I am trying to reproduce the simulations from the paper cited in all the LAMMPS DPD documentations: Groot and Warren, J Chem Phys, 107: 4423-4435 (1997). DOI: 10.1063/1.474784.
I am now having troubles simulating the bonded systems (simple polymer melt of a few chains) they describe.
In principle, it is just a simple
bond_style harmonic
bond_coeff * 1.0 0.0
, or alternatively, a
bond_style table linear 20
bond_coeff * linear_bond_coeff_2.table LIN
and some bonds in the initial structure (atom_style hybrid bond edpd
), together with the pair style:
special_bonds lj 1.0 1.0 1.0
special_bonds coul 1.0 1.0 1.0
pair_style dpd 1.0 1.0 ${seed}
pair_coeff * * 25 4.5
The issue is now, that this bond force is very weak. While LAMMPS happily runs this simulation, and I can reproduce e.g. the mean bond length, I am getting problems when I want to investigate results of properties that require the absolute coordinates, such as the radius of gyration or the mean square displacement, as, because of the weak bond force, some bonds reach a length > 0.5 * the box length, in which case the particle is pulled to the next periodic image. A system more than 100 times the size reported by Groot Warren has still sometimes shows this behaviour.
One may argue, that the bond forces should be computed in absolute terms. As I understand it, LAMMPS doesn’t, and behaves the way it does (computing the bond forces in a PBC corrected manner), in order to easily support infinite lattices and networks.
In literature, one can find enough references of people using infinite networks with this weak-bonded DPD potential, leading me to belive that there are “simple” ways to support both.
My question: are there “simple” ways also to introduce support of such weak bond terms into LAMMPS? Or do I have to find a different software package if I want to use such a weak bond potential with such strong pair forces/implement my own?