  We study the Lie symmetries of non-relativistic and relativistic higher order
constant motions, in $d$ spatial dimensions, like constant acceleration,
constant rate-of-change -of-acceleration (constant jerk), and so on. In the
non-relativistic case, these symmetries contain the $z=\frac 2N$ Galilean
conformal transformations, where $N$ is the order of the differential equation
that defines the constant motion. The dimension of this group grows with $N$.
  In the relativistic case the vanishing of the ($d+1$)-dimensional space-time
relativistic acceleration, jerk, snap, ... , is equivalent, in each case, to
the vanishing of a $d$-dimensional spatial vector. These vectors are the
$d$-dimensional non-relativistic ones plus additional terms that guarantee the
relativistic transformation properties of the corresponding $d+1$ dimensional
vectors. In the case of acceleration there are no corrections, which implies
that the Lie symmetries of zero acceleration motions are the same in the
non-relativistic and relativistic cases. The number of Lie symmetries that are
obtained in the relativistic case does not increase from the four-derivative
order (zero relativistic snap) onwards. We also deduce a recurrence relation
for the spatial vectors that in the relativistic case characterize the constant
motions.
