From chemistry-request $#at#$ ccl.net Fri Jun 26 04:53:50 1992 Date: Fri, 26 Jun 92 08:28:04 +0200 From: martin #at# biokth.sunet.SE Subject: Cut offs. To: "chemistry #at# ccl.net" #at# kth.sunet.SE Status: RO Hi, To my knowledge there are not many studies of how to treat cutoffs in the literature. However in Proteins: Struct. Funct. Genet. 6:32-45 (1989) there is a quite extensive study. They have used the CHARMM force field, however I think this may account for any similar force field. My opinion is that the cutoffs that one has to use is very dependent on how the electrostatics of the calculation is treated. I'm a Sybyl User that use the AMBER FF in Sybyl for dynamics and mechanics calculation of biomolecules. For vacuum calculations I use a cutoff of 10-12 A (distance dependent dielectric constant) and 8-10 A for solvent calculations. The effect of the cutoffs to the vdW forces is less important I think. These long range vdW forces does not have any large impact on the structure, but may of course change the total energy level of a calculation. Finally, I think that what may become even more important is to include polarizability to the electrostatics, especially for biomolecules. Not before that becomes real we will treat simulations of biomolecules in the best possible way. I have heard from a colleague about a new structure of an ion transporting protein which had a narrow channel where in one the sides of this channel it was up to 5-7 lysines or arginines and the other side contained about 4 aspartates or glutamates. These residues were clustered very near eachother. Would anybody think that a molecular dynamics simulation of this protein would be succesful using todays standard force fields ? I hesitate...... Any comments to the net regarding these questions would be very much welcomed by me, because I think it is very important for the improvement of the MD techniques in biological chemistry (which I think and hope is and will be a very useful tool). Greetings Martin Norin KTH Stockholm e-mail:martin /at\physchem.kth.se