
The radius of gyration \( k \) of the plate about an axis perpendicular to the plane is given by: \[ k = \sqrt{\frac{I_x + I_y}{m}} \] Where:
\( I_x = 0.2 \, \text{kg} \, \text{m}^2 \) is the moment of inertia about the x-axis,
\( I_y = 0.3 \, \text{kg} \, \text{m}^2 \) is the moment of inertia about the y-axis,
\( m = 2 \, \text{kg} \) is the mass of the plate. Substituting the values: \[ k = \sqrt{\frac{0.2 + 0.3}{2}} = \sqrt{\frac{0.5}{2}} = \sqrt{0.25} = 0.5 \, \text{m} = 50 \, \text{cm} \]
The correct answer is (A) : 50 cm.
The radius of gyration \( k \) about an axis is related to the moment of inertia \( I \) by the formula: \[ I = m k^2 \] where \( m \) is the mass of the object, and \( k \) is the radius of gyration about the axis. For the axis passing through the point O and perpendicular to the plane of the plate, the total moment of inertia \( I_z \) can be found using the parallel axis theorem: \[ I_z = I_x + I_y \] Given: - \( I_x = 0.2 \, \text{kg} \, \text{m}^2 \), - \( I_y = 0.3 \, \text{kg} \, \text{m}^2 \), - \( m = 2 \, \text{kg} \). The total moment of inertia is: \[ I_z = 0.2 + 0.3 = 0.5 \, \text{kg} \, \text{m}^2 \] Now, using the formula \( I_z = m k^2 \), we can solve for \( k \): \[ k^2 = \frac{I_z}{m} = \frac{0.5}{2} = 0.25 \] \[ k = \sqrt{0.25} = 0.5 \, \text{m} = 50 \, \text{cm} \] Thus, the radius of gyration is 50 cm.
Therefore, the correct answer is (A).
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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.
In a practical examination, the following pedigree chart was given as a spotter for identification. The students identify the given pedigree chart as 