00:02
In the first part of this problem, we have to compare the period of the simple pendulum with the length of the pendulum.
00:09
Let's try the expression for the period of the simple pendulum.
00:13
As t is equals to 2 pi square root of l divided by g.
00:18
Here, this l is the length of the pendulum and this g is the gravitational acceleration.
00:28
Since the t is proportional to the square root of l, which is the length of the pendulum, therefore shortening the length will decrease the period and consequently the panellation.
00:37
Pendulum will lose that time by taking the fast vibrations.
00:43
Now let's move to the part b of this problem.
00:46
So in part b, we have to find the difference between the time measured by the two pendulums.
00:54
So we need to calculate this delta t.
01:01
Now let's calculate the period of the unbroken pendulum.
01:06
So for unbroken pendulum, we can wide the period as t1 is equals to 2 pi square root of the length which is equal to 75 multiplied by 10x per minus 2 meter divided by the gravitational acceleration on the surface of earth that is equals to 9 .81 meter per second square so this will give us the value for this t1 as 1 .7 37 seconds now the number of vibrations taken by the by this pendulum in the 24 hours is written as so this is the number of vibrations.
01:56
It should be equal to the time taken by spondelum to complete this number of vibrations divided by the period of this pendulum which is t1.
02:04
So this can be written as 24 hours multiply by 3 ,600 seconds per hour divided by this period which is equal to 1 .737 seconds.
02:19
So from here we can wide the number of vibrations as n is equal to equals to 49 ,741.
02:32
So these are the number of vibrations taken by this pendulum...