To find the amplitude of the particle executing simple harmonic motion, we consider the given equation for displacement: \(y = A_0 + A \sin \omega t + B \cos \omega t\).
The general form for a simple harmonic motion (SHM) displacement is:
\(y = C \sin(\omega t + \phi)\)
Here, \(C\) is the amplitude of the motion.
We need to express the given equation in this form. We can use the approach of expanding the general equation using trigonometric identities:
Notice that the constant \(A_0\) does not affect the amplitude of these oscillations. Amplitude is determined by the maximum value of the oscillating part, which is \(\sqrt{A^2 + B^2}\).
Therefore, the amplitude of the oscillation is indeed given by:
\(\sqrt{A^2 + B^2}\)
Thus, the correct answer is option 2: \(\sqrt {A^2+B^2}\).