99 research outputs found

    Investigation of technological process zavaltsyuvannya balls in guiding transport mechanisms

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    Наведено конструкцію і принцип роботи пристрою для завальцювання кульок у направляючих у транспортних механізмах з попередньо підготовленим базовим отвором. Виведено аналітичні залежності для визначення силових, конструктивних і технологічних параметрів при завальцюванні кульок у транспортних направляючих парах тертя кочення, виготовлених з різних матеріалів.Present structure and principle of the device for zavaltsyuvannya balls in guiding the transport mechanisms of pre-prepared base hole. The derived analytical dependences for determination of power, structural and technological parameters in the balls by rolling in the transport steam rollingguides manufactured from different materials

    Blank assessment for ultra-small radiocarbon samples : chemical extraction and separation versus AMS

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    Author Posting. © Arizona Board of Regents on behalf of the University of Arizona, 2010. This article is posted here by permission of Dept. of Geosciences, University of Arizona for personal use, not for redistribution. The definitive version was published in Radiocarbon 52 (2010): 1322-1335.The Keck Carbon Cycle AMS facility at the University of California, Irvine (KCCAMS/UCI) has developed protocols for analyzing radiocarbon in samples as small as ~0.001 mg of carbon (C). Mass-balance background corrections for modern and 14C-dead carbon contamination (MC and DC, respectively) can be assessed by measuring 14C-free and modern standards, respectively, using the same sample processing techniques that are applied to unknown samples. This approach can be validated by measuring secondary standards of similar size and 14C composition to the unknown samples. Ordinary sample processing (such as ABA or leaching pretreatment, combustion/graphitization, and handling) introduces MC contamination of ~0.6 ± 0.3 μg C, while DC is ~0.3 ± 0.15 μg C. Today, the laboratory routinely analyzes graphite samples as small as 0.015 mg C for external submissions and ≅0.001 mg C for internal research activities with a precision of ~1% for ~0.010 mg C. However, when analyzing ultra-small samples isolated by a series of complex chemical and chromatographic methods (such as individual compounds), integrated procedural blanks may be far larger and more variable than those associated with combustion/graphitization alone. In some instances, the mass ratio of these blanks to the compounds of interest may be so high that the reported 14C results are meaningless. Thus, the abundance and variability of both MC and DC contamination encountered during ultra-small sample analysis must be carefully and thoroughly evaluated. Four case studies are presented to illustrate how extraction chemistry blanks are determined

    Anisotropic Singular Integrals in Product Spaces

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    Let AiA_i for i=1,2i=1, 2 be an expansive dilation, respectively, on Rn{\mathbb R}^n and Rm{\mathbb R}^m and A(A1,A2)\vec A\equiv(A_1, A_2). Denote by {\mathcal A}_\infty(\rnm; \vec A) the class of Muckenhoupt weights associated with A\vec A. The authors introduce a class of anisotropic singular integrals on Rn×Rm\mathbb R^n\times\mathbb R^m, whose kernels are adapted to A\vec A in the sense of Bownik and have vanishing moments defined via bump functions in the sense of Stein. Then the authors establish the boundedness of these anisotropic singular integrals on Lwq(Rn×Rm)L^q_w(\mathbb R^n\times\mathbb R^m) with q(1,)q\in(1, \infty) and wAq(Rn×Rm;A)w\in\mathcal A_q(\mathbb R^n\times\mathbb R^m; \vec A) or on Hwp(Rn×Rm;A)H^p_w(\mathbb R^n\times\mathbb R^m; \vec A) with p(0,1]p\in(0, 1] and wA(Rn×Rm;A)w\in\mathcal A_\infty(\mathbb R^n \times\mathbb R^m; \vec A). These results are also new even when w=1w=1.Comment: Sci. China Math., to appea

    Reemerging superconductivity at 48 K across quantum criticality in iron chalcogenides

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    Pressure plays an essential role in the induction1 and control2,3 of superconductivity in iron-based superconductors. Substitution of a smaller rare-earth ion for the bigger one to simulate the pressure effects has surprisingly raised the superconducting transition temperature Tc to the record high 55 K in these materials4,5. However, Tc always goes down after passing through a maximum at some pressure and the superconductivity eventually tends to disappear at sufficiently high pressures1-3. Here we show that the superconductivity can reemerge with a much higher Tc after its destruction upon compression from the ambient-condition value of around 31 K in newly discovered iron chalcogenide superconductors. We find that in the second superconducting phase the maximum Tc is as high as 48.7 K for K0.8Fe1.70Se2 and 48 K for (Tl0.6Rb0.4)Fe1.67Se2, setting the new Tc record in chalcogenide superconductors. The presence of the second superconducting phase is proposed to be related to pressure-induced quantum criticality. Our findings point to the potential route to the further achievement of high-Tc superconductivity in iron-based and other superconductors.Comment: 20 pages and 7 figure

    Local Hardy Spaces of Musielak-Orlicz Type and Their Applications

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    Let \phi: \mathbb{R}^n\times[0,\fz)\rightarrow[0,\fz) be a function such that ϕ(x,)\phi(x,\cdot) is an Orlicz function and ϕ(,t)Aloc(Rn)\phi(\cdot,t)\in A^{\mathop\mathrm{loc}}_{\infty}(\mathbb{R}^n) (the class of local weights introduced by V. S. Rychkov). In this paper, the authors introduce a local Hardy space hϕ(Rn)h_{\phi}(\mathbb{R}^n) of Musielak-Orlicz type by the local grand maximal function, and a local BMO\mathop\mathrm{BMO}-type space bmoϕ(Rn)\mathop\mathrm{bmo}_{\phi}(\mathbb{R}^n) which is further proved to be the dual space of hϕ(Rn)h_{\phi}(\mathbb{R}^n). As an application, the authors prove that the class of pointwise multipliers for the local BMO\mathop\mathrm{BMO}-type space bmoϕ(Rn)\mathop\mathrm{bmo}^{\phi}(\mathbb{R}^n), characterized by E. Nakai and K. Yabuta, is just the dual of L^1(\rn)+h_{\Phi_0}(\mathbb{R}^n), where ϕ\phi is an increasing function on (0,)(0,\infty) satisfying some additional growth conditions and Φ0\Phi_0 a Musielak-Orlicz function induced by ϕ\phi. Characterizations of hϕ(Rn)h_{\phi}(\mathbb{R}^n), including the atoms, the local vertical and the local nontangential maximal functions, are presented. Using the atomic characterization, the authors prove the existence of finite atomic decompositions achieving the norm in some dense subspaces of hϕ(Rn)h_{\phi}(\mathbb{R}^n), from which, the authors further deduce some criterions for the boundedness on hϕ(Rn)h_{\phi}(\mathbb{R}^n) of some sublinear operators. Finally, the authors show that the local Riesz transforms and some pseudo-differential operators are bounded on hϕ(Rn)h_{\phi}(\mathbb{R}^n).Comment: Sci. China Math. (to appear

    Collected Data for Tests on NACA 0015 Aerofoil with Chord of Length 0.275m. G.U. Aero Report 9209

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    Herein is presented the collected data for tests in which a NACA 0015 aerofoil with chord of length 0.275m, was subjected to a variety of displacements in pitch about the quarter-chord location at low Reynolds numbers

    Collected Data for Tests on NACA 0015 Aerofoil with Chord of Length 0.275m. G.U. Aero Report 9209

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    Herein is presented the collected data for tests in which a NACA 0015 aerofoil with chord of length 0.275m, was subjected to a variety of displacements in pitch about the quarter-chord location at low Reynolds numbers
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