Local nonlinear approximations to the growth of cosmic perturbations a
re developed, resulting in relations at a given epoch, between the pec
uliar velocity and gravity fields and their gradients. The continuity
equation and the gravitational field are computed exactly at that epoc
h, and only the equation of motion is approximated. The second-order r
elation is derived for arbitrary geometry and cosmological parameters.
Solutions are developed to fourth order for laminar spherical perturb
ations in an Einstein-de Sitter universe, with exact mass conservation
at all times, but the gain in accuracy for higher orders is modest. A
ll orders become important when the specific peculiar kinetic energy b
ecomes comparable to the peculiar gravitational potential 1/2v(2) simi
lar to phi, typically at relative, density perturbations, delta simila
r to 4. The general second-order relation, while implicit, is simple t
o solve. N-body simulations show that it provides moderate gains in ac
curacy over other local approximations. It can therefore be easily app
lied in the comparison of large-scale structures and velocities in the
quasi-linear regime, delta similar to 1-4, as well as in the reconstr
uction of the primordial perturbations from which they grew.