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Systems of ODEs with constant coefficients

We begin with a system of linear differential equations. (Higher order differential equations can be transformed to this form.) A general first-order linear system has the form  
 \begin{displaymath}
{d\over dt}X(t)= A X(t)+G(t)\end{displaymath} (1)
where X(t) and G(t) are $n\times 1$ vectors, A is an $n\times n$ matrix of constant coefficients.

For a homogeneous system,  
 \begin{displaymath}
{d\over dt}X(t)= A X(t),\end{displaymath} (2)
we need n linearly independent solutions to construct the general solution  
 \begin{displaymath}
X(t)=c_1\phi_1(t)+c_2\phi_2(t) +...+c_n\phi_n(t)\end{displaymath} (3)
where

\begin{displaymath}
\phi_i(t)=\pmatrix{\phi_{1i}\cr
\phi_{2i}\cr
...\cr
\phi_{ni} }.\end{displaymath}

We can write the solution as
\begin{displaymath}
X(t)=\Omega C,\end{displaymath} (4)
where

\begin{displaymath}
\Omega=\pmatrix{\phi_1 &
\phi_2 & ... & \phi_n}\end{displaymath}

is a matrix with the solutions as columns and

\begin{displaymath}
C=\pmatrix{c_1 & c_2 & ... & c_n}^T.\end{displaymath}

The matrix $\Omega$ is a fundamental matrix of the system $\dot X=AX$. Note

\begin{displaymath}
\Omega C=\pmatrix{\phi_1 & 
\phi_2 & ... & \phi_n} 
\pmatrix{c_1 \cr c_2 \cr ... \cr c_n}\end{displaymath}

$=c_1\phi_1+c_2\phi_2 + ... + c_n\phi_n$, which is the general solution.

Example 1

\begin{displaymath}
\dot x_1=x_1-4x_2,\quad \dot x_2=x_1+5x_2\end{displaymath}

\begin{displaymath}
\to \pmatrix{\dot x_1\cr \dot x_2}=\pmatrix{1 & -4\cr 1 & 5\cr} \pmatrix{x_1\cr
x_2}. \end{displaymath}

We can check by substitution that two linearly independent solutions are

\begin{displaymath}
\phi_1=\pmatrix{-2e^{3t}
\cr e^{3t} },\quad \phi_2=\pmatrix{(1-2t)e^{3t}\cr te^{3t}\cr}.\end{displaymath}

Thus, the general solution is

\begin{displaymath}
\pmatrix{x_1\cr x_2}=\pmatrix{ -2e^{3t}
& (1-2t)e^{3t}\cr e^{3t} &
te^{3t}\cr}\pmatrix{c_1\cr c_2}\end{displaymath}

\begin{displaymath}
=\pmatrix{ -2c_1e^{3t}+c_2 (1-2t)e^{3t}\cr
 c_1e^{3t} +c_2te^{3t}} .\end{displaymath}

Recall that: If C is any nonsingular matrix ( $\det C \ne 0$) with constant entries, then $\Omega C=\Psi$ is another fundamental matrix. Check this: $d\Psi/dt=d(\Omega C)/dt=A\Omega C= A\Psi$ and $\det\Psi=
\det(\Omega C) = \det\Omega \det C \ne 0$.


next up previous contents
Next: Eigenvalues and eigenvectors Up: Linear Stability Previous: Linear Stability
Michael Renardy
1998-07-13