期刊文献+

MEXICO风轮的气动性能预测 被引量:3

Prediction of aerodynamic performance for MEXICO rotor
下载PDF
导出
摘要 动量叶素法(blade element momentum,BEM)和计算流体力学方法(computational fluid dynamics,CFD)是预测风力机气动性能的常用方法,本文基于商用MATLAB和CFX软件,对MEXICO(Model Experiments In Controlled Conditions)风轮5种风速的轴向入流工况分别采用BEM和CFD方法进行气动性能预测,其中BEM方法计算时采用Shen叶尖修正,CFD方法选用SST紊流模型求解三维雷诺时均方程。研究表明,BEM和CFD方法计算的攻角最大相对误差分别为-0.402、0.099,试验获得的来流攻角沿叶片径向分布基本处于2种方法获得的结果之间,且在叶尖处更接近CFD计算的结果;试验获得的叶片轴向力沿叶片径向分布与2种方法的预测结果基本吻合,BEM和CFD 2种方法计算的轴向力最大相对误差分别为-0.139、-0.096,当叶片进入失速状态后,BEM方法计算的切向力最大相对误差达到-0.471,表明BEM方法的预测精度有待进一步提高,研究成果可为工程模型的修正与开发提供参考。 The aerodynamic performance of the MEXICO (Model EXperiments In Controlled cOnditions) rotor at five tunnel wind speeds is predicted by making use of BEM and CFD methods, respectively, using commercial MATLAB and CFD software. Due to the pressure differences on both sides of the blade, the tip-flow will produce secondary flow along the blade, consecutively resulting in decreases of torque. To overcome the above-mentioned issue, a variety of tip-correction models are developed, while most models overestimate the axial and tangential forces. To optimize accuracy, a new correction model summarized from CFD results by Shen is adopted in this paper. In order to accurately simulate the separation point and the separation area which is caused by the adverse pressure gradient, the CFD method using SST turbulence model is used to solve the three-dimensional Reynolds averaged equations. The first order upwind is used for the advection schemes, and the discrete equations are solved with simple algorithms. In addition, uniform velocity and static temperature are given as inlet boundary conditions, and static pressure is given as the circumferential outer boundary condition and the outlet boundary condition. The boundaries of fan-shaped both sides are defined as rotationally periodic connection, and the freeze rotor model is applied at the interface of the rotating and stationary domains, which means the relative position of rotating and stationary domains is fixed when calculating the flow field. Speed no-slip conditions are applied to solid walls such as blades. In this paper, two different meshing methods are used to generate a hexahedral grid for the rotating domain and a tetrahedral grid for stationary domain, between which comparison of the deviation of axial force on 60% blade cross section under the design condition (Vtun=15 m/s) leads to a clear decision of the better mesh method with less deviation. Taking the better mesh method into consideration, the final number of rotating domain grids is calculated according to verification of grid independence, with an amount of 2,961,385. The conclusion of this paper will be illustrated from the following points: first, the comparison of the calculated and the experimental angle of attack distribution along the span direction shows that the maximum relative errors of the attack angle calculated by BEM and CFD respectively are -0.402 and 0.099; it further illustrates that the experimental results are substantially between the results obtained by the two methods, and closer to the result of CFD at the blade tip. Meanwhile, the axial force on the blade increases with increasing radius, while the tangential force shows small change. All of the axial and tangential force in each section increases with increasing wind speed. Additionally, the maximum relative: errors of axial force calculated by BEM and CFD respectively are -0.139 and -0.096. In a word, the experimental data are in good agreement with the results calculated by BEM and CFD, confirming the reliability of the MEXICO data. Second, the SST turbulence model can better capture the flow separation on the blade and has high aerodynamic performance prediction accuracy for a horizontal axis wind turbine in axial inflow conditions. Finally, the comparisons of the axial and tangential forces as well as the contrast of the angle of attack indicate that the prediction accuracy of BEM method is high when the blade is not in the stall condition. However, the airfoil characteristic becomes unstable in the stall condition, and the maximum relative error of tangential force calculated by BEM is -0.471. As a result, prediction accuracy of the BEM method needs to be further improved.
出处 《农业工程学报》 EI CAS CSCD 北大核心 2013年第18期67-74,共8页 Transactions of the Chinese Society of Agricultural Engineering
基金 国家自然科学基金资助项目(50706041) 科技部国际科技合作计划资助项目(2010DFA64660) 扬州大学科技创新培育基金资助项目(2012CXJ048) 江苏省研究生科研创新计划(CXZZ12_0898)
关键词 风机 气动载荷 计算流体力学 攻角 fans, aerodynamic loads, computational fluid dynamics, angle of attack
  • 相关文献

参考文献30

  • 1Van Bussel G J W. The aerodynamics of horizontal-axis wind-turbine rotors explored with asymptotic expansion methods[D]. Ph.D. Thesis, Delft University of Technology, Holland. 1995.
  • 2Gupta S and Leishman J G. Dynamic Stall Modeling ofthe S809 Aerofoil and Comparison with Experiments[J]. Wind Energy, 2006, 9(6): 521 -547.
  • 3Himmelskamp H. Profile investigations on a rotating airscrew[D]. Ph.D. Thesis, Gottingen University, Germany, 1945.
  • 4Goankar G H and Peters D A. Review of dynamic inflow modelling for rotorcraft flight dynamics[J]. Vertica, 1988 2(3): 213-242.
  • 5Schepers J G and Snel H. Joint investigation of dynamic inflow effects and implementation of an engineering method[J]. ECN-C. 1995. 107.
  • 6刘雄,张宪民,陈严,叶枝全.基于动态入流理论的水平轴风力机动态气动载荷计算模型[J].太阳能学报,2009,30(4):412-419. 被引量:13
  • 7Larsen J W, Nielsen S R K, K.renk S. Dynamic stall model for wind turbine airfoils[J]. Journal of Fluids and Structures, 2007, 23(7): 959-982.
  • 8Tsang K K Y, Leung R C K, Wang X Q, et al. Dynamic stall behavior from unsteady force measurements[J]. Journal of Fluids and Structures, 2008, 24(1): 129-150.
  • 9李银然,李仁年,王秀勇,杨瑞.Gurney襟翼对风力机专用翼型气动性能的影响[J].流体机械,2011,39(1):16-19. 被引量:12
  • 10王琦峰,陈伯君,安亦然.大型风力机三维空气动力学数值模拟[J].空气动力学学报,2011,29(6):810-814. 被引量:10

二级参考文献94

共引文献123

同被引文献29

引证文献3

二级引证文献10

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部