ADVERTISEMENT RETURN TO ISSUEPREVArticleNEXTReaction of copper(I) hydride with organocopper(I) compoundsGeorge M. Whitesides, Joseph San Filippo Jr., Erwin R. Stredronsky, and Charles P. CaseyCite this: J. Am. Chem. Soc. 1969, 91, 23, 6542–6544Publication Date (Print):November 1, 1969Publication History Published online1 May 2002Published inissue 1 November 1969https://pubs.acs.org/doi/10.1021/ja01051a093https://doi.org/10.1021/ja01051a093research-articleACS PublicationsRequest reuse permissionsArticle Views779Altmetric-Citations60LEARN 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 InRedditEmail Other access optionsGet e-Alertsclose Get e-Alerts
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The asymptotic structure of near-tip stress and deformation fields is analyzed for cracks growing in elastic–perfectly plastic solids. A general formulation is presented for materials of arbitrary yield condition and associated flow rule, including anisotropic response, although detailed results are presented only for isotropic materials of the Huber–Mises type. Centered fan sectors of singular straining at a crack tip are shown to be general, independent of details of material response, as are also the types of plastic strain singularities associated with stationary and growing cracks. Previously results for the Huber–Mises material are recovered by specialization from the general formulation, some corrections are made, and recent work on using results of such a near-tip analysis as a basis for predicting plane strain stable crack growth is reviewed briefly.
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Development of highly-integrated, ultra-sensitive real-time electronic sensor arrays for detection of chemical and biological threats has been carried out by exploiting the unique electronic properties and integration potential of nanowire electronic devices. Silicon nanowires have been developed and assembled into arrays of sensor elements that provide highly-robust and specific ultra-sensitive species identification while at the same time dramatically reducing false positives. Sensor modalities developed in this project are based on nanowire field-effect transistors, where unique specificities of sensor elements for chemical and biological threats has been achieved through specific surface modification using designed chemical and biological receptors for threats of interest. Experiments have demonstrated biothreat (viruses and toxins) detection at better than 1 picomolar sensitivity, detection chemical (explosive) threats at better than 100 parts per billion sensitivity, simultaneous multiplexed detection from ten or more addressable nanowire sensing elements, and moreover, signal processing algorithms that allow for discrimination of real-false signals in presence of noise were developed.
The assignment of boundary values for the chemical potential and the calculation of energy release rates for the growth of creep cavities along grain boundaries by self-diffusion are discussed. It is assumed that the boundaries are flat and that surface and gran-boundary diffusion are the dominant transport mechanisms. As matter diffuses from the void surface into and along the grain boundary, misfit residual stresses are induced to alleviate the high stress concentration ahead of the cavity apex. As a result, it is shown that the contribution of strain energy terms to the chemical potential can be neglected in typical cases. Also, contrary to the Griffith crack extension model, the energy dissipation incurred by diffusive removal of material from the cavity surface and deposition in the grain boundary is a major term in the energy transfers associated with cavity growth. The primary energy sink in diffusive cavity growth arises from the work done by the grain-boundary normal stress when matter is inserted in the near-tip region by diffusion, and not from the loss of strain energy of matter that is removed from the cavity at its tip or from a work of bond separation. Thermodynamic restrictions on the angle formed by the void surfaces at their apex, where they join the grain boundary is described. The derivation of boundary values for the chemical potential is carried out in a manner appropriate for arbitrarily large but elastic distortions of material near the cavity tip and, by contrast to most previous work in the area. Rigorously the effects of surface tension, as distinct from surface energy, is included.