00:01
We know that the jerk j is defined as the rate of change of acceleration, d -a -d -t, and that's given to be constant.
00:14
So we can rewrite this, we separate it as d -a is equal to j -d -t.
00:24
And if we integrate both sides, we get that the acceleration a is equal to j times the integral of d -t.
00:32
And solving this integral we get that the acceleration a is equal to j times t plus a constant of integration c1 but we know at time t is equal to zero the acceleration is equal to a naught or a i our initial acceleration and therefore we can write acceleration a as the jerk times of time plus initial acceleration a i and hence we have an expression for the acceleration.
01:09
Now we can write the acceleration going one level deeper as dvd the rate of change of velocity.
01:18
And again we can separate this.
01:21
So a d t is equal to dv.
01:27
And this implies that velocity v, if we integrate both sides, is equal to the integral of a d t.
01:37
And here we'll substitute our expression for the acceleration that's the integral of j t plus a i d t and if we solve this integral we get that to be a half j t squared plus a i times t plus some constant of integration c2 but again we know that at t is equal to zero the velocity is simply the initial velocity, v .i.
02:15
So we can write this as a half j t squared plus a i times t plus initial velocity v...