The force acting on the object is \( F = -75y \).
According to Newton's second law, \( F = ma \), where \( m \) is the mass and \( a \) is the acceleration.
So, \( ma = -75y \).
The acceleration of the object is \( a = -\frac{75}{m} y \).
Given mass \( m = 3 \) kg, the acceleration is \( a = -\frac{75}{3} y = -25y \).
For simple harmonic motion, the acceleration is given by \( a = -\omega^2 y \), where \( \omega \) is the angular frequency.
Comparing the two expressions for acceleration, we have \( \omega^2 = 25 \), so \( \omega = 5 \) rad/s.
The velocity of the object in SHM is given by \( v = \omega \sqrt{A^2 - y^2} \), where \( A \) is the amplitude of the motion.
At the mean position, \( y = 0 \), and the velocity is maximum, \( v_{max} = \omega A \).
Given that the velocity at the mean position is \( v_{max} = 2.
5 \) ms\(^{-1} \).
So, \( 2.
5 = 5 A \).
The amplitude \( A = \frac{2.
5}{5} = 0.
5 \) m.
The maximum acceleration in SHM occurs at the extreme positions (\( y = \pm A \)) and is given by \( a_{max} = \omega^2 A \).
Substituting the values of \( \omega^2 \) and \( A \):
\( a_{max} = (25)(0.
5) = 12.
5 \) ms\(^{-2} \).