We show that the stationary quantum Hamilton-Jacobi equation of nonrel
ativistic 1D systems, underlying Bohmian mechanics, takes the classica
l form with partial derivative(q) replaced by partial derivative((q) o
ver cap) where d (q) over cap = dq/root 1-beta(2). The beta(2) term es
sentially coincides with the quantum potential that, like V - E, turns
out to be proportional to a curvature arising in projective geometry.
In agreement with the recently formulated equivalence principle, thes
e ''quantum transformations'' indicate that the classical and quantum
potentials deform space geometry. (C) 1998 Elsevier Science B.V.