A simple pendulum of time period 1s and length l is hung from a fixed support at O, such that the bob is at a distance H vertically above A on the ground (Fig. 14.11). The amplitude is θ0. The string snaps at θ = θ0 /2. Find the time taken by the bob to hit the ground. Also find distance from A where bob hits the ground. Assume θ0 to be small so that sine and cosine is equal to 1.

The angular displacement for the pendulum is given as,
----(1)
Where
is angular displacement at the given time t and
is the maximum angular displacement of the pendulum, and
is the angular frequency and t is the time t.
Given:
Time period T of oscillation is = 1s
Length of the pendulum is = ![]()
∴ ![]()
At
, ![]()
and,
at
the string snaps,
putting the above in equation (1)
![]()
![]()
![]()
![]()
now since pendulum moves in the circular motion it must have angular velocity. For that, we differentiate eq. (1)
![]()
But ![]()
∴ ![]()
At t=1/6 s
------(2)
But we have a following relation between angular and linear velocity,
, where v is the linear velocity and r is radius and in this case r is the length of the string of the pendulum
∴ ![]()
Putting the above in equation (2)
We get,
------(3)
∴ the linear velocity at t=1/6 s is given as above.
Now at this stage the string snaps and bob starts a parabolic motion with the above calculated velocity in the tangential direction, thus we need to resolve it into x and y axis component.
Let us look at the vertical component,
Let the bob be at a height
from the ground
Velocity along vertical axis,
![]()
Now using 2nd equation of motion, as the bob falls by H0 distance,
![]()
![]()
![]()
Now solving for t in the above quadratic equation we get,


Now neglecting the term containing
, we get,

This is the same time period for which the bob travels along the x-axis after snapping takes place.
And there is no acceleration in the x-axis we can use following equation,
------(4)
Where s is the distance travelled along the x-axis and using equation (3) we can write,
(given
)
![]()
∴ putting it in equation (4)

And
![]()
Since we are given that we can take
=1
We get,
![]()
∴ ![]()
Now the horizontal distance from the point A at the time it snaps is,
(since
is very)
∴ the distance at which it falls from the point A should be as follows,

The above is the final answer.
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