To solve this problem, we need to understand the concept of superposition of harmonic motions. Here, we have two displacements:
We are asked to find the resultant motion when these two displacements are superimposed. The resultant displacement can be expressed as:
$y = y_1 + y_2 = a \sin (\omega t) + b \cos (\omega t)$
This expression can be rewritten as a single sinusoidal function using the identity for phase addition:
$y = R \sin(\omega t + \phi)$
where $R$ is the amplitude of the resultant wave and $\phi$ is the phase angle. The amplitude $R$ is given by:
$R = \sqrt{a^2 + b^2}$
Hence, the resultant motion is simple harmonic with an amplitude of $ \sqrt{ a^2 + b^2 }$.
The correct answer is: simple harmonic with amplitude $ \sqrt{ a^2 + b^2 }$.