Trying to understand the connection between oscillations and vector DEs, how would I write the homogenous oscillator DE $$y’’+ 2\lambda y’ + w_0^2y = 0$$ as a first-order vector DE?
Any help would be greatly appreciated.
Trying to understand the connection between oscillations and vector DEs, how would I write the homogenous oscillator DE $$y’’+ 2\lambda y’ + w_0^2y = 0$$ as a first-order vector DE?
Any help would be greatly appreciated.
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Set
$z = y', \; z' = y''; \tag 1$
then the equation
$y'' + 2\lambda y' + \omega_0^2 y = 0 \tag 2$
becomes
$z' + 2\lambda z + \omega_0^2 y = 0, \tag 3$
that is,
$ z' = -2\lambda z - \omega_0^2 y; \tag 4$
if we now define
$\mathbf r = \begin{pmatrix} y \\ z \end{pmatrix}, \tag 5$
then
$\mathbf r' = \begin{pmatrix} y' \\ z' \end{pmatrix} = \begin{pmatrix} z \\ -2\lambda z - \omega_0^2 y \end{pmatrix} = \begin{bmatrix} 0 & 1 \\ -\omega_0^2 & -2\lambda \end{bmatrix} \begin{pmatrix} y \\ z \end{pmatrix} = \begin{bmatrix} 0 & 1 \\ -\omega_0^2 & -2\lambda \end{bmatrix} \mathbf r. \tag 6$
We have thus reduced the second-order scalar equation (2) to the first-order linear vector system
$\mathbf r^\prime = \begin{bmatrix} 0 & 1 \\ -\omega_0^2 & -2\lambda \end{bmatrix} \mathbf r, \tag 7$
as per request.