Definition. Let L be an oriented line and let u be the unit vector that defines the
orientation of L. Let p and q be two points on L. The oriented or signed distance from
p to q, denoted by ||pq||, is defined by
It is easy to check that if p π q, then ||pq|| is just the ordinary (unsigned) distance
|pq| if the vector pq induces the same orientation on L as u and -|pq| otherwise
(Exercise 1.6.6).
The angle between two vectors as defined in Section 1.3 is always a nonnegative
quantity, but sometimes it is convenient to talk about a signed angle, where the sign
of the angle is determined by the direction (counterclockwise or clockwise) that the
angle “sweeps” out.
Definition. Let u and v be two linearly independent vectors in the plane R
2
. If q is
the angle between u and v, define –
s
(u,v), the signed angle between u and v, by
This finishes our discussion of the local theory of orientation. We shall return to
the subject of orientation in Chapters 6 and 8 and define what is meant by an orien-
tation at a point of a “curved” space. We shall also consider global aspects of orien-
tation and what it might mean to say that an entire space is oriented. However, in
order not to leave the reader in a kind of limbo with respect to how the definitions of
this section fit into the whole picture, it is useful to give a brief sketch of what is to
come. Surfaces will serve as a good example.
Suppose that S is a smooth surface. What we mean by that is that S has a nice
tangent plane T
p
at every point p that varies continuously as we move from point to
point. Let us call the point where the tangent plane touches the surface its “origin.”
Since every tangent plane T
p
is a two-dimensional vector space, we already know what
it would mean to have an orientation s
p
for each T
p
separately. The family of orien-
tations O = {s
p
} is called an orientation for S if the orientations s
p
vary continuously
from point to point. To explain what is meant by the notion of a continuously varying
orientation, note that there is a well-defined one-to-one projection p
p
of a neighbor-
hood of the origin in T
p
onto a neighborhood of p in the surface. Figure 1.14 shows
otherwise.