Step 1: The formula for the radius of gyration \( K \) of a hollow cylinder about its central axis (the long axis of symmetry) is given by: \[ K = \sqrt{\frac{I}{M}} \] where \( I \) is the moment of inertia and \( M \) is the mass of the hollow cylinder.
Step 2: The moment of inertia \( I \) of a hollow cylinder about its central axis is: \[ I = M R^2 \] where \( R \) is the radius of the hollow cylinder.
Step 3: Substitute the expression for \( I \) into the formula for \( K \): \[ K = \sqrt{\frac{M R^2}{M}} = \sqrt{R^2} = R \] Thus, the radius of gyration \( K \) is equal to the radius \( R \) of the hollow cylinder.
For a uniform rectangular sheet shown in the figure, the ratio of moments of inertia about the axes perpendicular to the sheet and passing through \( O \) (the center of mass) and \( O' \) (corner point) is:
For the reaction:
\[ 2A + B \rightarrow 2C + D \]
The following kinetic data were obtained for three different experiments performed at the same temperature:
\[ \begin{array}{|c|c|c|c|} \hline \text{Experiment} & [A]_0 \, (\text{M}) & [B]_0 \, (\text{M}) & \text{Initial rate} \, (\text{M/s}) \\ \hline I & 0.10 & 0.10 & 0.10 \\ II & 0.20 & 0.10 & 0.40 \\ III & 0.20 & 0.20 & 0.40 \\ \hline \end{array} \]
The total order and order in [B] for the reaction are respectively: