Numerical simulation of a two-dimensional flapping wing in advanced mode

A two-dimensional model is built to describe the translation and the rotation of the hovering flapping movement. The equations of motion are derived for insect's flapping movement, and the model is implemented by the computational fluid dynamics(CFD) software FLUENT and it?s user defined function(UD...

Full description

Saved in:
Bibliographic Details
Published inJournal of hydrodynamics. Series B Vol. 29; no. 6; pp. 1076 - 1080
Main Author 梁志勇;魏亮;卢锦煜;覃小红
Format Journal Article
LanguageEnglish
Published Singapore Elsevier Ltd 01.12.2017
Springer Singapore
College of Science, Donghua University, Shanghai 201620, China%Key Laboratory of Textile Science and Technology, Ministry Education, College of Textiles, Donghua University, Shanghai 201620, China
Subjects
Online AccessGet full text
ISSN1001-6058
1878-0342
DOI10.1016/S1001-6058(16)60801-6

Cover

More Information
Summary:A two-dimensional model is built to describe the translation and the rotation of the hovering flapping movement. The equations of motion are derived for insect's flapping movement, and the model is implemented by the computational fluid dynamics(CFD) software FLUENT and it?s user defined function(UDF). It is shown that the lift coefficient changes slowly in the intermediate stage, there are two areas in which the lift coefficient changes dramatically, and the drag coefficient behaves quite differently when flapping up and down. The vortex distribution, the pressure distribution, and the velocity vector distribution in the advanced mode at different times follow quite various rules.
Bibliography:31-1563/T
A two-dimensional model is built to describe the translation and the rotation of the hovering flapping movement. The equations of motion are derived for insect's flapping movement, and the model is implemented by the computational fluid dynamics(CFD) software FLUENT and it?s user defined function(UDF). It is shown that the lift coefficient changes slowly in the intermediate stage, there are two areas in which the lift coefficient changes dramatically, and the drag coefficient behaves quite differently when flapping up and down. The vortex distribution, the pressure distribution, and the velocity vector distribution in the advanced mode at different times follow quite various rules.
Numerical simulation, micro flapping wing, advanced mode, unsteady aerodynamics, dynamic mesh
ISSN:1001-6058
1878-0342
DOI:10.1016/S1001-6058(16)60801-6