The ESFF Forcefield


Contents


Functional Form

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 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

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:


hydrogen types

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

carbon types

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

nitrogen types

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)

oxygen types

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')

sulfur types

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')

phosphorus

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

other second-row elements

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

other third-row elements

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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