Two different multibody dynamics formulations for the simulation of sy
stems experiencing material and geometric nonlinear deformations while
undergoing gross motion are presented in this paper. In the first, an
updated Lagrangean formulation is used to derive the equilibrium equa
tions of the flexible body while the finite element method is subseque
ntly applied to obtain a numerical description for the equations of mo
tion. The computational efficiency of the formulation is increased by
using a lumped mass description of the flexible body mass matrix and r
eferring the nodal accelerations to the inertial frame. In the resulti
ng equations of motion the flexible body mass matrix is constant and d
iagonal while the full nonlinear deformations and the inertia coupling
description are still preserved. In some cases the flexible component
s present zones of concentrated deformations resulting from local inst
abilities. The remaining structure of the system behaves either as rig
id bodies or as linear elastic bodies. The second formulation presents
a discrete model where all the nonlinear deformations are concentrate
d in the plastic hinges assuming the multibody components are as being
either rigid or flexible with linear elastodynamics. The characterist
ics of the plastic hinges are obtained from numerical or experimental
crush tests of specific structural components. The structural impact o
f a train carbody against a rigid wall and the performance of its end
underframe in a collision situation is studied with the objective of a
ssessing the relative merits of the formulations presented herein. The
results are compared with those obtained by experimental testing of a
full scale train and conclusions on the application of these methodol
ogies to large size models are drawn.