A quasi-implicit characteristic-based penalty finite-element method for incompressible laminar viscous flows

被引:10
|
作者
Jiang, Chen [1 ,2 ]
Zhang, Zhi-Qian [3 ]
Han, Xu [1 ]
Liu, Guirong [2 ]
Gao, Guang-Jun [4 ]
Lin, Tao [2 ]
机构
[1] Hunan Univ, State Key Lab Adv Technol Design & Mfg Vehicle Bo, Changsha 410082, Hunan, Peoples R China
[2] Univ Cincinnati, Dept Aerosp Engn & Engn Mech, Cincinnati, OH USA
[3] ASTAR, Inst High Performance Comp, Singapore, Singapore
[4] Cent S Univ, Sch Traff & Transportat Engn, Key Lab Traff Safety Track, Minist Educ, Changsha, Hunan, Peoples R China
基金
中国国家自然科学基金;
关键词
characteristic-Galerkin scheme; finite-element method; laminar flow; node-based smoothed finite-element method; penalty formulation; selective reduced integration; METHOD ES-FEM; G SPACE; TETRAHEDRAL ELEMENT; NUMERICAL-SOLUTION; PART I; FORMULATION; SIMULATION; ALGORITHM; EXPLICIT; SPLIT;
D O I
10.1002/nme.5738
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
In this paper, a novel characteristic-based penalty (CBP) scheme for the finite-element method (FEM) is proposed to solve 2-dimensional incompressible laminar flow. This new CBP scheme employs the characteristic-Galerkin method to stabilize the convective oscillation. To mitigate the incompressible constraint, the selective reduced integration (SRI) and the recently proposed selective node-based smoothed FEM (SNS-FEM) are used for the 4-node quadrilateral element (CBP-Q4SRI) and the 3-node triangular element (CBP-T3SNS), respectively. Meanwhile, the reduced integration (RI) for Q4 element (CBP-Q4RI) and NS-FEM for T3 element (CBP-T3NS) with CBP scheme are also investigated. The quasi-implicit CBP scheme is applied to allow a large time step for sufficient large penalty parameters. Due to the absences of pressure degree of freedoms, the quasi-implicit CBP-FEM has higher efficiency than quasi-implicit CBS-FEM. In this paper, the CBP-Q4SRI has been verified and validated with high accuracy, stability, and fast convergence. Unexpectedly, CBP-Q4RI is of no instability, high accuracy, and even slightly faster convergence than CBP-Q4SRI. For unstructured T3 elements, CBP-T3SNS also shows high accuracy and good convergence but with pressure oscillation using a large penalty parameter; CBP-T3NS produces oscillated wrong velocity and pressure results. In addition, the applicable ranges of penalty parameter for different proposed methods have been investigated.
引用
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页码:147 / 171
页数:25
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