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主动控制起落架建模与仿真 被引量:3
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作者 王海涛 w.g.price +1 位作者 李为吉 万小朋 《系统仿真学报》 EI CAS CSCD 北大核心 2008年第22期6261-6264,6272,共5页
建立了主动控制起落架系统的非线性模型和控制方程,对系统进行了稳定性分析,应用simulink对起落架主动控制系统进行了仿真,结果表明通过应用主动控制起落架系统,减小了飞机重心的垂直位移和起落架传递给机身的载荷,对提高飞机的滑行品... 建立了主动控制起落架系统的非线性模型和控制方程,对系统进行了稳定性分析,应用simulink对起落架主动控制系统进行了仿真,结果表明通过应用主动控制起落架系统,减小了飞机重心的垂直位移和起落架传递给机身的载荷,对提高飞机的滑行品质、提高乘客的舒适性、改善民用飞机在低等级机场上以及军用飞机在修复类或损坏类跑道上的使用等有着重要的意义。 展开更多
关键词 主动控制 起落架 振动冲击 缓冲器
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Secondary steady-state and time-periodic flows from a basic flow with square array of odd number of vortices
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作者 Zhimin CHEN w.g.price 《Applied Mathematics and Mechanics(English Edition)》 SCIE EI CSCD 2023年第3期447-458,共12页
In a magnetohydrodynamic(MHD)driven fluid cell,a plane non-parallel flow in a square domain satisfying a free-slip boundary condition is examined.The energy dissipation of the flow is controlled by the viscosity and l... In a magnetohydrodynamic(MHD)driven fluid cell,a plane non-parallel flow in a square domain satisfying a free-slip boundary condition is examined.The energy dissipation of the flow is controlled by the viscosity and linear friction.The latter arises from the influence of the Hartmann bottom boundary layer in a three-dimensional(3D)MHD experiment in a square bottomed cell.The basic flow in this fluid system is a square eddy flow exhibiting a network of N~2 vortices rotating alternately in clockwise and anticlockwise directions.When N is odd,the instability of the flow gives rise to secondary steady-state flows and secondary time-periodic flows,exhibiting similar characteristics to those observed when N=3.For this reason,this study focuses on the instability of the square eddy flow of nine vortices.It is shown that there exist eight bi-critical values corresponding to the existence of eight neutral eigenfunction spaces.Especially,there exist non-real neutral eigenfunctions,which produce secondary time-periodic flows exhibiting vortices merging in an oscillatory manner.This Hopf bifurcation phenomenon has not been observed in earlier investigations. 展开更多
关键词 two-dimensional(2D)Navier-Stokes equation non-parallel square vortex flow primary bifurcation secondary steady-state flow secondary time-periodic flow
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