A particle has two velocities of equal magnitude inclined to each other at an angle θ. If one of them is halved, the angle between the other and the original resultant velocity is bisected by the new resultant. Then θ is:
Solutions · 1
Official solution
Let both velocities have magnitude u. The original resultant R=2ucos2θ bisects the angle θ between them, so it makes angle 2θ with each. Halving one velocity and applying the angle bisector condition (via the angle bisector theorem in the relevant triangle) gives R′=u, and:
\[2u\cos\frac\theta2 = u \implies \cos\frac\theta2=\frac12=\cos60^{\circ} \implies \theta=120^{\circ}\]