The ESFF Forcefield
Contents
While the CVFF and CFF91 forcefields derive the forcefield
parameters by fitting ab initio and/or experimental data sets, ESFF
relies on atomic parameters coupled with rules for generating explicit
parameters. The rules embody physical reality and therefore tend to
break the redundancies and guarantee transferability. As much as
possible, the atomic parameters are directly determined from
experiment or calculated rather than fit.
Valence Energy
The analytic energy expressions for the ESFF forcefield are provided
in Eq. 3-3 along with schematic representations
in Figure 3-5. As in AMBER, only diagonal terms are included.
- Eq. 3-3:
-
The bond energy is represented by a Morse functional form, where the
bond dissociation energy D, the equilibrium bond length
r0, and the
anharmonicity parameters are needed. In constructing these parameters
from atomic parameters, the forcefield utilizes not only the atom
types and bond orders, but also considers whether the bond is endo or
exo to 3-, 4-, or 5-membered rings. The rules themselves depend on the
electronegativity, hardness, and ionization of the atoms as well as
atomic anharmonicities and the covalent radii and well depths. The
latter quantities are fit parameters, and the former three are
calculated.
The ESFF angle types are classified according to ring, symmetry, and
-bonding information into 5 groups:
- The normal class includes unconstrained angles as well as
those associated with 3-, 4-, and 5-membered rings. The ring angles
are further classified based on whether one (exo) or both bonds (endo)
are in the ring. Additionally, angles with only central atoms in a
ring are also differentiated.
- The linear class includes angles with central atoms having
sp hybridization, as well as angles between two axial ligands in a
metal complex.
- The perpendicular class is restricted to metal centers and
includes angles between axial and equatorial ligands around a metal
center.
- The equatorial class includes angles between equatorial
ligands of square planar (sqp), trigonal bipyramidal (tbp), octahedral
(oct), pentagonal bipyramidal (pbp), and hexagonal bipyramidal (hbp)
systems.
- The
system class includes
angle between pseudoatoms. This class is further differentiated in
terms of normal, linear, perpendicular, and equatorial types.
The rules that determine the parameters in the functional forms depend
on the ionization potential and, for equatorial angles, the
periodicity. In addition to these calculated quantities, the
parameters are functions of the atomic radii and well depths of the
central and end atoms of the angle, and, for planar angles, two
overlap quantities and the 1-3 equilibrium distances.
To avoid the discontinuities that occur in the commonly used cosine
torsional potential when one of the valence angle approaches 180°,
ESFF uses a functional form that includes the sine of the valence
angles in the torsion. These terms ensure that the function goes
smoothly to zero as either valence angle approaches 0° or 180°, as
it should. The rules associated with this expression depend on the
central bond order, ring size of the angles, hybridization of the
atoms, and two atomic parameters for the central atom which is
fit.
The functional form of the out-of-plane energy is the same as in CFF91, where the coordinate (
) is an average of the three possible angles
associated with the out-of-plane center. The single parameter that is
associated with the central atom is a fit quantity.
Nonbond Energy
Partial Charges
The charges are determined by minimizing the electrostatic energy with
respect to the charges under the constraint that the sum of the
charges is equal to the net charge on the molecule. This is equivalent
to equalization of electronegativities. The derivation of the rule
begins with the following equation for the electrostatic energy:
- Eq. 3-4:
-
where
is the electronegativity and
the hardness. The first term is just a Taylor
series expansion of the energy of each atom as a function of charge,
and the second is the Coulomb interaction law between charges. The
Coulomb law term introduces a geometry dependence that ESFF for the
time being ignores, by considering only topological neighbors at
effectively idealized geometries. Minimizing the energy with respect
to the charges leads to the following expression for the charge on
atom i:
- Eq. 3-5:
-
where
is the Lagrange multiplier for
the constraint on the total charge, which physically is the equalized
electronegativity of all the atoms. The 
term
contains the geometry-independent remnant of the full Coulomb
summation.
Eqns. 3-4 and 3-5 give a
totally delocalized picture of the charges in a relatively severe
approximation. To obtain reasonable charges as judged by, for example,
crystal packing calculations, some modifications to the above picture
have been made. Metals and their immediate ligands are treated with
the above prescription, summing their formal charges to get a net
fragment charge. Delocalized
systems are
treated in an analogous fashion. Finally,
systems are treated using a localized
approach in which the charges of an atom depend simply on its
neighbors. Note that this approach, unlike the straightforward
implementations based on the equalization of electronegativity,
does include some resonance effects in the
system.
The electronegativity and hardness in the above equations must be
determined. Previous authors have often determined them from
experimental ionization potentials and electron affinities; however,
these spectroscopic states do not correspond to the valence states
involved in molecules. For this reason, ESFF is based on
electronegativities and harnesses, calculated using density functional
theory as implemented in DMol. The orbitals are (fractionally)
occupied in ratios appropriate for the desired hybridization state,
and calculations are performed on the neutral atom as well as on
positive and negative ions. From these curves the electronegativities
and hardnesses can be obtained.
van der Waals Interactions
ESFF currently uses the 6-9 potential for the van der Waals
interactions. Since the van der Waals parameters must be consistent
with the charges, they are derived using rules that are consistent
with the charges. Starting with the London formula:
- Eq. 3-6:
-
where
is the polarizability and
IP the ionization potential of the atoms. The polarizability,
in a simple harmonic approximation, is proportional to
n/IP where n is the number of electrons. Across
any one row of the periodic table, the core electrons remain unchanged
so that the following form is reasonable:
- Eq. 3-7:
-
where a' and b' are adjustable parameters that should
depend on just the period, and neff is the effective
number of (valence) electrons. Further assuming that
is proportional to R3 and
that another equivalent expression to that in Eq. 3-6 is:
- Eq. 3-8:
-
where
is a well depth, the following
forms are deduced for the rules for van der Waals parameters:
- Eq. 3-9:
-
The van der Waals parameters are affected by the charge of the
atom. In ESFF we have found it sufficient to modify the ionization
potential (IP) of metal atoms according to their formal charge
and hardness:
- Eq. 3-10 :
-
and for nonmetals to account for the partial charges when calculating
the effective number of electrons.
ESFF atom types (Table 3-3) are determined by
hybridization, formal charge, and symmetry. In addition, the rules may
involve bond order, ring size, and whether bonds are endo or exo to
rings. For metal ligands the cis-trans and axial-equatorial
positioning is also considered. The addition of these latter types
affects only certain parameters (for example, bond order influences
only bond parameters) and thus are not as powerful as complete atom
types. In one sense they provide a further refinement of typing beyond
atom types.
Table 3-3. Atom Types for the First Three
Rows of the Periodic Table--ESFF
The ESFF forcefield has been parameterized to handle all elements up
to radon in the periodic table. For the atom types that are not listed
in this table, please refer to the $BIOSYM_LIBRARY/esff.frc file.
The format is:
- atom type
- description
and you may quickly jump to the classes of atom types by clicking:
- dw
- deuterium in heavy water
- h
- generic hydrogen
- hi
- hydrogen in charged imidazole ring (equiv. to h*)
- hw
- hydrogen in water (equiv. to h*)
- h*
- hydrogen bonded to nitrogen, oxygen
- h+
- charged hydrogen in cations
- c
- generic sp3 carbon
- ca
- general amino acid alpha carbon (sp3)
(equiv. to c)
- cg
- sp3 alpha carbon in glycine
(equiv. to c)
- ci
- carbon in charged imidazole ring (equiv. to cp)
- co
- sp3 carbon in acetals (equiv. to c)
- coh
- sp3 carbon in acetals with hydrogen
(equiv. to c)
- cp
- sp2 aromatic carbon with partial
double bond
- cr
- c in neutral arginine (equiv. to c=)
- cs
- sp2 aromatic carbon in 5-membered
ring next to S (equiv. to cp)
- ct
- sp carbon involved in a triple bond
- ct3
- sp carbon involved in CO
- c1
- sp3 carbon with 1 H 3 heavies
(equiv. to c)
- c2
- sp3 carbon with 2 H's, 2 heavies
(equiv. to c)
- c3
- sp3 carbon with 3 H's, 1 heavy
(equiv. to c)
- c5
- sp2 aromatic carbon in 5-membered
ring
- c5p
- sp2 aromatic carbon in 5-membered big
pi ring
- c'
- carbon in carbonyl (C=O) group
- c-
- c in charged carboxylate
- c+
- c in guanidinium group (equiv. to c=)
- c=
- generic sp2 carbon
- n
- generic sp2 nitrogen (in amides)
- na
- sp3 nitrogen in amines
- nb
- sp2 nitrogen in aromatic amines
- nh
- sp2 (3 [sp2] 2 [p]) nitrogen in 5-membered
ring
- nho
- sp2 nitrogen in 6-membered ring
- ni
- nitrogen in charged imidazole ring (equiv. to nh)
- no
- sp2 nitrogen in oxides of nitrogen
- np
- sp2 nitrogen in 5-membered ring
- nt
- sp nitrogen involved in a triple bond
- nt2
- central nitrogen involved in azide group
- nz
- sp nitrogen in N2
- n1
- sp2 nitrogen in charged arginine
(equiv. to n=)
- n2
- sp2 nitrogen (NH2) in guanidinium group
(HN=C(NH2)2) (equiv. to n=)
- n4
- sp3 nitrogen with 4 substituents
(equiv. to n+)
- n+
- sp3 nitrogen in protonated amines
- n=
- sp2 nitrogen in neutral arginine
(double bond)
- o
- generic sp3 oxygen in alcohol, ether,
or acid group
- oa
- sp3 oxygen in ester or acid
- oc
- sp3 oxygen in ether or acetals
(equiv. to o)
- oh
- oxygen bonded to hydrogen (equiv. to o)
- op
- sp2 aromatic in 5-membered ring
- os
- oxygen bonded to two silicons
- ot
- oxygen with hybridization sp
- o1
- oxygen bonded to oxygen
- o'
- oxygen having a single double bond
- o*
- oxygen in water
- o-
- double bonded oxygen in charged carboxylate COO-
(equiv. to o')
- s
- sp3 sulfur
- sp
- sulfur in an aromatic ring (e.g., thiophene)
- s1
- sp3 sulfur involved in (S-S) group of
disulfides
- s2d
- sulfur with oxidation number 4, two double sigma bond
- s3d
- sulfur with oxidation number 4, three sigma bond, (C3v)
- s4d
- sulfur with oxidation number 6, four sigma bond, (Td)
- s4l
- sulfur with coordination number 4 (C2v)
- s5l
- sulfur with coordination number 5 (D4h, C2v)
- s5t
- sulfur with coordination number 5 (D3h)
- s6
- sulfur with coordination number 6 (D4h,
D2h)
- s6o
- sulfur with coordination number 6 (Oh)
- s'
- S in thioketone group
- s-
- double bonded sulfur in charged phosphate PSS- or
PSO- (equiv. to s')
- p
- general phosphorous atom
- p4d
- phosphorous atom with oxidation number 5 and 4 sigma bonds
(CTd)
- p4l
- phosphorous atom with oxidation number 5 and 3 sigma bonds
(C2v)
- p5l
- phosphorous atom with oxidation number 5 and 3 sigma bonds
(D4h, C2v)
- p5t
- phosphorous atom with oxidation number 5 and 3 sigma bonds
(D3h)
- p53
- phosphorous atom with oxidation number 5 and 3 sigma bonds (planar)
- p6
- phosphorous atom with oxidation number 5 and 3 sigma bonds
(D4h, D2h)
- p6o
- phosphorous atom with oxidation number 5 and 3 sigma bonds
(Oh)
- p'
- sp2 phosphorous atom
- b
- boron sp3 atom
- bt
- boron sp atom
- b'
- boron sp2 atom
- Be
- berillium atom
- Be+
- berillium cation
- Be+2
- berillium cation
- f
- fluorine atom
- F
- fluorine anion
- Li
- lithium atom with s orbitals involved in bonding
- Li+
- lithium ion
- ne
- neon atom
- ar
- argon atom
- Al
- aluminum atom
- Al033
- aluminum atom with coordination number 3
- Al034
- aluminum atom with coordination number 4
- Al035
- aluminum atom with coordination number 5
- Al035s
- aluminum atom with coordination number 5 (D4h)
- Al035t
- aluminum atom with coordination number 5 (D3h)
- Al036
- aluminum atom with coordination number 6 (D4h,
D2h)
- Al036o
- aluminum atom with coordination number 6 (Oh)
- cl
- chlorine atom
- Cl
- chlorine ion
- cl'
- chlorine atom in oxo acid
- he
- helium atom
- Mg
- magnesium atom
- Mg025
- magnesium atom with 5 coordinations
- Mg025s
- magnesium atom with 5 coordinations (D4h)
- Mg025t
- magnesium atom with 5 coordinations (D3h)
- Mg026
- magnesium atom with 6 coordinations (D4h,
D2h)
- Mg026o
- magnesium atom with 6 coordinations
- Mg+
- magnesium +1 cation (Oh)
- Mg+2
- magnesium +2 cation
- Na
- sodium atom
- Na+
- sodium ion
- si
- silicon atom
- si4l
- silicon atom (D3h, C2v)
- si5l
- silicon atom (D4h)
- si5t
- silicon atom (D3h)
- si6
- silicon atom (D4h, D2h)
- si6o
- silicon atom (Oh)
- si'
- sp2 silicon atom
Rule for Metal Atom Types
The names of the atom types for metals are based on the symmetry of
the metal complex and on both the oxidation state and coordination
number of the metal. For example, Ag024t indicates an Ag that has an
oxidation level of 2+, is 4-coordinated, and has tetrahedral
symmetry. The following table lists the abbreviations used for the
symmetry types:
symbol symmetry
------------------------
l C2v
s D4h
t Td
o Oh
p D5h
h D2h, D3h
d Doo
Some metals with differing oxidation numbers and symmetries may be
handled with the same parameters. Here, a generic metal atom type is
used.
The oxidation number of a metal is determined according to:
-
-
where Qt is the total charge on the complex, and the
sums over Fqi and Fqj are the sums
of formal charges on atoms not bonded to metals and bonded to metals,
respectively. Nm is the number of metal atoms in
the complex, and Nb is the number of metal atoms
bonded to the jth ligand atom.
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