(1)
Rewrite the first equation: $x_{2} = \frac{1}{2}x_{1}' + \frac{1}{4}x_{1}$
Then, $x_{2}' = \frac{1}{2}x_{1}'' + \frac{1}{4}x_{1}'$
Plug into the second equation: $\frac{1}{2}x_{1}'' + \frac{1}{4}x_{1}' = -2x_{1} -\frac{1}{2}(\frac{1}{2}x_{1}' + \frac{1}{4}x_{1})$
Then, we get: $x_{1}'' + x_{1}' + \frac{17}{4}x_{1} = 0$ which is a second order ODE of $𝑥_{1}$
(2)
\begin{align*}
Let A &=
\begin{bmatrix}
-\frac{1}{2} & 2 \\
-2 & -\frac{1}{2}
\end{bmatrix}\\
A-\lambda I &=
\begin{bmatrix}
-\frac{1}{2} -\lambda & 2 \\
-2 & -\frac{1}{2} -\lambda
\end{bmatrix}\\
det(A-\lambda I) &= (\lambda + \frac{1}{2})^{2} + 4 = 0\\
\lambda + \frac{1}{2} &= \pm 2i\\
\lambda &= -\frac{1}{2} \pm 2i\\
\end{align*}
For $\lambda = -\frac{1}{2} + 2i$:
\begin{align*}
A-\lambda I &= \begin{bmatrix}
-2i & 2 \\
-2 & -2i
\end{bmatrix}\\
null\begin{bmatrix} -2i & 2 \\ -2 & -2i \end{bmatrix}
&= span{\begin{bmatrix} 1\\ i \end{bmatrix}\\}\\
so, \ the \ eigenvector \ V &= \begin{bmatrix} 1\\ i \end{bmatrix}\\
Then, \ e^{\lambda t}V &= e^{(-\frac{1}{2} + 2i)t}\begin{bmatrix} 1\\ i \end{bmatrix}\\
&= e^{-\frac{1}{2}t}e^{2it}\begin{bmatrix} 1\\ i \end{bmatrix}\\
&= e^{-\frac{1}{2}t}(cos2t + isin2t)\begin{bmatrix} 1\\ i \end{bmatrix}\\
&= \begin{bmatrix} cos2t + isin2t\\ icos2t - sin2t \end{bmatrix}\\
Thus, \ \phi_{1}(t) &= e^{-\frac{1}{2}t}\begin{bmatrix} cos2t\\- sin2t \end{bmatrix}\\
\phi_{2}(t) &= e^{-\frac{1}{2}t}\begin{bmatrix} sin2t\\cos2t \end{bmatrix}\\
Therefore, \ x_{1} &= c_{1}e^{-\frac{1}{2}t}cos2t + c_{2}e^{-\frac{1}{2}t}sin2t\\
x_{2} &= -c_{1}e^{-\frac{1}{2}t}sin2t + c_{2}e^{-\frac{1}{2}t}cos2t\\
Since, \ x_{1}(0) &= -2 \ and \ x_{2}(0) = 2\\
So, \ c_{1} &= -2 \ and \ c_{2} = 2\\
\end{align*}
Therefore,
\begin{align*}
x_{1} &= -2e^{-\frac{1}{2}t}cos2t + 2e^{-\frac{1}{2}t}sin2t\\
x_{2} &= 2e^{-\frac{1}{2}t}sin2t + 2e^{-\frac{1}{2}t}cos2t\\
\end{align*}