A ball of mass m is tied up with string and rotated along a horizontal circle of radius r. At an instant, its velocity is v, and tension in string is T. The force required for circular motion is:
T−mv²/r
T+mv²/r
mv²/r
Zero
Solution:
Let the string make an angle θ to the normal at the point of suspension. The horizontal component of tension provides the necessary centripetal force. Therefore, Tsinθ = mv²/r.