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1.
陆内碰撞体制流体作用及成矿作用研究的意义和现状 总被引：11，自引：0，他引：11
陆内碰撞作用和流体作用都是８０年代以来的研究前沿，它们的研究必然会大大促进成矿作用研究的发展，也是跟踪和超越世界地球科学先进水平的重要途径。中国拥有最多最复杂的陆内碰撞带，为中国学者开发有关研究并取得高水平成果提供了得天独厚的条件。对陆内碰撞、流体作用和成矿作用研究现状的分析表明，三者之间研究的相互结合是薄弱环节，限制了有关问题的深入，但为我国学者开发该方向的研究，取得领先于国家水平的成果，提供了 相似文献
2.
Sand injectites are structures that result from intrusion of fluidized sand into fractures. We have studied them in the Tampen Spur area of the North Sea, and have reproduced them experimentally, by driving compressed air through layers of sand, glass microspheres, and silica powder. The silica powder was cohesive and capable of hydraulic fracturing, whereas the sand and glass microspheres were almost non-cohesive and therefore able to fluidize. The models were dynamically similar to their natural counterparts, for as long as equilibrium was static. When the processes became dynamic, so that inertial forces were significant, the scaling was approximate and the corresponding Reynolds numbers differed. The experimental apparatus was a square box, 1 m × 1 m wide, resting on a grid of fluid diffusers. During the experiments, the fluid pressure increased, until it attained and surpassed the weight of overburden. Flat-lying hydraulic fractures, containing air, formed within cohesive and least permeable layers. Heterogeneities in material properties and layer thicknesses were responsible for localizing fracture networks. When any one network broke through to the surface, rapid flow of air through the fractures fluidized the underlying mobile materials and even depleted some of the layers. Some of the fluidized material extruded at the surface through vents, forming volcanoes and sheets. The remainder lodged at depth, forming sand injectites or laccoliths. Conical sand injectites formed preferentially, where layers had high resistance to bending. Laccoliths formed nearer the surface, where overlying layers had low resistance to bending. The experimental sand injectites were broadly similar to those in the Tampen Spur area of the North Sea, as well as other areas. 相似文献
3.
The Citlaltépetl Ignimbrite records one of the largest explosive events during the Holocene activity of Citlaltépetl Volcano
(Pico de Orizaba). Multiple pyroclastic flow units, a fall deposit, and some lahar units were emplaced between 8500–9000 y
B.P. as a result of repetitive but discrete explosive events. The whole ignimbrite resulted from discrete fluctuations in
eruptive intensity that decreased with time. The initial pyroclastic flow pulse was by far the most violent and widespread
event, and its deposits show conspicuous variations in structure and texture that could be associated with different mechanisms
of transport and emplacement. Subpopulation Sequential Fragmentation Transport (SFT) analyses were carried out in order to
determine the physical mechanisms that selectively concentrate or remove particles in the moving flows. We suggest that lateral
and temporal changes in the flow rheology, in which fluidization, yield strength, entrainment of atmospheric air, and sedimentation
played a dominant role in flow propagation and emplacement, may imprint a unique signature in the grain-size spectra. The
lowermost unit of the Citlaltépetl Ignimbrite can be envisaged by a model in which progressive aggradation near the vent became
replaced by en masse emplacement farther outward.
Received: 24 March 1998 / Accepted: 9 October 1998 相似文献
4.
Irregular wave-induced mud fluidization and wave spectrum transformation on muddy profiles are studied through representative wave technique. The constitutive equations of visco-elastic model are adopted for the rheological behavior of fluid mud, while the behavior of stationary mud is assumed to be elastic. A set of representative waves are employed to investigate wave–mud interaction. The results are verified using real field data. Comparing the performance of common representative waves, it is concluded that the phenomena can be better predicted by root mean square wave. 相似文献
5.
中国北方石墨矿床及赋矿孔达岩系碳同位素特征及有关问题讨论 总被引：24，自引：10，他引：14
本文综合了中国北方孔达岩系和石墨矿床的碳同位素数据 10 2件 ,发现片麻岩石墨 透辉岩石墨 <大理岩石墨 <石墨大理岩方解石 <大理岩方解石 ;混合岩化岩石中石墨δ1 3C总介于有机碳和无机碳之间 ;不同地体片麻岩石墨δ1 3C极为一致 ,变化于 - 2 2 .8‰～ - 2 1.48‰ ,略低于世界有机质平均值 - 2 6± 7‰ ;大理岩的原岩碳酸盐δ1 3C高于 2‰ ,与2 330～ 2 0 6 0 Ma期间全球性δ1 3Ccarb正向漂移事件一致。地质流体是碳同位素分馏、均一化的重要因素 ,是石墨矿床的 3种主要碳源之一 ,是碳的 5种存在形式之一 ,也是碳循环的重要媒介和方式 ;导致热液矿床δ1 3C=- 5‰左右的因素较多 ,依据δ1 3Ccalcite - 5‰得出成矿物质和流体来自地幔的结论值得怀疑 ;中国北方孔达岩系形成于古元古代 ,可能为 2 30 0～ 2 0 5 0 Ma。 相似文献
6.
Joseph S. Walder 《Bulletin of Volcanology》2000,62(2):105-118
Received: 15 March 1999 / Accepted: 9 December 1999 相似文献
7.
H.?MoriwakiEmail author T.?Inokuchi T.?Hattanji K.?Sassa H.?Ochiai G.?Wang 《Landslides》2004,1(4):277-288
A full-scale landslide experiment was conducted to clarify the failure process of a landslide triggered by rainfall, using a loose sandy soil. The experiment used a 23-m long and about 8-m high flume, consisting of three parts: an upper 30° slope section, a lower 10° slope section, and a horizontal section at the foot of the slope. The flume was sprinkled at a constant intensity of 100 mm/h. The landslide occurred first in the upper slope about 154 min after the sprinkling started, following a creep movement within 41 min. The sliding mass slid to a stop in about 5 s, compressing soils in the lower gentle slope and horizontal sections. The dynamic process related to slide movement and the fluctuation of subsurface water pressures during failure were measured and analyzed. Sequential visual observations provided a clear record of the slip surface during failure. The rapid increase of subsurface water pressure in the slope and horizontal soil layers was also recorded during failure. It was inferred that the increased water pressures in the upper slope resulted from collapse of loose soil structure during shearing in the translational slide, whereas those in the lower portion of the slope and horizontal sections resulted from a mix of soil compression and shearing by the sliding mass. 相似文献
8.
Armin Freundt 《Bulletin of Volcanology》1998,59(6):414-435
High-grade ignimbrites are thought to be deposited by pyroclastic flows at temperatures exceeding minimum welding temperature
or even solidus temperature. Corresponding pyroclastic-flow particles range from plastic to partially liquid and are able
to aggregate or coalesce. This contrasts with particles in pyroclastic flows producing unwelded ignimbrite, which are capable
of elastic grain interactions. The low aspect ratio and great areal extent of high-grade ignimbrites requires transport in
a particulate state either by (a) high-concentration mass flow facilitated by fluidizing gas reducing internal friction, or
by (b) expanded turbulent flow of low but downward increasing concentration. This paper presents experiments designed to investigate
the effects of plastic to liquid particles on these two contrasting transport mechanisms. Gas fluidization experiments using
polyethyleneglycole (PEG) powders heated above minimum sintering (Tms) and melting (Tm) temperatures cover a wide range of fluidization velocities (Umf>Ua>0.6·Ut) but are always in the bubbly fluidization regime similar to fluidized ignimbrite ash, where particle volume concentration
outside the bubbles is high (≈10–1). When the powders reach a critical temperature Tm≥T≥Tms, defluidization by catastrophic particle aggregation immediately commences in both stationary and laterally moving fluidized
beds as well as in experiments using mixtures of high- and low-Tm (≥30 wt.%) PEG powders, when T≥Tms of the lower-Tm powder. This indicates that extended particulate transport at T≥Tms is not possible at such high particle concentrations. In the turbulent flow experiments, liquid sprays of molten PEG or water,
vertically injected into a high-Re (>104) horizontal air flow, form a low-concentration (10–5 to 10–4) turbulent suspension current. Proximal formation of partially coalesced aggregates, which settle faster than individual
particles, causes the measured downstream decay of sedimentation rate to be steeper than predicted by theory of single solid-particle
sedimentation from turbulent suspensions. As particles become finer downstream and coalescence efficiency decreases in response
to cooling, more distally formed aggregates become too small and rare to modify sedimentation-rate decay from that of suspension
flows containing solid particles. The key difference between the two transport systems is particle concentration, C. Since
particle collision rate Rcoll∝C2, collision rates in fluidized beds are so high that all particles immediately aggregate when coalescence efficiency (1≥Ecoal≥0) is larger than 10-3. Low-concentration suspensions, on the other hand, require much higher values of Ecoal for significant aggregation to occur. Dilute pyroclastic flows will have higher particle volume fractions (≈10–3) than the experimental currents, but then viscous pyroclasts should have lower coalescence efficiencies than PEG droplets.
Experimental results thus support an expanded turbulent transport mechanism of pyroclastic flows generating extensive high-grade
ignimbrite sheets.
Received: 28 August 1996 / Accepted: 3 December 1997 相似文献
9.
In jigging, amplitude and frequency of pulsation, and feed characteristics are the most important process parameters. Effects of these parameters on particle segregation during jigging are studied and explained through experimental as well as numerical means by drawing parallel to liquid/solid fluidization process. This is permissible because jigging could also be viewed as a repetitive process of fluidization and defluidization. Unlike a normal fluidization process, in jigging, particle segregation takes place under rapid rate of change of water velocity. The rate of change of water velocity is decided by the maximum water velocity of the jig cycle, which in turn is controlled primarily by the amplitude. Experimental evidence of the role of maximum water velocity on jigging is given. Next, the feed to the jig that varies in both size and density is conceived as a mixture of many density variant binary systems. This way, the effect of feed characteristic is conveniently analyzed through several indicators of the binary feed namely size ratio, volume fraction, and particle size. Finally, the effect of frequency is studied by considering the particles in the jig bed analogous to tuned mass dampers. This concept is used to explain the preferential segregation of particles at certain jig frequency. 相似文献
10.
Goro Komatsu John W. Olsen Jens Orm Gaetano Di Achille David A. Kring Takafumi Matsui 《Geomorphology》2006,74(1-4):164-180
The Tsenkher structure, in the Gobi-Altai region of Mongolia, was studied using a wide array of remote sensing data and field observations. The structure has a shallow, 3.6 km wide, central depression bordered by a near-circular ridge (putative crater rim) with breaches to the northwest. The central depression is obliterated partially by fluvial infill through these breaches. Outside the ridge, the western side is a rugged terrain, but the eastern half is characterized by a concentric outer ridge that occurs at about one radius distance from the inner ridge. Although intrusion, salt tectonics and maar crater hypotheses cannot be completely ruled out, its morphology strongly implies an impact origin for the Tsenkher structure. If of impact origin, it has a well-preserved morphology and its position in the basin fills indicates that the formation may have occurred relatively recently, sometime during the late Tertiary or Quaternary. The outer ridge morphology is similar to rampart craters on Mars, whose formation has been attributed to fluidization of a water-rich target layer and ejecta materials, or to atmospheric entrainment and deposition of ejected materials. However, other hypotheses including erosional remnant of ejecta blanket, erosional scarp of structural rim uplift, multi-ring or deeply eroded crater rim of a peak-ring crater are also possible at this stage. A complex fluvial and probable lacustrine history is envisaged within the Tsenkher structure. The structure is also associated with archaeology, including Paleolithic and Bronze Age remains. 相似文献