[gmx-users] Peptide folding simulation
intra\sa175950
stephane.abel at cea.fr
Mon Jul 9 11:54:33 CEST 2012
Hi
To see folding events in your (very) long peptide in explicit solvent,
without doing long MD (> 100 ns), you will need to use more complex MD
approach such as REMD or metadynamics. REMD is implemented in gromacs, but
for the latter one, you can use plumed with GROMACS.
See for example http://www.plumed-code.org/
HTH
Stephane
------------------------------
Hi,
I have been trying to study folding of a peptide 24 residues long. I
did a simulation of 50 ns with explicit solvent, CHARMM FF, but I
was not able to find even a single folding event. Then I decided use
explicit solvent for simulation and I again simulated the peptide for
100 ns . This time again I ended with no folding events.
I know that in case of explicit solvent , a 50ns simulation time is
not enough to observe anything. But I did it to see the initial
behavior of the peptide in water. In take many random like
conformation but doesnot fold into a desired beta-hairpin. For the
explicit solvent simulation, I followed the lysozyme tutorial
parameters.
For implicit solvent simulation, I used the following parameters for
Energy minimization :
define = -DFLEXIBLE
constraints = none
integrator = steep
dt = 0.001 ; ps
nsteps = 30000
vdwtype = cut-off
coulombtype = cut-off
pbc = no
nstlist = 0
ns_type = simple
rlist = 0 ; this means all-vs-all (no cut-off),
which gets expensive for bigger systems
rcoulomb = 0
rvdw = 0
comm-mode = angular
comm-grps = Protein
optimize_fft = yes
;
; Energy minimizing stuff
;
emtol = 5.0
emstep = 0.01
;
; Implicit solvent
;
implicit_solvent = GBSA
gb_algorithm = Still ; HCT ; OBC
nstgbradii = 1
rgbradii = 0 ; [nm] Cut-off for the calculation of the
Born radii. Currently must be equal to rlist
gb_epsilon_solvent = 80 ; Dielectric constant for the implicit
solvent
; gb_saltconc = 0 ; Salt concentration for implicit
solvent models, currently not used
sa_algorithm = Ace-approximation
sa_surface_tension = -1
For MD I used the following : -
define = -DPOSRESHELIX ; -DFLEXIBLE -DPOSRES
constraints = none
integrator = md
dt = 0.001 ; ps
nsteps = 1000000000 ; 100000 ps = 100 ns
nstcomm = 10
nstcalcenergy = 10
nstxout = 1000 ; frequency to write coordinates to output
trajectory
nstvout = 0 ; frequency to write velocities to output
trajectory; the last velocities are always written
nstfout = 0 ; frequency to write forces to output
trajectory
nstlog = 1000 ; frequency to write energies to log
file
nstenergy = 1000 ; frequency to write energies to edr file
vdwtype = cut-off
coulombtype = cut-off
pbc = no
nstlist = 0
ns_type = simple
rlist = 0 ; this means all-vs-all (no cut-off), which
gets expensive for bigger systems
rcoulomb = 0
rvdw = 0
comm-mode = angular
comm-grps = system
optimize_fft = yes
; V-rescale temperature coupling is on
Tcoupl = v-rescale
tau_t = 0.1
tc_grps = system
ref_t = 300
; Pressure coupling is off
Pcoupl = no
; Generate velocites is on
gen_vel = yes
gen_temp = 300
gen_seed = -1
;
; Implicit solvent
;
implicit_solvent = GBSA
gb_algorithm = Still ; HCT ; OBC
nstgbradii = 1
rgbradii = 0 ; [nm] Cut-off for the calculation of the
Born radii. Currently must be equal to rlist
gb_epsilon_solvent = 80 ; Dielectric constant for the implicit
solvent
; gb_saltconc = 0 ; Salt concentration for implicit
solvent models, currently not used
sa_algorithm = Ace-approximation
sa_surface_tension = -1
So, finally I want to know where have I gone in my simulation
experiments, both implicit and explicit ?? ... Please reply .
----------------
BHARAT
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