双零加一对纯虚根特征值系统的最简规范形

针对双零加一对纯虚根特征值系统高维分岔问题,用矩阵表示法研究其系统的最简规范形。在传统规范形基础上,证明了只有线性算子值域补空间上的近恒同变换才能化简高阶规范形。引入这些近恒同变换,代入传统规范形中,利用待定系数法逐次化简规范形,得出最简规范形系数和传统规范形系数的关系。通过对k(k≥3)阶规范形系数方程的分析发现:化简规范形的个数完全由恒同变换个数决定,对确定的最简规范形式,其系数可由原方程系数唯一确定。得到了该类系统最简规范形的形式,并编制了不经中心流形降维,直接计算该类系统最简规范形系数的Mathematica程序。     

基于Gibbs矢量估计卫星轨道姿态的滤波算法研究

针对“矢量观测 陀螺”这种典型的三轴稳定卫星姿态确定系统模式,引入具有四元数优越性的Gibbs矢量作为姿态参数,提出了一种新的具有良好实时性能的轨道姿态估计方案。在方案设计中,为描述卫星轨道姿态的Gibbs矢量,推导出了基于四元数的运动学方程,并将QUEST法作为处理多矢量观测信息的压缩技术引入估计器,使得滤波修正算法得以简化。另外,针对单矢量观测情况,给出了能够加快状态估值收敛速度的改进协方差修正算法。仿真结果验证,新方案的姿态估计精度与传统的欧拉角估计法相当,而运算效率却明显高于欧拉角估计法。     

Regularization of Discontinuous Vector Fields on $${\mathbb{R}^3}$$ via Singular Perturbation

Singular perturbations problems in dimension three which are approximations of discontinuous vector fields are studied in this paper. The main result states that the regularization process developed by Sotomayor and Teixeira produces a singular problem for which the discontinuous set is a center manifold. Moreover, the definition of sliding vector field coincides with the reduced problem of the corresponding singular problem for a class of vector fields.      

Equivariant Sternberg–Chen Theorem

Smooth (C ) vector fields with linear symmetries and anti-symmetries are considered. We prove that provided symmetry group is compact then a smooth conjugacy in Sternberg–Chen Theorem can be chosen symmetric.     

Normal Forms for Control Systems at Singular Points

A normal form for open loop control systems is provided, based on their interpretation as skew product flows and on normal forms for nonautonomous differential equations.     

Weak Singularities of Planar Vector Fields Under Weak Perturbation

We characterize the elements of the set H _n of degree n homogeneous polynomial vector fields that are structurally stable with respect to perturbation in H _n , both on the plane and on the Poincaré sphere. We use this information to characterize elements of the set W _n of smooth vector fields on ² beginning with terms of order n at (0, 0) that are structurally stable in a neighborhood of (0, 0) under perturbation in W _n . We also determine the set of elements of H _n that are determining for topological equivalence at (0, 0), in the sense that the topological type of the singularity at (0, 0) is invariant under the addition of higher order terms.     

Complex Inner Product Averaging Method for Calculating Normal Form of Ode

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The Applications of a Modified Normal Form Approach

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Normal Forms for High Co-Dimension Bifurcations of Nonlinear Time-Periodic Systems with Nonsemisimple Eigenvalues

The normal forms for time-periodic nonlinear variational equations witharbitrary linear Jordan form undergoing bifurcations of highco-dimension are found. First, the equations are transformed via theLyapunov–Floquet (L–F) transformation into an equivalent form in whichthe linear matrix is constant with degenerate nonsemisimple lineareigenvalues while the nonlinear monomials have periodic coefficients. Byconsidering the resulting coupling of the bases of the near identitytransformation, the solvability condition for an arbitrary Jordan matrixis then derived. It is shown that time-independent and/or time-dependentnonlinear resonance terms remain in the normal form for various Jordanmatrices. Specifically, the normal forms for quadratic and cubicnonlinearities with the following linear Jordan forms are explicitlyderived: double zero eigenvalues (co-dimension two bifurcation), triplezero eigenvalues (co-dimension three bifurcation), and two repeatedpairs of purely imaginary eigenvalues (co-dimension two bifurcation). Acommutative system with cubic nonlinearities and a double inverted pendulum with a periodicfollower force are used as illustrative examples.     

Limit Cycles Appearing After Perturbation of Certain Multidimensional Vector Fields

Let an unperturbed multidimensional polynomial vector field have an invariant plane L and let the system restricted to this plane be Hamiltonian with a quadratic Hamilton function. Now take a polynomial perturbation of this system. The new system has an invariant surface close to L and the system restricted to it has a certain number of limit cycles. We strive to estimate this number. The linearization of this problem leads to estimation of the number of zeros of certain integral, which is a generalization of the abelian integral. We estimate this number of zeros by C ₁+C ₂ n, where n is the degree of the perturbation.     

Normal Forms and the Structure of Resonance Sets in Nonlinear Time-Periodic Systems

The structure of time-dependent resonances arising in themethod of time-dependent normal forms (TDNF) for one andtwo-degrees-of-freedom nonlinear systems with time-periodic coefficientsis investigated. For this purpose, the Liapunov–Floquet (L–F)transformation is employed to transform the periodic variationalequations into an equivalent form in which the linear system matrix istime-invariant. Both quadratic and cubic nonlinearities are investigatedand the associated normal forms are presented. Also, higher-orderresonances for the single-degree-of-freedom case are discussed. It isdemonstrated that resonances occur when the values of the Floquet multipliers result in MT-periodic (M = 1, 2,...) solutions. The discussion is limited to the Hamiltonian case (which encompasses allpossible resonances for one-degree-of-freedom). Furthermore, it is alsoshown how a recent symbolic algorithm for computing stability andbifurcation boundaries for time-periodic systems may also be employed tocompute the time-dependent resonance sets of zero measure in theparameter space. Unlike classical asymptotic techniques, this method isfree from any small parameter restriction on the time-periodic term inthe computation of the resonance sets. Two illustrative examples (oneand two-degrees-of-freedom) are included.     

Bifurcations on a Five-Parameter Family of Planar Vector Field

In this paper we consider a five-parameter family of planar vector fields where μ = (μ ₁, μ ₂, μ ₃, μ ₄, μ ₅), which is a small parameter vector, and c(0) ≠ 0. The family X _μ represents the generic unfolding of a class of nilpotent cusp of codimension five. We discuss the local bifurcations of X _μ, which exhibits numerous kinds of bifurcation phenomena including Bogdanov-Takens bifurcations of codimension four in Li and Rousseau (J. Differ. Eq. 79, 132–167, 1989) and Dumortier and Fiddelaers (In: Global analysis of dynamical systems, 2001), and Bogdanov-Takens bifurcations of codimension three in Dumortier et al. (Ergodic Theory Dynam. Syst. 7, 375–413, 1987) and Dumortier et al. (Bifurcations of planar vector fields. Nilpotent singularities and Abelian integrals, 1991). After making some rescalings, we obtain the truncated systems of X _μ . For a truncated system, all possible bifurcation sets and related phase portraits are obtained. When the truncated system is a Hamiltonian system, the bifurcation diagram and the related phase portraits are given too. Hopf bifurcations are studied for another truncated system. And it shows that the system has the Hopf bifurcations of codimension at most three, and at most three limit cycles occur in the small neighborhood of the Hopf singularity. Dedicated to Professor Zhifen Zhang in the occasion of her 80th birthday     

Orbital stability of periodic waves for the nonlinear Schrödinger equation

The nonlinear Schr?dinger equation has several families of quasi-periodic traveling waves, each of which can be parametrized up to symmetries by two real numbers: the period of the modulus of the wave profile, and the variation of its phase over a period (Floquet exponent). In the defocusing case, we show that these travelling waves are orbitally stable within the class of solutions having the same period and the same Floquet exponent. This generalizes a previous work (Gallay and Haragus, J. Diff. Equations, 2007) where only small amplitude solutions were considered. A similar result is obtained in the focusing case, under a non-degeneracy condition which can be checked numerically. The proof relies on the general approach to orbital stability as developed by Grillakis, Shatah, and Strauss, and requires a detailed analysis of the Hamiltonian system satisfied by the wave profile.     

基于遗传算法的机翼柔性蒙皮全参数优化设计

为解决变弯度机翼前缘柔性蒙皮结构设计问题,提出基于遗传算法的柔性蒙皮全参数优化方法。采用"刚度剪裁"设计理念,以大型远程飞机前缘为研究对象,通过优化变量缩减、设计区域规划和边界条件位移等效,对柔性蒙皮结构进行工程简化,在保证变形精度的同时达到降低模型复杂度的目的;基于遗传算法对蒙皮结构进行全参数同步优化,以获得混合优化变量的全局最优解。研究表明,该方法在兼顾优化效率和制造可实现的基础上,使前缘蒙皮变形的最小二乘误差(LSE)降低60%,最大偏移误差降低64%,可显著提高变形精度。     

Performance of Nonlinear Vibration Absorbers for Multi-Degrees-of-Freedom Systems Using Nonlinear Normal Modes

Linear vibration absorbers are a valuable tool used to suppressvibrations due to harmonic excitation in structural systems. Whilelimited evaluation of the performance of nonlinear vibrationabsorbers for nonlinear structures exists in the literature forsingle mode structures, none exists for multi-mode structures.Consequently, nonlinear multiple-degrees-of-freedom structures areevaluated. The theory of nonlinear normal modes is extended toinclude consideration of modal damping, excitation and smalllinear coupling, allowing estimation of vibration absorberperformance. The dynamics of the N +1-degrees-of-freedom system areshown to reduce to those of a two-degrees-of-freedom system on afour-dimensional nonlinear modal manifold, thereby simplifying theanalysis. Quantitative agreement is shown to require a higher-order model which is recommended for future investigation.     

考虑轴力作用时梁的弯曲损伤失效分析

对考虑轴力作用时梁的弯曲损伤进行了分析,推导了其损伤分析的基本方程,分析表明,中性轴随损伤的发展而偏移,有向上、向下和保持不动三种情况,其偏移的方向和范围完全由比例加载系数决定,并且在特定的比例加载系数时,中性轴能保持不动,最后获得了梁在弯曲损伤时的中性轴起始偏移点、极限偏移点和极限载荷的计算公式,以及它们的简化计算公式;讨论了损伤极限状态时轴力和弯矩的交互作用曲线;轴力对弯曲损伤的影响较为显著,有轴力作用时应尽可能考虑其影响。     

膜材碰撞接触分析的向量式有限元法

向量式有限元是以向量力学理论为分析基础并基于点值描述来获得结构体系行为的新型分析方法。在简要介绍向量式有限元三角形膜单元基本理论的基础上,针对膜材与刚体、膜材与膜材两类碰撞接触问题,提出了碰撞检测和碰撞响应的处理方法。通过膜材质点与三角形网格面之间的单向碰撞检测方法来处理膜结构的碰撞检测问题;结合罚函数法和中央差分位移式,提出基于中央差分式的罚接触力响应方法,同时赋予罚参数的选取规则,以处理膜结构的碰撞响应问题。在此基础上编制了向量式有限元膜单元的碰撞接触分析程序,并通过算例分析验证了理论推导和编制程序的可靠性和计算稳定性,体现出向量式有限元方法进行膜材碰撞接触分析的优势。     

Non-persistence of Homoclinic Connections for Perturbed Integrable Reversible Systems

The dynamics of an analytic reversible vector field (X,) is studied in with one real parameter close to 0; X=0 is a fixed point. The differential D_x (0,0) generates an oscillatory dynamics with a frequency of order 1—due to two simple, opposite eigenvalues lying on the imaginary axis—and it also generates a slow dynamics which changes from a hyperbolic type—eigenvalues are —to an elliptic type—eigenvalues are —as passes trough 0. The existence of reversible homoclinic connections to periodic orbits is known for such vector fields. In this paper we study a particular subclass of such vector fields, obtained by small reversible perturbations of the normal form. We give an explicit condition on the perturbation, generically satisfied, which prevents the existence of a homoclinic connections to 0 for the perturbed system. The normal form system of any order admits a reversible homoclinic connection to 0, which then does not survive under perturbation of higher order. It will be seen that normal form essentially decouples the hyperbolic and elliptic part of the linearization to any chosen algebraic order. However, this decoupling does not persist arbitrary reversible perturbation, which finally causes the appearance of small amplitude oscillations.     

Convergence of Birkhoff Normal form for Essentially Isochronous Systems

We reconsider the problem of the convergence of Birkhoff's normal form for a system of perturbed harmonic oscillators, under the condition that the system is essentially isochronous. In contrast with previous proofs based on the so called quadratically convergent method, the present proof uses only classical expansions in a parameter. This allows us to bring into light some mechanisms of accumulation of small divisors, which can be useful in more complicated and interesting cases. These same mechanisms allow us to prove the theorem with the Bruno condition on the frequencies in a very natural way.     

A Hybrid Boundary/Finite Element Method for Simulating Viscous Flows and Shapes of Droplets in Electric Fields

A mixed boundary element and finite element numerical algorithm for the simultaneous prediction of the electric fields, viscous flow fields, thermal fields and surface deformation of electrically conducting droplets in an electrostatic field is described in this paper. The boundary element method is used for the computation of the electric potential distribution. This allows the boundary conditions at infinity to be directly incorporated into the boundary integral formulation, thereby obviating the need for discretization at infinity. The surface deformation is determined by solving the normal stress balance equation using the weighted residuals method. The fluid flow and thermal fields are calculated using the mixed finite element method. The computational algorithm for the simultaneous prediction of surface deformation and fluid flow involves two iterative loops, one for the electric field and surface deformation and the other for the surface tension driven viscous flows. The two loops are coupled through the droplet surface shapes for viscous fluid flow calculations and viscous stresses for updating the droplet shapes. Computing the surface deformation in a separate loop permits the freedom of applying different types of elements without complicating procedures for the internal flow and thermal calculations. Tests indicate that the quadratic, cubic spline and spectral boundary elements all give approximately the same accuracy for free surface calculations; however, the quadratic elements are preferred as they are easier to implement and also require less computing time. Linear elements, however, are less accurate. Numerical simulations are carried out for the simultaneous solution of free surface shapes and internal fluid flow and temperature distributions in droplets in electric fields under both microgravity and earthbound conditions. Results show that laser heating may induce a non-uniform temperature distribution in the droplets. This non-uniform thermal field results in a variation of surface tension along the surface of the droplet, which in turn produces a recirculating fluid flow in the droplet. The viscous stresses cause additional surface deformation by squeezing the surface areas above and below the equator plane.