A particle of mass m attached to a string of length l is describing circular motion on a smooth plane inclined at an angle α with the horizontal. For the particle to reach the highest point its velocity at the lowest point should exceed :
Here, h=2l sin ∝
A is the lowest point and B the highest point. At B, in critical case tension is zero. Let velocity of particle at B at this instant be vB. Then
mg sinα=mv2Blor v2B=gl sinαNow v2A=v2B+2gh=(gl sinα)+2g(2l sinα)∴ vA=√5gl sinα