditions and then level of light. 相似文献
47.
Nicole A. Stroncik Andreas Klügel Thor H. Hansteen 《Contributions to Mineralogy and Petrology》2009,157(5):593-607
A thermobarometric and petrologic study of basanites erupted from young volcanic cones along the submarine portions of the
three El Hierro rift zones (NE-Rift, NW-Rift and S-Ridge) has been performed to reconstruct magma plumbing and storage beneath
the island. Mineral-melt thermobarometry applied to naturally quenched glass and clinopyroxene rims yields pressures ranging
from 350 to 1070 MPa with about 80% of the calculated pressures being in the range of 600–800 MPa. This corresponds to a depth
range of 19–26 km, implying that the main level of final crystal fractionation is within the uppermost mantle. No systematic
dependence between sample locality and fractionation pressures could be observed. Olivine and clinopyroxene crystals in the
rocks are complexly zoned and have, on an inter-sample as well as on an intra-sample scale, highly variable core and rim compositions.
This can best be explained by mixing of multiply saturated (olivine, magnetite, clinopyroxene, ilmenite), moderately evolved
magmas with more mafic magmas being either only saturated with olivine + spinel or with olivine + spinel + clinopyroxene.
The inter-sample differences indicate derivation from small, isolated magma chambers which have undergone distinct fractionation
and mixing histories. This is in contrast to oceanic intraplate volcanoes situated on plumes with high melt supply rates,
e.g. Kilauea Volcano (Hawaii), where magma is mainly transported through a central conduit system and stored in a shallow
magma chamber prior to injection into the rift zones. The plumbing system beneath El Hierro rather resembles the magma storage
systems beneath, e.g. Madeira or La Palma, indicating that small, intermittent magma chambers might be a common feature of
oceanic islands fed by plumes with relatively low fluxes, which results in only limited and periodic magma supply. 相似文献
48.
49.
After a summary of maximum likelihood (ML) estimation, the application of the ML-method is demonstrated by estimating parameters in a ball mill-hydrocyclone grinding circuit from flow and density measurements. The model with the estimated parameters is used to determine the time propagation of mill contents and size distribution. 相似文献
50.