Abstract:This paper presents a combined experimental and computational study into the aerodynamics and performance of a small scale Vertical Axis Wind Turbine (VAWT). Wind tunnel tests were carried out to ascertain overall performance of the turbine and two and three dimensional unsteady computational fluid dynamics (CFD) models were generated to help understand the aerodynamics of this performance.Wind tunnel performance results are presented for cases of different wind velocity, tip-speed ratio and solidity as well as rotor blade surface finish. It is shown experimentally that the surface roughness on the turbine rotor blades has a significant effect on performance. Below a critical wind speed (Reynolds number of 30,000) the performance of the turbine is degraded by a smooth rotor surface finish but above it, the turbine performance is enhanced by a smooth surface finish. Both two bladed and three bladed rotors were tested and a significant increase in performance coefficient is observed for the higher solidity rotors (three bladed rotors) over most of the operating range. Dynamic stalling behaviour and the resulting large and rapid changes in force coefficients and the rotor torque are shown to be the likely cause of changes to rotor pitch angle that occurred during early testing. This small change in pitch angle caused significant decreases in performance.The performance coefficient predicted by the two dimensional computational model is significantly higher than that of the experimental and the three dimensional CFD model. The predictions show that the presence of the over tip vortices in the 3D simulations is responsible for producing the large difference in efficiency compared to the 2D predictions. The dynamic behaviour of the over tip vortex as a rotor blade rotates through each revolution is also explored in the paper.
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Using e + e − collision data corresponding to a total integrated luminosity of 12.9 fb −1 collected with the BESIII detector at the BEPCII collider, the exclusive Born cross sections and the effective form factors of the reaction e + e − → Ξ − Ξ+ are measured via the single baryon-tag method at 23 center-of-mass energies between 3.510 and 4.843 GeV. Evidence for the decay ψ(3770) → Ξ − Ξ+ is observed with a significance of 4.5σ by analyzing the measured cross sections together with earlier BESIII results. For the other charmonium(-like) states ψ(4040), ψ(4160), Y (4230), Y (4360), ψ(4415), and Y (4660), no significant signal of their decay to Ξ − Ξ+ is found. For these states, upper limits of the products of the branching fraction and the electronic partial width at the 90% confidence level are provided.
Two-dimensional and three-dimensional contour bumps are designed and optimized for substantial wave drag reduction for an un-swept natural laminar flow (NLF) wing (RAE5243 aerofoil section) at transonic speeds. An NLF aerofoil wing is chosen in this study, as shock control is more crucial for such wings due to the requirement of favourable pressure gradients on a substantial part of the wing. For the validation purpose and to focus on the wave drag issues, the boundary layer is assumed to be fully turbulent from the leading edge. Key bump geometrical parameters including the maximum height, the length, and the crest position have been chosen for the parameterization of the two-dimensional and three-dimensional shock control bumps. For the three-dimensional bumps, an array of the contour bumps is installed spanwise on the transonic wing and their width and spanwise spacing are chosen as additional design parameters. Both the two-dimensional and the three-dimensional bump shapes are optimized using a discrete adjoint-based optimization method. The performance of the three-dimensional contour bumps are compared in detail with the similarly optimized two-dimensional bumps both at and around the design point. The results show that, for the NLF wing studied, the optimized three-dimensional bumps are as effective as the optimized two-dimensional bump in terms of total drag reduction at the given design point, despite the significant difference in their geometrical shapes. More importantly, in terms of the operational range for varying lift conditions for practical applications, the three-dimensional bumps outperform the two-dimensional bump by a substantial margin.
We report the observation of the X(3823) in the process e + e − → π + π − X(3823) → π + π − γχc1 with a statistical significance of 6.2σ, in data samples at center-of-mass energies √ s =4. 230, 4.260, 4.360, 4.420 and 4.600 GeV collected with the BESIII detector at the BEPCII electron positron collider. The measured mass of the X(3823) is (3821.7 ± 1.3 ± 0.7) MeV/c 2 , where the first error is statistical and the second systematic, and the width is less than 16 MeV at the 90% confidence level. The products of the Born cross sections for e + e − → π + π − X(3823) and the branching ratio B[X(3823) → γχc1,c2] are also measured. These measurements are in good agreement with the assignment of the X(3823) as the ψ(1 3 D2) charmonium state.PACS numbers: 13.20. Gd, 13.25.Gv, 14.40.Pq Since its discovery, charmonium -meson particles which contain a charm and an anti-charm quark -has been an excellent tool for probing Quantum Chromodynamics (QCD), the fundamental theory that describes the strong interactions between quarks and gluons, in the non-perturbative (low-energy, long-distance effects) regime, and remains of high interest both experimentally and theoretically. All of the charmonium states with masses that are below the open-charm threshold have been firmly established [1,2]; open-charm refers to mesons containing a charm quark (antiquark) and either an up or down antiquark (quark), such as D orD. However, the observation of the spectrum that are above the opencharm threshold remains unsettled. During the past decade, many new charmoniumlike states were discovered, such as the X(3872) [3], the Y (4260) [4,5] and the Z c (3900) [5][6][7]. These states provide strong evidence for the existence of exotic hadron states [8]. Although charged charmoniumlike states like the Z c (3900) provide convincing evidence for the existence of multi-quark states [9], it is more difficult to distinguish neutral candidate exotic states from conventional charmonium. Moreover, the study of transitions between charmonium(like) states, such as the Y (4260) → γX(3872) [10], is an important approach to probe their nature, and the connections between them. Thus, a more complete understanding of the charmonium(like) spectroscopy and their relations is necessary and timely. In this Letter, we report a search for the production of the ψ 2 state via the process e + e − → π + π − X, using 4.67 fb −1 data collected with the BESIII detector operating at the BEPCII storage ring [14] at center-of-mass (CM) energies that range from √ s = 4.19 to 4.60 GeV [15]. The ψ 2 candidates are reconstructed in their γχ c1 and γχ c2 decay modes, with χ c1,c2 → γJ/ψ and J/ψ → ℓ + ℓ − (ℓ = e or µ). A GEANT4-based [16] Monte Carlo (MC) simulation software package is used to optimize event selection criteria, determine the detection efficiency, and estimate the backgrounds. For the signal process, we generate 40,000 e + e − → π + π − X(3823) events at each CM energy indicated above, using an phase space model, with X(3823) → γχ c1,c2
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