Mechanics of adhesive contact on a power-law graded elastic half-space

We consider adhesive contact between a rigid sphere of radius R and a graded elastic half-space with Young's modulus varying with depth according to a power law E = E-0(z/c(0))(k) (0 < k < 1) while Poisson's ratio v remaining a constant. Closed-form analytical solutions are established for the critical force, the critical radius of contact area and the critical interfacial stress at pull-off. We highlight that the pull-off force has a simple solution of P-cr= -(k+3)pi R Delta gamma/2 where Delta gamma is the work of adhesion and make further discussions with respect to three interesting limits: the classical JKR solution when k = 0, the Gibson solid when k --> 1 and v = 0.5, and the strength limit in which the interfacial stress reaches the theoretical strength of adhesion at pull-off. (C) 2009 Elsevier Ltd. All rights reserved.

Adhesive behavior of two-dimensional power-law graded materials

In this paper, we investigate the adhesive contact between a rigid cylinder of radius R and a graded elastic half-space with a Young's modulus varying with depth according to a power-law, E = E-0(y/c(0))(k) (0 < k < 1), while the Poisson's ratio v remains constant. The results show that, for a given value of ratio R/C-0, a critical value of k exists at which the pull-off force attains a maximum; for a fixed value of k, the larger the ratio R/c(0), the larger the pull-off force is. For Gibson materials (i.e., k = 1 and v = 0.5), closed-form analytical solutions can be obtained for the critical contact half-width at pull-off and pull-off force. We further discuss the perfect stick case with both externally normal and tangential loads.

Das Klima um Grönland - 1996

Based on air temperature data from three sites of West and East Greenland, on ice charts for the area 54°N, 71°N and 20°W, 70°W, and on CTD profile observations around Greenland, the annual variability of climate is shown. Mean monthly air temperature data from Nuuk/West Greenland reveal the long-term interannual changes of air temperature anomalies. The warming trend which was observed during November, December 1995 was maintained into 1996 for about five months. Thus, spring warming of the near surface water layers, especially on the shallow bank areas off West Greenland has been favoured. As a result of mild air temperatures over most of 1996, sea ice conditions were about normal around Greenland and off eastern Canada. Subsurface observations indicate considerable warming of the 0-200 m water layer off West Greenland. The thermal anomaly of this layer amounts to +1.59K, which is the second highest value on record since the warm 1964 event. The warmer than normal conditions as recorded since November 1995 off East and West Greenland, point at intermediate warming which is characteristic of the second half of the recent decades. The long-term trend of air temperature anomalies off West Greenland points, however, still at cooling, a trend which is persistent since the early 1970s. As the potential driving mechanism for the intermediate warming in the Labrador Sea area, the sea level air pressure gradient between Iceland and the Azores is identified. The 1996 value of this gradient, the North Atlantic Oscillation (NAO) Index, is strongly negative and this represents the flow of mild air masses from the midlatitude Atlantic Ocean to the Greenland/Labrador Sea region. Accordingly, air temperature anomalies indicated unusual warming during the month of February which amounted to >2K in the region of Baffin Land, Labrador and Greenland.

Asymptotic analysis of thin plates under normal load and horizontal edge thrust

We consider the radially symmetric nonlinear von Kármán plate equations for circular or annular plates in the limit of small thickness. The loads on the plate consist of a radially symmetric pressure load and a uniform edge load. The dependence of the steady states on the edge load and thickness is studied using asymptotics as well as numerical calculations. The von Kármán plate equations are a singular perturbation of the Fӧppl membrane equation in the asymptotic limit of small thickness. We study the role of compressive membrane solutions in the small thickness asymptotic behavior of the plate solutions.

We give evidence for the existence of a singular compressive solution for the circular membrane and show by a singular perturbation expansion that the nonsingular compressive solution approach this singular solution as the radial stress at the center of the plate vanishes. In this limit, an infinite number of folds occur with respect to the edge load. Similar behavior is observed for the annular membrane with zero edge load at the inner radius in the limit as the circumferential stress vanishes.

We develop multiscale expansions, which are asymptotic to members of this family for plates with edges that are elastically supported against rotation. At some thicknesses this approximation breaks down and a boundary layer appears at the center of the plate. In the limit of small normal load, the points of breakdown approach the bifurcation points corresponding to buckling of the nondeflected state. A uniform asymptotic expansion for small thickness combining the boundary layer with a multiscale approximation of the outer solution is developed for this case. These approximations complement the well known boundary layer expansions based on tensile membrane solutions in describing the bending and stretching of thin plates. The approximation becomes inconsistent as the clamped state is approached by increasing the resistance against rotation at the edge. We prove that such an expansion for the clamped circular plate cannot exist unless the pressure load is self-equilibrating.

I. Rigid body penetration into brittle materials. II. Phase change effect on shock wave propagation

Part I.

We have developed a technique for measuring the depth time history of rigid body penetration into brittle materials (hard rocks and concretes) under a deceleration of ~ 10⁵ g. The technique includes bar-coded projectile, sabot-projectile separation, detection and recording systems. Because the technique can give very dense data on penetration depth time history, penetration velocity can be deduced. Error analysis shows that the technique has a small intrinsic error of ~ 3-4 % in time during penetration, and 0.3 to 0.7 mm in penetration depth. A series of 4140 steel projectile penetration into G-mixture mortar targets have been conducted using the Caltech 40 mm gas/ powder gun in the velocity range of 100 to 500 m/s.

We report, for the first time, the whole depth-time history of rigid body penetration into brittle materials (the G-mixture mortar) under 10⁵ g deceleration. Based on the experimental results, including penetration depth time history, damage of recovered target and projectile materials and theoretical analysis, we find:

1. Target materials are damaged via compacting in the region in front of a projectile and via brittle radial and lateral crack propagation in the region surrounding the penetration path. The results suggest that expected cracks in front of penetrators may be stopped by a comminuted region that is induced by wave propagation. Aggregate erosion on the projectile lateral surface is < 20% of the final penetration depth. This result suggests that the effect of lateral friction on the penetration process can be ignored.

2. Final penetration depth, P_max, is linearly scaled with initial projectile energy per unit cross-section area, e_s , when targets are intact after impact. Based on the experimental data on the mortar targets, the relation is P_max(mm) 1.15e_s (J/mm² ) + 16.39.

3. Estimation of the energy needed to create an unit penetration volume suggests that the average pressure acting on the target material during penetration is ~ 10 to 20 times higher than the unconfined strength of target materials under quasi-static loading, and 3 to 4 times higher than the possible highest pressure due to friction and material strength and its rate dependence. In addition, the experimental data show that the interaction between cracks and the target free surface significantly affects the penetration process.

4. Based on the fact that the penetration duration, t_max, increases slowly with e_s and does not depend on projectile radius approximately, the dependence of t_max on projectile length is suggested to be described by t_max(μs) = 2.08e_s (J/mm² + 349.0 x m/(πR²), in which m is the projectile mass in grams and R is the projectile radius in mm. The prediction from this relation is in reasonable agreement with the experimental data for different projectile lengths.

5. Deduced penetration velocity time histories suggest that whole penetration history is divided into three stages: (1) An initial stage in which the projectile velocity change is small due to very small contact area between the projectile and target materials; (2) A steady penetration stage in which projectile velocity continues to decrease smoothly; (3) A penetration stop stage in which projectile deceleration jumps up when velocities are close to a critical value of ~ 35 m/s.

6. Deduced averaged deceleration, a, in the steady penetration stage for projectiles with same dimensions is found to be a(g) = 192.4v + 1.89 x 10⁴, where v is initial projectile velocity in m/s. The average pressure acting on target materials during penetration is estimated to be very comparable to shock wave pressure.

7. A similarity of penetration process is found to be described by a relation between normalized penetration depth, P/P_max, and normalized penetration time, t/t_max, as P/P_max = f(t/t_max, where f is a function of t/t_max. After f(t/t_max is determined using experimental data for projectiles with 150 mm length, the penetration depth time history for projectiles with 100 mm length predicted by this relation is in good agreement with experimental data. This similarity also predicts that average deceleration increases with decreasing projectile length, that is verified by the experimental data.

8. Based on the penetration process analysis and the present data, a first principle model for rigid body penetration is suggested. The model incorporates the models for contact area between projectile and target materials, friction coefficient, penetration stop criterion, and normal stress on the projectile surface. The most important assumptions used in the model are: (1) The penetration process can be treated as a series of impact events, therefore, pressure normal to projectile surface is estimated using the Hugoniot relation of target material; (2) The necessary condition for penetration is that the pressure acting on target materials is not lower than the Hugoniot elastic limit; (3) The friction force on projectile lateral surface can be ignored due to cavitation during penetration. All the parameters involved in the model are determined based on independent experimental data. The penetration depth time histories predicted from the model are in good agreement with the experimental data.

9. Based on planar impact and previous quasi-static experimental data, the strain rate dependence of the mortar compressive strength is described by σ_f/σ⁰_f = exp(0.0905(log(έ/έ_0) ^1.14, in the strain rate range of 10^-7/s to 10³/s (σ⁰_f and έ are reference compressive strength and strain rate, respectively). The non-dispersive Hugoniot elastic wave in the G-mixture has an amplitude of ~ 0.14 GPa and a velocity of ~ 4.3 km/s.

Part II.

Stress wave profiles in vitreous GeO₂ were measured using piezoresistance gauges in the pressure range of 5 to 18 GPa under planar plate and spherical projectile impact. Experimental data show that the response of vitreous GeO₂ to planar shock loading can be divided into three stages: (1) A ramp elastic precursor has peak amplitude of 4 GPa and peak particle velocity of 333 m/s. Wave velocity decreases from initial longitudinal elastic wave velocity of 3.5 km/s to 2.9 km/s at 4 GPa; (2) A ramp wave with amplitude of 2.11 GPa follows the precursor when peak loading pressure is 8.4 GPa. Wave velocity drops to the value below bulk wave velocity in this stage; (3) A shock wave achieving final shock state forms when peak pressure is > 6 GPa. The Hugoniot relation is D = 0.917 + 1.711u (km/s) using present data and the data of Jackson and Ahrens [1979] when shock wave pressure is between 6 and 40 GPa for ρ₀ = 3.655 gj cm³ . Based on the present data, the phase change from 4-fold to 6-fold coordination of Ge⁺⁴ with O^-2 in vitreous GeO₂ occurs in the pressure range of 4 to 15 ± 1 GPa under planar shock loading. Comparison of the shock loading data for fused SiO₂ to that on vitreous GeO₂ demonstrates that transformation to the rutile structure in both media are similar. The Hugoniots of vitreous GeO₂ and fused SiO₂ are found to coincide approximately if pressure in fused SiO₂ is scaled by the ratio of fused SiO₂to vitreous GeO₂ density. This result, as well as the same structure, provides the basis for considering vitreous Ge0₂ as an analogous material to fused SiO₂ under shock loading. Experimental results from the spherical projectile impact demonstrate: (1) The supported elastic shock in fused SiO₂ decays less rapidly than a linear elastic wave when elastic wave stress amplitude is higher than 4 GPa. The supported elastic shock in vitreous GeO₂ decays faster than a linear elastic wave; (2) In vitreous GeO₂ , unsupported shock waves decays with peak pressure in the phase transition range (4-15 GPa) with propagation distance, x, as α 1/x^-3.35 , close to the prediction of Chen et al. [1998]. Based on a simple analysis on spherical wave propagation, we find that the different decay rates of a spherical elastic wave in fused SiO₂ and vitreous GeO₂ is predictable on the base of the compressibility variation with stress under one-dimensional strain condition in the two materials.

Sub-half-wavelength atom localization via two standing-wave fields

We propose a scheme for sub-half-wavelength atom localization in a four-level ladder-type atomic system, which is coupled by two classical standing-wave fields. We find that one of the standing-wave fields can help in enhancing the localization precision, and the other is of crucial importance in increasing the detecting probability and leading sub-half-wavelength localization.

Effects on the proton production from explosions of hydrogen clusters subjected to intense femtosecond laser fields

The dependence of the maximum and average energies of protons, which were produced in the interaction of an intense laser pulse (similar to 1 x 10(16) W cm(-2), 65 fs) with hydrogen clusters in a gas jet backed up to 80 bar at liquid nitrogen temperature (similar to 80 K), on the backing pressure has been studied. The general trend of the proton energy dependence on the square of the average cluster radius, which is determined by a calibrated Rayleigh scattering measurement, is similar to that described by theory under the single size approximation. Calculations are made to fit the experimental results under a simplified model by taking into account both a log-normal cluster size distribution and the laser intensity attenuation in the interaction volume. A very good agreement between the experimental proton energy spectra and the calculations is obtained in the high- energy part of the proton energy distributions, but a discrepancy of the fits is revealed in the low-energy part at higher backing pressures which are associated with denser flows. A possible mechanism which would be responsible for this discrepancy is discussed. Finally, from the fits, a variation of the cluster size distributions was revealed to be dependent on the gas backing pressure as well as on the evolving time of the gas flow of clusters.

Expressão e distribuição de CGRP, VEGF e TGF-β na gengiva dos dentes de ratos com periodontite induzida por ligadura: aspectos imunohistoquímicos

No momento em que há a agressão tecidual e a defesa inata é deflagrada, mediadores químicos são liberados no local afetado. Esses mediadores podem ser de origem celular tais como CGRP, VEGF e TGFß. Os objetivos desta pesquisa foram avaliar a expressão e distribuição de CGRP, TGFß e VEGF na gengiva do primeiro molar inferior esquerdo de rato no 7 e 14 dias após a indução por ligadura; a expressão e distribuição de CGRP, TGFß e VEGF na gengiva do dente contralateral correspondente sem ligadura, no 7 e 14 dias, e se a indução da periodontite por ligadura no dente experimental provoca uma inflamação na gengiva do dente contralateral correspondente no 7 e 14 dias após a ligadura. Para o desenvolvimento deste trabalho foram selecionados 15 ratos Rattus Novergicus, Albinus, Wistar. O grupo experimental de 12 ratos foi dividido em 2 subgrupos compostos por 6 ratos cada um deles distribuídos da seguinte maneira: os do subgrupo A1 permaneceram com a ligadura no primeiro molar inferior esquerdo por 7 dias e foram sacrificados; os do subgrupo A-2 -permaneceram com a ligadura no primeiro molar inferior esquerdo por 14 dias e foram sacrificados. Outros três animais constituíram o grupo controle. Após o sacrifício dos 12 animais dos grupos experimentais e controle suas mandíbulas foram colocadas em ácido etilenodiaminotetracético (EDTA) neutro para sofrerem descalcificação. Então foram processadas para inclusão em parafina e os cortes histológicos foram corados pela hematoxilina-eosina e submetidos à técnica imunohistoquímica para imunomarcação de CGRP, VEGF e TGFß. Aos 7 dias de ligadura observou-se na lâmina própria gengival, epitélio juncional e epitélio oral, expressiva marcação para CGRP. A expressão de VEGF foi intensa na lamina própria e com pouca ou nenhuma marcação no epitélio oral e juncional. O TGFß apresentou pouca marcação na lâmina própria ou nenhuma marcação no epitélio oral e juncional. Aos 14 dias de ligadura houve expressiva marcação de CGRP na lâmina própria, epitélios oral e juncional. O VEGF e o TGFß apresentaram muita marcação na lâmina própria e pouca ou nenhuma marcação no epitélio oral e juncional. Na gengiva dos dentes contralaterais nos 7 e 14 dias houve pouca marcação do CGRP do TGFß na lâmina própria e muita marcação do VEGF. Na gengiva dos dentes controle observou-se muita marcação do CGRP no epitélio juncional e oral e na lâmina própria. O TGFß e o VEGF se expressaram muito pouco ou não se expressaram. Devido à marcação expressiva do VEGF na lâmina própria dos dentes contralaterais, permanece inconclusiva a adequação do uso dos dentes contralaterais nos estudos experimentais das doenças periodontais, embora a expressão de TGFß e CGRP tenham sido menores nestes dentes. A maior marcação do CGRP, VEGF e TGFß nos animais com 14 dias de ligadura do que aos 7 dias demonstra a progressão do processo inflamatório crônico, não se observando processo de reparação cicatricial.

Análise da distribuição espacial da malária na Amazônia brasileira : enfoque municipal

Neste trabalho analisa-se a distribuição espacial da malária em nível municipal, na Amazônia brasileira utilizando-se técnicas de análise exploratória espacial e modelagem espacial. Na modelagem espacial foram utilizados o modelo de peso de evidências implementado num sistema de informações geográficas (ArcView) e modelos de regressão espacial. Os resultados mostram que existem: autocorrelação espacial da incidência da malária, determinantes ambientais da malária e diferenças na determinação e na distribuição doença por vivax e falciparum nas diversas regiões da Amazônia. Os resultados da análise foram discutidos vis à vis sua utilização para o controle da malária.

Seismic structure along transitions from flat to normal subduction: central Mexico, southern Peru, and southwest Japan

The fine-scale seismic structure of the central Mexico, southern Peru, and southwest Japan subduction zones is studied using intraslab earthquakes recorded by temporary and permanent regional seismic arrays. The morphology of the transition from flat to normal subduction is explored in central Mexico and southern Peru, while in southwest Japan the spatial coincidence of a thin ultra-slow velocity layer (USL) atop the flat slab with locations of slow slip events (SSEs) is explored. This USL is also observed in central Mexico and southern Peru, where its lateral extent is used as one constraint on the nature of the flat-to-normal transitions.

In western central Mexico, I find an edge to this USL which is coincident with the western boundary of the projected Orozco Fracture Zone (OFZ) region. Forward modeling of the 2D structure of the subducted Cocos plate using a finite-difference algorithm provides constraints on the velocity and geometry of the slab’s seismic structure in this region and confirms the location of the USL edge. I propose that the Cocos slab is currently fragmenting into a North Cocos plate and a South Cocos plate along the projection of the OFZ, by a process analogous to that which occurred when the Rivera plate separated from the proto-Cocos plate 10 Ma.

In eastern central Mexico, observations of a sharp transition in slab dip near the abrupt end of the Trans Mexican Volcanic Belt (TMVB) suggest a possible slab tear located within the subducted South Cocos plate. The eastern lateral extent of the USL is found to be coincident with these features and with the western boundary of a zone of decreased seismicity, indicating a change in structure which I interpret as evidence of a possible tear. Analysis of intraslab seismicity patterns and focal mechanism orientations and faulting types provides further support for a possible tear in the South Cocos slab. This potential tear, together with the tear along the projection of the OFZ to the northwest, indicates a slab rollback mechanism in which separate slab segments move independently, allowing for mantle flow between the segments.

In southern Peru, observations of a gradual increase in slab dip coupled with a lack of any gaps or vertical offsets in the intraslab seismicity suggest a smooth contortion of the slab. Concentrations of focal mechanisms at orientations which are indicative of slab bending are also observed along the change in slab geometry. The lateral extent of the USL atop the horizontal Nazca slab is found to be coincident with the margin of the projected linear continuation of the subducting Nazca Ridge, implying a causal relationship, but not a slab tear. Waveform modeling of the 2D structure in southern Peru provides constraints on the velocity and geometry of the slab’s seismic structure and confirms the absence of any tears in the slab.

In southwest Japan, I estimate the location of a possible USL along the Philippine Sea slab surface and find this region of low velocity to be coincident with locations of SSEs that have occurred in this region. I interpret the source of the possible USL in this region as fluids dehydrated from the subducting plate, forming a high pore-fluid pressure layer, which would be expected to decrease the coupling on the plate interface and promote SSEs.

Kinetic theory of normal quantum fluids

Close to equilibrium, a normal Bose or Fermi fluid can be described by an exact kinetic equation whose kernel is nonlocal in space and time. The general expression derived for the kernel is evaluated to second order in the interparticle potential. The result is a wavevector- and frequency-dependent generalization of the linear Uehling-Uhlenbeck kernel with the Born approximation cross section.

The theory is formulated in terms of second-quantized phase space operators whose equilibrium averages are the n-particle Wigner distribution functions. Convenient expressions for the commutators and anticommutators of the phase space operators are obtained. The two-particle equilibrium distribution function is analyzed in terms of momentum-dependent quantum generalizations of the classical pair distribution function h(k) and direct correlation function c(k). The kinetic equation is presented as the equation of motion of a two -particle correlation function, the phase space density-density anticommutator, and is derived by a formal closure of the quantum BBGKY hierarchy. An alternative derivation using a projection operator is also given. It is shown that the method used for approximating the kernel by a second order expansion preserves all the sum rules to the same order, and that the second-order kernel satisfies the appropriate positivity and symmetry conditions.

Ancylidae (Mollusca, Heterobranchia, Pulmonata, Basommatophora) do Estado do Rio de Janeiro, Brasil: morfologia, sistemática e distribuição geográfica

Os moluscos pateliformes de água doce da região Neotropical são comumente atribuídos a família Ancylidae sensu latum, abrangendo sete gêneros com pelo menos 13 espécies válidas e sete com identificação duvidosa. Os ancilídeos possuem pequenas dimensões, alcançam no máximo 15 mm de comprimento. Sua concha é frágil, composta por duas regiões, a protoconcha e a teleoconcha, as quais apresentam caracteres relevantes para a sistemática. Na parte mole as impressões musculares, a pigmentação do manto, o sistema reprodutor e a rádula são importantes para o estudo da família. Apesar de existirem vários registros de ocorrência para ancílideos no Estado do Rio de Janeiro (ERJ), existem poucos dados morfológicos. O principal objetivo deste estudo foi fornecer e ampliar as informações sobre a morfologia e distribuição geográfica das espécies de Ancylidae encontradas no ERJ. Os materiais utilizados foram procedentes de coletas próprias, material depositado em Coleções Científicas e dados de revisão bibliográfica. O estudo da morfologia comparada das conchas foi realizado com o auxílio de imagens de microscópio óptico e de varredura. Para a comparação das partes moles, os espécimes foram corados e dissecados sob lupa. Através da conquiliometria analisamos as diferenças inter e intrapopulacionais. Com este trabalho, a riqueza conhecida para Ancylidae no ERJ, aumentou de cinco para sete espécies: Burnupia sp., Ferrissia sp., Gundlachia radiata (Guilding, 1828),G. ticaga (Marcus & Marcus, 1962), Gundlachia sp., Hebetancylus moricandi (d`Orbigny, 1837) e Uncancylus concentricus (d`Orbigny, 1837). Gundlachia radiata e U. concentricus constituem novos registros para o ERJ, e G. radiata para a Região Sudeste. As três espécies com o maior número de registros de ocorrência no ERJ foram: G. ticaga (66%), Ferrissia sp. (37%) e Gundlachia sp. (18%). A ampla distribuição de G. ticaga pode ser devido à capacidade de suportar ambientes impactados. Em relação à morfologia, Burnupia sp. difere de Burnupia ingae Lanzer, 1991, única espécie deste gênero descrita para o Brasil, por apresentar diferenças na microescultura da concha e também na forma das impressões musculares. Ferrissia sp. difere de F. gentilis Lanzer, 1991, devido a diferenças na microescultura apical e número de cúspides no dente central da rádula. Gundlachia sp. é diferente de G. ticaga e G. radiata, por apresentar a abertura da concha mais arredondada, ápice mais recurvado, ultrapassando a borda da concha, pontuações irregulares em toda a protoconcha e forma dos músculos adutores anterior direito e posterior mais elíptica. A morfologia interna também mostra diferenças entre Gundlachia sp. e G. ticaga, como o apêndice terminal do útero e o número de folículos do ovoteste. Através das análises conquiliométricas, constatamos para os gêneros Burnupia, Ferrrissia e Gundlachia, que os índices morfométricos se mostraram melhores que as medidas lineares para a discriminação das espécies, provavelmente porque esses índices diminuem o efeito da amplitude de tamanho das conchas, que são fortemente influenciadas pelas variações ecofenotípicas. Contudo, os caracteres diagnósticos das conchas e das partes moles (impressões musculares) são indispensáveis para a identificação dos gêneros e espécies de Ancylidae. Palavras-chave: Mollusca. Moluscos de água doce. Morfologia. Distribuição geográfica. Estado do Rio de Janeiro.uscos.

Radio frequency studies of surface resistance and critical magnetic field of type I and type II superconductors

The surface resistance and the critical magnetic field of lead electroplated on copper were studied at 205 MHz in a half-wave coaxial resonator. The observed surface resistance at a low field level below 4.2°K could be well described by the BCS surface resistance with the addition of a temperature independent residual resistance. The available experimental data suggest that the major fraction of the residual resistance in the present experiment was due to the presence of an oxide layer on the surface. At higher magnetic field levels the surface resistance was found to be enhanced due to surface imperfections.

The attainable rf critical magnetic field between 2.2°K and T_c of lead was found to be limited not by the thermodynamic critical field but rather by the superheating field predicted by the one-dimensional Ginzburg-Landau theory. The observed rf critical field was very close to the expected superheating field, particularly in the higher reduced temperature range, but showed somewhat stronger temperature dependence than the expected superheating field in the lower reduced temperature range.

The rf critical magnetic field was also studied at 90 MHz for pure tin and indium, and for a series of SnIn and InBi alloys spanning both type I and type II superconductivity. The samples were spherical with typical diameters of 1-2 mm and a helical resonator was used to generate the rf magnetic field in the measurement. The results of pure samples of tin and indium showed that a vortex-like nucleation of the normal phase was responsible for the superconducting-to-normal phase transition in the rf field at temperatures up to about 0.98-0.99 T_c' where the ideal superheating limit was being reached. The results of the alloy samples showed that the attainable rf critical fields near T_c were well described by the superheating field predicted by the one-dimensional GL theory in both the type I and type II regimes. The measurement was also made at 300 MHz resulting in no significant change in the rf critical field. Thus it was inferred that the nucleation time of the normal phase, once the critical field was reached, was small compared with the rf period in this frequency range.

Composição e abundância das espécies de anfíbios e répteis em uma paisagem fragmentada de Mata Atlântica no Estado do Rio de Janeiro

Neste estudo, procuramos avaliar a composição e abundância de espécies de anfíbios e répteis em uma paisagem fragmentada de Mata Atlântica, no município de Cachoeiras de Macacu, Estado do Rio de Janeiro. Amostramos a herpetofauna da região na área contínua de floresta da Reserva Ecológica de Guapiaçu (REGUA), em 12 fragmentos do entorno com tamanhos e graus de isolamento diferentes, e áreas de pasto (matriz). Utilizamos para amostragem destes animais as metodologias de buscas ativas visuais e armadilhas de interceptação e queda, além de encontros ocasionais. No total foram registradas 55 espécies de anfíbios anuros pertencentes a 12 famílias e entre os répteis foram registradas 26 espécies, sendo uma espécie de anfisbena, uma de jacaré, nove de lagartos e 15 de serpentes. Para os anfíbios, houve uma dominância de espécies da família Hylidae, que representaram mais da metade do total de espécies encontradas no estudo. Já entre os répteis, houve uma predominância de espécies de serpentes da família Dipsadidae. Considerando apenas os registros feitos pelas metodologias empregadas, a área contínua de floresta da REGUA possui uma riqueza de espécies de anfíbios (N = 30) e de lagartos (N = 4) menor do que o conjunto de fragmentos (N = 36 e N = 8), mas superior ao que foi encontrado na matriz (N = 25 e N = 1). Entretanto, para os anfíbios, mais de um terço das espécies (N = 11) que ocorreu na mata contínua não ocorreu nos fragmentos ou na matriz, o que sugere que estas espécies podem ser mais sensíveis a alterações do hábitat. A maior riqueza de espécies encontrada no conjunto de fragmentos pode ser parcialmente explicada pelo fato de muitas espécies tanto de anfíbios quanto de lagartos que são típicas de áreas abertas, terem sua ocorrência favorecida neste tipo de condição de ambiente relativamente menos fechado dos fragmentos. Quando avaliamos o efeito de métricas da paisagem, observamos diferentes respostas entre os anfíbios e os lagartos. Enquanto para os anfíbios houve uma tendência de fragmentos mais distantes terem uma menor riqueza de espécies e de modos reprodutivos associados a estas espécies, para os lagartos a área dos fragmentos parece ser uma importante variável na estruturação das comunidades. Entretanto, por particularidades das características fisiológicas e ecológicas de anfíbios e lagartos, é possível que outros fatores expliquem a distribuição diferenciada das espécies. De forma geral, as áreas de matriz amostradas pareceram ser hostis a espécies florestais tanto de anfíbios quanto de lagartos. Além disso, para anfíbios, a presença de ambientes reprodutivos pode ser fator crucial para a ocorrência de algumas espécies. De forma similar ao encontrado em outros estudos, para a manutenção da diversidade de anfíbios e lagartos na paisagem fragmentada tratada neste estudo é necessário preservar o grande bloco florestal e aumentar a conectividade deste com os fragmentos, o que poderia permitir a área contínua servir de área-fonte de dispersores para os remanescentes florestais.

Adaptações transgeracionais do pâncreas endócrino em camundongos provenientes de restrição proteica materna In Utero

A exposição materna durante o período gestacional a uma dieta restrita em proteínas (LP) prejudica o desenvolvimento do pâncreas endócrino em sua prole e aumenta a susceptibilidade à hipertensão, diabetes e obesidade na vida adulta. Há evidências de que esse fenômeno pode persistir em gerações subsequentes. Objetivou-se avaliar o efeito da restrição proteica sobre o metabolismo da glicose e morfometria pancreática na prole F3 de camundongos ao nascimento e ao desmame. Para tanto, fêmeas virgens de camundongos Suíços (F0) foram acasaladas e receberam dieta normo-proteica (19% de proteína - NP) ou uma dieta isocalórica restrita em proteínas (5% de proteína - LP) durante toda a gravidez. Durante a lactação e o restante do experimento, todos os grupos receberam a dieta NP. Os filhotes machos foram nomeados F1 (NP1 e LP1). As fêmeas F1 e F2 foram acasaladas para produzir F2 e F3 (NP2, LP2, NP3 e LP3), respectivamente. Semanalmente, os filhotes foram pesados e calculada a taxa de crescimento alométrico (log [massa corporal] = log a + log b [idade]). Os animais foram sacrificados nos dias 1 e 21 de idade, a glicemia foi determinada e o pâncreas retirado, pesado e analisado por estereologia e imunofluorescência; a insulina foi mensurada aos 21 dias. Como resultados, os filhotes restritos na primeira geração (LP1) foram menores ao nascer, mas apresentaram um crescimento acelerado nos primeiros sete dias de vida, mostrando catch-up com os controles; a prole LP2 demonstrou a maior massa corporal ao nascimento e tiveram uma taxa de crescimento mais lenta durante a lactação; não houve diferença na massa corporal e na taxa de crescimento na geração F3. A massa de pâncreas foi diminuída em LP1-LP3 ao nascimento, contudo foi aumentada em LP2 ao desmame. A densidade de volume e o diâmetro das ilhotas foram menores em todos os grupos restritos no dia 1 e 21, somente LP1 teve o menor número de ilhotas. Ao nascer, a massa de células beta foi menor em LP1-LP3 e permaneceu baixa durante a lactação. No dia 1 e 21, os filhotes foram normoglicêmicos, entretanto foram hipoinsulinêmicos ao desmame. Portanto, a restrição de proteínas em camundongos durante a gestação produz alterações morfológicas nas ilhotas pancreáticas, sugerindo que a homeostase da glicose foi mantida por um aumento da sensibilidade à insulina durante os primeiros estágios de vida na prole ao longo de três gerações consecutivas.