We draw attention to a novel type of geometric gauge invariance relati
ng the autoparallel equations of motion in different Riemann-Cartan sp
acetimes with each other. The novelty lies in the fact that the equati
ons of motion are invariant even though the actions are not. As an app
lication we use this gauge transformation to map the action of a spinl
ess point particle in a Riemann-Cartan spacetime with a gradient torsi
on to a purely Riemann spacetime, in which the initial torsion appears
as a nongeometric external field. By extremizing the transformed acti
on in the usual way, we obtain the same autoparallel equations of moti
on as those derived in the initial space time with torsion via a recen
tly-discovered variational principle.