Step 1: Understanding the Concept
Motion is oscillatory if the displacement varies periodically with time. A displacement that stays constant at zero is not oscillation.
Step 2: Check options with different forms
\(y=A\sin\omega t+A\cos2\omega t\) is a sum of two periodic terms and repeats, so it is oscillatory. The forms \(A\cos\left(\omega t-\dfrac{\pi}{4}\right)\) and \(A\sin\left(\omega t-\dfrac{\pi}{4}\right)\) are simple harmonic.
Step 3: Simplify option (C)
\(\cos\left(\omega t+\dfrac{\pi}{2}\right)=-\sin\omega t\).
So \(y=A\sin\omega t-A\sin\omega t=0\) for all \(t\). The particle stays at rest.
Final Answer:
The equation \(y=A\sin\omega t+A\cos(\omega t+\pi/2)\) gives no oscillation.
\[ \boxed{\text{(C) }y=A\sin \omega t+A\cos (\omega t+\pi /2)} \]