The rotational inertia of a particle of mass \(m\) at a distance \(r\) from the axis of rotation is given by \(I = mr^2\).
For the first particle, the distance from the rotation axis is \(d\), so its rotational inertia is \(I_1 = md^2\).
For the second particle, the distance from the rotation axis is \(2d\), so its rotational inertia is \(I_2 = m(2d)^2 = 4md^2\).
The rotational inertia of a rod of mass \(M\) and length \(L\) about its center is given by \(\frac{1}{12}ML^2\).
Using the parallel axis theorem, the rotational inertia of a rod about an axis a distance \(x\) away from the center of mass is \(I = I_{cm} + Mx^2\).
For the first rod, the distance from the rotation axis to the center of mass is \(d/2\), so its rotational inertia is \(I_3 = \frac{1}{12}Md^2 + M(\frac{d}{2})^2 = \frac{1}{3}Md^2\).
For the second rod, the distance from the rotation axis to the center of mass is \(\frac{3d}{2}\), so its rotational inertia is \(I_4 = \frac{1}{12}Md^2 + M(\frac{3d}{2})^2 = \frac{7}{3}Md^2\).
The total rotational inertia of the combination is the sum of the rotational inertias of the two particles and the two rods:
\(I_{total} = I_1 + I_2 + I_3 + I_4 = md^2 + 4md^2 + \frac{1}{3}Md^2 + \frac{7}{3}Md^2 = 5md^2 + \frac{8}{3}Md^2\)
Substituting the given values: \(m = 0.80 \, kg\), \(M = 1.1 \, kg\), \(d = 0.057 \, m\),
\(I_{total} = 5(0.80)(0.057)^2 + \frac{8}{3}(1.1)(0.057)^2 = 0.013 + 0.0095 = 0.0225 \, kg \cdot m^2\)
The rotational kinetic energy is given by \(K = \frac{1}{2}I\omega^2\).
Substituting the values, \(I = 0.0225 \, kg \cdot m^2\) and \(\omega = 0.28 \, rad/s\):
\(K = \frac{1}{2}(0.0225)(0.28)^2 = 0.000882 \, J\)
(a) \\(\boxed{0.0225 \text{ kg} \cdot \text{m}^2}\\)
(b) \\(\boxed{0.000882 \text{ J}}\\)