Suppose we have a line with vector equation r = r0 + td. If t represents time, measured in some appropriate units (seconds, say), then for each value of t, the point with position vector r is at a new position, i.e. it moves along the line. It's always moving parallel to the direction vector, and we can ask: how fast is it moving?
Between any time t and time t+1, it moves from position r0 +
td to
r0 +
(t+1)d. Its displacement during this time is
thus
{r0 + (t+1)d} - {r0 + td} = d.
It covers this displacement in a time (t + 1) - t = 1 time unit. We thus have a displacement of size/direction d for every unit of time, i.e. the velocity of the point is d.
To summarize: if r = r0 + td describes the position at time t of a point moving along a line, then the direction vector d may be interpreted as the velocity vector of the point.
Using Vectors to Describe Lines | |||||
Introduction | The vector form of a line | The parametric form of a line | The symmetric form of a line | Finding lines | Uniform linear motion |