446 research outputs found

    On the constants in a Kato inequality for the Euler and Navier-Stokes equations

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    We continue an analysis, started in [10], of some issues related to the incompressible Euler or Navier-Stokes (NS) equations on a d-dimensional torus T^d. More specifically, we consider the quadratic term in these equations; this arises from the bilinear map (v, w) -> v . D w, where v, w : T^d -> R^d are two velocity fields. We derive upper and lower bounds for the constants in some inequalities related to the above bilinear map; these bounds hold, in particular, for the sharp constants G_{n d} = G_n in the Kato inequality | < v . D w | w >_n | <= G_n || v ||_n || w ||^2_n, where n in (d/2 + 1, + infinity) and v, w are in the Sobolev spaces H^n, H^(n+1) of zero mean, divergence free vector fields of orders n and n+1, respectively. As examples, the numerical values of our upper and lower bounds are reported for d=3 and some values of n. When combined with the results of [10] on another inequality, the results of the present paper can be employed to set up fully quantitative error estimates for the approximate solutions of the Euler/NS equations, or to derive quantitative bounds on the time of existence of the exact solutions with specified initial data; a sketch of this program is given.Comment: LaTeX, 39 pages. arXiv admin note: text overlap with arXiv:1007.4412 by the same authors, not concerning the main result

    Anurans using in biomonitoring of uranium wastes’ influence on zoocoenosis

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    Đ”ĐŸŃĐ»Ń–ĐŽĐ¶Đ”ĐœĐœŃ ĐČплОĐČу ĐČŃ–ĐŽŃ…ĐŸĐŽŃ–ĐČ ĐżŃ–ĐŽĐżŃ€ĐžŃ”ĐŒŃŃ‚ĐČ Ń–Đ· ĐżĐ”Ń€Đ”Ń€ĐŸĐ±ĐșĐž ŃƒŃ€Đ°ĐœĐŸĐČĐŸŃ— руЮо ĐżĐŸĐșазалО, Ń‰ĐŸ Ń”ĐŽĐžĐœĐžĐč ĐČОЎ Đ·Đ”ĐŒĐœĐŸĐČĐŸĐŽĐœĐžŃ…, яĐșĐžĐč ĐŒĐ”ŃˆĐșає у ŃŃ‚Ń–Ń‡ĐœĐžŃ… ĐČĐŸĐŽĐ°Ń… – ĐŸĐ·Đ”Ń€ĐœĐ° жаба (Rana ridibunda). ĐžŃĐŸĐ±ĐžĐœĐž старшох ĐČіĐșĐŸĐČох груп Ń†ŃŒĐŸĐłĐŸ ĐČОЎу Đ°ĐŒŃ„Ń–Đ±Ń–Đč частĐșĐŸĐČĐŸ ĐżŃ€ĐžŃŃ‚ĐŸŃŃƒĐČĐ°Đ»ĐžŃŃ ĐŽĐŸ ĐČплОĐČу ĐżĐŸĐ»ŃŽŃ‚Đ°ĐœŃ‚Ń–ĐČ ŃŃ‚Ń–Ń‡ĐœĐžŃ… ĐČĐŸĐŽ Đ·Đ° Ń€Đ°Ń…ŃƒĐœĐŸĐș Đ·ĐŒŃ–ĐœĐž Ń„Ń–Đ·Ń–ĐŸĐ»ĐŸĐłĐŸ-Đ±Ń–ĐŸŃ…Ń–ĐŒŃ–Ń‡ĐœĐžŃ… ĐżĐ°Ń€Đ°ĐŒĐ”Ń‚Ń€Ń–ĐČ ĐŸŃ€ĐłĐ°ĐœŃ–ĐČ, Ń‰ĐŸ Đ±Đ”Ń€ŃƒŃ‚ŃŒ Đ°ĐșтоĐČĐœŃƒ участь у ĐŒĐ”Ń‚Đ°Đ±ĐŸĐ»Ń–Đ·ĐŒŃ–.Â Đ”ĐŸŃĐ»Ń–ĐŽĐ¶Đ”ĐœĐœŃ ĐČплОĐČу ĐČŃ–ĐŽŃ…ĐŸĐŽŃ–ĐČ ĐżŃ–ĐŽĐżŃ€ĐžŃ”ĐŒŃŃ‚ĐČ Ń–Đ· ĐżĐ”Ń€Đ”Ń€ĐŸĐ±ĐșĐž ŃƒŃ€Đ°ĐœĐŸĐČĐŸŃ— руЮо ĐżĐŸĐșазалО, Ń‰ĐŸ Ń”ĐŽĐžĐœĐžĐč ĐČОЎ Đ·Đ”ĐŒĐœĐŸĐČĐŸĐŽĐœĐžŃ…, яĐșĐžĐč ĐŒĐ”ŃˆĐșає у ŃŃ‚Ń–Ń‡ĐœĐžŃ… ĐČĐŸĐŽĐ°Ń… – ĐŸĐ·Đ”Ń€ĐœĐ° жаба (Rana ridibunda). ĐžŃĐŸĐ±ĐžĐœĐž старшох ĐČіĐșĐŸĐČох груп Ń†ŃŒĐŸĐłĐŸ ĐČОЎу Đ°ĐŒŃ„Ń–Đ±Ń–Đč частĐșĐŸĐČĐŸ ĐżŃ€ĐžŃŃ‚ĐŸŃŃƒĐČĐ°Đ»ĐžŃŃ ĐŽĐŸ ĐČплОĐČу ĐżĐŸĐ»ŃŽŃ‚Đ°ĐœŃ‚Ń–ĐČ ŃŃ‚Ń–Ń‡ĐœĐžŃ… ĐČĐŸĐŽ Đ·Đ° Ń€Đ°Ń…ŃƒĐœĐŸĐș Đ·ĐŒŃ–ĐœĐž Ń„Ń–Đ·Ń–ĐŸĐ»ĐŸĐłĐŸ-Đ±Ń–ĐŸŃ…Ń–ĐŒŃ–Ń‡ĐœĐžŃ… ĐżĐ°Ń€Đ°ĐŒĐ”Ń‚Ń€Ń–ĐČ ĐŸŃ€ĐłĐ°ĐœŃ–ĐČ, Ń‰ĐŸ Đ±Đ”Ń€ŃƒŃ‚ŃŒ Đ°ĐșтоĐČĐœŃƒ участь у ĐŒĐ”Ń‚Đ°Đ±ĐŸĐ»Ń–Đ·ĐŒŃ–. The research of influence of wastes of uranium ore processing enterprises showed that only one amphibian species inhabits the sewage – the lake frog. Individuals of senior age groups of this species partly adapted to pollutants influence due to the change of physiology-biochemical parameters of the organs, which actively participate in metabolism

    Analysis of data on the relation between eddies and streaky structures in turbulent flows using the placebo method

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    An artificially synthesized velocity field with known properties is used as a test data set in analyzing and interpreting the turbulent flow velocity fields. The objective nature of this approach is utilized for studying the relation between streaky and eddy structures. An analysis shows that this relation may be less significant than is customarily supposed

    Haemostasis modulation by calix[4]arene methylenebisphosphonic acid C-145 and its sulfur-containing analogue

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    C-145 (octasodium salt of calix[4]arene-tetra-methylenebisphosphonic acid) was previously considered as specific anti-сoagulant agent that affects fibrin polymerization and does not notably influence other parameters of coagulation system. C-145S (octasodium salt of thiacalix[4]arene-tetra-methylenebisphosphonic acid) possessing wider hydrophobic hole was expected to be more effective antithrombotic agent than C-145. The aim of present work was to compare the action of both organic compounds on fibrin polymerization, fibrinolysis, platelets and endothelial cells. The change of turbidity during fibrin clot formation induced by APTT-reagent and digestion induced by tPA was estimated. Turbidity study was used for the estimation of polymeric fibrin hydrolysis by plasmin in the presence of thiacalix[4]arene C-145S and calix[4]arene C-145. Effects of thiacalix[4]arene C-145S and calix[4]arene C-145 on the activation of Glu-plasminogen by streptokinase were studied using chromogenic substrate S2251. Platelet aggregation study was performed using aggregometry. Stimulated Ca2+ efflux from endoplasmic reticulum and cytoplasm were determined using specific Ca2+-sensitive probes targeted to endoplasmic reticulum (Mag-Fluo-4) and cytoplasm (FURA-2) by spectrofluorimetry. Both C-145 and C-145S decreased the final turbidity of clot and prolonged clot lysis time in blood plasma in comparison to control value. C-145 was shown to be the more effective fibrinolysis inhibitor when studied in model system of polymerized fibrin desAB. C-145S but not C-145 induced concentration changes of Ca2+ in cytoplasm of resting platelets and significantly inhibited (up to 30%) Ca2+ efflux from endoplasmic reticulum of platelets activated by ADP. Both C-145 and C-145S stimulated the proliferation of endothelial cells of PAE cell line. The effect of C-145S was more prominent. In conclusion, calix[4]arene C 145S proved to be the more potent inhibitor of fibrin polymerization in comparison to C-145, which suggested earlier as anticoagulant agent. C-145S proved to have much more outlined inhibitory action on Ca2+-signaling in platelets and stimulatory effect on endothelial cells proliferation. Thus C-145 remained the most prospective molecular platform for the development of antithrombotic agent

    Novel monoclonal antibody to fibrin(ogen) αC-region for detection of the earliest forms of soluble fibrin

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    Obtaining new monoclonal antibodies (mAbs) towards fibrin(ogen) and its fragments is an important task for studying mechanisms of blood clot formation, searching for novel antithrombotic agents and developing immunodiagnostics. The aim of the present work was to create and characterize a new mAb towards the fibrin(ogen) αХ-region. We surmise that having a specific mAb towards this flexible part of the molecule will allow us to study the role of the αХ-region in fibrin polymerization and also to develop an approach for detecting the earliest forms of soluble fibrin by sandwich ELISA. Using hybridoma technology we ĐŸbtained mAb 1-5A to the αC-region of fibrinogen.. It was characterized using several variations of ELISA and Western blot. Application of specific proteases together with MALDI-TOF analysis allowed us to localize its epitope that is located in fragment 537-595 of the Aα-chain of fibrin(ogen). МAb 1-5A can be used as a detecting tag-antibody in sandwich ELISA for the quantification of the earliest forms of soluble fibrin which are uncleaved by plasmin and preserved C-terminal portions of αC-regions. These earliest forms of soluble fibrin are direct evidence of blood coagulation system activation, thrombin generation and the danger of intravascular thrombus formation. Their determination will provide additional, more accurate information about the state of the blood coagulation system and the risk of blood clotting, which is very important for the timely and correct selection of adequate antithrombotic therapy. MAb 1-5A effectively binds the αC-containing molecules of fibrinogen and fibrin in blood plasma. It also can be used for studying protein-protein and protein-cellular interactions of the αC-regions of fibrin(ogen)

    Measurement of antiproton production from antihyperon decays in pHe collisions at √sNN=110GeV

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    The interpretation of cosmic antiproton flux measurements from space-borne experiments is currently limited by the knowledge of the antiproton production cross-section in collisions between primary cosmic rays and the interstellar medium. Using collisions of protons with an energy of 6.5 TeV incident on helium nuclei at rest in the proximity of the interaction region of the LHCb experiment, the ratio of antiprotons originating from antihyperon decays to prompt production is measured for antiproton momenta between 12 and 110GeV\!/c . The dominant antihyperon contribution, namely Λ¯ → pÂŻ π+ decays from promptly produced Λ¯ particles, is also exclusively measured. The results complement the measurement of prompt antiproton production obtained from the same data sample. At the energy scale of this measurement, the antihyperon contributions to antiproton production are observed to be significantly larger than predictions of commonly used hadronic production models

    Measurement of τL using the Bs0 →J/ψη decay mode

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    Using a proton–proton collision data sample collected by the LHCb detector and corresponding to an integrated luminosity of 5.7fb-1 , the lifetime of the light Bs0 mass eigenstate, τL , is measured using the Bs0→J/ψη decay mode to be τL=1.445±0.016(stat)±0.008(syst)ps. A combination of this result with a previous LHCb analysis using an independent dataset corresponding to 3 fb - 1 of integrated luminosity gives τL=1.452±0.014±0.007±0.002ps, where the first uncertainty is statistical, the second due to the uncorrelated part of the systematic uncertainty and the third due to the correlated part of the systematic uncertainty

    A study of CP violation in the decays B±→[K+K-π+π-]Dh± (h= K, π) and B±→[π+π-π+π-]Dh±

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    The first study of CP violation in the decay mode B±→[K+K-π+π-]Dh± , with h= K, π , is presented, exploiting a data sample of proton–proton collisions collected by the LHCb experiment that corresponds to an integrated luminosity of 9 \,fb - 1 . The analysis is performed in bins of phase space, which are optimised for sensitivity to local CP asymmetries. CP -violating observables that are sensitive to the angle Îł of the Unitarity Triangle are determined. The analysis requires external information on charm-decay parameters, which are currently taken from an amplitude analysis of LHCb data, but can be updated in the future when direct measurements become available. Measurements are also performed of phase-space integrated observables for B±→[K+K-π+π-]Dh± and B±→[π+π-π+π-]Dh± decays

    Observation of Cabibbo-suppressed two-body hadronic decays and precision mass measurement of the Ωc0\Omega_{c}^{0} baryon

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    The first observation of the singly Cabibbo-suppressed Ωc0→Ω−K+\Omega_{c}^{0}\to\Omega^{-}K^{+} and Ωc0→Ξ−π+\Omega_{c}^{0}\to\Xi^{-}\pi^{+} decays is reported, using proton-proton collision data at a centre-of-mass energy of 13 TeV13\,{\rm TeV}, corresponding to an integrated luminosity of 5.4 fb−15.4\,{\rm fb}^{-1}, collected with the LHCb detector between 2016 and 2018. The branching fraction ratios are measured to be B(Ωc0→Ω−K+)B(Ωc0→Ω−π+)=0.0608±0.0051(stat)±0.0040(syst)\frac{\mathcal{B}(\Omega_{c}^{0}\to\Omega^{-}K^{+})}{\mathcal{B}(\Omega_{c}^{0}\to\Omega^{-}\pi^{+})}=0.0608\pm0.0051({\rm stat})\pm 0.0040({\rm syst}), B(Ωc0→Ξ−π+)B(Ωc0→Ω−π+)=0.1581±0.0087(stat)±0.0043(syst)±0.0016(ext)\frac{\mathcal{B}(\Omega_{c}^{0}\to\Xi^{-}\pi^{+})}{\mathcal{B}(\Omega_{c}^{0}\to\Omega^{-}\pi^{+})}=0.1581\pm0.0087({\rm stat})\pm0.0043({\rm syst})\pm0.0016({\rm ext}). In addition, using the Ωc0→Ω−π+\Omega_{c}^{0}\to\Omega^{-}\pi^{+} decay channel, the Ωc0\Omega_{c}^{0} baryon mass is measured to be M(Ωc0)=2695.28±0.07(stat)±0.27(syst)±0.30(ext) MeV/c2M(\Omega_{c}^{0})=2695.28\pm0.07({\rm stat})\pm0.27({\rm syst})\pm0.30({\rm ext})\,{\rm MeV}/c^{2}, improving the precision of the previous world average by a factor of four.Comment: All figures and tables, along with any supplementary material and additional information, are available at https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2023-011.html (LHCb public pages
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