To solve this problem, we can use the principle of conservation of energy, which states that the total energy of a system remains constant. In this case, the initial energy of the system is equal to the final energy of the system.
Initially, the object is at rest and has only potential energy due to its height above the ground. The potential energy is given by mgh, where m is the mass of the object, g is the acceleration due to gravity, and h is the height.
As the object falls, it gains kinetic energy due to its motion. The kinetic energy is given by 1/2mv^2, where m is the mass of the object and v is its velocity.
At the same time, the spherical shell and the pulley are rotating due to the tension in the cord. The rotational energy of the shell is given by 1/2Iω^2, where I is the moment of inertia of the shell and ω is its angular velocity. Similarly, the rotational energy of the pulley is given by 1/2Iω^2, where I is the moment of inertia of the pulley and ω is its angular velocity.
Since the cord does not slip on the pulley, the linear velocity of the object is equal to the angular velocity of the pulley, and the angular velocity of the shell is half of the angular velocity of the pulley.
Using the conservation of energy principle, we can equate the initial potential energy of the object to the final total energy of the system, which includes the kinetic energy of the object and the rotational energy of the shell and pulley.
Thus, we have:
mgh = 1/2mv^2 + 1/2I(ω^2 + ω^2)
Substituting the given values, we get:
(0.60 kg)(9.8 m/s^2)(0.82 m) = 1/2(0.60 kg)v^2 + 1/2(3.0*10^-3 kg*m^2)(ω^2 + (1/2ω)^2)
Solving for v, we get:
v = 1.46 m/s
Therefore, the speed of the object when it has fallen 82 cm after being released from rest is 1.46 m/s.