An ecosystem-based composite spatial model for floodplain vulnerability assessment: a case study of Artigas,Uruguay

Floods are natural processes that constitute a hazard to society when associated to improper land use. Anthropic activities in floodplains are a factor of vulnerability that converts a natural hazard into a threat factor, eventually leading to disaster. Nowadays, natural and social complex processes demand integrated assessments in order to improve their understanding, helping decision making over sustainable use of territory, as well as integrating society’s activity in ecosystems and potentials, restrictions and benefits that society obtain from them. In this context, the objective of this work was to build a composite vulnerability model for a floodplain under urban influence, using an integrated assessment approach. This model was based on three dimensions; threat, fragility and an ecosystem services provision. These dimensions were calculated using both primary and secondary information, and weights by specialists. Main results show that the area presents high vulnerability with an increasing gradient towards high and urbanized areas, associated with an important number and relevant ecosystem services. Also, a spatial heterogeneity of the three dimensions emerged, making evident this area’s complexity and the need of integrated assessments to approach it. The composite vulnerability model proposed presents an elevated potential for natural and social processes analysis in floodplains, which is crucial for these territory management. Moreover, these integrated dimensions could contribute to decision making in different levels, as well as generating important supplies for environmental management and land planning.

     

Local isotropy and anisotropy in the sheared and heated atmospheric surface layer

Longitudinal velocity and temperature measurements above a uniform dry lakebed were used to investigate sources of eddy-motion anisotropy within the inertial subrange. Rather than simply test the adequacy of locally isotropic relations, we investigated directly the sources of anisotropy. These sources, in a daytime desert-like climate, include: (1) direct interaction between the large-scale and small-scale eddy motion, and (2) thermal effects on the small-scale eddy motion. In order to explore these two anisotropy sources, we developed statistical measures that are sensitive to such interactions. It was found that the large-scale/small-scale interaction was significant in the inertial subrange up to 3 decades below the production scale, thus reducing the validity of the local isotropy assumption. The anisotropy generated by thermal effects was also significant and comparable in magnitude to the former anisotropy source. However, this thermal anisotropy was opposite in sign and tended to counteract the anisotropy generated by the large-scale/smallscale interaction. The thermal anisotropy was attributed to organized ramp-like patterns in the temperature measurements. The impact of this anisotropy cancellation on the dynamics of inertial subrange eddy motion was also considered. For that purpose, the Kolmogorov-Obukhov structure function equation, as derived from the Navier-Stokes equations for locally isotropic turbulence, was employed. The Kolmogorov-Obukhov structure function equation in conjunction with Obukhov's constant skewness closure hypothesis reproduced the measured second- and third-order structure functions. Obukhov's constant skewness closure scheme, which is also based on the local isotropy assumption, was verified and was found to be in good agreement with the measurements. The accepted 0.4 constant skewness value derived from grid turbulence experiments overestimated our measurements. A suggested 0.26 constant skewness value, which we derived from Kolmogorov's constant, was found to be adequate.     

A laboratory simulation of mesoscale flow interaction with the Alps

A series of laboratory experiments, aimed at the simulation of some aspects of Alpine lee cyclogenesis has been carried out in the rotating tank of the Coriolis Laboratory of LEGI-IMG in Grenoble. Dynamic and thermodynamic processes, typical of baroclinic development triggered by the orography, were simulated. The background flow simulating the basic state of the atmosphere consisted of a stream of intermediate density fluid introduced at the interface between two fluid layers. The structure of the intermediate current was established by mixing fluid obtained from the upper layer of fresh water with fluid removed from the heavier salty layer below.The dynamical similarity parameters are the Rossby (Ro), Burger (Bu) and Ekman (Ek) numbers, although this last, owing to its small values, need not be matched between model and prototype, since viscous effects are not important for small time scales. The flow in both the prototype and laboratory simulation is characterized by hydrostatics; this requires (Ro²δ²/Bu)1 (where δ=H/L is the aspect ratio of the obstacle) which is clearly satisfied, in the atmosphere and oceans, and for the laboratory experiment.A range of experiments for various Rossby and Burger numbers were conducted which delimited the region of parameter space for which background flows akin to that found to the northwest of the Alps prior to baroclinic cyclogenesis events, were observed.One such experiment was carried out by placing a model of the Alps at the appropriate place in the flow field. The subsequent motion in the laboratory was observed and dye tracer motions were used to obtain the approximate particle trajectories. The density field was also analyzed to provide the geopotential field of the simulated atmosphere. Using standard transformations from the similarity analysis, the laboratory observations were related to the prototype atmosphere. The flow and the geopotential fields gave results compatible with the particular atmospheric event presented.     

Modélisation géométrique 3D des granites stéphaniens du massif du Pelvoux (Alpes,France)

The structural analysis and the 3D modelling of Stephanian granites of the Pelvoux Massif characterize an emplacement along sinistral NW–SE- and dextral NE–SW-trending shear zones in the Pelvoux and in the Aiguilles Rouges–Mont Blanc Massifs, respectively. This Carboniferous shear system is consistent with a north–south extension direction known in the whole Variscan belt at this time. To cite this article: P. Strzerzynski et al., C. R. Geoscience 337 (2005).     

The effect of thermal treatment on the 57Fe Mössbauer spectrum of beryl

Mössbauer spectra (MS) of blue, green and yellow beryl (ideally Be₃Al₂Si₆O₁₈) containing approximately 1% of iron were obtained at 295 and 500 K. Room temperature (RT) spectra of both blue and green samples showed the presence of an asymmetric Fe²⁺ doublet (ΔE _Q~2.7 mm/s, δ~1.1 mm/s), with a very broad low-velocity peak. There is no clear evidence for the presence of a ferric component. The MS of the yellow sample at RT consists of an intense central absorption with parameters typical for Fe³⁺ (ΔE _Q~0.4 mm/s, δ~0.29 mm/s), plus an apparently symmetrical Fe²⁺ doublet. This sample acquires a light-blue shade upon heating in air at about 620 K. Thermal treatments at high temperatures caused no significant changes in the MS, but the green and yellow beryl acquire a blue colour. All these results are interpreted in relation to the existence of channel water and the distribution of iron among the available crystallographic sites.     

A simple model accounting for the uptake,transport, and deposition of wind‐eroded mineral particles in the hyperarid coastal Atacama Desert of northern Chile

As previously observed in marine sediments collected downwind of African or South American continental sources, recent studies of sediment cores collected at the bottom of Mejillones Bay in north Chile (23°S) show a laminated structure in which the amount of particles of aeolian origin and their size create significant differences between the layers. This suggests inter‐annual to inter‐decadal variations in the strength of the local southerly winds responsible for (1) the erosion of the adjacent hyperarid surface of the Mejillones Pampa, and (2) the subsequent transport of the eroded particles towards the bay. A simple model accounting for the vertical uptake, transport, and deposition of the particles initially set into motion by wind at the surface of the pampa is proposed. This model, which could be adapted to other locations, assumes that the initial rate of (vertical) uptake is proportional to the (horizontal) saltation flux quantified by means of White's equation, that particles are lifted to a height (H), increasing with the magnitude of turbulence, and that sedimentation progressively removes the coarsest particles from the air column as it moves towards the bay. In this model, the proportionality constant (A) linking the vertical flux of particles with the horizontal flux, and the injection height (H) control the magnitude and size distribution of the deposition flux in the bay. Their values are determined using the wind speed measured over the pampa and the size distribution of particles collected in sediment traps deployed in the bay as constraints. After calibration, the model is used to assess the sensitivity of the deposition flux to the wind intensity variations. The possibility of performing such quantitative studies is necessary for interpreting precisely the variability of the aeolian material in the sediment cores collected at the bottom of Mejillones Bay. Copyright © 2010 John Wiley & Sons, Ltd.     

Tectonics and volcanism along the Pacific Marginal Zone of Central America

The relation of volcanism to tectonics in the Central American region has been established by a review of the literature as well as by field and photogeological work of the authors. The association of a deep trench off the Pacific coast, a parallel seismic belt, and a similarly oriented chain of volcanic vents farther inland, has been recognized by numerous earlier workers. These features form a tectonic unit, and are here termed the Pacific marginal zone.Seismic foci on the northeastern edge of the southern part of the Middle American Trench define a fault zone which dips under the continent and suggests movement of the oceanic plate underneath the Central American continent.An impressive chain of volcanic cones and associated shallow seismic foci is aligned along a prominent graben, best developed in Nicaragua where it is known as the Nicaraguan Depression. This feature probably originated in late Tertiary time. The southeastern end of the graben terminates at the northern ranges of the Talamanca Cordillera in Costa Rica. At the Gulf of Fonseca the trend of the graben changes from NW to E-W; the graben continues as the Central Depression of El Salvador at a higher elevation. Only the fault of the seaward border of the graben is defined in Guatemala, where it is represented by a NW trending volcanic chain.In Nicaragua and El Salvador the oldest cones are situated on the north-eastern boundary fault zone of the graben. These include remnants of the largest volcanic structures of the region. All the active volcanoes are on the southwestern boundary fault belt. Cross fracturing of this fault system controlled later northerly trending cone alignments, often with the youngest cones on the south end.The main graben and associated faults are considered results of tensional stresses on the crest of geanticlinal arching on the landward side of the Middle American Trench. This arching is believed to be due to regional compression originated by the movement of the oceanic plate against the mainland.In northwestern Central America the youngest stresses produced N-S normal faults that are marked by well-defined scarps. These stresses may be the result of right-lateral motion along the underthrust fault zone. The complex Comayagua graben north of the Gulf of Fonseca, the Ipala graben and associated faults in southeastern Guatemala, and the Guatemala City graben are all north-south features illustrating the extent and youth of this structural trend.The distribution of volcanic vents along the Nicaraguan Depression and the N-S trends underscores the close tectonic control of volcanism.

---

Zusammenfassung Der Zusammenhang zwischen Tektonik und Vulkanismus im mittelamerikanischen Raum wird aufgezeigt aufgrund einer Literaturdurchsicht und feldgeologischer Arbeiten der Verfasser. Die Beziehungen zwischen einem Tiefseegraben vor der pazifischen Küste, einem dem Festland parallelen seismischen Gürtel und einer ebenso orientierten Vulkankette weiter im Inland sind von früheren Bearbeitern bereits erkannt worden. Diese drei Einheiten werden hier zusammengefaßt und als pazifische Randzone bezeichnet.Erdbebenherde am Nordostrand des mittelamerikanischen Tiefseegrabens weisen auf eine Störungszone hin, die unter den Kontinent einfällt. Der Bewegungssinn spricht für ein Abtauchen der ozeanischen Platte unter das mittelamerikanische Festland.Eine eindrucksvolle Vulkankette und die mit ihr verbundenen Erdbebenherde sind längs eines bedeutenden Grabens aufgereiht, der in Nicaragua am deutlichsten ausgebildet ist und dort Nicaragua-Senke genannt wird. Diese tektonische Einheit entstand wahrscheinlich im Jung-Tertiär. Der Graben beginnt im Südosten an den nördlichen Ausläufern der Talamanca-Kordillere in Costa Rica.In Nicaragua verläuft er NW. Am Golf von Fonseca schwenkt er in eine E-W-Richtung und setzt sich in El Salvador in einem höheren Niveau als Zentral-Depression fort. In Guatemala ist nur der Südrand des Grabens erkennbar. Er ist gekennzeichnet durch eine in NW-Richtung aufgereihte Vulkankette. In Nicaragua und El Salvador liegen die ältesten Vulkane auf dem nordöstlichen Grenzbruch des Grabens. Zu dieser Gruppe zählen die größten Rumpfvulkane. Die meisten Kegel und alle tätigen Vulkane liegen hingegen auf dem südwestlichen Grenzbruchstreifen. Auf Querbrüchen haben sich jüngere, nördlich ausgerichtete Kegelreihen gebildet. Die jüngsten Kegel liegen meistens am südlichen Ende der Querbrüche.Es wird angenommen, daß der Hauptgraben und seine Störungen im Scheitel einer zum mittelamerikanischen Tiefseegraben parallel verlaufenden Aufwölbung entstanden sind. Die Aufwölbung kann auf Kompression der ozeanischen Platte gegen das Festland zurückgeführt werden.Im nordwestlichen Zentralamerika bewirkten jüngere Beanspruchungen die Bildung von N-S-Brüchen, die heute morphologisch als Steilkanten hervortreten. Diese Beanspruchungen können durch rechtslaterale Bewegungen entlang der pazifischen Störungszone ausgelöst worden sein. Beispiele dieser N-S-Struktur sind: Die Comayagua-Grabenzone, nördlich des Golfs von Fonseca, der Ipala-Graben und sein Störungssystem in Südost-Guatemala und der Guatemala-Stadt-Graben. Diese N-S-Störungen kennzeichnen das Ausmaß und das geringe Alter der Grabenbildung.Die Anordnung der Vulkane entlang der Nicaragua-Senke und der N-S-Brüche stellen die engen Beziehungen zwischen Tektonik und Vulkanismus in der pazifischen Randzone Mittelamerikas heraus.

---

Resumen Mediante información tomada de la literatura, trabajos de campo e interpretation fotogeológica, se establece la relación entre el volcanismo y la tectónica en la región de América Central. Se usa la denominación de zona marginal del Pacífico para identificar, como una unidad, la asociación ya reconocida por otros autores de la profunda Fosa Mesoamericana frente a la costa del Pacífico de America Central y las franjas paralelas de actividad sísmica y de cadenas volcánicas.Los focos sísmicos en el borde nororiental de la Fosa Mesoamericana definen una gran zona de afallamiento inclinada hacia el continente, cuyos movimientos indican que un bloque de la corteza oceánica se sumerge bajo la porción continental de America Central.Una imponente serie de conos volcánicos, asociada a focos sísmicos poco profundos, está situada a lo largo de un gran graben conocido como Depresión de Nicaragua, por ser en ese país donde aparece más claramente definido. Este graben, que posiblemente se originó durante el Terciario tardío, termina en su extremo suroriental contra las estribaciones de la parte norte de la Cordillera de Talamanca, en Costa Rica. En Nicaragua el graben está orientado hacia el NW hasta el Golfo de Fonseca donde toma un rumbo E-W a través de El Salvador, donde se encuentra a mayor elevación. En Guatemala se conoce únicamente una línea de fallas, la más próxima al mar, definida por una cadena de volcanes que tiene nuevamente dirección NW.En Nicaragua y El Salvador los conos volcánicos más antiguos están situados a lo largo de las fallas que limitan al graben en su lado nororiental. Allí se encuentran las ruinas de los edificos volcánicos más grandes de la región. La mayoría de los conos que incluye todos los actualmente activos, se localizan a lo largo de las fallas del borde suroccidental del graben. Fracturas transversales controlan la localization de varios grupos de conos alineados de N-S. Los volcanes más jóvenes se encuentran frecuentemente en el extremo sur.Se postula que el graben principal y otras fallas del mismo sistema han sido formados como resultado de esfuerzos de tensión, en la cresta de un geanticlinal que resultó del arqueamiento del lado terrestre de la zona marginal del Pacífico. Dicho arqueamiento se cree que resulta de la compresión regional debida al movimiento del bloque oceánico contra el continente.En la parte noroccidental de América Central los esfuerzos más recientes produjeron fallas orientadas N-S, fácilmente identificables por sus bien marcadas escarpas. Estos esfuerzos pueden haber resultado del desplazamiento dextromóvil a lo largo de las zonas de afallamiento paralelas a la Fosa Mesoamericana.El complejo graben de Comayagua, al norte del Golfo de Fonseca, y los graben de Ipala y de la Ciudad de Guatemala, orientados también de norte a sur, ilustran la extension y la joven edad de las fracturas.La distribución de los focos volcánicos a lo largo de la Depresión de Nicaragua y de las fracturas N-S muestran de manera evidente, la estrecha relación que existe entre la tectónica y la localización del volcanismo en la zona marginal del Pacifico de America Central.

---

, - . - , . . , , . , , - . - Talamanca Kordillere -. - - . Fanseca . . , , . - . . . , . . - N-S , . . : Comayagua, Fanseca, Ipala - . - . , .

     

Temporal features in thunder days in the United States

1901–80 data for the contiguous U.S. show that secular variability of thunder days was very much less than that of precipitation or of frequency of extra tropical cyclones. Overall, there may have been a slight decline, but more evident was an increase to the thirties followed by a falling off, broken only by a peak in the seventies. These up-and-down movements were evident in most months of the year and regions of the U.S. The general decrease, however, was clear only in the South East and replaced by an increase in the Upper Great Lakes region. Secular variation in thunder day frequency was slightly correlated positively with that of extra tropical cyclone frequency and negatively with sea level pressure. The analysis also confirmed well known seasonal and regional patterns of thunder activity.