This data was created in 2017 by Michael P. Allen [email protected]/[email protected] and Dominic J. Tildesley [email protected] ("the authors"), to accompany the book Computer Simulation of Liquids, second edition, 2017 ("the text"), published by Oxford University Press ("the publishers").
Creative Commons CC0 Public Domain Dedication. To the extent possible under law, the authors have dedicated all copyright and related and neighboring rights to this data to the PUBLIC domain worldwide. This data is distributed without any warranty. You should have received a copy of the CC0 Public Domain Dedication along with this data. If not, see http://creativecommons.org/publicdomain/zero/1.0/.
The authors and publishers make no warranties about the data, and disclaim liability for all uses of the data, to the fullest extent permitted by applicable law. The authors and publishers do not recommend use of this data for any purpose. It is made freely available, solely to clarify points made in the text. When using or citing the data, you should not imply endorsement by the authors or publishers.
Here we provide data suitable to test the programs pair_distribution.f90
and pair_distribution.py
,
which are available in the Examples repository.
The file pair_distribution_data.zip
contains
a set of 500 configurations
of N=256 Lennard-Jones atoms,
cut (but not shifted) at Rc=2.5σ,
at the usual state point ρ=0.75, T=1.0.
The interval between configurations was 100 MC sweeps.
For more details about the programs,
and a plot of the results from this data set,
refer to the Fortran GUIDE
or the Python GUIDE.
Here we provide data suitable to test the program grint.f90
,
which is available in the Examples repository.
The file grint_data.zip
contains
a set of 100 configurations from a simulation of
a system of N=10000 atoms, interacting through
the Lennard-Jones potential cut (but not shifted) at Rc=2.5σ,
in a cubic box of side 30σ, at a temperature T=0.90.
For this system, ρG ≈ 0.024, ρL ≈ 0.713.
Output files from grint.f90
with default parameters are also provided.
The slices for z>0 (z1 in the liquid) and
c<0 (z2 further in the liquid) most resemble homogeneous liquid
pair distribution functions. Those with z<0, c>0, where both particles are
on the gas side, are the most noisy and show least structure.
For more details about the program,
refer to the Fortran GUIDE.