00:01
In this example, we're going to be working with vector addition, and we're also going to be looking at the relationship between forces and acceleration.
00:07
Okay, so we have three different graphs.
00:09
We have three cases.
00:13
In each case, there are three forces acting on an object.
00:17
Our object will have a constant mass for all three cases, m equals 1 kilogram.
00:24
Okay, so we have three forces acting on this object that give it an acceleration.
00:30
We are shown a graph that has two of those forces drawn in.
00:34
What we wanna do is use the information about the acceleration and the two forces that we have drawn to draw in the third force vector.
00:43
Okay, so here's the first one, and hopefully this will clear things up a little bit.
00:47
I know it's kind of hard to explain.
00:49
So we have this coordinate grid where we have x and y, both of these axes are labeled in newtons.
00:58
Okay, and we have a force, force 1.
01:04
Okay, so this is my force vector 1, f1, and this goes to the point 2, 1.
01:14
Okay, then we have force 2, and this goes to the point, this will be f2.
01:23
This point is negative 2, 2.
01:28
Okay, then we have a third force, f3.
01:31
We don't know where that is yet, but we know for these three forces, the acceleration of my object a equals 2 meters per second squared, and that's in the positive x direction.
01:45
Okay, so i have to sum up all of my forces, my three forces, to give me a total.
01:53
So we're gonna have f1 plus f2 plus f3 has to equal 2 newtons.
02:04
In the positive x direction, all right, we know that our mass is just 1 kilogram, so 2 newtons divided by 1 kilogram is 2 meters per second squared.
02:15
Okay, so what is this third force vector that we need to find? well, let's look at force 2 plus force 1.
02:23
We see the x components are gonna cancel out.
02:27
We're gonna be left with a y component of 3 newtons, so we need to get rid of that.
02:35
So in the negative direction, we need our new force, force 3 needs to go down to negative 3.
02:43
And in the y direction, or sorry, the x direction, we have 0, we want 2.
02:48
So it's gonna be 2, 3.
02:51
Our third force vector, force 3, will look like positive 2, negative 3.
02:58
So this is positive 2.
03:00
Our third force vector is gonna look something like this.
03:03
Force 3, and that goes to positive 2, negative 3.
03:07
Okay, so we're gonna do the exact same thing for the second case...