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:
\(\therefore \text{sphere reaches first}\)
In a Vernier caliper, \(N+1\) divisions of vernier scale coincide with \(N\) divisions of main scale. If 1 MSD represents 0.1 mm, the vernier constant (in cm) is: