To determine the velocity ratio of two particles with identical mass under constant centripetal force, utilize the centripetal force formula: \(F_c = \frac{mv^2}{r}\). Here, \(m\) denotes particle mass, \(v\) signifies particle velocity, and \(r\) represents the radius of curvature.
Given that the masses are equal and the centripetal force is constant, we can equate the expressions for both particles and derive their ratio:
\(\frac{mv_1^2}{r_1} = \frac{mv_2^2}{r_2}\).
This simplifies to:
\(\frac{v_1^2}{r_1} = \frac{v_2^2}{r_2}\).
Rearranging to establish the relationship between their velocities and radii yields:
\(v_1^2 \cdot r_2 = v_2^2 \cdot r_1\).
With the radii given in the ratio \(r_1 : r_2 = 3:4\), substitution results in:
\(v_1^2 \cdot 4 = v_2^2 \cdot 3\).
Solving for the velocity ratio \(\frac{v_1}{v_2}\):
\(\frac{v_1^2}{v_2^2} = \frac{3}{4}\).
Taking the square root of both sides provides the final velocity ratio:
\(\frac{v_1}{v_2} = \frac{\sqrt{3}}{2}\).
Therefore, the velocities are in the ratio \(\sqrt{3} : 2\).

A body of mass $100 \;g$ is moving in a circular path of radius $2\; m$ on a vertical plane as shown in the figure. The velocity of the body at point A is $10 m/s.$ The ratio of its kinetic energies at point B and C is: (Take acceleration due to gravity as $10 m/s^2$)

A sportsman runs around a circular track of radius $ r $ such that he traverses the path ABAB. The distance travelled and displacement, respectively, are:
