abpo (c47b1)
Adaptively Biased Path Optimization (ABPO) Method
He Huang
Bradley M. Dickson
Carol B. Post
* Description | Introduction and algorithm
* Syntax | Description of commands and options
* Remarks | Implementation remarks
* Examples | Usage examples
* References | References
He Huang
Bradley M. Dickson
Carol B. Post
* Description | Introduction and algorithm
* Syntax | Description of commands and options
* Remarks | Implementation remarks
* Examples | Usage examples
* References | References
Top
Introduction and Algorithm.
ABPO is a path optimization method that works in collective variable (CV) space.
It combines the optimization algorithm of the finite temperature string (FTS)
method and the sampling power of an adaptive biasing potential (ABP) scheme.
In a multi-dimensional CV space, it finds transition paths between two
meta-stable regions, and provides the potential of mean force (PMF) along the
path. When applied to a one-dimensional CV space, it can be used as a pure
sampling approach to evaluate the PMF associated with the single CV.
For path optimization, ABPO uses the iterative scheme of the FTS method to
evolve an initial path to the principal curve associated with the system. In
each iteration, the vicinity of the current path is sampled, and the mean
positions of the sampling on the hyperplanes perpendicular to the path are
calculated. The path is then updated to the curve connecting these mean
positions. At convergence, the path recovers the principal curve.
Within each iteration, sampling is carried out with an ABP scheme which is both
flexible and efficient. Unlike the original FTS method, which performs
independent samplings each restricted to a discrete hyperplane or cell
perpendicular to the path, ABPO allows dynamics trajectories to diffuse along
the path. It only restricts the sampling dynamics within the tube-shaped space
around the path by applying a one-sided harmonic tube-wall potential.
Moreover, the diffusion in the direction of the path is accelerated by the
following adaptive biasing potential:
Vb = kb * T * b / (1 - b) * ln[c * h(lambda, t) + 1], (1)
where h is a mollified/smoothed histogram counting the samples that fall around
each slice of the path tube parameterized by lambda, the arc-length along the
path. Vb learns from the sampling history recorded in h to offset the original
potential of mean force (PMF) of lambda. The parameter b ranges from 0.0 to 1.0
and controls the bias strength. At convergence, Vb approaches -b times the PMF
of lambda. The parameter c controls how tightly Vb and h are coupled. Specifying
a finite number for c is equivalent to 'pre-deposit' some visits or time evenly
into all bins of the histogram to avoid fast change of Vb at the beginning of
the sampling.
The sampling is further aided by running multiple dynamics trajectories/replicas
in parallel. At the beginning of each iteration, ABPO launches a number of
independent adaptively biased dynamics trajectories, which proceed in blocks of
timesteps. At the end of each block, the histograms from all trajectories are
pooled together to check whether all tube slices have been sampled for at least
a certain amount of time. When the sampling threshold is reached, the path is
updated to the combined mean positions and the PMF is calculated from the
combined histogram.
As in FTS, ABPO treats the collective variable space as a skewed space in which
distance is measured with respect to the inverse of a pseudo-diffusion tensor D.
Such a treatment allows the principal curve to be invariant upon a change of
variable within the collective variable space. In the current scheme, we assume
D as constant and evaluate it with unbiased dynamics before initiating any path
optimization.
The following flow chart summarizes the optimization algorithm:
1. Current path = initial path.
2. While not converged, repeat:
2.1. Launch n independent ABP trajectories in the current path tube.
2.2. While sampling threshold not reached, repeat:
2.2.1. Run N steps of biased dynamics with each trajectory.
2.3. Pool samples from all trajectories together, calculate PMF from the
combined histogram, update the current path to the mean sampling
positions on the tube slices.
Introduction and Algorithm.
ABPO is a path optimization method that works in collective variable (CV) space.
It combines the optimization algorithm of the finite temperature string (FTS)
method and the sampling power of an adaptive biasing potential (ABP) scheme.
In a multi-dimensional CV space, it finds transition paths between two
meta-stable regions, and provides the potential of mean force (PMF) along the
path. When applied to a one-dimensional CV space, it can be used as a pure
sampling approach to evaluate the PMF associated with the single CV.
For path optimization, ABPO uses the iterative scheme of the FTS method to
evolve an initial path to the principal curve associated with the system. In
each iteration, the vicinity of the current path is sampled, and the mean
positions of the sampling on the hyperplanes perpendicular to the path are
calculated. The path is then updated to the curve connecting these mean
positions. At convergence, the path recovers the principal curve.
Within each iteration, sampling is carried out with an ABP scheme which is both
flexible and efficient. Unlike the original FTS method, which performs
independent samplings each restricted to a discrete hyperplane or cell
perpendicular to the path, ABPO allows dynamics trajectories to diffuse along
the path. It only restricts the sampling dynamics within the tube-shaped space
around the path by applying a one-sided harmonic tube-wall potential.
Moreover, the diffusion in the direction of the path is accelerated by the
following adaptive biasing potential:
Vb = kb * T * b / (1 - b) * ln[c * h(lambda, t) + 1], (1)
where h is a mollified/smoothed histogram counting the samples that fall around
each slice of the path tube parameterized by lambda, the arc-length along the
path. Vb learns from the sampling history recorded in h to offset the original
potential of mean force (PMF) of lambda. The parameter b ranges from 0.0 to 1.0
and controls the bias strength. At convergence, Vb approaches -b times the PMF
of lambda. The parameter c controls how tightly Vb and h are coupled. Specifying
a finite number for c is equivalent to 'pre-deposit' some visits or time evenly
into all bins of the histogram to avoid fast change of Vb at the beginning of
the sampling.
The sampling is further aided by running multiple dynamics trajectories/replicas
in parallel. At the beginning of each iteration, ABPO launches a number of
independent adaptively biased dynamics trajectories, which proceed in blocks of
timesteps. At the end of each block, the histograms from all trajectories are
pooled together to check whether all tube slices have been sampled for at least
a certain amount of time. When the sampling threshold is reached, the path is
updated to the combined mean positions and the PMF is calculated from the
combined histogram.
As in FTS, ABPO treats the collective variable space as a skewed space in which
distance is measured with respect to the inverse of a pseudo-diffusion tensor D.
Such a treatment allows the principal curve to be invariant upon a change of
variable within the collective variable space. In the current scheme, we assume
D as constant and evaluate it with unbiased dynamics before initiating any path
optimization.
The following flow chart summarizes the optimization algorithm:
1. Current path = initial path.
2. While not converged, repeat:
2.1. Launch n independent ABP trajectories in the current path tube.
2.2. While sampling threshold not reached, repeat:
2.2.1. Run N steps of biased dynamics with each trajectory.
2.3. Pool samples from all trajectories together, calculate PMF from the
combined histogram, update the current path to the mean sampling
positions on the tube slices.
Top
Description of Commands and Options
As mentioned above, multiple trajectories/replicas may be used to enhance the
sampling process. ABPO takes use of the communication layer provided by the
ensemble module to realize inter-replica communication. It is therefore
implemented as a subcommand of the ENSEmble command. When compiling CHARMM, the
ABPO method is built by adding the option '--with-abpo', e.g.
$> ./configure --with-abpo
$> make -C build/cmake install
The ABPO options activate ENSEmble automatically, and therefore requires MPI.
Before running ABPO, the NENSem keyword of the ENSEemble command needs to be
called to specify the number of replicas. Note that NENSem has to be a factor of
the total number of processes.
Following is the Syntax of the ABPO command:
ENSEmble ABPO { SETCv repeat ( cv-spec ) }
{ DTNS dtns-spec }
{ OPTI opti-spec }
It has three sub-commands, each associated with one of the following three steps
involved in a complete optimization process: (1) Define collective variables.
(2) Evaluate the D tensor. (3) Optimize the path. These sub-commands and
available options are describe below:
---------------------------------------------------------------------------
ENSEmble ABPO SETCv repeat ( cv-spec )
cv-spec = { DIST NP int repeat ( real atom-spec x 2 ) }
{ DSEL atom-selection x 2 }
{ ASEL atom-selection x 3 }
{ TSEL atom-selection x 4 }
atom-spec = { segid resid iupac }
---------------------------------------------------------------------------
This command defines the collective variables (CVs), each specified with a
cv-spec statement. In the current version, a CV can be one of the following
types:
[DIST] specifies a CV as a linear combination of a set of internal distances:
CV_dist = sum_i c_i * d_i
[NP int] specifies the number of distances that go into the linear
combination. Each individual distance is specified by a [real atom-spec
x 2] statement, which gives the coefficient c_i as a real number, and
specifies the two atoms that define d_i.
[DSEL] specifies a CV as the distance between the centers-of-mass of two
atom-selections. The distance is represented in the unit of angstroms.
[ASEL] specifies a CV as the angle formed by the centers-of-mass of three
atom-selections. The angle is represented in radius and ranges from zero
to pi.
[TSEL] specifies a CV as the torsion angle formed by the centers-of-mass of four
atom-selections. The torsion angle is represented in radius and ranges
from -pi to pi.
---------------------------------------------------------------------------
ENSEmble ABPO DTNS dtns-spec
dtns-spec = [DSTEps int] [DFRQ int]
---------------------------------------------------------------------------
This command sets up options for evaluating the D tensor. Before invoking
DTNS, at least one CV has to be defined.
The following table describes the options that apply to DTNS:
Keyword Default Purpose
DSTEps 1000 Length of dynamics in timesteps for evaluating D.
DFRQ 100 Interval in timesteps at which the instantaneous value of D
is evaluated.
While the DTNS command sets up D evaluation options, it does not trigger any
dynamics run. The dynamics run will be triggered by the next DYNAmics command
(» dynamc ). The NSTE option of the DYNA command will be ignored and the
number specified by DSTEps in the DTNS command will be used as the number of
timesteps. The IUNC and IUNW options will also be ignored. When the dynamics
run finishes, a file named invd.dat will be generated under the current
directory, which stores the inverse of the evaluated D tensor.
Running the DTNS command generates the following data under the current
directory:
- [FILE] invd.dat: inverse of the D tensor
- [DIR] eval_d: directory that includes:
- [FILE] repXXX.dcd: trajectory file for replica XXX
- [FILE] repXXX.rst: restart file for replica XXX
---------------------------------------------------------------------------
ENSEmble ABPO OPTI opti-sepc
opti-spec = [REST] [BCYC int] [ECYC int] [TEMP real] -
[MNBL int] [BSTE int] [MINC real] [SMOO real] -
[NPNT int] [MOLL real] [RTUB real] [FTUB real] [LOOP] -
[BFCT real] [CFCT real] [CVFR int]
---------------------------------------------------------------------------
This command sets up options for path optimization. Before invoking OPTI, the
CVs have to be defined and the invd.dat file has to be present under the current
directory.
The following table describes the options that apply to OPTI:
Keyword Default Purpose
BCYC 1 Index of the starting cycle.
ECYC BCYC Index of the ending cycle.
REST false When present, restart a previous optimization run. Load
restarting information from the path.snap file under the
directory for BCYC.
TEMP 300.0 Temperature. Should be the same as the dynamics
temperature.
MNBL 20 Maximal number of dynamics blocks to run in each
optimization cycle.
BSTE 1000 Number of timesteps to run in each dynamics block.
MINC 100 Sampling threshold in timesteps. Update the path and enter
the next cycle when the histogram reaches this value
everywhere along the path.
NPNT 100 Number of points the path is discretized into.
MOLL 0.05 Ratio of the standard deviation of the Gaussian mollifier
used to smooth the histogram to total path length.
RTUB 1.0 Radius of the path tube in (angstrom g^{1/2}).
Note that distance is measured with respect to D^{-1}.
FTUB 1.0 Force constant of the tube wall potential in (kcal/g/angstrom^2).
Again, note that distance is measured with respect to D^{-1},
therefore FTUB should be adjusted according to D^{-1} to achieve
desired restraining strength. Rule of thumb is to use a smaller
FTUB when the norm of D^{-1} is large, and vise versa.
LOOP false When present, treat the path as a loop, i.e., treat the
two end points as neighbors.
BFCT 0.8 Strength of the adaptive bias, which ranges from 0.0 to 1.0.
Same as the parameter b in Eqn (1). The dynamics is
unbiased with value 0.0, analogous to metadynamics with
value 1.0, and analogous to well-tempered metadynamics
with values in between. (see Ref [2])
PRED 1000 Total timesteps that are 'pre-deposited' into the histogram.
This number divided by NPNT is the time deposited into
each tube-slice at the beginning of each cycle.
SMOO 0.05 Ratio of the standard deviation of the Gaussian mollifier
used to smooth the path to total path length.
CVFR 100 Frequency for outputing the positions in the collective variable
space
Like the DTNS command, the OPTI command does not trigger any dynamics run.
Instead, the dynamics run will be triggered by the next DYNAmics command.
The NSTE option of the DYNA command will be ignored and the length of the
dynamics will be controlled by options specified with the OPTI command.
Running the OPTI command generates the following data under the current directory:
- [DIR] cycXXX: directory for cycle XXX, includes:
- [FILE] mean.dat: mean sampling positions on all tube slices
- [FILE] smean.dat: mean.dat after smoothing, initial path for next cycle
- [FILE] pmf.dat: PMF with respect to path arc length
- [DIR] repXXX: directory for replica XXX, includes:
- [FILE] blockXXX.dcd: trajectory file for dynamics block XXX
- [FILE] blockXXX.rst: restart file for dynamics block XXX
- [FILE] blockXXX.cv: trajectory in the collective variable space
Description of Commands and Options
As mentioned above, multiple trajectories/replicas may be used to enhance the
sampling process. ABPO takes use of the communication layer provided by the
ensemble module to realize inter-replica communication. It is therefore
implemented as a subcommand of the ENSEmble command. When compiling CHARMM, the
ABPO method is built by adding the option '--with-abpo', e.g.
$> ./configure --with-abpo
$> make -C build/cmake install
The ABPO options activate ENSEmble automatically, and therefore requires MPI.
Before running ABPO, the NENSem keyword of the ENSEemble command needs to be
called to specify the number of replicas. Note that NENSem has to be a factor of
the total number of processes.
Following is the Syntax of the ABPO command:
ENSEmble ABPO { SETCv repeat ( cv-spec ) }
{ DTNS dtns-spec }
{ OPTI opti-spec }
It has three sub-commands, each associated with one of the following three steps
involved in a complete optimization process: (1) Define collective variables.
(2) Evaluate the D tensor. (3) Optimize the path. These sub-commands and
available options are describe below:
---------------------------------------------------------------------------
ENSEmble ABPO SETCv repeat ( cv-spec )
cv-spec = { DIST NP int repeat ( real atom-spec x 2 ) }
{ DSEL atom-selection x 2 }
{ ASEL atom-selection x 3 }
{ TSEL atom-selection x 4 }
atom-spec = { segid resid iupac }
---------------------------------------------------------------------------
This command defines the collective variables (CVs), each specified with a
cv-spec statement. In the current version, a CV can be one of the following
types:
[DIST] specifies a CV as a linear combination of a set of internal distances:
CV_dist = sum_i c_i * d_i
[NP int] specifies the number of distances that go into the linear
combination. Each individual distance is specified by a [real atom-spec
x 2] statement, which gives the coefficient c_i as a real number, and
specifies the two atoms that define d_i.
[DSEL] specifies a CV as the distance between the centers-of-mass of two
atom-selections. The distance is represented in the unit of angstroms.
[ASEL] specifies a CV as the angle formed by the centers-of-mass of three
atom-selections. The angle is represented in radius and ranges from zero
to pi.
[TSEL] specifies a CV as the torsion angle formed by the centers-of-mass of four
atom-selections. The torsion angle is represented in radius and ranges
from -pi to pi.
---------------------------------------------------------------------------
ENSEmble ABPO DTNS dtns-spec
dtns-spec = [DSTEps int] [DFRQ int]
---------------------------------------------------------------------------
This command sets up options for evaluating the D tensor. Before invoking
DTNS, at least one CV has to be defined.
The following table describes the options that apply to DTNS:
Keyword Default Purpose
DSTEps 1000 Length of dynamics in timesteps for evaluating D.
DFRQ 100 Interval in timesteps at which the instantaneous value of D
is evaluated.
While the DTNS command sets up D evaluation options, it does not trigger any
dynamics run. The dynamics run will be triggered by the next DYNAmics command
(» dynamc ). The NSTE option of the DYNA command will be ignored and the
number specified by DSTEps in the DTNS command will be used as the number of
timesteps. The IUNC and IUNW options will also be ignored. When the dynamics
run finishes, a file named invd.dat will be generated under the current
directory, which stores the inverse of the evaluated D tensor.
Running the DTNS command generates the following data under the current
directory:
- [FILE] invd.dat: inverse of the D tensor
- [DIR] eval_d: directory that includes:
- [FILE] repXXX.dcd: trajectory file for replica XXX
- [FILE] repXXX.rst: restart file for replica XXX
---------------------------------------------------------------------------
ENSEmble ABPO OPTI opti-sepc
opti-spec = [REST] [BCYC int] [ECYC int] [TEMP real] -
[MNBL int] [BSTE int] [MINC real] [SMOO real] -
[NPNT int] [MOLL real] [RTUB real] [FTUB real] [LOOP] -
[BFCT real] [CFCT real] [CVFR int]
---------------------------------------------------------------------------
This command sets up options for path optimization. Before invoking OPTI, the
CVs have to be defined and the invd.dat file has to be present under the current
directory.
The following table describes the options that apply to OPTI:
Keyword Default Purpose
BCYC 1 Index of the starting cycle.
ECYC BCYC Index of the ending cycle.
REST false When present, restart a previous optimization run. Load
restarting information from the path.snap file under the
directory for BCYC.
TEMP 300.0 Temperature. Should be the same as the dynamics
temperature.
MNBL 20 Maximal number of dynamics blocks to run in each
optimization cycle.
BSTE 1000 Number of timesteps to run in each dynamics block.
MINC 100 Sampling threshold in timesteps. Update the path and enter
the next cycle when the histogram reaches this value
everywhere along the path.
NPNT 100 Number of points the path is discretized into.
MOLL 0.05 Ratio of the standard deviation of the Gaussian mollifier
used to smooth the histogram to total path length.
RTUB 1.0 Radius of the path tube in (angstrom g^{1/2}).
Note that distance is measured with respect to D^{-1}.
FTUB 1.0 Force constant of the tube wall potential in (kcal/g/angstrom^2).
Again, note that distance is measured with respect to D^{-1},
therefore FTUB should be adjusted according to D^{-1} to achieve
desired restraining strength. Rule of thumb is to use a smaller
FTUB when the norm of D^{-1} is large, and vise versa.
LOOP false When present, treat the path as a loop, i.e., treat the
two end points as neighbors.
BFCT 0.8 Strength of the adaptive bias, which ranges from 0.0 to 1.0.
Same as the parameter b in Eqn (1). The dynamics is
unbiased with value 0.0, analogous to metadynamics with
value 1.0, and analogous to well-tempered metadynamics
with values in between. (see Ref [2])
PRED 1000 Total timesteps that are 'pre-deposited' into the histogram.
This number divided by NPNT is the time deposited into
each tube-slice at the beginning of each cycle.
SMOO 0.05 Ratio of the standard deviation of the Gaussian mollifier
used to smooth the path to total path length.
CVFR 100 Frequency for outputing the positions in the collective variable
space
Like the DTNS command, the OPTI command does not trigger any dynamics run.
Instead, the dynamics run will be triggered by the next DYNAmics command.
The NSTE option of the DYNA command will be ignored and the length of the
dynamics will be controlled by options specified with the OPTI command.
Running the OPTI command generates the following data under the current directory:
- [DIR] cycXXX: directory for cycle XXX, includes:
- [FILE] mean.dat: mean sampling positions on all tube slices
- [FILE] smean.dat: mean.dat after smoothing, initial path for next cycle
- [FILE] pmf.dat: PMF with respect to path arc length
- [DIR] repXXX: directory for replica XXX, includes:
- [FILE] blockXXX.dcd: trajectory file for dynamics block XXX
- [FILE] blockXXX.rst: restart file for dynamics block XXX
- [FILE] blockXXX.cv: trajectory in the collective variable space
Top
Implementation Remarks
The ABPO module does not supply a standard mechanism to detect convergence of
the optimization process. The user may monitor the progress by plotting any
meaningful metric of the distance between the current path and each previous
path (For example, see Ref [1]). Ideally, such distance curve should go to zero
while convergence is approached. In practice with the presence of sampling
error, the distance curve approaches a non-zero plateau, the height of which
depends on the specific system as well as sampling accuracy.
In the current version, the OPTI command can only be called for once in a single
optimization with first a larger then a smaller RTUB is desired, do it in two
seperate runs.
Implementation Remarks
The ABPO module does not supply a standard mechanism to detect convergence of
the optimization process. The user may monitor the progress by plotting any
meaningful metric of the distance between the current path and each previous
path (For example, see Ref [1]). Ideally, such distance curve should go to zero
while convergence is approached. In practice with the presence of sampling
error, the distance curve approaches a non-zero plateau, the height of which
depends on the specific system as well as sampling accuracy.
In the current version, the OPTI command can only be called for once in a single
optimization with first a larger then a smaller RTUB is desired, do it in two
seperate runs.
Top
Usage Examples
Note: to keep things easy, ABPO always assumes the current directory, i.e, the
directory where CHARMM is launched as the working directory. Input files
(init.dat and invd.dat) will be searched there, and all output files will be
directed there. Make sure to 'cd' into the desired working directory before
running CHARMM.
1) Optimize a path for the transition of the alanine dipeptide between
its configurations C7eq and C7ax with four replicas. init.dat specifies
a straight line, and reads:
-1.45 1.30
1.22 -1.22
!-----------------------------------------------------------------------------------
! Load parameter, topology, psf and coornidate files
! Setup nonbond interactions
set temp 300
scalar fbeta set 5 sele all end
ensemble nensem 4
ensemble abpo setcv -
tsel sele type clp end sele type nl end sele type ca end sele type crp end -
tsel sele type nl end sele type ca end sele type crp end sele type nr end
! Evaluate the D
ensemble abpo dtns dsteps 50000
dyna leap lang tbath @temp timestep 0.001 -
nsavc 100 nprint 1000 IPRFrq 10000
! Run path optimization
ensemble abpo opti -
temp @temp bcyc 1 ecyc 10 npnt 500 moll 0.05 bfct 0.90 pred 500 -
rtube 0.2 ftube 50.0 smooth 0.05 -
mnblock 40 bstep 10000 minc 50
dyna leap lang tbath @temp timestep 0.001 -
nsavc 100 nprint 1000 IPRFrq 10000
2) Restart the calculation of 1) and optimize for ten more cycles
!-----------------------------------------------------------------------------------
! Load parameter, topology, psf
! Coornidate will be loaded from the .rst files saved under cyc010/repXXX
! Setup nonbond interactions
set temp 300
scalar fbeta set 5 sele all end
ensemble nensem 4
ensemble abpo setcv -
tsel sele type clp end sele type nl end sele type ca end sele type crp end -
tsel sele type nl end sele type ca end sele type crp end sele type nr end
! No need to run dtns again because invd.dat is already generated in the previous run
ensemble abpo opti rest bcyc 10 ecyc 20
dyna leap lang tbath @temp timestep 0.001 -
nsavc 100 nprint 1000 iprfrq 10000
3) Calculate the pmf of two sodium ions in vacuum as a function of the distance
between them. Use ten replicas. init.dat specifies the distance range, and reads:
2.00 10.00
!-----------------------------------------------------------------------------------
! Load parameter, topology, psf and coornidate files
! Setup nonbond interactions
set temp 300
scalar fbeta set 5 sele all end
ensemble nensem 4
ensemble abpo setcv -
tsel sele type clp end sele type nl end sele type ca end sele type crp end -
tsel sele type nl end sele type ca end sele type crp end sele type nr end
! For one-dimensional CV space, 'ensemble abpo dtns' may be ommitted by
! manually creating a file named invd.dat that holds a single number 1.0.
ensemble abpo opti -
temp @temp bcyc 1 ecyc 1 npnt 500 moll 0.05 bfct 0.90 pred 500 -
rtube 0.0 ftube 10.0 smooth 0.05 -
mnblock 40 bstep 100000 minc 500
dyna leap lang tbath @temp timestep 0.001 -
nsavc 100 nprint 1000 iprfrq 10000
Testcase: c38test/abpo.inp
Usage Examples
Note: to keep things easy, ABPO always assumes the current directory, i.e, the
directory where CHARMM is launched as the working directory. Input files
(init.dat and invd.dat) will be searched there, and all output files will be
directed there. Make sure to 'cd' into the desired working directory before
running CHARMM.
1) Optimize a path for the transition of the alanine dipeptide between
its configurations C7eq and C7ax with four replicas. init.dat specifies
a straight line, and reads:
-1.45 1.30
1.22 -1.22
!-----------------------------------------------------------------------------------
! Load parameter, topology, psf and coornidate files
! Setup nonbond interactions
set temp 300
scalar fbeta set 5 sele all end
ensemble nensem 4
ensemble abpo setcv -
tsel sele type clp end sele type nl end sele type ca end sele type crp end -
tsel sele type nl end sele type ca end sele type crp end sele type nr end
! Evaluate the D
ensemble abpo dtns dsteps 50000
dyna leap lang tbath @temp timestep 0.001 -
nsavc 100 nprint 1000 IPRFrq 10000
! Run path optimization
ensemble abpo opti -
temp @temp bcyc 1 ecyc 10 npnt 500 moll 0.05 bfct 0.90 pred 500 -
rtube 0.2 ftube 50.0 smooth 0.05 -
mnblock 40 bstep 10000 minc 50
dyna leap lang tbath @temp timestep 0.001 -
nsavc 100 nprint 1000 IPRFrq 10000
2) Restart the calculation of 1) and optimize for ten more cycles
!-----------------------------------------------------------------------------------
! Load parameter, topology, psf
! Coornidate will be loaded from the .rst files saved under cyc010/repXXX
! Setup nonbond interactions
set temp 300
scalar fbeta set 5 sele all end
ensemble nensem 4
ensemble abpo setcv -
tsel sele type clp end sele type nl end sele type ca end sele type crp end -
tsel sele type nl end sele type ca end sele type crp end sele type nr end
! No need to run dtns again because invd.dat is already generated in the previous run
ensemble abpo opti rest bcyc 10 ecyc 20
dyna leap lang tbath @temp timestep 0.001 -
nsavc 100 nprint 1000 iprfrq 10000
3) Calculate the pmf of two sodium ions in vacuum as a function of the distance
between them. Use ten replicas. init.dat specifies the distance range, and reads:
2.00 10.00
!-----------------------------------------------------------------------------------
! Load parameter, topology, psf and coornidate files
! Setup nonbond interactions
set temp 300
scalar fbeta set 5 sele all end
ensemble nensem 4
ensemble abpo setcv -
tsel sele type clp end sele type nl end sele type ca end sele type crp end -
tsel sele type nl end sele type ca end sele type crp end sele type nr end
! For one-dimensional CV space, 'ensemble abpo dtns' may be ommitted by
! manually creating a file named invd.dat that holds a single number 1.0.
ensemble abpo opti -
temp @temp bcyc 1 ecyc 1 npnt 500 moll 0.05 bfct 0.90 pred 500 -
rtube 0.0 ftube 10.0 smooth 0.05 -
mnblock 40 bstep 100000 minc 500
dyna leap lang tbath @temp timestep 0.001 -
nsavc 100 nprint 1000 iprfrq 10000
Testcase: c38test/abpo.inp
Top
References
[1] Dickson, B. M.; Huang, H. & Post, C. B.
Unrestrained computation of free energy along a path.
J Phys Chem B, 2012, 116, 11046-11055
[2] Dickson, B. M.
Approaching a parameter-free metadynamics.
Phys Rev E, 2011, 84, 037701
References
[1] Dickson, B. M.; Huang, H. & Post, C. B.
Unrestrained computation of free energy along a path.
J Phys Chem B, 2012, 116, 11046-11055
[2] Dickson, B. M.
Approaching a parameter-free metadynamics.
Phys Rev E, 2011, 84, 037701