1) Saddle-homoclinic bifurcation
鞍点同宿分岔
2) saddle-node bifurcation
鞍点分岔
1.
Closest saddle-node bifurcation boundary in control parameter space;
动态电力系统求取最近鞍点分岔边界的新方法
3) homoclinic bifurcation
同宿分岔
1.
The available range of the homoclinic bifurcation criterions are extended from the weakly nonlinear oscillation system to the strongly nonlinear oscillation system.
以改进的规范形理论为基础,采用强非线性振动问题的分析方法,拓展了原有弱非线性振动系统同宿分岔判据的适用范围。
2.
By virtue of the singular point theory of one-dimension diffusion process and the stochastic averaging approach of energy envelope, the bifurcation behavior of a homoclinic bifurcation system, which is in the presence of parametric white noise and is concealed behind a cedimension two bifurcation point, is investigated.
利用一维扩散过程的奇点理论并结合能量包络的随机平均法,考查“隐藏在余维2分岔点之后”的同宿分岔系统受参激白噪声影响的分岔行为。
5) Saddle-node bifurcation
鞍结点分岔
1.
Efds + uf = Efdsc + ufc is saddle-node bifurcation value corresponding to collapse of the power system.
Efds+uf=Efdsc+ufc是鞍结点分岔值,相应于电力系统崩溃。
6) saddle node bifurcation
鞍结点分岔
1.
The saddle node bifurcation and Hopf bifurcation characteristics of a simple power system are calculated and analyzed by Continuation Method.
运用延拓法对一个简单电力系统的鞍结点分岔和Hopf分岔进行计算分析,并与其它文献的计算方法和结果进行了比较。
2.
We demonstrate that the type of intermittent chaos transitions in this model is saddle node bifurcation,according to the critical scaling exponent of the average time between bursts,the pair of periodic orbits and unstable periodic orbits and their corresponding Liyapunov exponents.
我们根据阵发时间间隔长度平均值的临界标度指数、稳定与不稳定周期轨道对以及2种轨道对应的李雅普诺夫指数的正负等3个方面论证了该模型阵发混沌的相变机制为鞍结点分岔。
补充资料:上宿
1.值夜。
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