The problem involves understanding the concept of the radius of gyration for different axes of a uniform disc. The radius of gyration \( k \) is defined as \( k = \sqrt{\frac{I}{m}} \), where \( I \) is the moment of inertia and \( m \) is the mass of the object.
For a thin uniform disc of radius \( R \), the moment of inertia \( I \) about an axis through its center and perpendicular to its plane is \( I_c = \frac{1}{2}mR^2 \). Hence, the radius of gyration \( k_c \) about this axis is:
\( k_c = \sqrt{\frac{\frac{1}{2}mR^2}{m}} = \sqrt{\frac{1}{2}}R \)
The moment of inertia \( I_d \) about the diameter of the disc is \( I_d = \frac{1}{4}mR^2 \). Therefore, the radius of gyration \( k_d \) about the diameter is:
\( k_d = \sqrt{\frac{\frac{1}{4}mR^2}{m}} = \frac{R}{2} \)
Thus, the ratio of the radius of gyration about the center perpendicular axis to that about the diameter is given by:
\( \frac{k_c}{k_d} = \frac{\sqrt{\frac{1}{2}}R}{\frac{R}{2}} = \sqrt{2} \)
The correct ratio is therefore \( \sqrt{2}:1 \).
A cylindrical tube \(AB\) of length \(l\), closed at both ends, contains an ideal gas of \(1\) mol having molecular weight \(M\). The tube is rotated in a horizontal plane with constant angular velocity \(\omega\) about an axis perpendicular to \(AB\) and passing through the edge at end \(A\), as shown in the figure. If \(P_A\) and \(P_B\) are the pressures at \(A\) and \(B\) respectively, then (consider the temperature to be same at all points in the tube) 
As shown in the figure, radius of gyration about the axis shown in \(\sqrt{n}\) cm for a solid sphere. Find 'n'. 
When rod becomes horizontal find its angular velocity. It is pivoted at point A as shown. 
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The output (Y) of the given logic implementation is similar to the output of an/a …………. gate.