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Added input files for the anthracene system
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; 3d1_GMX_OPLS.itp created by acpypi (Rev: 250) on Wed Sep 23 14:49:10 2009 | ||
[ defaults ] | ||
; nbfunc comb-rule gen-pairs fudgeLJ fudgeQQ | ||
1 3 yes 0.5 0.5 | ||
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[ atomtypes ] | ||
;name bond_type mass charge ptype sigma epsilon Amb | ||
CH CA 13.019 0 A 3.74119144658246e-01 0.502658843994140e+00 ; | ||
C CA 12.011 0 A 3.36109739624996e-01 0.405868318433803e+00 ; | ||
DUM CA 12.011 0.000 A 0 0 | ||
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[ bondtypes ] | ||
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[ angletypes ] | ||
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[ dihedraltypes ] | ||
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[ atomtypes ] | ||
opls_111 OW 15.99940 0.000 A 3.15061e-01 6.363864e-01 | ||
opls_112 HW 1.00800 0.000 A 0.00000e-01 0.000000e-01 | ||
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[ moleculetype ] | ||
; molname nrexcl | ||
SOL 1 | ||
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[ atoms ] | ||
1 opls_111 1 SOL OW 1 -0.834 | ||
2 opls_112 1 SOL HW1 1 0.417 | ||
3 opls_112 1 SOL HW2 1 0.417 | ||
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[ settles ] | ||
; i j funct length | ||
1 1 0.09572 0.15139 | ||
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[ exclusions ] | ||
1 2 3 | ||
2 1 3 | ||
3 1 2 | ||
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[ moleculetype ] | ||
;name nrexcl | ||
COM 3 | ||
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[ atoms ] | ||
; nr type resinr residue atom cgnr charge mass | ||
1 CH 1 COM C1 1 0 13.01900 | ||
2 CH 1 COM C2 2 0 13.01900 | ||
3 CH 1 COM C5 5 0 13.01900 | ||
4 CH 1 COM C6 6 0 13.01900 | ||
5 CH 1 COM C9 9 0 13.01900 | ||
6 CH 1 COM C10 10 0 13.01900 | ||
7 CH 1 COM C13 13 0 13.01900 | ||
8 CH 1 COM C14 14 0 13.01900 | ||
9 C 1 COM C15 15 0 12.01100 | ||
10 C 1 COM C16 16 0 12.01100 | ||
11 C 1 COM C19 19 0 12.01100 | ||
12 C 1 COM C20 20 0 12.01100 | ||
13 CH 1 COM C21 21 0 13.01900 | ||
14 CH 1 COM C22 22 0 13.01900 | ||
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[ bonds ] | ||
; ai aj funct r k | ||
1 2 1 1.3900e-01 417333.6 ; C1 - C2 - | ||
1 3 1 1.3900e-01 417333.6 ; C1 - C5 - | ||
2 4 1 1.3900e-01 417333.6 ; C2 - C6 - | ||
3 9 1 1.3900e-01 417333.6 ; C5 - C15 - | ||
4 10 1 1.3900e-01 417333.6 ; C6 - C16 - | ||
5 9 1 1.3900e-01 417333.6 ; C9 - C15 - | ||
5 11 1 1.3900e-01 417333.6 ; C9 - C19 - | ||
6 10 1 1.3900e-01 417333.6 ; C10 - C16 - | ||
6 12 1 1.3900e-01 417333.6 ; C10 - C20 - | ||
7 11 1 1.3900e-01 417333.6 ; C13 - C19 - | ||
7 13 1 1.3900e-01 417333.6 ; C13 - C21 - | ||
8 12 1 1.3900e-01 417333.6 ; C14 - C20 - | ||
8 14 1 1.3900e-01 417333.6 ; C14 - C22 - | ||
9 10 1 1.3900e-01 417333.6 ; C15 - C16 - | ||
11 12 1 1.3900e-01 417333.6 ; C19 - C20 - | ||
13 14 1 1.3900e-01 417333.6 ; C21 - C22 - | ||
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[ pairs ] | ||
; ai aj funct | ||
1 5 1 ; C1 - C9 | ||
1 10 1 ; C1 - C16 | ||
2 6 1 ; C2 - C10 | ||
2 9 1 ; C2 - C15 | ||
3 4 1 ; C5 - C6 | ||
3 6 1 ; C5 - C10 | ||
3 11 1 ; C5 - C19 | ||
4 5 1 ; C6 - C9 | ||
4 12 1 ; C6 - C20 | ||
5 6 1 ; C9 - C10 | ||
5 8 1 ; C9 - C14 | ||
5 13 1 ; C9 - C21 | ||
6 7 1 ; C10 - C13 | ||
6 14 1 ; C10 - C22 | ||
7 8 1 ; C13 - C14 | ||
7 9 1 ; C13 - C15 | ||
8 10 1 ; C14 - C16 | ||
9 12 1 ; C15 - C20 | ||
10 11 1 ; C16 - C19 | ||
11 14 1 ; C19 - C22 | ||
12 13 1 ; C20 - C21 | ||
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[ angles ] | ||
; ai aj ak funct theta cth | ||
1 2 4 1 1.2000e+02 4.2000e+02 ; C1 - C2 - C6 - - | ||
1 3 9 1 1.2000e+02 4.2000e+02 ; C1 - C5 - C15 - - | ||
2 1 3 1 1.2000e+02 4.2000e+02 ; C2 - C1 - C5 - - | ||
2 4 10 1 1.2000e+02 4.2000e+02 ; C2 - C6 - C16 - - | ||
3 9 5 1 1.2000e+02 4.2000e+02 ; C5 - C15 - C9 - - | ||
3 9 10 1 1.2000e+02 4.2000e+02 ; C5 - C15 - C16 - - | ||
4 10 6 1 1.2000e+02 4.2000e+02 ; C6 - C16 - C10 - - | ||
4 10 9 1 1.2000e+02 4.2000e+02 ; C6 - C16 - C15 - - | ||
5 9 10 1 1.2000e+02 4.2000e+02 ; C9 - C15 - C16 - - | ||
5 11 7 1 1.2000e+02 4.2000e+02 ; C9 - C19 - C13 - - | ||
5 11 12 1 1.2000e+02 4.2000e+02 ; C9 - C19 - C20 - - | ||
6 10 9 1 1.2000e+02 4.2000e+02 ; C10 - C16 - C15 - - | ||
6 12 8 1 1.2000e+02 4.2000e+02 ; C10 - C20 - C14 - - | ||
6 12 11 1 1.2000e+02 4.2000e+02 ; C10 - C20 - C19 - - | ||
7 11 12 1 1.2000e+02 4.2000e+02 ; C13 - C19 - C20 - - | ||
7 13 14 1 1.2000e+02 4.2000e+02 ; C13 - C21 - C22 - - | ||
8 12 11 1 1.2000e+02 4.2000e+02 ; C14 - C20 - C19 - - | ||
8 14 13 1 1.2000e+02 4.2000e+02 ; C14 - C22 - C21 - - | ||
9 5 11 1 1.2000e+02 4.2000e+02 ; C15 - C9 - C19 - - | ||
10 6 12 1 1.2000e+02 4.2000e+02 ; C16 - C10 - C20 - - | ||
11 7 13 1 1.2000e+02 4.2000e+02 ; C19 - C13 - C21 - - | ||
12 8 14 1 1.2000e+02 4.2000e+02 ; C20 - C14 - C22 - - | ||
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[ dihedrals ] ; impropers | ||
; i j k l func phase kd | ||
3 5 9 10 2 180 167.4231 ; C5- C9- C15- C16 | ||
4 6 10 9 2 180 167.4231 ; C6- C10- C16- C15 | ||
5 7 11 12 2 180 167.4231 ; C9- C13- C19- C20 | ||
6 8 12 11 2 180 167.4231 ; C10- C14- C20- C19 | ||
3 2 1 4 2 0 167.4231 ; C5 C2 C1 C6 added | ||
1 4 2 10 2 0 167.4231 ; C1 C6 C2 C16 added | ||
2 10 4 9 2 0 167.4231 ; C2 C16 C6 C15 added | ||
4 9 10 3 2 0 167.4231 ; C6 C15 C16 C5 added | ||
10 3 9 1 2 0 167.4231 ; C16 C5 C15 C1 added | ||
9 1 3 2 2 0 167.4231 ; C15 C1 C5 C2 added | ||
5 10 9 6 2 0 167.4231 ; C9 C16 C15 C10 added | ||
9 6 10 12 2 0 167.4231 ; C15 C10 C16 C20 added | ||
10 12 6 11 2 0 167.4231 ; C16 C20 C10 C19 added | ||
6 11 12 5 2 0 167.4231 ; C10 C19 C20 C9 added | ||
12 5 11 9 2 0 167.4231 ; C20 C9 C19 C15 added | ||
11 9 5 10 2 0 167.4231 ; C19 C15 C9 C16 added | ||
7 12 11 8 2 0 167.4231 ; C13 C20 C19 C14 added | ||
11 8 12 14 2 0 167.4231 ; C19 C14 C20 C22 added | ||
12 14 8 13 2 0 167.4231 ; C20 C22 C14 C21 added | ||
8 13 14 7 2 0 167.4231 ; C14 C21 C22 C13 added | ||
14 7 13 11 2 0 167.4231 ; C22 C13 C21 C19 added | ||
13 11 7 12 2 0 167.4231 ; C21 C19 C13 C20 added | ||
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[ system ] | ||
; Name | ||
Anthracene Benzene Null Transform in water | ||
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[ molecules ] | ||
; Compound #mols | ||
COM 1 | ||
SOL 1073 |
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; Run control | ||
integrator = md-vv | ||
tinit = 0 | ||
dt = 0.002 | ||
nsteps = 100000000 | ||
comm_mode = Linear | ||
nstcomm = 1 | ||
nstfout = 0 | ||
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; Output control | ||
nstlog = 1000 | ||
nstcalcenergy = 1 | ||
nstenergy = 1000 | ||
nstxout_compressed = 1000 | ||
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; Neighborsearching and short-range nonbonded interactions | ||
nstlist = 10 | ||
pbc = xyz | ||
rlist = 1.0 | ||
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; Electrostatics | ||
coulombtype = PME | ||
rcoulomb = 0.9 | ||
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; van der Waals | ||
vdwtype = Cut-off | ||
vdw_modifier = Potential-switch | ||
rvdw_switch = 0.8 | ||
rvdw = 0.9 | ||
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; Apply long range dispersion corrections for Energy and Pressure | ||
DispCorr = AllEnerPres | ||
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; Spacing for the PME/PPPM FFT grid | ||
fourierspacing = 0.1 | ||
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; EWALD/PME/PPPM parameters | ||
pme_order = 6 | ||
ewald_rtol = 1e-06 | ||
ewald_geometry = 3d | ||
epsilon_surface = 0 | ||
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; Temperature coupling | ||
tcoupl = v-rescale | ||
tc_grps = System | ||
tau_t = 2.0 | ||
ref_t = 300 | ||
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; Pressure coupling is on for NPT | ||
pcoupl = no | ||
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; refcoord_scaling should do nothing since there are no position restraints. | ||
gen_vel = yes | ||
gen_temp = 300 | ||
gen_seed = -1 | ||
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; options for bonds | ||
constraints = h-bonds | ||
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; Type of constraint algorithm | ||
constraint_algorithm = lincs | ||
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; Highest order in the expansion of the constraint coupling matrix | ||
lincs_order = 4 | ||
lincs_iter = 2 | ||
continuation = no | ||
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; Free energy calculation | ||
free_energy = expanded | ||
calc_lambda_neighbors = -1 | ||
sc_alpha = 0.5 | ||
sc_power = 1 | ||
couple_moltype = COM | ||
couple_lambda0 = vdw | ||
couple_lambda1 = none | ||
couple_intramol = no | ||
init_lambda_state = 0 | ||
nstdhdl = 100 | ||
dhdl_print_energy = total | ||
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; Seed for Monte Carlo in lambda space | ||
lmc_seed = -1 | ||
lmc_gibbsdelta = -1 | ||
lmc_forced_nstart = 0 | ||
symmetrized_transition_matrix = no | ||
nst_transition_matrix = 100000 | ||
; wl-scale = 0.8 | ||
; wl-ratio = 0.8 | ||
; init-wl-delta = 0.5 | ||
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; expanded ensemble variables | ||
nstexpanded = 100 | ||
lmc_stats = no | ||
lmc_move = metropolized-gibbs | ||
; lmc-weights-equil = wl-delta | ||
; weight-equil-wl-delta = 0.001 | ||
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; lambda-states = 1 2 3 4 5 6 7 8 | ||
vdw_lambdas = 0.0 0.18 0.42 0.57 0.68 0.76 0.86 1.0 | ||
init_lambda_weights = 0.0 4.32298 9.25799 11.45557 11.88643 10.43653 6.22252 3.39715 |
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; Run control | ||
integrator = md-vv | ||
tinit = 0 | ||
dt = 0.002 | ||
nsteps = 12500000 ; 25 ns | ||
comm-mode = Linear | ||
nstcomm = 1 | ||
nstfout = 0 | ||
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; Output control | ||
nstlog = 1000 | ||
nstcalcenergy = 1 | ||
nstenergy = 1000 | ||
nstxout-compressed = 1000 | ||
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; Neighborsearching and short-range nonbonded interactions | ||
nstlist = 10 | ||
pbc = xyz | ||
rlist = 1.0 | ||
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; Electrostatics | ||
coulombtype = PME | ||
rcoulomb = 0.9 | ||
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; van der Waals | ||
vdw-type = Cut-off | ||
vdw_modifier = Potential-switch | ||
rvdw-switch = 0.8 | ||
rvdw = 0.9 | ||
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; Apply long range dispersion corrections for Energy and Pressure | ||
DispCorr = AllEnerPres | ||
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; Spacing for the PME/PPPM FFT grid | ||
fourierspacing = 0.10 | ||
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; EWALD/PME/PPPM parameters | ||
pme_order = 6 | ||
ewald_rtol = 1e-06 | ||
ewald_geometry = 3d | ||
epsilon_surface = 0 | ||
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; Temperature coupling | ||
tcoupl = v-rescale | ||
tc_grps = System | ||
tau_t = 2.0 | ||
ref_t = 300 | ||
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; Pressure coupling is on for NPT | ||
pcoupl = no | ||
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; refcoord_scaling should do nothing since there are no position restraints. | ||
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gen_vel = yes | ||
gen-temp = 300 | ||
gen-seed = -1; need to randomize the seed each time. | ||
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; options for bonds | ||
constraints = h-bonds ; we only have C-H bonds here | ||
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; Type of constraint algorithm | ||
constraint-algorithm = lincs | ||
continuation = no | ||
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; Highest order in the expansion of the constraint coupling matrix | ||
lincs-order = 4 | ||
lincs-iter = 2 | ||
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; Free energy calculation | ||
free_energy = yes | ||
calc-lambda-neighbors = -1 | ||
sc-alpha = 0.5 | ||
sc-power = 1 | ||
couple-moltype = COM | ||
couple-lambda0 = vdw | ||
couple-lambda1 = none | ||
couple-intramol = no | ||
init-lambda-state = 0 | ||
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nstdhdl = 100 | ||
dhdl-print-energy = total | ||
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; Seed for Monte Carlo in lambda space | ||
; lmc-seed = 1000 | ||
; lmc-gibbsdelta = -1 | ||
; lmc-forced-nstart = 0 | ||
; symmetrized-transition-matrix = no | ||
; nst-transition-matrix = 100000 | ||
;wl-scale = 0.8 | ||
;wl-ratio = 0.8 | ||
;init-wl-delta = 0.5 | ||
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; expanded ensemble variables | ||
; nstexpanded = 10 | ||
; lmc-stats = no | ||
; lmc-move = metropolized-gibbs | ||
;lmc-weights-equil = wl-delta | ||
; weight-equil-wl-delta = 0.001 | ||
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; lambda-states = 1 2 3 4 5 6 7 8 | ||
vdw-lambdas = 0.00 0.18 0.42 0.57 0.68 0.76 0.86 1.00 |
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