If a body moves from to , then from to , it has moved from to ! We define addition of vectors (represented as line segments) in this way: .
Now let be the points with position vectors a, b. The point with position vector is found as follows. Let be parallel to , with the same length, so that is a parallelogram. Then is the required point, since
Let and . When we move along line segments corresponding to and , we add , then to the first coordinate. By doing both, we add . So in component form, the obvious formula applies:
Clearly, .
We write (of course) for . If have position vectors , then , since , in other words .