00:01
And this problem, they give us a chart here that i have reproduced.
00:09
And they give us a bunch of speeds.
00:11
So in increments of 20, they tell us how the kilometers per hour, the distance of 20, 40, 60, 80, and 100 kilometers per hour.
00:21
And then they tell us this first row here is the distance that we go before we would hit hit the break.
00:31
So basically it's our reaction time distance.
00:33
So we see something we want to stop.
00:37
And so there's some reaction time before we start the actual break, actually break.
00:42
And then once we start to actually break, we then slow down.
00:46
So what this shows is if we, if we plot this, you can see this is very linear.
00:53
And that's just because our reaction time is pretty much the same, no matter what speed we're going.
00:58
So the distance we travel, increases linearly with the speed.
01:07
So if we plot that, we get very close to a line.
01:12
And if we fit that line, as they said, s is due, we get 0 .417 times the velocity minus 0 .02.
01:23
So this is very close to 0.
01:25
We would expect that, you know, if v was zero, then this should probably be 0.
01:30
But it was this little small offset because of the, you know, just kind of the noise and the data.
01:37
You might set that to zero for just based on, you know, that the reaction time distance should be zero when the speed is zero.
01:48
And so then the braking, so this is the distance that we travel after we start breaking.
01:56
And if we plot this, it looks very quadratic.
01:59
And that's basic because you're dissipating energy and the energy increase.
02:03
With the velocity squared.
02:06
So to get rid of all the energy, you would expect to have a quadratic function so that this is going to grow quadratically with v squared.
02:14
And indeed it does.
02:16
And so we plot this, and we make a quadratic fit, quadratic model, and we get 0 .00557 v squared plus 0 .00143v plus 0 .043v and again it makes it.
02:34
For physical reasons, you might say this should be zero, because if v is zero, then we would expect this to be zero.
02:44
But again, we can, whether you keep this or not, it's a very minor offset when you're talking about these other terms and as far as their magnitude goes.
02:58
So the total distance then is just the sum of these two.
03:05
So we just add them up.
03:07
We get this quadratic term.
03:09
This is pretty much dominates the linear term compared to that.
03:15
And then we get these, you know, this offset here.
03:18
And again, we could maybe say that was zero for, just for physical reasons that if you're not traveling any, if you're not moving, then your stopping distance should be zero.
03:29
But again, this is very small compared to these when you plug in, you know, these respective values here...