The work performed by the force \( F = 20 \, N \) is calculated as: \[ W_f = F \cdot d = 20 \times 1 = 20 \, J \] This work represents the change in the wheel's kinetic energy: \[ KE = \frac{1}{2} I \omega^2 \] The moment of inertia \( I \) is determined using \( I = MR^2 \), with \( M = 10 \, \text{kg} \) and \( R = 0.1 \, \text{m} \): \[ I = 10 \times (0.1)^2 = 0.1 \, \text{kg m}^2 \] Equating the work done to the change in kinetic energy allows us to solve for \( \omega \): \[ 20 = \frac{1}{2} \times 0.1 \times \omega^2 \quad \Rightarrow \quad \omega = 20 \, \text{rad/s} \]