Step 1: Understand the concept of SHM.
In Simple Harmonic Motion (SHM), the displacement of the particle is given by:
\[
x = A \cos(\omega t + \phi)
\]
where \( A \) is the amplitude, \( \omega \) is the angular frequency, \( t \) is the time, and \( \phi \) is the phase constant.
Step 2: Given conditions.
At \( t = 0 \), the particle is at the centre, so \( x(0) = 0 \).
The particle is initially moving towards the left, which means the velocity is negative.
Step 3: Velocity in SHM.
The velocity in SHM is given by:
\[
v = -A \omega \sin(\omega t + \phi)
\]
Since the particle starts at the centre and moves to the left, the phase constant \( \phi \) is \( 0 \).
So, the displacement and velocity equations become:
\[
x = A \cos(\omega t) \quad \text{and} \quad v = -A \omega \sin(\omega t)
\]
Step 4: Find the position and velocity at \( t = 3T/4 \).
At \( t = 3T/4 \), the angular position is:
\[
x = A \cos\left(\omega \cdot \frac{3T}{4}\right) = A \cos\left(\frac{3\pi}{2}\right) = 0
\]
So, the particle is at the centre.
Step 5: Find the velocity.
The velocity at \( t = 3T/4 \) is:
\[
v = -A \omega \sin\left(\frac{3\pi}{2}\right) = A \omega
\]
Thus, the particle is moving with maximum speed towards the left.