(a) Figure shows the solution of the problem with the help of phasor. Horizontal component of velocity at `Q` gives the required direction.
of velocity at `t = 0` so we will choose it.
In `DeltaOSQ : costheta = (sqrt(3)//2A)/(A) = (sqrt(3))/(2) rArr theta = (pi)/(6)`
Now `phi = (3pi)/(2) - (pi)/(6) = (8pi)/(6) = (4pi)/(3)`
So equation of `SHM` is ` x = A sin(omegat + (4pi)/(3))`
(b) Now to reach the particle at left extreme point it will travel angle `theta` along the circle. So time taken,
`t = (pi)/(omega) = (pi)/(6omega) rArr t = (T)/(12)sec`
(c) To reach the particle at mean position at mea n position it will travel angle `alpha = (pi)/(2) + (pi)/(6) = (2pi)/(3)`
So, time taken `= (alpha)/(omega) = (T)/(3) sec`.