737 research outputs found

    Анализ эффСктивности процСссов планирования элСктроснабТСния Π² Π₯Π°Ρ€ΡŒΠΊΠΎΠ²ΡΠΊΠΎΠΌ Ρ€Π΅Π³ΠΈΠΎΠ½Π΅

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    Π•Ρ„Π΅ΠΊΡ‚ΠΈΠ²Π½Ρ–ΡΡ‚ΡŒ процСсів СлСктропостачання Π·Π°ΠΏΡ€ΠΎΠΏΠΎΠ½ΠΎΠ²Π°Π½ΠΎ ΠΎΡ†Ρ–Π½ΡŽΠ²Π°Ρ‚ΠΈ Π½Π΅ Ρ‚Ρ–Π»ΡŒΠΊΠΈ Π²Π΅Π»ΠΈΡ‡ΠΈΠ½ΠΎΡŽ ΠΏΠΎΠΌΠΈΠ»ΠΊΠΈ прогнозування, Π° ΠΉ ΠΊΡ–Π»ΡŒΠΊΡ–ΡΡ‚ΡŽ Π½Π΅Π³Π°Ρ‚ΠΈΠ²Π½ΠΈΡ… Ρ– ΠΏΠΎΠ·ΠΈΡ‚ΠΈΠ²Π½ΠΈΡ… ΠΏΠΎΠΌΠΈΠ»ΠΎΠΊ, Ρ‰ΠΎ Π²ΠΈΠΌΡ–Ρ€ΡŽΡŽΡ‚ΡŒΡΡ Π·Π° ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠΎΡŽ Π’Π΅ΠΉΠ»Π°. Π’ΠΈΠΊΠΎΠ½Π°Π½ΠΎ Π°Π½Π°Π»Ρ–Π· ΠΏΠ»Π°Π½ΠΎΠ²Π°Π½ΠΈΡ… Ρ– Ρ„Π°ΠΊΡ‚ΠΈΡ‡Π½ΠΈΡ… Π΄ΠΎΠ±ΠΎΠ²ΠΈΡ… обсягів СлСктроспоТивання Π² Π₯Π°Ρ€ΠΊΡ–Π²ΡΡŒΠΊΠΎΠΌΡƒ Ρ€Π΅Π³Ρ–ΠΎΠ½Ρ– Π² 2008 Ρ– 2009 Ρ€ΠΎΠΊΠ°Ρ…. ΠžΡ†Ρ–Π½Π΅Π½ΠΎ ΠΏΠΎΠΌΠΈΠ»ΠΊΠΈ ΠΏΠ΅Ρ€Π΅ΠΎΡ†Ρ–Π½ΠΊΠΈ Ρ– Π½Π΅Π΄ΠΎΠΎΡ†Ρ–Π½ΠΊΠΈ Ρ„Π°ΠΊΡ‚ΠΈΡ‡Π½ΠΈΡ… обсягів, обчислСні складові Π·Π°Π³Π°Π»ΡŒΠ½ΠΎΡ— ΠΏΠΎΠΌΠΈΠ»ΠΊΠΈ Ρ– ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, Ρ‰ΠΎ ΠΏΠ΅Ρ€Π΅Π²Π°ΠΆΠ°Ρ” ΠΏΠΎΠΌΠΈΠ»ΠΊΠ° Π½Π΅ΠΏΠΎΠ²Π½ΠΎΡ— ΠΊΠΎΠ²Π°Ρ€Ρ–Π°Ρ†Ρ–Ρ— ΠΏΡ€ΠΎΠ³Π½ΠΎΠ·ΠΎΠ²Π°Π½ΠΈΡ… Ρ– Ρ„Π°ΠΊΡ‚ΠΈΡ‡Π½ΠΈΡ… Π·Π½Π°Ρ‡Π΅Π½ΡŒ Π΄ΠΎΠ±ΠΎΠ²ΠΈΡ… обсягів Ρ€ΠΈΠ½ΠΊΡƒ споТивачів АК "Π₯Π°Ρ€ΠΊΡ–Π²ΠΎΠ±Π»Π΅Π½Π΅Ρ€Π³ΠΎ".The effectiveness of the processes of electricity supply was offered to assess not only with the magnitude of forecasting error, but with the number of negative and positive errors, measured by the method of Theil. The analysis of planned and actual daily volume of electricity in Kharkov region in 2008 and 2009 is realized. Errors of revaluation and underestimation of actual volumes are estimated, components of the general error are calculated and shown that the error of incomplete covariance for predicted and actual values of daily volumes of the market of consumers АК of "Kharkovo-blenergo" prevails

    Superconductor-to-Spin-Density-Wave Transition in Quasi-One-Dimensional Metals with Ising Anisotropy

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    We study a mechanism for superconductivity in quasi-one-dimensional materials with Ising anisotropy. In an isolated chain Ising anisotropy opens a spin gap; if inter-chain coupling is sufficiently weak, single particle hopping is suppressed and the physics of coupled chains is controlled by a competition between pair hopping and exchange interaction. Spin density wave and triplet superconductivity phases are found separated by a first order phase transition. For particular parameter values a second order transition described by SO(4) symmetry is found.Comment: 18 pages, 1 figur

    Epistatic Interactions in {NS5A} of Hepatitis {C} Virus Suggest Drug Resistance Mechanisms

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    Hepatitis C virus (HCV) causes a major health burden and can be effectively treated by direct-acting antivirals (DAAs). The non-structural protein 5A (NS5A), which plays a role in the viral genome replication, is one of the DAAs’ targets. Resistance-associated viruses (RAVs) harbouring NS5A resistance-associated mutations (RAMs) have been described at baseline and after therapy failure. A mutation from glutamine to arginine at position 30 (Q30R) is a characteristic RAM for the HCV sub/genotype (GT) 1a, but arginine corresponds to the wild type in the GT-1b; still, GT-1b strains are susceptible to NS5A-inhibitors. In this study, we show that GT-1b strains with R30Q often display other specific NS5A substitutions, particularly in positions 24 and 34. We demonstrate that in GT-1b secondary substitutions usually happen after initial R30Q development in the phylogeny, and that the chemical properties of the corresponding amino acids serve to restore the positive charge in this region, acting as compensatory mutations. These findings may have implications for RAVs treatment

    Intersecting Loop Models on Z^D: Rigorous Results

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    We consider a general class of (intersecting) loop models in D dimensions, including those related to high-temperature expansions of well-known spin models. We find that the loop models exhibit some interesting features - often in the ``unphysical'' region of parameter space where all connection with the original spin Hamiltonian is apparently lost. For a particular n=2, D=2 model, we establish the existence of a phase transition, possibly associated with divergent loops. However, for n >> 1 and arbitrary D there is no phase transition marked by the appearance of large loops. Furthermore, at least for D=2 (and n large) we find a phase transition characterised by broken translational symmetry.Comment: LaTeX+elsart.cls; 30 p., 6 figs; submitted to Nucl. Phys. B; a few minor typos correcte

    Two phase transitions in the fully frustrated XYXY model

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    The fully frustrated XYXY model on a square lattice is studied by means of Monte Carlo simulations. A Kosterlitz-Thouless transition is found at TKTβ‰ˆ0.446T_{\rm KT} \approx 0.446, followed by an ordinary Ising transition at a slightly higher temperature, Tcβ‰ˆ0.452T_c \approx 0.452. The non-Ising exponents reported by others, are explained as a failure of finite size scaling due to the screening length associated with the nearby Kosterlitz-Thouless transition.Comment: REVTEX file, 8 pages, 5 figures in uuencoded postscrip

    Evidence for Complex Subleading Exponents from the High-Temperature Expansion of the Hierarchical Ising Model

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    Using a renormalization group method, we calculate 800 high-temperature coefficients of the magnetic susceptibility of the hierarchical Ising model. The conventional quantities obtained from differences of ratios of coefficients show unexpected smooth oscillations with a period growing logarithmically and can be fitted assuming corrections to the scaling laws with complex exponents.Comment: 10 pages, Latex , uses revtex. 2 figures not included (hard copies available on request

    Space Station Freedom ground data system: Design and operations

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    Over the previous year the Space Station Freedom (SSF) Program (SSFP) ground data distribution system has become independent of a number of data systems that were to have been provided by other National Aeronautics and Space Administration (NASA) programs. Consequently, the SSFP has outlined the basic architecture of a new data system dedicated to supporting SSF requirements. This has been accomplished through a complete redesign of the ground network and a reallocation of selected functions. There are a number of aspects of the new ground data distribution system that are unique among NASA programs. These considerations make SSF ground data distribution one of the most extensive and complex data management challenges encountered in the arena of Space Operations. A description of this system comprises the main focus of the paper

    Roughening Induced Deconstruction in (100) Facets of CsCl Type Crystals

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    The staggered 6-vertex model describes the competition between surface roughening and reconstruction in (100) facets of CsCl type crystals. Its phase diagram does not have the expected generic structure, due to the presence of a fully-packed loop-gas line. We prove that the reconstruction and roughening transitions cannot cross nor merge with this loop-gas line if these degrees of freedom interact weakly. However, our numerical finite size scaling analysis shows that the two critical lines merge along the loop-gas line, with strong coupling scaling properties. The central charge is much larger than 1.5 and roughening takes place at a surface roughness much larger than the conventional universal value. It seems that additional fluctuations become critical simultaneously.Comment: 31 pages, 9 figure

    Measurements of the Exerted Pressure by Pelvic Circumferential Compression Devices

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    Data on the efficacy and safety of non-invasive Pelvic Circumferential Compression Devices (PCCDs) is limited. Tissue damage may occur if a continuous pressure on the skin exceeding 9.3 kPa is sustained for more than two or three hours. The aim of this study was to gain insight into the pressure build-up at the interface, by measuring the PCCD-induced pressure when applying pulling forces to three different PCCDs (Pelvic Binder((R)) , SAM-Sling ((R)) and T-POD((R)) ) in a simplified model. The resulting exerted pressures were measured at four 'anatomical' locations (right, left, posterior and anterior) in a model using a pressure measurement system consisting of pressure cuffs. The exerted pressure varied substantially between the locations as well as between the PCCDs. Maximum pressures ranged from 18.9-23.3 kPa and from 19.2-27.5 kPa at the right location and left location, respectively. Pressures at the posterior location stayed below 18 kPa. At the anterior location pressures varied markedly between the different PCCDs. The circumferential compression by the different PCCDs showed high pressures measured at the four locations using a simplified model. Difference in design and functional characteristics of the PCCDs resulted in different pressure build-up at the four locations. When following the manufacturer's instructions, the exerted pressure of all three PCCDs tested exceeded the tissue damaging level (9.3 kPa). In case of prolonged use in a clinical situation this might put patients at risk for developing tissue damage

    Berry phase and adiabaticity of a spin diffusing in a non-uniform magnetic field

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    An electron spin moving adiabatically in a strong, spatially non-uniform magnetic field accumulates a geometric phase or Berry phase, which might be observable as a conductance oscillation in a mesoscopic ring. Two contradicting theories exist for how strong the magnetic field should be to ensure adiabaticity if the motion is diffusive. To resolve this controversy, we study the effect of a non-uniform magnetic field on the spin polarization and on the weak-localization effect. The diffusion equation for the Cooperon is solved exactly. Adiabaticity requires that the spin-precession time is short compared to the elastic scattering time - it is not sufficient that it is short compared to the diffusion time around the ring. This strong condition severely complicates the experimental observation.Comment: 16 pages REVTEX, including 3 figure
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