A bob of mass m is suspended from point O by a massless string of length l as shown. At the bottommost point it is given a velocity u=√12gl for l=1m and m=1kg, match the following two columns when string becomes horizontal (g=10ms−2)
Given : u=√12gl m=1kg l=1 m g=10m/s2
Let the velocity of the bob be v when the string becomes horizontal.
Using work-energy theorem : W=ΔK.E
∴ −mgl=12mv2−12mu2
OR −2gl=v2−(12gl) ⟹v=√10gl
∴ v=√10×10×1=10 m/s
Radial acceleration, ar=v2l=1021=100 m/s2
Tension in the string, T=mar=1×100=100 N
Tangential acceleration, at=mg=1×10=10 N
∴ Total acceleration, a=√a2r+a2t=√(100)2+(10)2=10√101=100.5 m/s2