The crack tip stress and deformation field is analyzed for an ideally plastic ordered NiAl single crystal of B2 (BCC type) structure which has only three independent slip systems at room temperature, the (100)(100) systems. For the crack on the (010) plane growing in the (101) direction, only one of these systems is capable of sustaining considerable plane plastic flow. It involves slip planes lying parallel to the crack tip, making an angle of 90 degrees with the crack plane, and has the yield condition sigma 12=+or- tau 0 (1 is the cracking direction, 2 the crack plane normal, and tau 0 the critical resolved shear stress). An elastic-ideally plastic asymptotic solution is derived in which the stress field has a In r type singularity, with a shearing discontinuity at 90 degrees . These features are verified and more fully quantified by a finite element solution.
Long-chain ω-hydroxyalkanethiols [HS(CH 2 ) n OH] coordinate to gold surfaces through the sulfur atom and produce ordered, hydrophilic monolayers in which the hydroxyl groups are exposed at the outer surface. Coadsorption of two ω-hydroxyalkanethiols of different chain lengths n resulted in the formation of a monolayer having a disordered surface region that was markedly less hydrophilic than the homogeneous, hydroxylic surface formed from either pure compound. By controlling the composition of the monolayer, it was also possible to control simultaneously the degree of order in the surface and its hydrophilicity. In the monolayers containing a mixture of alkanethiol components, these components apparently did not phase-segregate into macroscopic islands, but were dispersed on a molecular scale.
ADVERTISEMENT RETURN TO ISSUEPREVArticleNEXTConversion of a protein to a homogeneous asymmetric hydrogenation catalyst by site-specific modification with a diphosphinerhodium(I) moietyMichael E. Wilson and George M. WhitesidesCite this: J. Am. Chem. Soc. 1978, 100, 1, 306–307Publication Date (Print):January 1, 1978Publication History Published online1 May 2002Published inissue 1 January 1978https://pubs.acs.org/doi/10.1021/ja00469a064https://doi.org/10.1021/ja00469a064research-articleACS PublicationsRequest reuse permissionsArticle Views3103Altmetric-Citations489LEARN 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
Atomic force microscopy was used to characterize the sliding of molybdenum oxide (MoO 3 ) nanocrystals on single-crystal molybdenum disulfide (MoS 2 ) surfaces. Highly anisotropic friction was observed whereby MoO 3 nanocrystals moved only along specific directions of the MoS 2 surface lattice. The energy per unit area to move the MoO 3 nanocrystals along their preferred sliding direction was an order of magnitude less than required to slide macroscopic MoS 2 -bearing contacts. This extreme friction anisotropy was exploited to fabricate multicomponent MoO 3 nanostructures. These reversibly interlocking structures could serve as the basis for devices such as mechanical logic gates.
No abstract is provided for this article.
[1] Material contrasts across faults are a common occurrence, and it is important to understand if these material contrasts can influence the path of rupture propagation. Here we examine models, solved numerically, of rupture propagation through one type of geometric complexity, that of a fault branch stemming from a planar main fault on which rupture initiates. This geometry, with a material contrast across the main fault, could be representative of either a mature strike-slip fault or a subduction zone interface. We consider branches in both the compressional and extensional quadrants of the fault, and material configurations in which the branch fault is in either the stiffer or the more compliant material as well as configurations with no material contrast. We find that there are regimes in which this elastic contrast can influence the rupture behavior at a branching junction, but there are also stress states for which the branch activation will not depend on the orientation of the mismatch. For the scenarios presented here, both compressional and extensional side branches are more likely to rupture if the branch is on the side of the fault with the more compliant material versus the stiffer material. The stresses induced on the branch fault, by rupture traveling on the main fault, are different for the two orientations of material contrast. We show how the interactions between rupture on the two faults determine which faults are activated.
Plastic deformation processes have been studied in high speed silicon sheet growth using finite element analysis. Stress and strain rate distributions are calculated for steady-state growth of thin sheet under plane stress conditions. Predictions of the model are used to examine factors affecting residual stress and buckle formation for growth of silicon ribbon by the EFG method.