00:01
In this problem, we have been given that there is a signboard and the weight of the signboard which acts at the center of mass.
00:08
That is given as fg and the width of the signboard is 2l as shown here.
00:17
It hangs from a beam which is light and that's horizontally placed.
00:22
So there is a cable supporting here and we need to determine the tension that's acting on this cable.
00:28
So let's consider the tension t and we can take the component of this tension, so it will be t sine theta and t cost theta respectively.
00:39
So in order to figure out the tension, we consider the moment about this point, let's say o.
00:45
So the net clockwise moment that will be because of the weight, so that's fg into its perpendicular distance from this point o.
00:54
That's d plus l.
00:55
And this is equal to the total anti -clockwise moment that's because of the perpendicular component of the tension.
01:04
So that will be t -sign theta into its perpendicular distance.
01:08
So that will be d plus 2l.
01:10
So from here we can solve and get the value of the tension that will be fg into d plus l divided by sine theta into d plus 2l.
01:22
And that's the value of this tension force.
01:26
In the next case, we have to figure out the components of the reaction force that's exerted by the wall.
01:33
So let's consider the force fx and fxy that's acting at this point.
01:42
So in this case, if we apply the idea that the total force in the x and y directions are balanced, because the complete system is given to be in equilibrium here...