Lines will correspond to our usual notion of line.
Distances will be defined using the Minkowski dot
product, so that the distance between events
and
is
. We can then get
the length of a curved line by cutting it into small, approximately
straight segments, and adding the lengths of each segment as found
using this formula.
First, note the qualitative difference in 'timelike' and 'spacelike'
vectors, as indicated by the unit imaginary number i found in timelike
vectors. Also note that distances are linear -- that
. In addition, the 'spheres' of
spacetime - the loci of points a given distance from another - are
hyperbolae in the Euclidean sense.
We can also define the hyperbolic angle between two timelike,
future-pointing vectors, again use the Minkowski dot product. Where
Euclidean angles are defined by
, angles in
spacetime are defined by the analogous formula
,
where * represents the Minkowski product, and the last two norms are the
Minkowski norms.