We are given the following: - Mass of the solid sphere \( M = 20 \, \text{kg} \), - Diameter of the sphere \( D = 20 \, \text{cm} = 0.2 \, \text{m} \), - The moment of inertia is to be calculated about the tangent to the sphere. The moment of inertia \( I_{\text{sphere}} \) of a solid sphere about its center of mass is given by the formula: \[ I_{\text{sphere}} = \frac{2}{5} M R^2, \] where \( M \) is the mass and \( R \) is the radius of the sphere.
Step 1: Moment of inertia about the center For a sphere with mass \( M = 20 \, \text{kg} \) and radius \( R = \frac{D}{2} = \frac{0.2}{2} = 0.1 \, \text{m} \), the moment of inertia about the center is: \[ I_{\text{center}} = \frac{2}{5} \times 20 \times (0.1)^2 = \frac{2}{5} \times 20 \times 0.01 = 0.08 \, \text{kgm}^2. \]
Step 2: Using the parallel axis theorem To find the moment of inertia about a tangent to the sphere, we use the parallel axis theorem: \[ I_{\text{tangent}} = I_{\text{center}} + M R^2. \] Substituting the values: \[ I_{\text{tangent}} = 0.08 + 20 \times (0.1)^2 = 0.08 + 20 \times 0.01 = 0.08 + 0.2 = 0.28 \, \text{kgm}^2. \] Thus, the moment of inertia about the tangent to the sphere is \( 0.28 \, \text{kgm}^2 \).
Therefore, the correct answer is option (3).
A tube of length 1m is filled completely with an ideal liquid of mass 2M, and closed at both ends. The tube is rotated uniformly in horizontal plane about one of its ends. If the force exerted by the liquid at the other end is \( F \) and the angular velocity of the tube is \( \omega \), then the value of \( \alpha \) is ______ in SI units.
A force of 49 N acts tangentially at the highest point of a sphere (solid) of mass 20 kg, kept on a rough horizontal plane. If the sphere rolls without slipping, then the acceleration of the center of the sphere is