We present high-spatial resolution studies of the density field as pre
dicted by Lagrangian perturbation approximations up to the third order
. The first-order approximation is equivalent to the ''Zel'dovich appr
oximation'' for the type of initial data analyzed. The study is perfor
med for two simple models which allow studying of typical features of
the clustering process in the early non-linear regime. We calculate th
e initial perturbation potentials as solutions of Poisson equations al
gebraically, and automate this calculation for a given initial random
density field. The presented models may also be useful for other quest
ions addressed to Lagrangian perturbation solutions and for the compar
ison of different approximation schemes. In an accompanying paper we i
nvestigate a detailed comparison with various N-body integrators using
these models (Karakatsanis et al. 1996). Results of the present paper
include the following: 1. the collapse is accelerated significantly b
y the higher-order corrections confirming previous results by Moutarde
et al. (1991); 2. the spatial structure of the density patterns predi
cted by the ''Zel'dovich approximation'' differs much from those predi
cted by the second- and third-order Lagrangian approximations; 3. seco
nd-order effects amount to internal substructures such as ''second gen
eration'' -pancakes, -filaments and -clusters, as are also observed in
N-body simulations; 4. the third-order effect gives rise to substruct
uring of the secondary mass-shells. The hierarchy of shell-crossing si
ngularities that form features small high-density clumps at the inters
ections of caustics which we interprete as gravitational fragmentation
.