The formula for acceleration (\( a \)) of an object rolling down an incline is given by:
\(a = \frac{g \sin \theta}{1 + \frac{K^2}{R^2}}\)
Where: - \( g \) is the acceleration due to gravity, - \( \theta \) is the angle of the incline, - \( K \) is the radius of gyration of the object, - \( R \) is the radius of the object.
For a disc, the value of \( \frac{K^2}{R^2} \) is:
\(\frac{K^2}{R^2} = \frac{1}{2} = 0.5\)
For a sphere, the value of \( \frac{K^2}{R^2} \) is:
\(\frac{K^2}{R^2} = \frac{2}{5} = 0.4\)
From the formula for acceleration, we see that the value of \( \frac{K^2}{R^2} \) for the sphere is smaller than for the disc. Therefore, the acceleration of the sphere is greater than the acceleration of the disc:
\(a(\text{sphere}) > a(\text{disc})\)
Since the acceleration of the sphere is greater than the acceleration of the disc, the sphere reaches the bottom of the incline first:
\(\therefore \text{sphere reaches first}\)
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.