143,999 research outputs found
Smarandache Directionally n-Signed Graphs — A Survey
No full textFor graph theory terminology and notation in this paper we follow the book [3]. All graphs considered here are finite and simple. There are two ways of labeling the edges of a graph by an ordered n-tuple (a1, a2, · · · , an
DLN Reddy
No full textDLN Reddy's new group of paintings combines a tranquil and simultaneously aggressive current. The paneled paintings are dense and have a sweeping flourish to them that feels almost supernatural. Upon closer inspection couples and bodies float and engage in erotica in what seems like a stadium or theatre setting
An Improved Formulation and Analysis of Reddy Beam Model for Framed Structures
No full textA structural analysis of framed structures using the finite element method considering both the Bernoulli-Euler and the Timoshenko beam theories can be performed adopting cubic interpolation functions that yield analytical solutions for the displacements. However, these theories may not provide stress results with sufficient accuracy. In such cases, it is necessary to employ higher order beam formulations, that may require a high level of discretization. Therefore, this study proposes an enhanced Reddy beam element, obtained by considering interpolation functions calculated directly from the solution of the differential equation system. This solution minimizes the impact of structural discretization on the analysis, and framed structures can be effectively modeled considering the minimum number of elements required to describe the geometry. The results obtained by the proposed formulation were compared against classical beam theories and the Reddy beam model adopting conventional shape functions, showing the efficacy of the proposed element in simulating the elastic behavior of framed structures in a FEM-like procedure
An enhanced Hencky bar-chain model for bending, buckling and vibration analyses of Reddy beams
No full textThis paper is concerned with the development of the so-called Hencky bar-chain model for the bending, buckling, and vibration analyses of non-uniform thick beams. The conventional Hencky bar chain model comprises a finite number of rigid segments connected by frictionless hinges and elastic rotational springs and lumped masses at the joints. The key contribution of this paper is to enhance the Hencky bar chain model for the analysis of thick beams through the adoption of a third-order shear deformable (or Reddy) beam theory to allow for the effect of transverse shear deformation. The paper also shows the validity of the analogies between the enhanced Hencky bar-chain model and the central finite difference method for solving partial differential equation systems that have been observed for the Euler-Bernoulli beam model
Switching Equivalence in Symmetric n-Sigraphs-V
No full textIntroducing a new notion S-antipodal symmetric n-sigraph of a symmetric n-sigraph and its properties are obtained. Also giving the relation between antipodal symmetric n-sigraphs and S-antipodal symmetric n-sigraphs. Further, discussing structural characterization of S-antipodal symmetric n-sigraphs
Penser les énergies depuis les Suds : une anthologie de textes d’Amulya K. N. Reddy (1930-2006)
No full textInternational audienceUne anthologie de textes d’Amulya K. N. Reddy (1930-2006), sous la direction de Frédéric CailleAmulya Kumar Narayana Reddy (1930-2006) a 43 ans, en 1973, lorsqu’il commence ses recherches sur les questions d’énergie et de « technologies appropriées » pour les pays en émergence et leurs nombreuses populations rurales. Membre de l’Institut Indien des Sciences depuis sept ans, il abandonne une carrière brillante de chercheur et de professeur en électrochimie. Il créera un centre de recherche expérimental dans un village du sud de l’Inde, sera un pionnier au niveau mondial des « centres énergétiques ruraux » et des petites centrales villageoises à méthanisation (biogaz), avant de devenir le premier grand spécialiste international des énergies renouvelables issu d’un pays des Suds. Figure iconique dans le monde anglo-saxon sur ces questions, précurseur de la notion de « mix » et de « systèmes » énergétiques, il défendra constamment une approche des énergies soucieuse des besoins des plus modestes, de la gouvernance par les populations concernées, et du respect des milieux naturels. Au long des quarante années de sa seconde carrière, il publie plus de trois cents articles en anglais. Le présent ouvrage présente la première traduction en français de sept d’entre eux
Analytical solution for a 5-parameter beam displacement model
No full textIn this paper, a new beam model based on a 5-parameter displacement field, accounting for an enhanced kinematics and able to reproduce the Poisson effect, is proposed. The displacement field enriches the classical three-parameter Timoshenko beam with two new parameters capable to simulate the shortening effect over the thickness. The related differential equations, derived from a variational formulation, are analytically solved and implemented in a deformation method approach, capable of solving structural problems of beams with general geometry, boundary and load conditions. Several numerical applications are developed, highlighting the characteristic of the proposed 5-parameters model and comparing the results with those obtained using the classical Bernoulli, Timoshenko and Reddy beam models. Numerical results show that, although for homogeneous beam the differences in terms of generalized stress and displacement are generally very small, the proposed model returns local stress enriched by the new parameters, with more significant differences where the Poisson effect is more pronounced
A closed-form solution for buckling analysis of orthotropic Reddy plates and prismatic plate structures
No full textThis paper presents an analytical solution for elastic buckling problems of thick, composite prismatic plates subjected to uniaxial or biaxial compressive loads. Based on Reddy's third-order shear deformation theory and the Green-Lagrange deformation measure, the governing equations and natural boundary conditions of the plate are derived using Hamilton's principle, and solved analytically using the Navier and Levy-type solution methods.
A large number of configurations are analyzed, and the effects of geometric and material properties on the buckling of both isotropic and orthotropic prismatic plates, as well as transversely anisotropic sandwich plates, are determined with a reduced computational effort. A comparison with results available in the literature, also determined by considering alternative plate models, shows the accuracy of the proposed approach
Atopobathynella operculata Reddy, 2008, sp. n.
No full textAtopobathynella operculata sp. n. (Figs 1–4) Type locality and material examined. The River Godavari at Rajahmundry town (16 o 9 ’ N 81 o 47 ’ E), South India. The sampling site is located almost in the middle of the river basin wherefrom sand is being regularly mined and transported ashore. Here the riverbed has a deposit of fine sand and detritus particles, but with little or no clay, and is devoid of any macrophytic vegetation. Tidal influence from the nearby Bay of Bengal is non-existent, hence freshwater conditions prevail throughout the year. Holotype female (dissected and mounted on 4 slides, catalogue no. SMF 32211). Allotype male (undissected, catalogue no. SMF 32212). Female paratype 1 (undissected, catalogue no. SMF 32212). Female paratype 2 (dissected on one slide, catalogue no. SMF 32213). Female paratype 3 (undissected, catalogue no. SMF 32214). Male paratype (dissected on one slide, catalogue no. SMF 32215). All are kept in the collection of the Deutsches Zentrum für Marine Biodiversitätsforschung (DZMB) at Wilhelmshaven (Germany), being a department of the Senckenberg Museum und Forschungsinstitut, Frankfurt (SMF). Leg. Y. Ranga Reddy, 24 December 2002. Description of adult female. Total body length of holotype 1.41 mm, of paratypes 1.34–1.56 mm. Body elongated, almost cyclindrical, segments progressively widening and lengthening towards posterior end. All body segments including head with numerous perforations. Head only about 16 % longer than wide. Anal operculum massive, plate-like, somewhat subtriangular in outline, producing backwards and almost reaching the end of caudal furca (Fig. 1 A, B). Pleotelson with 1 seta on either side; seta smooth and much shorter than caudal furca. Furca elongately oval in ventral view (Fig. 1 B), but almost subquadrate in lateral view (Fig. 1 A), nearly 1.5 times longer than wide, with 2 apical spines of similar size, 1 small inner spine, and 2 unequal plumose setae. Furcal organ small and ventral. Antennule (Fig. 2 A): with 3 -segmented peduncle and with 3 -segmented inner flagellum, outer flagellum reduced. Whole antennule slender (9 times longer than maximum width), 42 % longer than head. Length of the 3 segments of the stem greater than that of the remainder of the outer flagellum. First segment of peduncle longest, twice as long as its own width, with a group of 2 ventral and 1 dorsal plumose setae at distal outer corner, 1 long dorsal seta in the distal half, and 1 tiny seta at distal inner corner. Second segment slightly shorter than first segment, with a group of 3 ventral and 1 dorsal plumose setae near distal outer corner and 1 short, slender seta at distal inner corner. Third segment with 1 long seta on outer distal margin, 1 dorsal plumose seta at distal outer corner; 2 short setae, 1 dorsal and 1 ventral, near distal inner corner. First segment of inner flagellum with a group of 3 unequal dorsal setae in the distal half (these setae seem to be the rest of the reduced and fused outer flagellum), 1 ventral plumose seta below apophysis; apophysis distinct but slender, reaching proximal fourth of next segment, with 1 apical and 1 ventral, subapical plumose setae. Second segment of inner flagellum with a group of 1 simple seta and 3 aesthetascs, which are longer than next segment, at distal outer corner; 1 long apical and 1 short ventral setae at distal inner angle. Terminal segment slenderest, with 4 setae and 3 aesthetascs. Antenna (Fig. 2 B): small, 1 -segmented, only slightly dilated distally, with 2 terminal unequal plumose setae and 1 short, subterminal, simple seta; lateral seta absent. Labrum (Fig. 2 C): flat, symmetrical in ventral view and characteristic in shape. Free margin straight, bearing 2 small median teeth, flanked on either side by 4 acuminate curved teeth, gradually increasing in size laterally, and with 1 smaller somewhat blunt tooth on either side; tubular pore with long, thick-walled, proximally dilated tube, occurring ventrally on either side at base of lateral main tooth. Also, fine spinules, in rows, discernible on ventral surface, as illustrated. Mandible (Fig. 2 D–G): distal part of pars incisiva with 3 teeth, proximal tooth small; all teeth pointed in lateral view (Fig. 2 D–F), but blunt in frontal view (Fig. 2 G). Pars molaris (“Borstenlobus”) articulate, consisting of 5 claws; distal one defined at base, strongly developed into plate-like structure (Fig. 2 D, E) (almost cylindrical in a different view as in Fig. 2 F), apical margin concave and finely denticulate; 2 additional denticles also occurring below denticulate margin (Fig. 2 E), 3 spinules seen at base of pars molaris on distal margin. Palp 1 -segmented, only slightly longer than wide, bearing a long terminal seta. Maxillule (Fig. 2 H): with 2 endites. Proximal endite small, subquadrate, twice as long as wide, carrying 2 unequal, serrulate, claw-like spines, and 1 tiny spinule; also, a simple, triangular lobe lying at base of endite. Distal endite straight, slender, 2.4 times as long as wide, armed with 3 terminal claws of similar size, 2 subterminal claws, all claws with serrulate inner margin, and 3 subterminal setae on distal outer margin. Maxilla (Fig. 2 I): 4 -segmented, second and third segments half fused, with 2, (4, 12), and 1 setae, respectively; distalmost segment tiny. Thoracopods I–VII (Fig. 3 A–C): well developed, length gradually increasing from pairs I–III, last 4 pairs almost similar in size; thoracopods II–VII with 1 -segmented epipod each. Coxa with distinct, pointed projection at distal inner border; basis of thoracopods II–VI alone with inner marginal seta. Exopod 1 -segmented, with 2 very unequal terminal setae and 1 short subterminal seta on ventral side; subterminal seta absent on thoracopod I alone. Endopod 4 -segmented. Setal formulae: Th. I, 1 +0/0+ 1 / 1 +0/ 2 (0); Th. II–IV, 0+0/0+ 1 /0+ 1 / 1 (0); Th. V–VII, 0+0/0+ 1 /0+0/ 1 (0). Thoracopod VIII (Fig. 1 C): minute, sharply pointed, denticle-like structure. Pleopod 1 (Fig. 1 C): represented by 1 strong, plumose seta. Uropod (Fig. 1 A–B): sympod slender, 4.4 times as long as wide, bearing 4 spines in a row on distal inner margin and 1 short, simple seta on dorso-lateral surface almost opposite to spine row; distalmost spine stout, straight, 31 % longer than other spines, which are acutely pointed and almost equal in size. Exopod cylindrical, nearly 6 times as long as wide, measuring 42 % of sympod length and bearing 2 apical, unequal setae, outer seta spiniform, unipinnate and less than half the length of inner, bipinnate seta. Endopod sickle-shaped, reaching 62 % of sympod length, lateral margins smooth, but a longitudinal of fine spinules at about the middle of proximal part, in lateral view; a single long, plumose seta at about midlength of outer margin. Description of adult male (Fig. 4 A–C). Total body length of allotype 1.52 mm, of paratype 1.46 mm. Body and all appendages except antennule and thoracopod VIII as in female. Antennule (Fig. 4 A): same as in female except for antennal organ on second segment; second segment 1.5 times as long as wide, antennal organ seen as a massive protuberance at distal inner angle, tip rounded with an opening. Thoracopod VIII (Fig. 4 B–C) rather small so that the constituent parts are difficult to make out and interpret. Protopod massive but without prominent penial region. In latero-external view (Fig. 4 B) two structures are discernible, one with 2 and one without setae. In ventral view (Fig. 4 C) the structure with 2 setae is extended into a spoon-like projection and is interpreted here as a basexopod with a basipodal seta (the bigger one) and an exopodal seta (the smaller one). The other structure without setae can be seen in ventral view (Fig. 4 C) as a conical projection reaching the spoon-like projection of the basexopod. This structure is interpreted here as the external lobe. Where both meet, the internal and the dentate lobe also converge. Dentate lobe with a few denticles can be seen in latero-external view (Fig. 4 B). Comparison with other species will reveal whether the interpretation presented here is tenable. Intraspecific variation. The number of spines borne by the sympod of uropod is either 4 or 5. Etymology. The specific name refers to the prominent anal operculum (Latin adjective operculatus, operire = to close, cover); gender feminine. Ecology. At the type locality, the new species was found as strays in the surficial sediments of knee-deep waters of an exposed island at the middle of the river bed. It was greatly dominated by Habrobathynella. The fauna that co-occurred with the new species was diverse but not rich, and included the following: Bathynellacea: Habrobathynella schminkei Ranga Reddy, 2004, and Habrobathynella sp. Copepoda: Bryocyclops sp., Paracyclops sp., Parastenocaris curvispinus Enckell, 1970, Parastenocaris gayatri Ranga Reddy, 2001, Elaphoidella sp., Mesochra wolskii Jakubisiak, 1933, Nitocra?lacustris (Schmankevitsch, 1875), Folioquinpes chathamensis (G.O. Sars, 1905), and Phyllognathopus viguieri (Maupas, 1892). Cladocera: Macrothrix sp., chydorids. Other taxa were: unidentified oligochaetes, nematodes, mites, and insect larvae.Published as part of Reddy, Ranga, 2008, A new species of the genus Atopobathynella Schminke, 1973 (Crustacea, Syncarida, Bathynellacea) from the hyporheic zone of the River Godavari, South India, pp. 52-60 in Zootaxa 1829 on pages 53-58, DOI: 10.5281/zenodo.18316
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