00:01
Okay, so a car was moving at 66 feet per second, and we increased the speed to 88 feet per second over a distance of 440 feet.
00:18
Okay, and we're asking, we're saying constant acceleration.
00:23
So acceleration equals some constant.
00:29
Of velocity would then be an integral of that, right? because acceleration is the derivative of velocity.
00:41
So velocity is linear with respect to time.
00:48
And then displacement, velocity is the derivative of displacement, is then c over 2 t squared plus some other constant d.
01:03
Okay.
01:04
So what do we know? we know that v of 0 is 66.
01:11
So, oh, sorry, this should be plus d.
01:17
And then, okay, let's not take, let's not find displacement yet.
01:22
V of 0 is 66.
01:24
So that means d is 66.
01:28
So, okay, v of t is ct plus 66.
01:36
Okay, now d of t is c.
01:40
Over to t squared plus 66 t plus some new constant e okay and now we know that d of zero we're just going to call that zero so that means e equals zero if we put in zero over here and um okay and there's some time t we'll call it uh t equals a here then we know that v of a is 88 and d of a and d of a is 440.
02:18
Okay, v of a is 88 gives us that ca plus 66 is 88.
02:24
And d of a is 440 gives us that c over 2a squared plus 66a and e is zero is 440.
02:38
Okay, so now we have two equations and two variables.
02:43
So this should be enough to solve for both big c and a...