00:01
Okay, so definitely the best thing to do here is to start with a force diagram and to kind of picture what's happening here.
00:06
So if i have this little hill, it's actually a pretty gentle slope.
00:14
Okay, so this is 3 .2 degrees.
00:19
Okay, and i'm going to imagine a little truck on it or car or whatever vehicle they say that it is.
00:30
So what we're thinking is what are the forces on it, right? so first i have the force of its weight.
00:39
Well, actually, let me back up.
00:41
I have, yes, i have the force of its weight towards the center of the earth.
00:46
I also have the force, but basically the component of that weight that's actually going to want to move us down the hill, make it roll down the hill, which is m .g.
00:57
Sign of 3 .2.
01:00
I also have the force of dragon.
01:05
Force of drag.
01:08
Pushing us forward, i have the force from the actual motor itself.
01:15
So i also want it to move at a constant velocity, which, if you recall, means that there's zero net force.
01:22
So that means that for my equations, i want net force equals zero, which will also equal the force of the motor.
01:31
Assuming, by the way, assuming we consider up the slope positive direction, down the slope negative direction.
01:38
That's kind of help right here.
01:39
So it's a positive force going up the slope due to the motor.
01:42
A negative force of drag pulling us back, or rather pushing us back, and a negative force of gravity pulling us down the hill, which stated is 3 .2.
02:00
Okay, so i also want to know, i'm going to mention it now, that power equals work over time, okay, which remember that work is change in energy, but assuming we're starting from rest, that's basically just energy, right? another way we can think of this is force times distance.
02:26
Do not confuse this with this, right? this is force subdistance.
02:30
F subd, meaning the force to the direct, but this is force times the actual distance i've traveled over time.
02:38
And i'm also going to go a little bit further.
02:40
We know that because we're moving at a constant velocity, the distance is just velocity times time.
02:47
So really, this is just velocity times time over time.
02:52
So in this particular situation, because velocity is constant, power is just force times velocity, which makes things way easier.
03:01
So, okay, let's see here.
03:04
What are we going to do? so i have this equation right here.
03:08
I'm going to solve for the force of the motor.
03:11
The force of the motor is the force to drag plus m .g sine of 3 .2.
03:27
So this is my force, right? so i know if i just multiply by my velocity, i'm going to have power, right? so i can say force times velocity equals power, right, which is equal to this whole thing times velocity.
03:43
So i'm going to have force 2 to drag plus mg sign of 3 .2 times the velocity.
03:55
Okay...