discussing a little theory
Consider the figure ...
In this fig. we will find out what should be the velocity of the bob at the lowest position so that the string becomes slack ( i,e, T = 0 ) at the horizontal diameter..
Now the weight acts perpendicular to the tension at this position and so has no component along the string....
So taking v =velocity at that point and T = tension and l = length of string....
we have T = mv2/l..
Now let u = velocity of the bob at lowest position so that the bob acquires velocity = v at the horizontal diameter....
So ... 1/2.mu2 = 1/2mv2 + mgl
or v2 = u2 - 2gl
Using this in equ^n of T.... we have
T = m(u2 - 2gl)/l
If string becomes slack.... T = 0
i,e, m(u2 - 2gl)/l = 0
or u2 - 2gl = 0
or u =
2gl So we see that if velocity at lowest position should be equal to
2gl such that the string becomes slack at the horizontal diameter...
And see HCV-1 page 128 , example 8 where you will find that the velocity at lowest position such that the bob complets a full circle is
5gl .
So we conclude that....
if velocity is less than
2gl, then string becomes slack below the horizontal diameter. if velocity =
2gl, then string becomes slack at horizontal diameter.. if velocity is greater than
2gl but less than
5gl, then string becomes slack in the region between the horizontal diameter and the topmost position....