FORCE FIELDS FOR UPACK

Bouke P. van Eijck, Department of Crystal and Structural Chemistry, Bijvoet Center for Biomolecular Research, Utrecht University, Padualaan 8, 3584 CH Utrecht, The Netherlands. E-mail: vaneyck@chem.uu.nl or vaneijck@xs4all.nl.

 

For information on the standard UPACK package, see the main manual .

 

Force fields

As discussed in the main manual, the force field is defined by the file upack/tops/ffname.ff. As an example for the Buckingham potential, the Williams and Starr [1] force field for benzene can be found in benz.ff. Here we shall discuss Lennard-Jones type force fields for carbohydrates in some detail. For the first stage (program pack12) we used the force field UNITAT, which was developed from GROMOS87 [2] by optimizing geometric crystal data for 23 carbohydrate molecules [3]. In the final stage it is better to use an all-atom force field. In this way the computations take less time; but note that some additional all-atom structures may be found if that force field is used right from the beginning.

 

United-atom force fields for monosaccharides and polyalcohols

Atom types:
 

HO

hydroxyl H

OA

hydroxyl O

OS

ether O in ring and exocyclic OCH3 group

CS0

C atom without H in sugar ring

CS1

united CH1 group in sugar ring

CS2

united CH2 group in sugar ring and exocyclic CH2OH group

CH3

united CH3 group

Entries in the force field files refer to the Lennard-Jones potential; energy units are kcal/mol, distance units Angstrom. Every C-C bond separates two of the following charge groups:
 

CH3

0.00

CS2

0.00

C-O-H

0.15, -0.50, 0.35

C-O-C

0.18, -0.36, 0.18

C-O-C-O-H

0.20, -0.36, 0.31, -0.50, 0.35

C-O-C-O-CH3

0.15, -0.36, 0.17, -0.36, 0.17

C-O-C-O-CS2

0.16, -0.36, 0.17, -0.36, 0.16

C-O-C-O-C-O-C

0.14, -0.36, 0.40, -0.36, 0.40, -0.36, 0.14

All-atom force fields for monosaccharides and polyalcohols

Many force fields depend on atomic charges from ab-initio quantumchemical calculations. For carbohydrates, with their high conformational flexibility, this is rather unpractical. Carbohydrate force fields with fixed standard charges have been proposed by Ha et al [4], Kouwijzer et al [5] and Damm et al [6]. We have compared the rankings of the experimental structures in a test set of 15 molecules for these force fields [7], and found that the third force field (OPLS) gives the best results. Nevertheless, it is not superior to UNITAT and we have not been able to develop an all-atom force field that performs better. Polarization, although theoretically necessary to account for the cooperativity of hydrogen bonds, gave no improvement at all.

The OPLS parameters can be found in file opls.ff, the two other force fields in the files ha.ff and milou.ff. All these force fields use the Lennard-Jones potential; in the OPLS force field all 1...4 interactions are scaled by 0.5. A cutoff of at least 10 A or, preferably, Ewald summation should be used. No improper dihedrals are necessary.

Atom types:
 

HO

hydroxyl H

HC

aliphatic H

OA

hydroxyl oxygen

OS

ether oxygen in ring

OE

hydroxyl oxygen in exocyclic CH2OH group

CA

anomeric carbon atom

CS

other ring carbon atoms

CE

exocyclic carbon atom

The charges in the OPLS force field are found by the following rule: each bond carries a "bond increment" which contributes equal positive and negative charges to the two atoms involved.
 

Negative side

Positive side

Bond increment

OA (anomeric)

HO

0.435

OA (other)

HO

0.418

OA

C

0.265

OS, OE

C

0.200

C

C

0 (dividing charge groups)

CA

HC

0.10

C (with OH group)

HC

0.06

C (other)

HC

0.03

All-atom force fields for carboxylic acids

As discussed in Ref. [8], we have made a few changes and extensions in the OPLS force field for the modelling of carboxylic acids (the "OPLS-AC" force field). This extension is only a first try, and is by no means fully optimized. The parameters are included in the file opls.ff; charges are as published in Ref. [8].

Atom types:
 

C

C in COOH

O

=O in COOH

OZ

-O in COOH

HZ

H in COOH

CS

aliphatic C

HC

H on C or CS

OA

hydroxyl O

HO

hydroxyl H

All-atom force fields for aromatic systems

Due to conjugation, each aromatic system is unique in principle: geometry parameters and charges have to be derived from theoretical chemistry. For simple chloro- and bromo substituted benzenes a few standard parameters are available in UPACK [9]. For structure generation Lennard-Jones parameters can be taken from the file opls.ff. Buckingham parameters, mostly taken from the publications of Williams and Price, are available in the file will.ff. In both files intramolecular parameters were taken rather arbitrarily.

Atom types:
 

CR61

united-atom benzene CH group

CR

united-atom central C atom or all-atom aromatic C

HR

aromatic H

Cl

chlorine

Br

bromine

Every C-C bond separates two charge groups:
 

CR61

  0.00

CR-HR

-0.10, +0.10  (+/- 0.15 in will.ff)

CR-Cl

+0.10, -0.10

CR-Br

+0.10, -0.10

References


1. D. E. Williams and T. L. Starr, Comput.
Chem. 1 (1977) 173-177.
2. W. F. van Gunsteren and H. J. C. Berendsen, GROMOS, Groningen molecular simulation package, University of Groningen, 1987.
3. B. P. van Eijck and J. Kroon, J. Comput. Chem. 20 (1999) 799-812.
4. S. N. Ha, A. Giammona, M. Field and J. W. Brady, Carboh.
Res. 180 (1988) 207-221.
5. M. L. C. E. Kouwijzer, B. P. van Eijck, S. J. Kroes and J. Kroon, J. Comput. Chem. 14 (1993) 1281-1289.
6. W. Damm, A. Frontera, J. Tirado-Rives and W. L. Jorgensen, J. Comput.
Chem. 16 (1997) 1955-1970.
7. B. P. van Eijck and J. Kroon, J. Comput. Chem. 20 (1999) 799-812.
8. B. P. van Eijck, J. Comput. Chem. 23 (2002) 456-462.
9. B. P. van Eijck, Phys. Chem. Chem. Phys.  4 (2002) 4789-4794.
 

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