22.5 Summary of Work and Kinetic Energy
Let's review what we've done this week. We've seen that the work done by a force along a trajectory from point A to point B can be written as the integral of the dot product of that force, with the displacement going from point A to point B, where we note that this integral, in general, must be evaluated over the particular path taken from point A to point B. This is called a line integral or a path integral. And again, I want to emphasize the value of this integral depends, in general, on the path taken from point A to point B. And you could understand that if you considered the fact that, in general, the force is a function of position. And so if you go along different paths, the dot product of the force with a particular path may be different, even though you're going between the same end points. Now, the reason that the work is a useful concept is that it allows us to understand how the kinetic energy of an object-- so the kinetic energy is 1/2mv squar...