00:01
In this problem we have been given that there is a mass which is hung with the help of light inextensible string here.
00:09
And this block is having mass of 0 .5 kilograms.
00:14
And it is given that it is executing simple harmonic motion whose displacement is given as x equals to a times cos omega -t.
00:27
And in this oscillation, it is found that the mass completes 20 cycles in 80 seconds.
00:37
So 20 cycles is completed in 80 seconds.
00:41
That's what we have been given here.
00:43
So we need to determine first the time period.
00:50
So here we can observe and get the frequency.
00:54
So 20 cycle is completed in 80 seconds.
00:57
That means one cycle will be completed in 80 by 20 seconds.
01:04
So that would be four seconds.
01:07
So here the frequency comes out to be 1 by 4 hertz.
01:13
And using this frequency, we can get the time period by reciprocating this frequency.
01:19
So that comes out to be 4 seconds.
01:21
Now that's the time period of oscillation of this block.
01:25
And now we need to figure out the angular frequency.
01:29
So from the frequency that we have computed in part one, we can figure out the angular frequency omega by using 2 pi f.
01:37
So we multiply 2 pi with the frequency 1 by 4.
01:41
So that comes out to be 2 pi radiance per second.
01:45
So when we simplify, we get this as 6 .28 radiance per second.
01:51
Now this is the angular frequency of this mass.
01:58
And next we need to figure out.
02:00
The spring constant.
02:03
So in order to get the spring constant, we use the idea that k is equal to or k by m is equal to omega square.
02:15
So from here we can rearrange and get the spring constant by one multiplying mass with omega square.
02:22
So we take the mass that's 0 .5 and take the square of omega that we just now figured out...