Applying a linear transformation to a system of differential equations

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I am reading the book: Nonlinear Oscillations, Dynamical System and Bifurcations of Vector Fields (Guckenheimer and Holmes), chapter 2: An introduction to chaos.

About Van der Pol's equation, it can be expressed as the system

$(*) \ \ \begin{align} \dot{x} &= y-\alpha \Phi(x)\\ \dot{y} &= -x + \beta p(\theta) \\ \dot{\theta} &= 1 \end{align}$

Taking $\alpha\ll 1$, $\beta = 0$(unforced) and $\Phi(x)=\frac{x^3}{3}-x$, the system $(*)$ can be considered as a perturbation of: $$\dot{x}=y, \ \ \ \dot{y}=-x$$

Now, using the transformation: $$\begin{pmatrix}u\\v\end{pmatrix} =\begin{pmatrix}\cos(t)& -\sin(t)\\ -\sin(t)& -\cos(t)\end{pmatrix}\begin{pmatrix}x\\y\end{pmatrix} $$

The system $(*)$ becomes: $$\dot{u} = -\alpha \cos(t)\left[(u\cos(t)-v\sin(t))^3/3-(u\cos(t)-v\sin(t))\right]$$ $$\dot{v} = -\alpha \sin(t)\left[(u\cos(t)-v\sin(t))^3/3-(u\cos(t)-v\sin(t))\right]$$

The goal of applying this transformation is, in the next step to apply average method to the system.

My problem is:

I already applied the transformation to the system: $$\begin{pmatrix}\dot{u}\\ \dot{v}\end{pmatrix} =\begin{pmatrix}\cos(t)& -\sin(t)\\ -\sin(t)& -\cos(t)\end{pmatrix}\begin{pmatrix}\dot{x}\\ \dot{y}\end{pmatrix}, $$ and using the expressions for $\dot{x}, \dot{y}$, I obtained:

$$\dot{u} = -v -\alpha \cos(t)\left((u\cos(t)-v\sin(t))^3/3-(u\cos(t)-v\sin(t))\right)$$ $$\dot{v} = u -\alpha \sin(t)\left((u\cos(t)-v\sin(t))^3/3-(u\cos(t)-v\sin(t))\right)$$

What I am doing wrong? Are the authors just considering the non-linear part of the "new system"? Thanks.

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When you differentiate $$\begin{pmatrix}u\\v\end{pmatrix}=\begin{pmatrix}\cos(t)& -\sin(t)\\ -\sin(t)& -\cos(t)\end{pmatrix}\begin{pmatrix}x\\y\end{pmatrix}$$

You must also differentiate the $\sin$ and $\cos$, for example $$u=\cos(t) x - \sin(t) y$$ leads to $$\dot{u}=\cos(t) \dot{x} -\sin(t) \dot{y} -\sin(t) x -\cos(t) y.$$


On a side note, are you sure of the transformation ?

The goal of such transform is to obtain $\dot{u}=\dot{v}=0$ in the case $\alpha=0$.

As in the case $\alpha=0$ the solution is of the form

\begin{equation*} \begin{pmatrix}x \\ y \end{pmatrix} = \begin{pmatrix}\cos(t) & \sin(t) \\- \sin(t)& \cos(t) \end{pmatrix} \begin{pmatrix}x_0 \\ y_0 \end{pmatrix} \end{equation*}

so we obtain \begin{equation*} \begin{pmatrix}u \\ v \end{pmatrix} = \begin{pmatrix}\cos(t)²-\sin(t)^2 & -2 \cos(t)\sin(t) \\-2 \cos(t)\sin(t)& \sin(t)^2-\cos(t)^2 \end{pmatrix} \begin{pmatrix}x_0 \\ y_0 \end{pmatrix} \end{equation*} which is not a constant.

As in the method of the variation of parameters the change of variables should be \begin{equation*} \begin{pmatrix}x \\ y \end{pmatrix} = \begin{pmatrix}\cos(t) & \sin(t) \\- \sin(t)& \cos(t) \end{pmatrix} \begin{pmatrix}u \\ v \end{pmatrix} \end{equation*} i.e \begin{equation*} \begin{pmatrix}u \\ v \end{pmatrix} = \begin{pmatrix}\cos(t) & \sin(t) \\- \sin(t)& \cos(t) \end{pmatrix}^{-1} \begin{pmatrix}x \\ y \end{pmatrix}=\begin{pmatrix}\cos(t) & -\sin(t) \\ \sin(t)& \cos(t) \end{pmatrix} \begin{pmatrix}x \\ y \end{pmatrix}. \end{equation*}

We obtain in this case $$\dot{u}=-\sin(t) x +\cos(t) \dot{x} -\cos(t) y -\sin(t) \dot{y}$$ and using the equation $$\dot{u}=-\sin(t) x +\cos(t) (y-\alpha \Phi(x)) -\cos(t) y -\sin(t) (-x)=0-\alpha \cos(t) \Phi(x)$$