(a) Hint: In SHM, the acceleration is directly proportional to the displacement.
Step 1: Find the velocity of the particle.
Given, \(y = 3 cos (\frac{\pi}{4}-\omega t)\)
The velocity of the particle,
\(v= \frac{dy}{dt} = \frac{d}{dt}[3 cos(\frac{\pi}{4}-\omega t)]\)
\(-3(-\omega)sin(\frac{\pi}{4}-\omega t)\)
\(= 3\omega sin(\frac{\pi}{4}- \omega t)\)
Step 2: Find the acceleration of the particle.
Acceleration, \(a = \frac{dv}{dt} = \frac{d}{dt}[3\omega sin(\frac{\pi}{4}-\omega t)]\)
ω) cos(π/4-ωt)=-3ω2cos(π/4-ωt)=-3ω2cos(π/4-ωt)
ω2y
As acceleration, a
Hence, due to negative sign motion is SHM.
Step 3: Find the time period of the motion.
Clearly, from the equation,
ω
ω⇒T'=2π/ω=2π/ω
So, the motion is SHM with period