Table of Contents
In this work, we have developed a general AMBER force field (GAFF) for
rational drug design. GAFF is compatible with the AMBER force field and it
has parameters for almost all the organic molecules made of C, N, O, H, S,
P, F, Cl, Br and I. As a complete force field, GAFF is suitable for study of
a great number of molecules (such as database searching) in an automatic fashion.
Molecular mechanics are the key component in the armamentarium used by
computational chemists for rational drug design and many other tasks. Force
fields are the cornerstone of molecular mechanics. A successful force field
in drug design should work well both for the biological molecules and the
organic molecules. AMBER force fields have a good reputation for
the study of proteins and nucleic acids. However, the fact that AMBER
only has limited parameters for organic molecules prevents it from being
widely used in drug design. Therefore, it is necessary to develop a
general AMBER force field that works for most pharmaceutical molecules.
It should also be as compatible as possible with the traditional AMBER
force fields. Our objective is to develop a general, complete, and compatible
force field for rational drug design.
Similar to the other AMBER force fields, the GAFF also applies
the following simple harmonic functional form:
Here, req and qeq are equilibrium structural
parameters; Kr,
Kq,
Vn
are force constants; n is multiplicity and gamma is phase angle for torsional
angle parameters. Details will be given below on how these parameters were
derived.
Compared to traditional AMBER force field, atom types in GAFF are more
general and cover most of the organic chemical space.Table I lists the
basic (a) and special (b) atom types in GAFF.
Table I (a). Basic Atom Types in GAFF
Atom type |
Description |
Atom type |
Description |
c
c1
c2
c3
ca |
sp2 C in C=O, C=S
sp1 C
sp2 C, aliphatic
sp3 C
sp2 C, aromatic |
o
oh
os
|
sp2 O in C=O, COO-
sp3 O in hydroxyl group
sp3 O in ether and ester
|
n
n1
n2
n3
n4
na
nh
no |
sp2 N in amide
sp1 N
sp2 N with 2 subst.
readl double bond
sp3 N with 3 subst.
sp3 N with 4 subst.
sp2 N with 3 subst
amine N connected
to the aromatic rings
N in nitro group |
s2
sh
ss
s4
s6 |
sp2 S (p=S, C=S etc)
sp3 S in thiol group
sp3 S in -SR and SS
hypervalent S, 3 subst.
hypervalent S, 4 subst. |
hc
ha
hn
ho
hs
hp |
H on aliphatic C
H on aromatic C
H on N
H on O
H on S
H on P |
f
cl
br
i |
any F
any Cl
any Br
any I |
p2
p3
p4
p5 |
sp2 P (C=P etc)
sp3 P, 3 subst.
hypervalent P, 3 subst.
hypervalent P, 4 subst. |
Table I (b). Special Atom Types in GAFF
Atom type |
Description |
Atom type |
Description |
h1
h2
h3
h4
h5
  |
H on aliphatic C with 1 EW group;
H on aliphatic C with 2 EW group;
H on aliphatic C with 3 EW group;
H on aromatic C with 4 EW group;
H on aromatic C with 5 EW group;
  |
cc(cd)
ce(cf)
cp(cq)
cu
cv
cx
cy |
inner sp2 C in conj. ring systems
inner sp2 C in conj. chain systems
bridge aromatic C
sp2 C in three-memberred rings
sp2 C in four-memberred rings
sp3 C in three-memberred rings
sp3 C in four-memberred rings |
n
nb
nc(nd)
sx
sy |
aromatic nitrogen
inner sp2 N in conj. ring systems
inner sp2 N in conj. chain systems
conj. S, 3 subst.
conj. S, 4 subst. |
pb
pc(pd)
pe(pf)
px
py |
aromatic phosphorus
inner sp2 P in conj. ring systems
inner sp2 P in conj. chain systems
conj. P, 3 subst.
conj. P, 4 subst. |
EW: electron-withdraw group
The charge method used in GAFF is HF/6-31G* RESP charge. However, AM1-BCC,
which was parameterized to reproduce the HF/6-31G* RESP charges can be
applied in case of large amount of calculations, such as database searching.
The van der Waals parameters of GAFF are as same as those used by the traditional
AMBER force field.
There are several resources to derive the reference bond length req,
including the statistic mean values of bond lengths from X-ray and neutron
diffraction as well as high level ab initio calculations (MP2/6-31G* ).
Force constants were derived using the following empirical function forms:
Here, m and Kij were determined using bond length parameters
in traditional AMBER force field. As a compromise, the parameter m in the above
equation is set to 4.0. Fitting details are shown in Figure 1-3.
The parameters are listed in Table II.
Figure 1
Figure 2
Figure 3
Table II. Bond length parameterization
i |
j |
rij |
Kij |
i |
j |
rij |
Kij |
H |
H |
0.738 |
4.661 |
H |
C |
1.090 |
6.217 |
H |
N |
1.010 |
6.057 |
H |
O |
0.96 |
5.794 |
H |
F |
0.920 |
5.600 |
H |
Cl |
1.280 |
6.937 |
H |
Br |
1.410 |
7.301 |
H |
I |
1.600 |
7.802 |
H |
P |
1.410 |
7.257 |
H |
S |
1.340 |
7.018 |
C |
C |
1.526 |
7.643 |
C |
N |
1.470 |
7.504 |
C |
O |
1.440 |
7.347 |
C |
F |
1.370 |
7.227 |
C |
Cl |
1.800 |
8.241 |
C |
Br |
1.940 |
8.478 |
C |
I |
2.160 |
8.859 |
C |
P |
1.830 |
8.237 |
C |
S |
1.820 |
8.117 |
N |
N |
1.441 |
7.634 |
N |
O |
1.420 |
7.526 |
N |
F |
1.420 |
7.475 |
N |
Cl |
1.750 |
8.266 |
N |
Br |
1.930 |
8.593 |
N |
I |
2.120 |
8.963 |
N |
P |
1.720 |
8.212 |
N |
S |
1.690 |
8.073 |
O |
O |
1.460 |
7.561 |
O |
F |
1.410 |
7.375 |
O |
Cl |
1.700 |
8.097 |
O |
Br |
1.790 |
8.276 |
O |
I |
2.110 |
8.854 |
O |
P |
1.640 |
7.957 |
O |
S |
1.650 |
7.922 |
F |
F |
1.406 |
7.358 |
F |
Cl |
1.648 |
7.947 |
F |
P |
1.500 |
7.592 |
F |
S |
1.580 |
7.733 |
Cl |
Cl |
2.031 |
8.648 |
Cl |
I |
2.550 |
9.309 |
Cl |
P |
2.040 |
8.656 |
Cl |
S |
2.030 |
8.619 |
Br |
Br |
2.337 |
9.012 |
Br |
I |
2.671 |
9.380 |
Br |
P |
2.240 |
8.729 |
Br |
S |
2.210 |
8.728 |
I |
I |
2.836 |
9.511 |
I |
P |
2.490 |
9.058 |
I |
S |
2.560 |
9.161 |
P |
P |
2.324 |
8.805 |
P |
S |
2.120 |
8.465 |
S |
S |
2.038 |
8.316 |
The following list the source of reference bond angles:
The force constant Kqwas also estimated using
an empirical function as the following. The parameters are listed in Table
III.
Table III. Parameters of bond angle force constant calculations
Element |
C |
Z |
H |
0.0 |
0.784 |
C |
1.339 |
1.183 |
N |
1.300 |
1.212 |
O |
1.249 |
1.219 |
F |
0.000 |
1.166 |
Cl |
0.000 |
1.272 |
Br |
0.000 |
1.378 |
I |
0.000 |
1.398 |
P |
0.906 |
1.620 |
S |
1.448 |
1.280 |
The following is the strategy to develop torsional angle parameters.
-
Perform torsional angle scanning to get the rotational profile at MP4/6-311G(d,p)//
MP2/6-31G* level
-
Apply PARMSCAN to find the best torsional angle parameters to reproduce
the rotational profile
Totally, 200 general torsional angle parameters were developed in GAFF, which
gave an average unsigned error of 0.5 kcal/mol to MP4/6-311G(d,p) energies.
Figure 4. An example: rotation profiles of X-c-c-X
9.a How well does GAFF predict the molecular structures?
Table IV Comparison of GAFF and other force fields in reproducing geometries of
75 crystallographic structures
|
GAFF |
MMFF94 |
DREIDING |
TRIPOS
5.2 |
CHARMm |
RMS of Atomic Displacement (Å) |
0.34 |
0.47 |
0.24 |
0.25 |
0.44 |
RMS of Bond Length Deviation (Å) |
0.027 |
0.021 |
0.035 |
0.025 |
~ |
RMS of Bond Angle Deviation (°) |
2.2 |
2.0 |
3.22 |
2.5 |
~ |
9.b How well does GAFF predict the inter-molecular energies?
Table V How well does GAFF perform in calculating the inter-molecular
energies of 22 base pairs. All the comparison are made to the MP2/6-311G* energies.
|
GAFF/BCC |
GAFF/RESP |
PARM99/RESP |
RMS of Atomic Displacements (Å) |
0.56 |
0.49 |
0.19 |
RMS of DE
Compared to ab initio (kcal/mol) |
2.50 |
0.67 |
0.77 |
9.c How well does GAFF predict the intra-molecular energies?
Table VI Performances of widely used force field in reproducing
the relative
energies for 55 compounds. Comparison are made to the experiment.
|
GAFF/BCC |
AMBER
(parm99) |
MMFF |
MM3 |
CHARMm |
Unsigned Average Error (kcal/mol) |
0.51 |
0.28 |
0.43 |
0.52 |
0.57 |
RMS Deviation (kcal/mol) |
0.69 |
0.40 |
0.54 |
0.75 |
0.76 |
In this work, we have developed a general AMBER force field. We hope it
is an ideal molecular mechanical tool in rational drug design. We have
finished a total of 2000 MP2/6-31G* optimizations and 1260 MP4/6-311G(d,p)
single point calculations. From the three test cases, encouraging results were
achieved. It is notable that in the third test case, GAFF has comparable
performance to those of CHARMm and MM3, although GAFF applies very general
force field parameters and crude charge approach.
Compared to other widely
used fields, GAFF has the following distinguishing features. First of all,
it is a complete force field, which means all the parameters are available,
no parameter-missing happens to GAFF; secondly, this force field is very
general and it covers almost all the organic chemical spaces; finally, GAFF is
compatible to the AMBER force field. We believe that the combination of GAFF
with traditional AMBER will offer a useful molecular mechanical tool for
rational drug design, especially for things like binding free energy calculations.
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