Systems undergoing first-order phase transitions are accompanied by free en
ergy barriers which separate the free energy minima characterizing the co-e
xisting phases. These barriers grows with increasing system size. With conv
entional Monte Carlo simulation methods the characteristic time for crossin
g the barriers grows exponentially with system size and the system will nec
essarily get trapped in one of the free energy minima. In order to escape f
rom this trapping, various novel simulation schemes (e.g., multicanonical/m
ultimagnetical sampling, entropic sampling and simulated tempering) have be
en proposed and successfully applied to model systems. All these methods co
mbine an iterative scheme with histogram reweighting techniques. We apply h
ere another variant of these methods, which involves the use of shape funct
ions, which are added to the model Hamiltonian in order to level out the fr
ee energy barriers. One of the virtues of this approach is the transparent
formulation of the common philosophy underlying all the different so-called
'non-Boltzmann' simulational schemes devised to overcome free energy barri
ers. The basic principles of the method are presented. The easy adaption of
the method to different model systems is demonstrated by application to tw
o case studies, a multi-state lattice model for phase equilibria in a binar
y lipid bilayer, and a two-dimensional lattice gas model which exhibits int
erfacial melting, which are known to be notoriously difficult to study by c
onventional Monte Carlo methods, The practical aspects of the implementatio
n of the method are discussed, The results demonstrate the efficiency and v
ersatility of the shape function method, (C) 1999 Elsevier Science B.V. All
rights reserved.