Now let's turn our attention to the meaning of a definite integral of a vector-valued function. The context in which this will make the most sense is where the function we integrate is a velocity function. That is,
∫ba⇀v(t)dt
We know that the antiderivative of velocity is position and that this definite integral gives us the change in position over the time interval, a≤t≤b. In other words,
∫ba⇀v(t)dt=⇀r(b)−⇀r(a)
Thus, the definite integral of velocity over a time interval a≤t≤b gives us the displacement vector that indicates the change in position over this time interval.
In general, the definite integral
∫ba⇀r(t)dt=⇀q(b)−⇀q(a), where ⇀q(t) is the antiderivative of ⇀r(t),
gives us a change in the antiderivative of our vector-valued function over the given inteval [a,b]. This will always be a constant vector that would fit from tip to tip of the vectors given by the antiderivative function at t=a and t=b, respectively (assuming the vectors were placed in standard position).