Let's analyze the motion of both beads, P and Q, on the semi-circular and straight paths respectively.
1. Bead P on the semi-circular path:
As bead P slides down the semi-circular string without friction, it undergoes circular motion under the force of gravity.
The path of P is a semi-circle with radius \( R \). The length of the path is \( \pi R / 2 \).
The acceleration of bead P is due to the gravitational component along the arc, \( g \sin \theta \), and the time taken is given by: \(t_P = \frac{\pi R}{2v_P}\), where \( v_P \) is the average velocity.
2. Bead Q on the straight path:
Bead Q is ejected horizontally at 45° with initial speed. Therefore, bead Q follows a projectile motion.
The time, \( t_Q \), for bead Q to reach point A is determined by the straight-line distance and the horizontal component of its initial velocity.
Comparison of \( t_P \) and \( t_Q \):
The path travelled by P is longer than that of Q due to semi-circular motion versus straight-line travel.
The horizontal component of Q’s velocity is greater than the average velocity of P along the arc due to lack of any component counteracting this motion.
Conclusion:
Considering both the path length and velocity components, \(t_P \lt t_Q\) holds true.