The parallel index of refraction is defined as
![]() | (41) |
Here Bj are the contravariant coordinates of B, given by
![]() | (42) |
where
![]() | (43) |
such that the contravariant coordinates of B are
![]() | (44) |
where α is the angle between to
such that
![]() | (45) |
Because is orientated outward we have -π∕2 < α < π∕2. Then (??) yields
![]() | (46) |
where P = and T =
.