From: Francesco Pietra (chiendarret_at_gmail.com)
Date: Thu Jul 26 2018 - 12:54:12 CDT
Hi Jerome
During my jogging I recognized to have missed the prot ocolin my mail. I
was too late, anyway the protocol follows:
outputenergies       1000
outputtiming         1000
outputpressure       1000
restartfreq          1000
XSTFreq              1000
dcdFreq              5000
hgroupcutoff         2.8
switching            on
switchdist           10.0
cutoff               12.0
pairlistdist         14.0
wrapAll              on
langevin             on
langevintemp         300.0
langevindamping      2.0
langevinpiston       on
langevinpistontarget 1
langevinpistonperiod 100
langevinpistondecay  100
langevinpistontemp   300
StrainRate           0.0 0.0 0.0
useGroupPressure     yes
PME                  yes
PMETolerance         10e-6
PMEInterpOrder       4
PMEGridSpacing       1
timestep            0.5
fullelectfrequency   2
nonbondedfreq        1
rigidbonds           water
stepspercycle        20
alch                 on
alchType             FEP
alchFile             npt-15_frwd.fep
alchCol              B
alchOutFile          frwd-08.fepout
alchOutFreq          50
alchVdwLambdaEnd     1.0
alchElecLambdaStart  0.5
alchVdWShiftCoeff    4.0
alchEquilSteps       100000
set numSteps         400000
runFEP  0.80  1.00  0.01  $numSteps
On Thu, Jul 26, 2018 at 6:48 PM Jérôme Hénin <jerome.henin_at_ibpc.fr> wrote:
> Hi,
>
> That is more or less an expected physical effect when the excluded volume
> due to LJ repulsion disappears. In principle the soft-core potentials were
> introduced to limit this effect (that is, to spread it over a broader range
> of lambda and remove the singularity). You can try experimenting with
> softer soft-core potentials by increasing the value of alchVdwShiftCoeff
> from its default of 5 Å^2. Just note that the risk with too much softening
> is to allow atoms of opposite charges to overlap, which leads to an
> electrostatic catastrophe (singular Coulomb energy). So the goal is to keep
> the barrier high enough that those clashes don't occur as long as the
> Coulomb potential is nonzero. If you are using a protocol that separates
> the contributions entirely, that is alchElecLambdaStart
> >= alchVdwLambdaEnd, then there is no such risk and I suppose anything goes.
>
> Jerome
>
> On Thu, 26 Jul 2018 at 17:46, Francesco Pietra <chiendarret_at_gmail.com>
> wrote:
>
>> Hello
>> With every ligand-receptor FEP that I am carrying out with NAMD2.12, I
>> noticed a sudden drop in the /\A values when when approaching lambda = 1.0,
>> which seems to me prone to introducing large errors. I understand what
>> happens in the system under such conditions, however i wonder whether the
>> trend is out of the norm because I am missing some control.
>>
>> For example, for a ligand-receptor FEP divided into five sectors (in
>> order to keep the calculations for each sector within 24hr), the
>> ParseFEP.log for the 0.8-1.0 sector (lambda 0.01, 20 windows) reports
>> lambda//\A
>> ......................
>> ....................
>> 0.9000/1.2495
>> 0.9100/1.2395
>> 0.9200/1.1549
>> 0.9300/1.0130
>> 0.9400/0.6102
>> 0.9500/-0.0087
>> 0.9600/-1.8900
>> 0.9700/-3.8335
>> 0.9800/-6.8530
>> 0.9900/-10.5326
>> 1.0000/-15.9730
>>
>> Thanks for advice
>> francesco pietra
>>
>
This archive was generated by hypermail 2.1.6 : Tue Dec 31 2019 - 23:20:07 CST