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CHARMM Force field

The CHARMM force field energy is given as:

E=bondsKb(bb0)2+UBKUB(SS0)2+anglesKθ(θθ0)2+
dihedralsKχ(1+cos(nχδ))+impropersKϕ(ϕϕ0)2
+nonbond{ϵij[(rijminrij)122(rijminrij)6]+qiqj4πϵ0ϵrij}+residuesVcmap(ϕ,ψ)

where the bond stretch and bending terms are given harmonically, Kb and Kθ are the bond force constant and bond angle constant respectively and are taken from the force field. The improper angle term is also given harmonically with ω being the improper angle and Kω being the force constant of the improper.

The non-bonded terms are given via a Force Field Method and Force Field Method. The dihedral term is sinusoidal term in which n is the periodicity of the dihedral angle and δ is the phase shift. The Urey-Bradley (UB) term defines interactions between 1,3 pairs and is a quadratic function of the distance, S, between atoms one and three. It is only very rarely used within the CHARMM force field.

The CMAP term[1] [2] is a backbone correction term for proteins based on ab initio quantum mechanical (QM) calculations. The CMAP term greatly improves structural and dynamical results obtained from crystalline or solution phase
simulations.


  1. D. I. Freedberg, R. M. Venable, A. Rossi, T. E. Bull, and R. W. Pastor. Discriminating the helical forms of peptides by NMR and molecular dynamics simulation. J. Am. Chem. Soc., 126:10478–10484, 2004. ↩︎

  2. M. Buck, S. Bouguet-Bonnet, R. W. Pastor, and A. D. MacKerell. Importance of the CMAP correction to the CHARMM22 protein force field: Dynamics of hen lysozyme. Biophys. J., 90:L36–L38, 2006. ↩︎