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An effective procedure is developed for estimating the maximum response of a class of torsionally‐coupled, multistory buildings due to earthquake ground motion characterized by smooth response spectra. Several properties characterize this class of buildings, the most important of which is that all frames (spanning along either of two orthogonal directions) have proportional lateral stiffness matrices. It is demonstrated that the maximum response of such a torsionally‐coupled, N‐story building in its njth mode of vibration can be determined exactly by analyzing: (1) The response in the jth vibration mode (j=1,2,…,N) of the corresponding torsionally‐uncoupled, N‐story system; and (2) the response in the nth vibration mode (n=1, 2 for a one‐way symmetric plan) of an associated torsionally‐coupled, one‐story system. The total response is then determined by an appropriate modal combination rule.
Ferromagnetic shape memory alloys (FSMAs) and magnetic shape memory alloys (MSMAs) are metallic alloys that can undergo inelastic responses when exposed to magnetic fields. Several constitutive models have been proposed so far to model the behaviors of FSMAs. In this work, the effects of loading history on reorientation start conditions are considered, and it is shown that reorientation start conditions are not fixed values; rather, they change with respect to the amount of loading history. To consider the effects of loading history on reorientation start conditions, an available phase diagram in stress-field space is generalized to reorientation surfaces in stress-field-loading history space. Correspondingly, kinetic laws are derived in a continuum framework to be used with the reorientation surfaces to determine the amount of the martensitic variant 2 volume fraction. Based on the geometry of the reorientation surfaces, conditions that must be satisfied to ensure the continuation of reorientations are obtained. Available experimental findings validate the proposed model and the reorientation surfaces.
The Great Recession that started in 2008 has drawn constant comparisons with the Great Depression that unfolded in 1929. This paper documents how the response of policy makers in the current episode has been markedly different from the one observed in the 1920s and 1930s and to what extent this different behavior has followed the lessons from the historical analysis of the Great Depression. The historical account is also used to discuss probable changes to the world´s economic landscape regarding both trade and financial globalization.
Kinetic stability of aluminium
Abstract not Available.
We present an algorithm to recover three-dimensional shape i.e. surface orientation and relative depth from a single segmented image. It is assumed that the scene is composed of opaque regular solid objects bounded by piecewise smooth surfaces with no markings or texture. Also it is assumed that the reflectance map E=R(n) is known. For the canonical case of lambertian surfaces illuminated by a point light source, this implies knowing the light source direction. <p> Solutions for simplified versions of this problem have been proposed by Sugihara for the case of polyhedra, and by Horn et al for the case of a single smooth surface patch given the surface orientation on the patch boundary. This work presents the first solution for the general case. <p> A variational formulation of line drawing and shading constraints in a common framework is developed. Finding the 3-D shape which best satisfies these constraints is a difficult global optimization problem. The problem is made tractable by precomputing line labels at junctions using the algorithm developed in [Malik '85]. The global constraints are partitioned into constraint sets corresponding to the faces, edges and vertices in the scene. For a face the constraints are given by Horn's image irradiance equation. We develop a variational formulation of the constraints at an edge -- both from the known direction of the image curve corresponding to the edge and shading. The associated Euler-Lagrange differential equation completely captures the local information. At a vertex, the constraints are modelled by a system of non-linear equations. <p> An algorithm has been developed to solve this system of constraints. We are now studying various refinements intended to make the algorithm robust in the presence of image noise
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ADVERTISEMENT RETURN TO ISSUEPREVArticleNEXTContinuous rods of macroporous polymer as high-performance liquid chromatography separation mediaFrantisek. Svec and Jean M. J. FrechetCite this: Anal. Chem. 1992, 64, 7, 820–822Publication Date (Print):April 1, 1992Publication History Published online1 May 2002Published inissue 1 April 1992https://doi.org/10.1021/ac00031a022RIGHTS & PERMISSIONSArticle Views2584Altmetric-Citations840LEARN ABOUT THESE METRICSArticle Views are the COUNTER-compliant sum of full text article downloads since November 2008 (both PDF and HTML) across all institutions and individuals. These metrics are regularly updated to reflect usage leading up to the last few days.Citations are the number of other articles citing this article, calculated by Crossref and updated daily. Find more information about Crossref citation counts.The Altmetric Attention Score is a quantitative measure of the attention that a research article has received online. Clicking on the donut icon will load a page at altmetric.com with additional details about the score and the social media presence for the given article. Find more information on the Altmetric Attention Score and how the score is calculated. Share Add toView InAdd Full Text with ReferenceAdd Description ExportRISCitationCitation and abstractCitation and referencesMore Options Share onFacebookTwitterWechatLinked InReddit PDF (406 KB) Get e-Alerts Get e-Alerts
An entry from the Cambridge Structural Database, the world’s repository for small molecule crystal structures. The entry contains experimental data from a crystal diffraction study. The deposited dataset for this entry is freely available from the CCDC and typically includes 3D coordinates, cell parameters, space group, experimental conditions and quality measures.