mliuzzolino
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Homework Statement
Show that there is a certain ellipsoidal region E of the form rx2 + σy2 + σ(z-2r)2 ≤ C such that all trajectories of the Lorenz equations eventually enter E and stay in there forever.
Homework Equations
Lorenz Equations:
\dot{x} = \sigma (y - x)
\dot{y} = rx - xz - y
\dot{z} = xy - bz
V is the volume.
The Attempt at a Solution
V = rx^2 + \sigma y^2 + \sigma(z-2r)^2
\dot{V} = 2rx\dot{x} + 2\sigma y \dot{y} + 2 \sigma(z - 2r) \dot{z}
\dfrac{1}{2} \dot{V} = rx(\sigma y - \sigma x) + \sigma y (rx - xz - y) + (\sigma z - 2 \sigma r)(xy - bz)
\Rightarrow \dfrac{1}{2 \sigma} \dot{V} = -rx^2 - y^2 -bz^2 + 2bz
\Rightarrow \dot{V} < 0
Therefore, all trajectories of the Lorenz equations eventually enter E and stay in there forever.
I am not sure I approached this problem correctly, and the additional challenge problem states to try and obtain the smallest possible value of C with this attracting property. Did I miss something in my workthrough above involving C? If I subtract it from both sides of the original inequality and involve it in the workthrough involving the change in volume, isn't the value of C irrelevant given that its derivative is zero (being that it's a constant) ?