A particle suspended by a thread of length ′l′ is projected horizontally with a velocity √3gl at the lowest point. The height from the bottom at which the tension in the string becomes zero is :
When no external force is acting on the particle then,
ΔK.E.+ΔP.E.=0
Let at heighth the tension in thread becomes zero and the radial force acting at this height is given as and the height at which particle makes angleθis given as
h=l+lcosθ
Fnet=T+mgcosθ
LetvBbe speed of the particle whenT=0,
Fr=mv2Bl
Now on equating above two equations we get
v2B=glcosθ
By using law of conservation we get
12mglcosθ+32mgl−mgl(1+cosθ)=0
cosθ=−13
By substitutingcosθ=1inh=l+lcosθwe get
h=2l3