00:01
So in this problem we need to start with our free body diagram of the beam.
00:05
And so we have the two masses which are going to cause some weight, effect as a weight acting on the beam.
00:13
M1, which we don't know, and m2, which is 7 kilograms.
00:22
Now there's going to be a force from the fulcrum.
00:25
Now obviously this is going to be upwards because the fulcrum needs to hold the beam up, otherwise the weight would just cause it to fall down forever.
00:32
The whole beam is 15 meters long.
00:41
Now the beam also has a weight of 9 .5 kilograms, so to the force multiplied by the acceleration to gravity g.
00:56
And these are also going to be m1g and m2g to be the forces.
00:59
Now the weight, if this is a uniform beam, we model to act on the center 7 .5 meters from the end.
01:09
Now for the dimensions that we're told, the fulcrum is 5 meters, which means this distance here 2 .5 meters.
01:17
And we're going to need that a bit later.
01:22
And the distances between the two masses are 3 meters and 7 meters to the fulcrum, respectively.
01:36
So let's pick an axis, and i picked my axis to be the fulcrum.
01:40
Pretty convenient place, we can get rid of the unknown end and get our one unknown m1 right away.
01:48
So that is pretty helpful.
01:51
So that is our free body diagram.
01:53
Now we want to look at b to find the mass 1 to hold the beam in equilibrium.
01:59
Well, the mass 1 is going to affect whether the beam rotates.
02:03
So we're going to look at sum of moments equal to 0 to be in equilibrium.
02:08
Counterclockwise positive by convention.
02:11
Now a moment is a force times a distance, and depending on the direction.
02:15
So m1 we see is a positive moment...