The behaviour of a system containing a mass traveling on a cantilever
beam is considered. The mass is induced to move by an applied force as
opposed to the case which has been considered in most literature wher
e the position of the moving mass is assumed to be known and independe
nt of the motion of the beam. Furthermore, the system to be discussed
has the unique characteristic that the motions of the mass and the bea
m are coupled. The mathematical model of the system includes two coupl
ed nonlinear integral/partial differential equations which are impossi
ble to solve analytically and are difficult to solve numerically in th
eir original form. As a remedy, the solution is discretized into space
and time functions and the equations of motion are reduced to a set o
f ordinary differential equations. The shape function is chosen so tha
t it satisfies the boundary conditions of the beam as well as the tran
sient conditions imposed by the traveling mass. This choice of the sha
pe function, which considers the mass-beam interaction, provides an im
provement over the conventional method of using a simple cantilever be
am mode shapes. The ordinary differential equations of motion using th
e 'improved' shaped functions, are solved numerically to obtain the dy
namic behaviour of the system. The results illustrate the validity of
the model, and demonstrate the advantages of the 'improved' model to t
he 'un-improved' equations.