航空学报
航空學報
항공학보
ACTA AERONAUTICA ET ASTRONAUTICA SINICA
2010年
2期
238-243
,共6页
卓丛山%钟诚文%李凯%解建飞%张勇
卓叢山%鐘誠文%李凱%解建飛%張勇
탁총산%종성문%리개%해건비%장용
格子Boltzmann方法%高雷诺数流动%非均匀%贴体网格%翼型
格子Boltzmann方法%高雷諾數流動%非均勻%貼體網格%翼型
격자Boltzmann방법%고뢰낙수류동%비균균%첩체망격%익형
lattice Boltzmann method%high Reynolds number flow,non-uniform%body-fitted mesh,airfoil
采用格子Boltzmann方法(LBM)的二维9速度(D2Q9)模型和贴体网格,通过引入非均匀网格插值方法和非平衡态外推边界处理,分别结合Baldwin-Lomax(B-L)湍流模型和Spalart-Allmaras(S-A)湍流模型,对高雷诺数Re≥5×10~5下的NACA0012翼型绕流进行了数值模拟和对比研究,两者的结果与CFL3D的结果和实验结果均吻合的很好,相比之下,采用S-A模型能更好地预测失速迎角,其处理分离流动的能力要强于B-L模型.改进后的LBM适用于非均匀贴体网格,曲边边界,计算简单,并可应用于更复杂的高雷诺数流动中.
採用格子Boltzmann方法(LBM)的二維9速度(D2Q9)模型和貼體網格,通過引入非均勻網格插值方法和非平衡態外推邊界處理,分彆結閤Baldwin-Lomax(B-L)湍流模型和Spalart-Allmaras(S-A)湍流模型,對高雷諾數Re≥5×10~5下的NACA0012翼型繞流進行瞭數值模擬和對比研究,兩者的結果與CFL3D的結果和實驗結果均吻閤的很好,相比之下,採用S-A模型能更好地預測失速迎角,其處理分離流動的能力要彊于B-L模型.改進後的LBM適用于非均勻貼體網格,麯邊邊界,計算簡單,併可應用于更複雜的高雷諾數流動中.
채용격자Boltzmann방법(LBM)적이유9속도(D2Q9)모형화첩체망격,통과인입비균균망격삽치방법화비평형태외추변계처리,분별결합Baldwin-Lomax(B-L)단류모형화Spalart-Allmaras(S-A)단류모형,대고뢰낙수Re≥5×10~5하적NACA0012익형요류진행료수치모의화대비연구,량자적결과여CFL3D적결과화실험결과균문합적흔호,상비지하,채용S-A모형능경호지예측실속영각,기처리분리류동적능력요강우B-L모형.개진후적LBM괄용우비균균첩체망격,곡변변계,계산간단,병가응용우경복잡적고뢰낙수류동중.
Simulation of a high Reynolds number flow(Re≥5×10~5)around an airfoil(NACA00l2)using the Lattice Boltzmann method(LBM)is performed in this article.The present method chooses a two-dimensional 9-velocity(D2Q9)model and uses a non-uniform body-fitted mesh.Originally,the LBM is an incompressible flow solver in orthogonal coordinates.In order to resolve the boundary layer of the airfoil accurately,the algorithm is extended to generalized coordinates.Meanwhile,a non-equilibrium extrapolation scheme for the wall boundary condition is adopted.In order to calculate high Reynolds number flows,the present method is combined with the Baldwin-Lomax(B-L)turbulence model and the Spalart-Allmaras(S-A)turbulence model respectively.The results agrees well with the CFL3D solver results and experimental data.Compared with the B-L model,the S-A model can give more accurate prediction of the static stall angle and show better ability of separated flow simulation.The present method is suitable for problems of non-uniform body-fitted mesh and eurvilinear boundary,and its calculation is simple.It can be applied to more complex high Reynolds number flows.