444,998 research outputs found

    The inner radio jet region and the complex environment of SS433

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    We present multi-frequency VLBA+VLA observations of SS433 at 1.6, 5 and 15 GHz. These observations provide the highest angular resolution radio spectral index maps ever made for this object. Motion of the components of SS433 during the observation is detected. In addition to the usual VLBI jet structure, we detect two radio components in the system at an anomalous position angle. These newly discovered radio emitting regions might be related to a wind-like equatorial outflow or to an extension of the accretion disk. We show that the radio core component is bifurcated with a clear gap between the eastern and western wings of emission. Modelfitting of the precessing jets and the moving knots of SS433 shows that the kinematic centre -- i.e. the binary -- is in the gap between the western and eastern radio core components. Spectral properties and observed core position shifts suggest that we see a combined effect of synchrotron self-absorption and external free-free absorption in the innermost AU-scale region of the source. The spatial distribution of the ionized matter is probably not spherically symmetric around the binary, but could be disk-like.Comment: Accepted for publication by Astronomy and Astrophysic

    Interesting dynamics at high mutual inclination in the framework of the Kozai problem with an eccentric perturber

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    We study the dynamics of the 3-D three-body problem of a small body moving under the attractions of a star and a giant planet which orbits the star on a much wider and elliptic orbit. In particular, we focus on the influence of an eccentric orbit of the outer perturber on the dynamics of a small highly inclined inner body. Our analytical study of the secular perturbations relies on the classical octupole hamiltonian expansion (third-order theory in the ratio of the semi-major axes), as third-order terms are needed to consider the secular variations of the outer perturber and potential secular resonances between the arguments of the pericenter and/or longitudes of the node of both bodies. Short-period averaging and node reduction (Laplace plane) reduce the problem to two degrees of freedom. The four-dimensional dynamics is analyzed through representative planes which identify the main equilibria of the problem. As in the circular problem (i.e. perturber on a circular orbit), the "Kozai-bifurcated" equilibria play a major role in the dynamics of an inner body on quasi-circular orbit: its eccentricity variations are very limited for mutual inclination between the orbital planes smaller than ~40^{\deg}, while they become large and chaotic for higher mutual inclination. Particular attention is also given to a region around 35^{\deg} of mutual inclination, detected numerically by Funk et al. (2011) and consisting of long-time stable and particularly low eccentric orbits of the small body. Using a 12th-order Hamiltonian expansion in eccentricities and inclinations, in particular its action-angle formulation obtained by Lie transforms in Libert & Henrard (2008), we show that this region presents an equality of two fundamental frequencies and can be regarded as a secular resonance. Our results also apply to binary star systems where a planet is revolving around one of the two stars.Comment: 12 pages, 9 figures, accepted for publication in MNRA

    A General Relativistic Magnetohydrodynamics Simulation of Jet Formation

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    We have performed a fully three-dimensional general relativistic magnetohydrodynamic (GRMHD) simulation of jet formation from a thin accretion disk around a Schwarzschild black hole with a free-falling corona. The initial simulation results show that a bipolar jet (velocity โˆผ0.3c\sim 0.3c) is created as shown by previous two-dimensional axisymmetric simulations with mirror symmetry at the equator. The 3-D simulation ran over one hundred light-crossing time units (ฯ„S=rS/c\tau_{\rm S} = r_{\rm S}/c where rSโ‰ก2GM/c2r_{\rm S} \equiv 2GM/c^2) which is considerably longer than the previous simulations. We show that the jet is initially formed as predicted due in part to magnetic pressure from the twisting the initially uniform magnetic field and from gas pressure associated with shock formation in the region around r=3rSr = 3 r_{\rm S}. At later times, the accretion disk becomes thick and the jet fades resulting in a wind that is ejected from the surface of the thickened (torus-like) disk. It should be noted that no streaming matter from a donor is included at the outer boundary in the simulation (an isolated black hole not binary black hole). The wind flows outwards with a wider angle than the initial jet. The widening of the jet is consistent with the outward moving torsional Alfv\'{e}n waves (TAWs). This evolution of disk-jet coupling suggests that the jet fades with a thickened accretion disk due to the lack of streaming material from an accompanying star.Comment: 27 pages, 8 figures, revised and accepted to ApJ (figures with better resolution: http://gammaray.nsstc.nasa.gov/~nishikawa/schb1.pdf

    Computational Study of Hypersonic Flow Past Spiked Blunt Body Using RANS and DSMC Method

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    AbstractHypersonic vehicles when moving at very high speeds experience the problem of drag and heating. One of the ways to reduce this drag and heating is by the use of an aerospike. In the present study, the flow around a blunted body fitted with an aerospike is analyzed using a commercial software ANSYS Fluent and an open source Direct Simulation Monte Carlo (DSMC) code, called as dsmcFoam in OpenFOAM, at a high Mach number (M=6) at different length to diameter ratios (L/D = 1.5, 2) at an angle of attack 0o. The aerospike placed in front of the body replaces the strong detached shock wave ahead of the body with a system of weaker oblique shock waves. A recirculation region is developed between the shock and the blunt body, which acts like a streamlined profile, thus reducing the drag and wall heat flux

    ์ˆ˜์ง์ถ• ํ’๋ ฅ๋ฐœ์ „๊ธฐ ์ฃผ์œ„ ์œ ๋™์— ๊ด€ํ•œ ์ˆ˜์น˜ ํ•ด์„ ์—ฐ๊ตฌ ๋ฐ ์ž๋™ ๋””ํ”Œ๋ ‰ํ„ฐ๋ฅผ ์ด์šฉํ•œ ์œ ๋™ ์ œ์–ด

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    ํ•™์œ„๋…ผ๋ฌธ (์„์‚ฌ)-- ์„œ์šธ๋Œ€ํ•™๊ต ๋Œ€ํ•™์› : ๊ณต๊ณผ๋Œ€ํ•™ ๊ธฐ๊ณ„ํ•ญ๊ณต๊ณตํ•™๋ถ€(๋ฉ€ํ‹ฐ์Šค์ผ€์ผ ๊ธฐ๊ณ„์„ค๊ณ„์ „๊ณต), 2019. 2. ์ตœํ•ด์ฒœ.We perform large eddy simulation with an immersed boundary method to analyze the flow around a vertical axis wind turbine (VAWT). We verify the performance of a three-blade VAWT with the tip speed ratio at the Reynolds number of 80,000 based on the rotor diameter and free-stream velocity. The blades of the VAWT undergo rotational motion due to the free-stream velocity, and dynamic stall occurs as the blades angle of attack exceeds the static stall angle. Flow separation and vortex shedding occur during dynamic stall and the blades pass through the wake from the preceding blades. In the upwind region, the power of a blade increases with increasing angle of attack, but decreases as flow separates at the leading edge of the blade and a large leading edge vortex is formed. On the other hand, the power of a blade changes mildly in the downwind region. We apply an automatic moving deflector (AMD), inspired by secondary feather of a birds wing, to the inner surfaces of blades where flow separation occurs during dynamic stall. When flow separation occurs, the AMD pops up automatically suppressing the leading edge vortex formation. Then, the pressure distribution on the blades surface changes and drag is reduced. Consequently, the performance of the VAWT is enhanced at the tip speed ratios lower than 1.2.๋ณธ ์—ฐ๊ตฌ์—์„œ๋Š” ์ˆ˜์ง์ถ• ํ’๋ ฅ๋ฐœ์ „๊ธฐ ํšŒ์ „์ต ์ฃผ๋ณ€์˜ ์œ ๋™ ๋ฐ ๊ณต๋ ฅ์„ฑ๋Šฅ์„ ๋ถ„์„ํ•˜๊ธฐ ์œ„ํ•ด ์ฃผ ์œ ๋™ ์†๋„์™€ ํšŒ์ „ ์ง๊ฒฝ์„ ๊ธฐ์ค€์œผ๋กœ ํ•œ ๋ ˆ์ด๋†€์ฆˆ ์ˆ˜ 80,000์—์„œ ํฐ ์—๋”” ๋ชจ์‚ฌ ์‹œ๋ฎฌ๋ ˆ์ด์…˜์„ ์ˆ˜ํ–‰ํ•˜์˜€๋‹ค. Tip speed ratio์— ๋”ฐ๋ฅธ ์ˆ˜์ง์ถ• ํ’๋ ฅ๋ฐœ์ „๊ธฐ์˜ ํšจ์œจ ๋ณ€ํ™”๋ฅผ ๊ฒ€์ฆํ•˜๊ณ , ์ตœ์  tip speed ratio์—์„œ ํšŒ์ „์ต ์œ„์น˜์— ๋”ฐ๋ฅธ ๊ณต๋ ฅ์„ฑ๋Šฅ ํŠน์„ฑ์„ ๋ถ„์„ํ•˜์˜€๋‹ค. ์ƒ๋ฅ˜์ง€์—ญ์—์„œ ํšŒ์ „์ต์˜ ๋ฐ›์Œ๊ฐ์ด ์ฆ๊ฐ€ํ•จ์— ๋”ฐ๋ผ ํšŒ์ „์ต์˜ ์–‘๋ ฅ์ด ํ•ญ๋ ฅ๋ณด๋‹ค ํฌ๊ฒŒ ์ƒ์Šนํ•˜๋‹ค๊ฐ€, ์ฃผ๋ณ€์—์„œ ์œ ๋™๋ฐ•๋ฆฌ์™€ ์™€๋ฅ˜๋ฐœ์ƒ์ด ์ผ์–ด๋‚˜๊ณ  ๋™์  ์‹ค์†์ด ๋ฐœ์ƒํ•˜์—ฌ ์–‘๋ ฅ์ด ํฌ๊ฒŒ ๊ฐ์†Œํ•˜๊ฒŒ ๋œ๋‹ค. ๋ฐ˜๋ฉด, ํ•˜๋ฅ˜์ง€์—ญ์—์„œ๋Š” ์œ ๋™ ๋ณ€ํ™”์—๋„ ๋ถˆ๊ตฌํ•˜๊ณ  ํšŒ์ „์ต์˜ ๊ณต๋ ฅ์„ฑ๋Šฅ์˜ ๋ณ€ํ™”๊ฐ€ ๊ฑฐ์˜ ์ผ์–ด๋‚˜์ง€ ์•Š๋Š”๋‹ค. ์ƒ๋ฅ˜์ง€์—ญ์—์„œ ๋™์  ์‹ค์†์ด ์ผ์–ด๋‚  ๋•Œ ํšŒ์ „์ต์˜ ๊ณต๋ ฅ์„ฑ๋Šฅ์„ ํ–ฅ์ƒ์‹œํ‚ค๊ธฐ ์œ„ํ•ด automatic moving deflector (AMD)๋ฅผ ์ ์šฉํ•˜์˜€๋‹ค. ๋™์  ์‹ค์† ๊ณผ์ •์—์„œ AMD๋Š” ์œ ๋™์— ์˜ํ•ด ์ž๋™์œผ๋กœ ์—ด๋ฆฌ๊ฒŒ ๋‹ซํžˆ๊ฒŒ ๋˜๊ณ , AMD๊ฐ€ ์—ด๋ฆด ๋•Œ ์œ ๋™๋ฐ•๋ฆฌ์™€ ์™€๋ฅ˜ ๋ฐœ์ƒ์ด ์–ต์ œ๋จ์— ๋”ฐ๋ผ ํ•ญ๋ ฅ์ด ๊ฐ์†Œํ•˜๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€๋‹ค. ๊ฒฐ๊ณผ์ ์œผ๋กœ ์ˆ˜์ง์ถ• ํ’๋ ฅ๋ฐœ์ „๊ธฐ์˜ ํšจ์œจ์€ tip speed ratio๊ฐ€ 0.8๊ณผ 1์ผ ๋•Œ ํ–ฅ์ƒ๋˜๋Š” ๊ฒƒ์„ ํ™•์ธํ•˜์˜€๋‹ค.Abstract i Contents iii List of Figures iv List of Tables vi Nomenclature vii Chapter 1. Introduction 1 Chapter 2. Numerical details 4 2.1. Aerodynamics and geometry of VAWT 4 2.2. Governing equations 5 2.3. Computational domain and boundary conditions 6 2.4. Geometry of automatic moving deflector 7 Chapter 3. Numerical Results 11 3.1. Performance of the VAWT 11 3.2. Overall flow structure 11 3.3. Unsteady aerodynamics of blade 12 3.3.1 Variation of power 12 3.3.2 Flow characteristics around the blade 13 3.3.3 Aerodynamic forces 14 Chapter 4. Flow Control 31 4.1. Introduction about an automatic moving deflector 31 4.2. Control results 32 Summary and conclusion 41 Reference 42 Abstract in Korean 46Maste

    Compact formulae, dynamics and radiation of charged particles under synchro-curvature losses

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    We consider the fundamental problem of charged particles moving along and around a curved magnetic field line, revising the synchro-curvature radiation formulae introduced by Cheng and Zhang (1996). We provide more compact expressions to evaluate the spectrum emitted by a single particle, identifying the key parameter that controls the transition between the curvature-dominated and the synchrotron-dominated regime. This parameter depends on the local radius of curvature of the magnetic field line, the gyration radius, and the pitch angle. We numerically solve the equations of motion for the emitting particle by considering self-consistently the radiative losses, and provide the radiated spectrum produced by a particle when an electric acceleration is balanced by its radiative losses, as it is assumed to happen in the outer gaps of pulsar's magnetospheres. We compute the average spectrum radiated throughout the particle trajectory finding that the slope of the spectrum before the peak depends on the location and size of the emission region. We show how this effect could then lead to a variety of synchro-curvature spectra. Our results reinforce the idea that the purely synchrotron or curvature losses are, in general, inadequate to describe the radiative reaction on the particle motion, and the spectrum of emitted photons. Finally, we discuss the applicability of these calculations to different astrophysical scenarios.Comment: 9 pages, 5 figures, 2 tables. Accepted for publication in MNRAS main journal. References update

    Numerical investigation on the aerodynamic characteristics of high-speed train under turbulent crosswind

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    Increasing velocity combined with decreasing mass of modern high-speed trains poses a question about the influence of strong crosswinds on its aerodynamics. Strong crosswinds may affect the running stability of high-speed trains via the amplified aerodynamic forces and moments. In this study, a simulation of turbulent crosswind flows over the leading and end cars of ICE-2 high-speed train was performed at different yaw angles in static and moving ground case scenarios. Since the train aerodynamic problems are closely associated with the flows occurring around train, the flow around the train was considered as incompressible and was obtained by solving the incompressible form of the unsteady Reynolds-averaged Navierโ€“Stokes (RANS) equations combined with the realizable k-epsilon turbulence model. Important aerodynamic coefficients such as the side force and rolling moment coefficients were calculated for yaw angles ranging from โˆ’30ยฐ to 60ยฐ and compared with the results obtained from wind tunnel test. The dependence of the flow structure on yaw angle was also presented. The nature of the flow field and its structure depicted by contours of velocity magnitude and streamline patterns along the trainโ€™s cross-section were presented for different yaw angles. In addition, the pressure coefficient around the circumference of the train at different locations along its length was computed for yaw angles of 30ยฐ and 60ยฐ. The computed aerodynamic coefficient outcomes using the realizable k-epsilon turbulence model were in good agreement with the wind tunnel data. Both the side force coefficient and rolling moment coefficients increase steadily with yaw angle till about 50ยฐ before starting to exhibit an asymptotic behavior. Contours of velocity magnitude were also computed at different cross-sections of the train along its length for different yaw angles. The result showed that magnitude of rotating vortex in the lee ward side increased with increasing yaw angle, which leads to the creation of a low-pressure region in the lee ward side of the train causing high side force and roll moment. Generally, this study shows that unsteady CFD-RANS methods combined with an appropriate turbulence model can present an important means of assessing the crucial aerodynamic forces and moments of a high-speed train under strong crosswind conditions

    Broadband microwave burst produced by electron beams

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    Theoretical and experimental study of fast electron beams attracts a lot of attention in the astrophysics and laboratory. In the case of solar flares the problem of reliable beam detection and diagnostics is of exceptional importance. This paper explores the fact that the electron beams moving oblique to the magnetic field or along the field with some angular scatter around the beam propagation direction can generate microwave continuum bursts via gyrosynchrotron mechanism. The characteristics of the microwave bursts produced by beams differ from those in case of isotropic or loss-cone distributions, which suggests a new tool for quantitative diagnostics of the beams in the solar corona. To demonstrate the potentiality of this tool, we analyze here a radio burst occurred during an impulsive flare 1B/M6.7 on 10 March 2001 (AR 9368, N27W42). Based on detailed analysis of the spectral, temporal, and spatial relationships, we obtained firm evidence that the microwave continuum burst is produced by electron beams. For the first time we developed and applied a new forward fitting algorithm based on exact gyrosynchrotron formulae and employing both the total power and polarization measurements to solve the inverse problem of the beam diagnostics. We found that the burst is generated by a oblique beam in a region of reasonably strong magnetic field (โˆผ200โˆ’300\sim 200-300 G) and the burst is observed at a quasi-transverse viewing angle. We found that the life time of the emitting electrons in the radio source is relatively short, ฯ„lโ‰ˆ0.5\tau_l \approx 0.5 s, consistent with a single reflection of the electrons from a magnetic mirror at the foot point with the stronger magnetic field. We discuss the implications of these findings for the electron acceleration in flares and for beam diagnostics.Comment: Astrophysical Journal, accepted: 26 pages, 8 figure

    Numerical investigation on the aerodynamic characteristics of high-speed train under turbulent crosswind

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    Increasing velocity combined with decreasing mass of modern high-speed trains poses a question about the influence of strong crosswinds on its aerodynamics. Strong crosswinds may affect the running stability of high-speed trains via the amplified aerodynamic forces and moments. In this study, a simulation of turbulent crosswind flows over the leading and end cars of ICE-2 high-speed train was performed at different yaw angles in static and moving ground case scenarios. Since the train aerodynamic problems are closely associated with the flows occurring around train, the flow around the train was considered as incompressible and was obtained by solving the incompressible form of the unsteady Reynolds-averaged Navierโ€“Stokes (RANS) equations combined with the realizable k-epsilon turbulence model. Important aerodynamic coefficients such as the side force and rolling moment coefficients were calculated for yaw angles ranging from โˆ’30ยฐ to 60ยฐ and compared with the results obtained from wind tunnel test. The dependence of the flow structure on yaw angle was also presented. The nature of the flow field and its structure depicted by contours of velocity magnitude and streamline patterns along the trainโ€™s cross-section were presented for different yaw angles. In addition, the pressure coefficient around the circumference of the train at different locations along its length was computed for yaw angles of 30ยฐ and 60ยฐ. The computed aerodynamic coefficient outcomes using the realizable k-epsilon turbulence model were in good agreement with the wind tunnel data. Both the side force coefficient and rolling moment coefficients increase steadily with yaw angle till about 50ยฐ before starting to exhibit an asymptotic behavior. Contours of velocity magnitude were also computed at different cross-sections of the train along its length for different yaw angles. The result showed that magnitude of rotating vortex in the lee ward side increased with increasing yaw angle, which leads to the creation of a low-pressure region in the lee ward side of the train causing high side force and roll moment. Generally, this study shows that unsteady CFD-RANS methods combined with an appropriate turbulence model can present an important means of assessing the crucial aerodynamic forces and moments of a high-speed train under strong crosswind conditions
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