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 \( \omega \): \[ 20 = \frac{1}{2} \times 0.1 \times \omega^2 \quad \Rightarrow \quad \omega = 20 \, \text{rad/s} \]
Two point charges 2q and q are placed at vertex A and centre of face CDEF of the cube as shown in figure. The electric flux passing through the cube is : 
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).
