Jhenrique said:
If a system of first-order ODEs like ##\frac{d\vec{r}}{dt}=A\vec{r}## have as solution ##\vec{r} = C_1 \exp(\lambda_1 t)\hat{v}_1 + C_2 \exp(\lambda_2 t)\hat{v}_2## (being λ the eigenvalues and v the eigenvectors), so, given a system of second-order ODEs, like ##A \frac{d^2 \vec{r}}{dt^2} + B \frac{d\vec{r}}{dt} + C \vec{r} = \vec{0}##, which is the solution for it?
To the best of my knowledge, you don't normally see 2nd-order matrix equations like the one you show. None of the texbooks on ODE that I have (around 5 of them) have this as a topic, I don't believe.
Going back to your first equation, if the solution involves two eigenvalues and two eigenvectors, it must be that the matrix is 2 X 2, so what you show as a solution is not the general solution for the vector ODE
r' = A
r.
An important application of vector ODEs is to convert second-order and higher order ODEs into first order vector DEs.
For example, you can convert the second-order ODE is y'' - 3y' + 2y = 0 using these substitutions:
u = y
v = y' = u'
Then y'' = u', so we have this system of first order DEs:
v' - 3v + 2u = 0
u' = v
or,
u' = v
v' = -2u + 3v
This system can be written in matrix form as
$$ \vec{r}' = \begin{bmatrix}0 & 1 \\ -2 & 3 \end{bmatrix}\vec{r}$$
where
$$ \vec{r} = \begin{bmatrix} u \\ v \end{bmatrix}$$
Using a similar process, a third-order DE can be tranformed to a first-order vector equation with a 3 x 3 matrix, and a fourth-order DE can be transformed to a first-order vector equation with a 4 x 4 matrix, and so on.