A3.6 B3.4

Dynamics of Differential Equations | Part II, 2001

(i) Define a hyperbolic fixed point x0x_{0} of a flow determined by a differential equation x˙=f(x)\dot{x}=f(x) where xRnx \in R^{n} and ff is C1C^{1} (i.e. differentiable). State the Hartman-Grobman Theorem for flow near a hyperbolic fixed point. For nonlinear flows in R2R^{2} with a hyperbolic fixed point x0x_{0}, does the theorem necessarily allow us to distinguish, on the basis of the linearized flow near x0x_{0} between (a) a stable focus and a stable node; and (b) a saddle and a stable node? Justify your answers briefly.

(ii) Show that the system:

x˙=(μ+1)+(μ3)xy+6x2+12xy+5y22x36x2y5xy2y˙=22x+(μ5)y+4xy+6y22x2y6xy25y3\begin{aligned} &\dot{x}=-(\mu+1)+(\mu-3) x-y+6 x^{2}+12 x y+5 y^{2}-2 x^{3}-6 x^{2} y-5 x y^{2} \\ &\dot{y}=2-2 x+(\mu-5) y+4 x y+6 y^{2}-2 x^{2} y-6 x y^{2}-5 y^{3} \end{aligned}

has a fixed point (x0,0)\left(x_{0}, 0\right) on the xx-axis. Show that there is a bifurcation at μ=0\mu=0 and determine the stability of the fixed point for μ>0\mu>0 and for μ<0\mu<0.

Make a linear change of variables of the form u=xx0+αy,v=xx0+βyu=x-x_{0}+\alpha y, v=x-x_{0}+\beta y, where α\alpha and β\beta are constants to be determined, to bring the system into the form:

u˙=v+u[μ(u2+v2)]v˙=u+v[μ(u2+v2)]\begin{aligned} &\dot{u}=v+u\left[\mu-\left(u^{2}+v^{2}\right)\right] \\ &\dot{v}=-u+v\left[\mu-\left(u^{2}+v^{2}\right)\right] \end{aligned}

and hence determine whether the periodic orbit produced in the bifurcation is stable or unstable, and whether it exists in μ<0\mu<0 or μ>0\mu>0.

Typos? Please submit corrections to this page on GitHub.