Step 1: Read the velocity equation.
We have $v_{x} = 22\cos\!\left(\dfrac{\pi t}{2}\right)$ cm s$^{-1}$. Compare with $v = v_{0}\cos(\omega t)$.
Step 2: Find $\omega$ and the time period.
So $\omega = \dfrac{\pi}{2}$ rad s$^{-1}$, and $T = \dfrac{2\pi}{\omega} = 4$ s. The biggest speed is $v_{0}=22$.
Step 3: Find the amplitude.
\[ A = \frac{v_{0}}{\omega} = \frac{22}{\pi/2} = \frac{44}{\pi} \approx 14.0 \text{ cm} \]
Step 4: Split the total time.
Total time is $4.5$ s. One full period is $4$ s, leaving $0.5$ s extra. In one full period the body covers $4A$.
Step 5: Distance in the extra $0.5$ s.
Starting from the centre, position is $x = A\sin(\omega t)$. At $t=0.5$ s, $x = A\sin\!\left(\dfrac{\pi}{4}\right) = \dfrac{A}{\sqrt{2}}$. That is the extra distance from the centre.
Step 6: Add it all up.
\[ \text{Distance} = 4A + \frac{A}{\sqrt{2}} = 14.0\,(4 + 0.707) \approx 65.9 \text{ cm} \]So the total distance is $65.9$ cm, which is option 3.
\[ \boxed{65.9 \text{ cm}} \]