N-Body simulations are a very important tool in the study of formation of
large scale structures. Much of the progress in understanding the physics of
high redshift universe and comparison with observations would not have been
possible without N-Body simulations. Given the importance of this tool, it is
essential to understand its limitations as ignoring the limitations can easily
lead to interesting but unreliable results. In this paper we study the
limitations arising out of the finite size of simulation volume. This finite
size implies that modes larger than the size of the simulation volume are
ignored and a truncated power spectrum is simulated. If the simulation volume
is large enough then the mass in collapsed haloes expected from the full power
spectrum and from the truncated power spectrum should match. We propose a
quantitative measure based on this approach that allows us to compute the
minimum box size for an N-Body simulation. We find that the required box size
for simulations of LCDM model at high redshifts is much larger than is
typically used. We can also use this approach to quantify the effect of
perturbations at large scales for power law models and we find that if we fix
the scale of non-linearity, the required box size becomes very large as the
index becomes small. The appropriate box size computed using this approach is
also an appropriate choice for the transition scale when tools like MAP (Tormen
and Bertschinger, 1996) that add the contribution of the missing power are
used.Comment: 7 pages, 8 figures, Accepted for publication in the MNRA