special_bonds keyword values ...
one or more keyword/value pairs may be appended
keyword = amber or charmm or dreiding or fene or lj/coul or lj or coul or angle or dihedral or one/five
amber values = none charmm values = none dreiding values = none fene values = none lj/coul values = w1,w2,w3 w1,w2,w3 = weights (0.0 to 1.0) on pairwise Lennard-Jones and Coulombic interactions lj values = w1,w2,w3 w1,w2,w3 = weights (0.0 to 1.0) on pairwise Lennard-Jones interactions coul values = w1,w2,w3 w1,w2,w3 = weights (0.0 to 1.0) on pairwise Coulombic interactions angle value = yes or no dihedral value = yes or no one/five value = yes or no
special_bonds amber special_bonds charmm special_bonds fene dihedral no special_bonds lj/coul 0.0 0.0 0.5 angle yes dihedral yes special_bonds lj 0.0 0.0 0.5 coul 0.0 0.0 0.0 dihedral yes
Set weighting coefficients for pairwise energy and force contributions between pairs of atoms that are also permanently bonded to each other, either directly or via one or two intermediate bonds. These weighting factors are used by nearly all pair styles in LAMMPS that compute simple pairwise interactions. Permanent bonds between atoms are specified by defining the bond topology in the data file read by the read_data command. Typically a bond_style command is also used to define a bond potential. The rationale for using these weighting factors is that the interaction between a pair of bonded atoms is all (or mostly) specified by the bond, angle, dihedral potentials, and thus the non-bonded Lennard-Jones or Coulombic interaction between the pair of atoms should be excluded (or reduced by a weighting factor).
These weighting factors are NOT used by pair styles that compute many-body interactions, since the “bonds” that result from such interactions are not permanent, but are created and broken dynamically as atom conformations change. Examples of pair styles in this category are EAM, MEAM, Stillinger-Weber, Tersoff, COMB, AIREBO, and ReaxFF. In fact, it generally makes no sense to define permanent bonds between atoms that interact via these potentials, though such bonds may exist elsewhere in your system, e.g. when using the pair_style hybrid command. Thus LAMMPS ignores special_bonds settings when many-body potentials are calculated. Please note, that the existence of explicit bonds for atoms that are described by a many-body potential will alter the neighbor list and thus can render the computation of those interactions invalid, since those pairs are not only used to determine direct pairwise interactions but also neighbors of neighbors and more. The recommended course of action is to remove such bonds, or - if that is not possible - use a special bonds setting of 1.0 1.0 1.0.
Unlike some commands in LAMMPS, you cannot use this command multiple times in an incremental fashion: e.g. to first set the LJ settings and then the Coulombic ones. Each time you use this command it sets all the coefficients to default values and only overrides the one you specify, so you should set all the options you need each time you use it. See more details at the bottom of this page.
The Coulomb factors are applied to any Coulomb (charge interaction) term that the potential calculates. The LJ factors are applied to the remaining terms that the potential calculates, whether they represent LJ interactions or not. The weighting factors are a scaling prefactor on the energy and force between the pair of atoms. A value of 1.0 means include the full interaction; a value of 0.0 means exclude it completely.
The first of the 3 coefficients (LJ or Coulombic) is the weighting factor on 1-2 atom pairs, which are pairs of atoms directly bonded to each other. The second coefficient is the weighting factor on 1-3 atom pairs which are those separated by 2 bonds (e.g. the two H atoms in a water molecule). The third coefficient is the weighting factor on 1-4 atom pairs which are those separated by 3 bonds (e.g. the first and fourth atoms in a dihedral interaction). Thus if the 1-2 coefficient is set to 0.0, then the pairwise interaction is effectively turned off for all pairs of atoms bonded to each other. If it is set to 1.0, then that interaction will be at full strength.
For purposes of computing weighted pairwise interactions, 1-3 and 1-4 interactions are not defined from the list of angles or dihedrals used by the simulation. Rather, they are inferred topologically from the set of bonds specified when the simulation is defined from a data or restart file (see read_data or read_restart commands). Thus the set of 1-2,1-3,1-4 interactions that the weights apply to is the same whether angle and dihedral potentials are computed or not, and remains the same even if bonds are constrained, or turned off, or removed during a simulation.
The two exceptions to this rule are (a) if the angle or dihedral keywords are set to yes (see below), or (b) if the delete_bonds command is used with the special option that re-computes the 1-2,1-3,1-4 topologies after bonds are deleted; see the delete_bonds command for more details.
The amber keyword sets the 3 coefficients to 0.0, 0.0, 0.5 for LJ interactions and to 0.0, 0.0, 0.8333 for Coulombic interactions, which is the default for a commonly used version of the AMBER force field, where the last value is really 5/6. See (Cornell) for a description of the AMBER force field.
The charmm keyword sets the 3 coefficients to 0.0, 0.0, 0.0 for both LJ and Coulombic interactions, which is the default for a commonly used version of the CHARMM force field. Note that in pair styles lj/charmm/coul/charmm and lj/charmm/coul/long the 1-4 coefficients are defined explicitly, and these pairwise contributions are computed as part of the charmm dihedral style - see the pair_coeff and dihedral_style commands for more information. See (MacKerell) for a description of the CHARMM force field.
The dreiding keyword sets the 3 coefficients to 0.0, 0.0, 1.0 for both LJ and Coulombic interactions, which is the default for the Dreiding force field, as discussed in (Mayo).
The fene keyword sets the 3 coefficients to 0.0, 1.0, 1.0 for both LJ and Coulombic interactions, which is consistent with a coarse-grained polymer model with FENE bonds. See (Kremer) for a description of FENE bonds.
The lj/coul, lj, and coul keywords allow the 3 coefficients to be set explicitly. The lj/coul keyword sets both the LJ and Coulombic coefficients to the same 3 values. The lj and coul keywords only set either the LJ or Coulombic coefficients. Use both of them if you wish to set the LJ coefficients to different values than the Coulombic coefficients.
The angle keyword allows the 1-3 weighting factor to be ignored for individual atom pairs if they are not listed as the first and last atoms in any angle defined in the simulation or as 1,3 or 2,4 atoms in any dihedral defined in the simulation. For example, imagine the 1-3 weighting factor is set to 0.5 and you have a linear molecule with 4 atoms and bonds as follows: 1-2-3-4. If your data file defines 1-2-3 as an angle, but does not define 2-3-4 as an angle or 1-2-3-4 as a dihedral, then the pairwise interaction between atoms 1 and 3 will always be weighted by 0.5, but different force fields use different rules for weighting the pairwise interaction between atoms 2 and 4. If the angle keyword is specified as yes, then the pairwise interaction between atoms 2 and 4 will be unaffected (full weighting of 1.0). If the angle keyword is specified as no which is the default, then the 2,4 interaction will also be weighted by 0.5.
The dihedral keyword allows the 1-4 weighting factor to be ignored for individual atom pairs if they are not listed as the first and last atoms in any dihedral defined in the simulation. For example, imagine the 1-4 weighting factor is set to 0.5 and you have a linear molecule with 5 atoms and bonds as follows: 1-2-3-4-5. If your data file defines 1-2-3-4 as a dihedral, but does not define 2-3-4-5 as a dihedral, then the pairwise interaction between atoms 1 and 4 will always be weighted by 0.5, but different force fields use different rules for weighting the pairwise interaction between atoms 2 and 5. If the dihedral keyword is specified as yes, then the pairwise interaction between atoms 2 and 5 will be unaffected (full weighting of 1.0). If the dihedral keyword is specified as no which is the default, then the 2,5 interaction will also be weighted by 0.5.
The one/five keyword enable calculation and storage of a list of 1-5 neighbors in the molecular topology for each atom. It is required by some pair styles, such as pair_style amoeba and pair_style hippo.
LAMMPS stores and maintains a data structure with a list of the first, second, and third neighbors of each atom (within the bond topology of the system). If new bonds are created (or molecules added containing atoms with more special neighbors), the size of this list needs to grow. Note that adding a single bond always adds a new first neighbor but may also induce *many* new second and third neighbors, depending on the molecular topology of your system. Using the extra/special/per/atom keyword to either read_data or create_box reserves empty space in the list for this N additional first, second, or third neighbors to be added. If you do not do this, you may get an error when bonds (or molecules) are added.
If you reuse this command in an input script, you should set all the options you need each time. This command cannot be used a second time incrementally. E.g. these two commands:
special_bonds lj 0.0 1.0 1.0 special_bonds coul 0.0 0.0 1.0
are not the same as
special_bonds lj 0.0 1.0 1.0 coul 0.0 0.0 1.0
In the first case you end up with (after the second command):
LJ: 0.0 0.0 0.0 Coul: 0.0 0.0 1.0
while only in the second case do you get the desired settings of:
LJ: 0.0 1.0 1.0 Coul: 0.0 0.0 1.0
This happens because the LJ (and Coul) settings are reset to their default values before modifying them, each time the special_bonds command is issued.
All 3 Lennard-Jones and 3 Coulombic weighting coefficients = 0.0, angle = no, dihedral = no.
(Cornell) Cornell, Cieplak, Bayly, Gould, Merz, Ferguson, Spellmeyer, Fox, Caldwell, Kollman, JACS 117, 5179-5197 (1995).
(Kremer) Kremer, Grest, J Chem Phys, 92, 5057 (1990).
(MacKerell) MacKerell, Bashford, Bellott, Dunbrack, Evanseck, Field, Fischer, Gao, Guo, Ha, et al, J Phys Chem, 102, 3586 (1998).
(Mayo) Mayo, Olfason, Goddard III, J Phys Chem, 94, 8897-8909 (1990).