240 research outputs found

    Using of Tendinous Plasty in Treatment of Patients with Flexor Tendons of 2–5 Fingers Injury in “Critical” Zone

    Get PDF
    Injury of both superficial and deep tendons of fingers flexors needs to carry out tendinous plasty with excision of distal part of superficial flexor muscle tendon. Use of length measuring method for tendinous transplant allows us to avoid the flexion contracture in future and appearance of functional insufficiency of flexion during postoperative period and rehabilitation of patient

    Simulation study of the digital temperature sensor operation in case of a non-standard mechanical impact of the NPP equipment

    Get PDF
    The article presents the results of an experimental study relevant to the effective organization of temperature control of thermomechanical equipment at nuclear power plants (turbines, pumps, steam generators, deaerators, etc.). Bench studies of the reaction of the DS18B20 digital intelligent temperature sensor, which is supposed to be introduced at Ukrainian nuclear power plants, to the application of external compression force to its body, which may occur under conditions typical for the operation of equipment operating at nuclear power plants, have been carried out. An electrical circuit diagram has been developed for a reset signal simulation device (for bench modeling of a sensor application system). The issues of identifying a sign in the sensor output signal informing about the effect of an external compression force on its body are considered. The technique of bench experiments and processing of research results necessary to address the issue of introducing new digital measuring equipment for temperature control of thermomechanical equipment of nuclear power plants is given.Представлено результати експериментального дослідження, актуального для ефективної організації контролю температури тепломеханічного обладнання на АЕС (турбін, насосів, парогенераторів, деаераторів та ін.). Проведено стендові дослідження реакції цифрового інтелектуального датчика температури DS18B20, передбачуваного до впровадження на АЕС України, на дію зовнішньої сили стиснення на його корпус, яка може виникнути в умовах, характерних для експлуатації діючого на АЕС обладнання. Розроблена електрична принципова схема пристрою імітації сигналу «скидання» (для стендового моделювання системи застосування датчика). Розглянуто питання виявлення у вихідному сигналі датчика ознаки, що інформує про вплив зовнішньої сили стиснення на його корпус. Наведено методику проведення стендових експериментів та обробки результатів досліджень, необхідних для вирішення питання про впровадження нових цифрових засобів вимірювальної техніки для контролю температури тепломеханічного обладнання АЕС.Представлены результаты экспериментального исследования, актуального для эффективной организации контроля температуры тепломеханического оборудования на АЭС (турбин, насосов, парогенераторов, деаэраторов и др.). Проведены стендовые исследования реакции цифрового интеллектуального датчика температуры DS18B20, предполагаемого к внедрению на АЭС Украины, на приложение внешней силы сжатия на его корпус, которая может возникнуть в условиях, характерных для эксплуатации действующего на АЭС оборудования. Разработана электрическая принципиальная схема устройства имитации сигнала «сброс» (для стендового моделирования системы применения датчика). Рассмотрены вопросы выявления в выходном сигнале датчика признака, информирующего о воздействии внешней силы сжатия на его корпус. Приведена методика проведения стендовых экспериментов и обработки результатов исследований, необходимых для решения вопроса о внедрении новых цифровых средств измерительной техники для контроля температуры тепломеханического оборудования АЭС

    SURGICAL TREATMENT OF PATIENTS WITH HALLUX VALGUS BY MINI-APPARATUS OF EXTERNAL FIXATION

    Get PDF
    The authors of article suggest methods of surgical correction of pathology by means of fixation of the first metatarsal bone with specialconstruction ofmini-apparatus for externalfixation. This approach provides decrease of recovery period, reduces complications riskas well as deformation relapse

    Measurement of K^+ \to \pi^0 \mu^+ \nu \gamma decay using stopped kaons

    Full text link
    The K^+ \to \pi^0 \mu^+ \nu \gamma (Kμ3γK_{\mu 3 \gamma}) decay has been measured with stopped positive kaons at the KEK 12 GeV proton synchrotron. A Kμ3γK_{\mu 3 \gamma} sample containing 125 events was obtained. The partial branching ratio Br(Kμ3γ,Eγ>30MeV,θμ+γ>20)Br(K_{\mu 3 \gamma}, E_{\gamma}>30 {\rm MeV}, \theta_{\mu^+ \gamma}>20^{\circ}) was found to be [2.4±0.5(stat)±0.6(syst)]×105[2.4 \pm 0.5(stat) \pm 0.6(syst)]\times 10^{-5}, which is in good agreement with theoretical predictions.Comment: 12 pages, 3 figures, to be published in Physics Letters

    Measurement of direct photon emission in K+π+π0γK^+ \to \pi^+ \pi^0 \gamma decay using stopped positive kaons

    Full text link
    The radiative decay K+π+π0γK^+ \to \pi^+ \pi^0 \gamma (Kπ2γK_{\pi 2 \gamma}) has been measured with stopped positive kaons. A Kπ2γK_{\pi 2 \gamma} sample containing 4k events was analyzed, and the Kπ2γK_{\pi 2 \gamma} branching ratio of the direct photon emission process was determined to be [6.1±2.5(stat)±1.9(syst)]×106[6.1\pm2.5({\rm stat})\pm1.9({\rm syst})]\times 10^{-6}. No interference pattern with internal bremsstrahlung was observed.Comment: 12 pages, 6 figures, 2 tables, to be published in Phys. Lett.

    Measurement of Γ(Kμ3)/Γ(Ke3)\Gamma(K_{\mu 3})/\Gamma(K_{e3}) ratio using stopped positive kaons

    Full text link
    The ratio of the K+π0μ+νK^{+}\to \pi^{0} \mu^{+} \nu (Kμ3+K_{\mu3}^+) and K+π0e+νK^{+}\to \pi^{0} e^{+} \nu (Ke3+K_{e3}^+) decay widths, Γ(Kμ3)/Γ(Ke3)\Gamma(K_{\mu 3})/\Gamma(K_{e3}), has been measured with stopped positive kaons. Kμ3+K_{\mu3}^+ and Ke3+K_{e3}^+ samples containing 2.4×104\times 10^4 and 4.0×104\times 10^4 events, respectively, were analyzed. The Γ(Kμ3)/Γ(Ke3)\Gamma(K_{\mu3})/\Gamma(K_{e3}) ratio was obtained to be 0.671±\pm0.007(stat.)±\pm0.008(syst.) calculating the detector acceptance by a Monte Carlo simulation with the assumption of μ\mu-ee universality in Kl3+K_{l3}^+ decay. The coefficient of the q2q^2 dependent term of the f0f_0 form factor was also determined to be λ0\lambda_0=0.022±\pm0.005(stat.)±\pm0.004(syst.).Comment: 12 pages, 6 figure

    Measurement of the View the tt production cross-section using eμ events with b-tagged jets in pp collisions at √s = 13 TeV with the ATLAS detector

    Get PDF
    This paper describes a measurement of the inclusive top quark pair production cross-section (σtt¯) with a data sample of 3.2 fb−1 of proton–proton collisions at a centre-of-mass energy of √s = 13 TeV, collected in 2015 by the ATLAS detector at the LHC. This measurement uses events with an opposite-charge electron–muon pair in the final state. Jets containing b-quarks are tagged using an algorithm based on track impact parameters and reconstructed secondary vertices. The numbers of events with exactly one and exactly two b-tagged jets are counted and used to determine simultaneously σtt¯ and the efficiency to reconstruct and b-tag a jet from a top quark decay, thereby minimising the associated systematic uncertainties. The cross-section is measured to be: σtt¯ = 818 ± 8 (stat) ± 27 (syst) ± 19 (lumi) ± 12 (beam) pb, where the four uncertainties arise from data statistics, experimental and theoretical systematic effects, the integrated luminosity and the LHC beam energy, giving a total relative uncertainty of 4.4%. The result is consistent with theoretical QCD calculations at next-to-next-to-leading order. A fiducial measurement corresponding to the experimental acceptance of the leptons is also presented

    Search for H→γγ produced in association with top quarks and constraints on the Yukawa coupling between the top quark and the Higgs boson using data taken at 7 TeV and 8 TeV with the ATLAS detector

    Get PDF
    A search is performed for Higgs bosons produced in association with top quarks using the diphoton decay mode of the Higgs boson. Selection requirements are optimized separately for leptonic and fully hadronic final states from the top quark decays. The dataset used corresponds to an integrated luminosity of 4.5 fb−14.5 fb−1 of proton–proton collisions at a center-of-mass energy of 7 TeV and 20.3 fb−1 at 8 TeV recorded by the ATLAS detector at the CERN Large Hadron Collider. No significant excess over the background prediction is observed and upper limits are set on the tt¯H production cross section. The observed exclusion upper limit at 95% confidence level is 6.7 times the predicted Standard Model cross section value. In addition, limits are set on the strength of the Yukawa coupling between the top quark and the Higgs boson, taking into account the dependence of the tt¯H and tH cross sections as well as the H→γγ branching fraction on the Yukawa coupling. Lower and upper limits at 95% confidence level are set at −1.3 and +8.0 times the Yukawa coupling strength in the Standard Model

    The performance of the jet trigger for the ATLAS detector during 2011 data taking

    Get PDF
    The performance of the jet trigger for the ATLAS detector at the LHC during the 2011 data taking period is described. During 2011 the LHC provided proton–proton collisions with a centre-of-mass energy of 7 TeV and heavy ion collisions with a 2.76 TeV per nucleon–nucleon collision energy. The ATLAS trigger is a three level system designed to reduce the rate of events from the 40 MHz nominal maximum bunch crossing rate to the approximate 400 Hz which can be written to offline storage. The ATLAS jet trigger is the primary means for the online selection of events containing jets. Events are accepted by the trigger if they contain one or more jets above some transverse energy threshold. During 2011 data taking the jet trigger was fully efficient for jets with transverse energy above 25 GeV for triggers seeded randomly at Level 1. For triggers which require a jet to be identified at each of the three trigger levels, full efficiency is reached for offline jets with transverse energy above 60 GeV. Jets reconstructed in the final trigger level and corresponding to offline jets with transverse energy greater than 60 GeV, are reconstructed with a resolution in transverse energy with respect to offline jets, of better than 4 % in the central region and better than 2.5 % in the forward direction

    Search for dark matter produced in association with a hadronically decaying vector boson in pp collisions at sqrt (s) = 13 TeV with the ATLAS detector

    Get PDF
    A search is presented for dark matter produced in association with a hadronically decaying W or Z boson using 3.2 fb−1 of pp collisions at View the MathML sources=13 TeV recorded by the ATLAS detector at the Large Hadron Collider. Events with a hadronic jet compatible with a W or Z boson and with large missing transverse momentum are analysed. The data are consistent with the Standard Model predictions and are interpreted in terms of both an effective field theory and a simplified model containing dark matter
    corecore