2.4 Integration
If we know the position x of t of an object as a function of time, we can use differentiation to calculate its velocity and its acceleration at later times. Essentially, by taking the derivatives of the position, we know everything there is to know about the motion. Sometimes, however, we'll want to go in the other direction. We'll have the acceleration as a function of time and we'll want to find the velocity as a function of time, or the position as a function of time. We'll use a technique called integration, and let's see how that works. To begin with, suppose we have a constant acceleration. So our acceleration a of t is some constant a 0. In that case, we know that this constant acceleration can be written as the change in velocity delta v over some time interval delta t, and therefore that the change in velocity delta v over some time interval delta t can just be written as a 0 acceleration, the constant acceleration, times the elapsed time delt...