针对旋转倒立摆自动起摆的控制问题,提出了基于BVP算法的自动起摆控制策略。该方法将倒立摆起摆控制问题转化成求解非线性方程的两点边值问题(Two-point BoundaryValue Problem BVP),构造了含参变量具有傅立叶级数形式的起摆力矩函数,...针对旋转倒立摆自动起摆的控制问题,提出了基于BVP算法的自动起摆控制策略。该方法将倒立摆起摆控制问题转化成求解非线性方程的两点边值问题(Two-point BoundaryValue Problem BVP),构造了含参变量具有傅立叶级数形式的起摆力矩函数,将力矩函数代入倒立摆系统,利用Matlab工具箱中的bvp4c函数求解两点边值条件,获得起摆过程的起摆控制的时间序列。基于BVP算法的起摆控制的求解,本质上属于开环前馈控制。为了抑制参数摄动,进行了平衡点附近的稳摆控制设计。稳摆设计是针对系统模型不稳定性和非最小相位特性分别进行的。对起摆、稳摆及其切换过程进行了仿真和实验研究,验证了所提出的自动起摆控制策略的有效性。展开更多
本文运用数值计算的方法研究了包含周期刺激项Acos(ω_0t)的BVP(Bonhoeffer-van der Pol)模型随控制参数ω_0变化出现的分岔、混沌和阵发混沌.结果表明,受环境周期性变化的影响,在适当的条件下,一类可兴奋细胞系统表现出的复杂的电生理...本文运用数值计算的方法研究了包含周期刺激项Acos(ω_0t)的BVP(Bonhoeffer-van der Pol)模型随控制参数ω_0变化出现的分岔、混沌和阵发混沌.结果表明,受环境周期性变化的影响,在适当的条件下,一类可兴奋细胞系统表现出的复杂的电生理活动是与混沌行为密切相关的.展开更多
The existence of positive solutions to second-order periodic BVPs-u'+Mu =j(t, u),t(0) = u(2π),u'(0) = '(2π) and u'+ Mu = I(t, u), u(0) = u(2π), u'(0) = u'(2π)is proved by a simple appliCati...The existence of positive solutions to second-order periodic BVPs-u'+Mu =j(t, u),t(0) = u(2π),u'(0) = '(2π) and u'+ Mu = I(t, u), u(0) = u(2π), u'(0) = u'(2π)is proved by a simple appliCation of a Fixed point Theorem in cones due to Krasnoselskii.展开更多
The existence of positive radial solutions to the second order semilinear elliptic BVPΔu(X)+g(|X|)f(u(X))=0, R 1<|X|<R 2, u(X)=0, |X|=R 1 or |X|=R 2is considered. A general existence criterion and se...The existence of positive radial solutions to the second order semilinear elliptic BVPΔu(X)+g(|X|)f(u(X))=0, R 1<|X|<R 2, u(X)=0, |X|=R 1 or |X|=R 2is considered. A general existence criterion and several existence theorems of positive radial solution are established. Here it is not required that lim l→0f(l)/l and lim l→∞f(l)/l exist.展开更多
We explore the complicated bursting oscillations as well as the mechanism in a high-dimensional dynamical system.By introducing a periodically changed electrical power source in a coupled BVP oscillator, a fifth-order...We explore the complicated bursting oscillations as well as the mechanism in a high-dimensional dynamical system.By introducing a periodically changed electrical power source in a coupled BVP oscillator, a fifth-order vector field with two scales in frequency domain is established when an order gap exists between the natural frequency and the exciting frequency.Upon the analysis of the generalized autonomous system, bifurcation sets are derived, which divide the parameter space into several regions associated with different types of dynamical behaviors. Two typical cases are focused on as examples,in which different types of bursting oscillations such as sub Hopf/sub Hopf burster, sub Hopf/fold-cycle burster, and doublefold/fold burster can be observed. By employing the transformed phase portraits, the bifurcation mechanism of the bursting oscillations is presented, which reveals that different bifurcations occurring at the transition between the quiescent states（QSs） and the repetitive spiking states（SPs） may result in different forms of bursting oscillations. Furthermore, because of the inertia of the movement, delay may exist between the locations of the bifurcation points on the trajectory and the bifurcation points obtained theoretically.展开更多
A conventional complex variable boundary integral equation （CVBIE） in plane elasticity is provided. After using the Somigliana identity between a particular fundamental stress field and a physical stress field, an a...A conventional complex variable boundary integral equation （CVBIE） in plane elasticity is provided. After using the Somigliana identity between a particular fundamental stress field and a physical stress field, an additional integral equality is obtained. By adding both sides of this integral equality to both sides of the conventional CVBIE, the amended boundary integral equation （BIE） is obtained. The method based on the discretization of the amended BIE is called the amended influence matrix method. With this method, for the Neumann boundary value problem （BVP） of an interior region, a unique solution for the displacement can be obtained. Several numerical examples are provided to prove the efficiency of the suggested method.展开更多
文摘针对旋转倒立摆自动起摆的控制问题,提出了基于BVP算法的自动起摆控制策略。该方法将倒立摆起摆控制问题转化成求解非线性方程的两点边值问题(Two-point BoundaryValue Problem BVP),构造了含参变量具有傅立叶级数形式的起摆力矩函数,将力矩函数代入倒立摆系统,利用Matlab工具箱中的bvp4c函数求解两点边值条件,获得起摆过程的起摆控制的时间序列。基于BVP算法的起摆控制的求解,本质上属于开环前馈控制。为了抑制参数摄动,进行了平衡点附近的稳摆控制设计。稳摆设计是针对系统模型不稳定性和非最小相位特性分别进行的。对起摆、稳摆及其切换过程进行了仿真和实验研究,验证了所提出的自动起摆控制策略的有效性。
文摘The existence of positive solutions to second-order periodic BVPs-u'+Mu =j(t, u),t(0) = u(2π),u'(0) = '(2π) and u'+ Mu = I(t, u), u(0) = u(2π), u'(0) = u'(2π)is proved by a simple appliCation of a Fixed point Theorem in cones due to Krasnoselskii.
文摘The existence of positive radial solutions to the second order semilinear elliptic BVPΔu(X)+g(|X|)f(u(X))=0, R 1<|X|<R 2, u(X)=0, |X|=R 1 or |X|=R 2is considered. A general existence criterion and several existence theorems of positive radial solution are established. Here it is not required that lim l→0f(l)/l and lim l→∞f(l)/l exist.
基金Project supported by the National Natural Science Foundation of China(Grant No.21276115)
文摘We explore the complicated bursting oscillations as well as the mechanism in a high-dimensional dynamical system.By introducing a periodically changed electrical power source in a coupled BVP oscillator, a fifth-order vector field with two scales in frequency domain is established when an order gap exists between the natural frequency and the exciting frequency.Upon the analysis of the generalized autonomous system, bifurcation sets are derived, which divide the parameter space into several regions associated with different types of dynamical behaviors. Two typical cases are focused on as examples,in which different types of bursting oscillations such as sub Hopf/sub Hopf burster, sub Hopf/fold-cycle burster, and doublefold/fold burster can be observed. By employing the transformed phase portraits, the bifurcation mechanism of the bursting oscillations is presented, which reveals that different bifurcations occurring at the transition between the quiescent states（QSs） and the repetitive spiking states（SPs） may result in different forms of bursting oscillations. Furthermore, because of the inertia of the movement, delay may exist between the locations of the bifurcation points on the trajectory and the bifurcation points obtained theoretically.
文摘A conventional complex variable boundary integral equation （CVBIE） in plane elasticity is provided. After using the Somigliana identity between a particular fundamental stress field and a physical stress field, an additional integral equality is obtained. By adding both sides of this integral equality to both sides of the conventional CVBIE, the amended boundary integral equation （BIE） is obtained. The method based on the discretization of the amended BIE is called the amended influence matrix method. With this method, for the Neumann boundary value problem （BVP） of an interior region, a unique solution for the displacement can be obtained. Several numerical examples are provided to prove the efficiency of the suggested method.
