Step 1: Take the Laplace transform of the whole equation.
Using \(\mathcal{L}\{y''\}=s^2Y(s)-sy(0)-y'(0)\) and \(\mathcal{L}\{y'\}=sY(s)-y(0)\), and since \(y(0)=0\) and \(y'(0)=0\), these reduce to \(\mathcal{L}\{y''\}=s^2Y(s)\) and \(\mathcal{L}\{y'\}=sY(s)\). Also \(\mathcal{L}\{\delta(x-5)\}=e^{-5s}\).
So the transformed equation is \(2s^2Y(s)+sY(s)+2Y(s)=e^{-5s}\), which gives
\[
Y(s) = \frac{e^{-5s}}{2s^2+s+2}
\]
Step 2: Rewrite the denominator by completing the square.
\[
2s^2+s+2 = 2\left[\left(s+\frac{1}{4}\right)^2 + \frac{15}{16}\right]
\]
so \(\dfrac{1}{2s^2+s+2} = \dfrac{1}{2}\cdot\dfrac{1}{(s+\frac14)^2+\frac{15}{16}}\).
Step 3: Invert the Laplace transform.
Using \(\mathcal{L}^{-1}\left\{\dfrac{1}{(s+a)^2+w^2}\right\} = \dfrac{1}{w}e^{-at}\sin(wt)\) with \(a=\frac14\) and \(w=\dfrac{\sqrt{15}}{4}\), the inverse transform of \(\dfrac{1}{2s^2+s+2}\) is
\[
g(t) = \frac{1}{2}\cdot\frac{4}{\sqrt{15}}e^{-t/4}\sin\left(\frac{\sqrt{15}}{4}t\right) = \frac{2}{\sqrt{15}}e^{-t/4}\sin\left(\frac{\sqrt{15}}{4}t\right)
\]
Because of the factor \(e^{-5s}\), the time-shift property gives \(y(x) = g(x-5)\) for \(x>5\) (and \(y(x)=0\) for \(x<5\)).
Step 4: Evaluate at \(x=10\) and check the wrong options.
\[
y(10) = g(5) = \frac{2}{\sqrt{15}}e^{-5/4}\sin\left(\frac{5\sqrt{15}}{4}\right)
\]
Options (A) and (C) use \(\dfrac{10}{\sqrt{15}}\) with argument \(\dfrac{\sqrt{15}}{4}\), mixing up the coefficient and forgetting to shift the argument by the delay of 5, so they are wrong. Options (C) and (D) use a growing exponential \(e^{5/4}\) instead of the decaying \(e^{-5/4}\) that this damped system must have, so they are also wrong.
Final Answer:
\[ \boxed{y(10)=\frac{2}{\sqrt{15}}e^{-5/4}\sin\left(\frac{5\sqrt{15}}{4}\right)} \]