00:01
Here in this given problem these are the 2 digit supports horizontal ceiling and vertical wall.
00:09
Then the 2 strings this is the string c b and another string a b and the ball attached with the string third string having a mass m.
00:30
So, its weight mg will be acting vertically down.
00:34
This point that is b here this is a this point is c and if we draw a horizontal line passing through this b this angle theta 1 and that angle here this is theta 2.
00:53
Suppose tension in this string b c that is t b c and here in this string a b suppose this is t a b.
01:06
Now the values given here theta 1 is 60 degree, theta 2 that is 20 degree, mass of this ball that is 2 .0 kilogram.
01:21
So, these tensions may be resolved into 2 components for t b c that is having that will be having its horizontal component as t b c cos theta 1 and its vertical component t b c sin theta 1.
01:41
Then horizontal component of t a b that is t a b cos theta 2 and vertical component t a b sin theta 2.
01:56
So, in the first part of the problem where we have to find the tension in the string a b means t a b we have to find.
02:05
First of all as the system is in equilibrium.
02:08
So, there should be no net force along x axis summation of f x that should be equal to 0...