The ELECTRIC driver has been written by Jessica Nash and Taylor Barnes, from the MolSSI. Read the documentation here.
This repository contains a driver that uses the MolSSI Driver Interface to perform electric field analysis of Tinker trajectories which use the AMOEBA forcefield. This currently works as a post-processing tool, meaning that you run simulations as normal using Tinker, then analyze the trajectories using MDI-enabled Tinker and this driver.
Using this tool, you can calculate the electric field along a bond or between atoms due to molecules or residues in the system.
To get started with ELECTRIC, you should first clone this repository:
git clone --recurse-submodules https://github.com/WelbornGroup/ELECTRIC.git
If you are using conda, you can create an environment with the appropriate dependencies using the provided environment.yaml file:
cd ELECTRIC
conda env create -f environment.yaml
Installation of ELECTRIC and MDI-enabled Tinker are bundled in one convenient build script.
./build.sh
In certain environments, it may be necessary to manually set the compilers.
This can be done when calling the build.sh script.
For example, to compile on NERSC's Cori system, you can do:
module load PrgEnv-gnu
git clone --recurse-submodules https://github.com/WelbornGroup/ELECTRIC.git
cd ELECTRIC
CC=cc FC=ftn ./build.sh
Upon successfull building, you will have the ELECTRIC driver in ELECTRIC/ELECTRIC/ELECTRIC.py, and the needed Tinker executable (dynamic.x) in ELECTRIC/modules/Tinker/build/tinker/source/dynamic.x . The location of these files can be found in text files in ELECTRIC/test/locations/ELECTRIC and ELECTRIC/test/locations/Tinker_ELECTRIC. You will need these for using ELECTRIC.
In order to run ELECTRIC, you will need to be in a python environment which has numpy and pandas installed.
If you are using conda, the provided environment.yaml and created environment will have the necessary dependencies.
If you are not using the provided conda environment, you will need to make sure that you have NumPy and pandas installed to use ELECTRIC.
You can now run a quick test of the driver by changing directory to the ELECTRIC/test/bench5 directory and running the tcp.sh script:
./tcp.sh
This script will run a short Tinker dynamics simulation that includes periodic boundary conditions. This command is on line 20 of the provided file. This is a standard Tinker call, as you would normally run a simulation. If you are performing post processing on a simulation, you will not use this line.
${TINKER_LOC} bench5 -k bench5.key 10 1.0 0.001999 2 300.00 > Dynamics.log
The script then launches an instance of Tinker as an MDI engine, which will request a connection to the driver and then listen for commands from the driver. This command is similar to running a simulation with Tinker, except that it uses a modified Tinker input file (more on this below), and adds an additional command line argument which passes information to MDI (-mdi "role ENGINE -name NO_EWALD -method TCP -port 8022 -hostname localhost"):
{TINKER_LOC} bench5 -k no_ewald.key -mdi "-role ENGINE -name NO_EWALD -method TCP -port 8022 -hostname localhost" 10 1.0 0.001999 2 300.00 > no_ewald.log &
The script will then launch an instance of the driver in the background, which will listen for connections from an MDI engine:
python ${DRIVER_LOC} -probes "1 40" -snap bench5.arc -mdi "-role DRIVER -name driver -method TCP -port 8022" --bymol &
The driver's output should match the reference output file (proj_totfield.csv) in the sample_analysis directory.
In general, running a calculation with the driver requires the following steps:
-
Run a dynamics simulation with Tinker.
This simulation should be run with periodic boundary conditions (if desired), and should print snapshots of its results to a single file (i.e.,coordinates.arc). If each snapshot was instead written to a different file (i.e.,coordinates.001,coordinates.002, etc.) then you may concatenate them into a single file. -
Create a new Tinker keyfile.
This keyfile should be identical to the one used in Step 1, except that it must not include periodic boundary conditions and must not use an Ewald summation. This means that in the.keyfile for running the driver, you should not have ana-axiskeyword, or keywords related to Ewald. -
Launch one (or more; see the
--nenginesoption below) instance(s) of Tinker as an MDI engine, using the keyfile created in Step 2.
This is done in the same way you launch a normal Tinker simulation (by launching thedynamic.xexecutable) except that the-mdicommand-line option is added. However, it is very important that the reference coordinates you use do not have periodic boundary information. So, if when you originally ran the simulation you started it with a snapshot from a previous simulation run, make sure to create a new snapshot to launch the simulation from which does not include box information on line 2.
The argument to the -mdi command-line option details how Tinker should connect to the driver; its possible arguments are described in the MDI documentation.
When in doubt, we recommend doing -mdi "-role ENGINE -name NO_EWALD -method TCP -port 8021 -hostname localhost"
When run as an engine, Tinker should be launched in the background; this is done by adding an ampersand (&) at the end of the launch line.
-
Launch the driver. The driver accepts a variety of command-line options, which are described in detail below. One possible launch command would be:
python ${DRIVER_LOC} -probes "1 2 10" -snap coordinates.arc -mdi "-role DRIVER -name driver -method TCP -port 8021" --byres ke15.pdb --equil 51 --nengines 15 &
where DRIVER_LOC is the path to ELECTRIC.py which you set during the configuration step.
The output will be written to proj_totfield.csv.
It is useful to write a script that performs Steps 3 and 4, especially if the calculations are intended to be run on a shared cluster. Such a script might look like:
# location of required codes
DRIVER_LOC=$(cat ../locations/ELECTRIC)
TINKER_LOC=$(cat ../locations/Tinker_ELECTRIC)
# number of instances of Tinker to run as an engine
nengines=18
# set the number of threads used by each code
export OMP_NUM_THREADS=1
# launch Tinker as an engine
for i in $( eval echo {1..$nengines} )
do
${TINKER_LOC} coordinates.in -k no_ewald.key -mdi "-role ENGINE -name NO_EWALD -method TCP -port 8021 -hostname localhost" 10 1.0 1.0 2 300 > no_ewald${i}.log &
done
# launch the driver
python ${DRIVER_LOC} -probes "32 33 59 60" -snap coordinates.arc -mdi "-role DRIVER -name driver -method TCP -port 8021" --byres ke15.pdb --equil 51 --nengines ${nengines} &
wait
In addition to the above examples of using TCP/IP sockets for communication between ELECTRIC and Tinker, it is also possible to establish communication between the codes using the Message Passing Interface (MPI). Information about launching codes using MPI communication is available here. This approach is likely to be preferable when running on large supercomputing clusters.
Note that on systems that manage MPI jobs using SLURM, it is necessary to use srun to launch jobs rather than direct calls to mpiexec.
Example scripts for launching on NERSC's Cori system are provided at ELECTRIC/test/bench5/cori.sh (for running with a single instance of Tinker) and ELECTRIC/test/bench5/cori5.sh (for running with multiple instances of Tinker).
Before running one of these scripts, you will need to change the --account SBATCH option to your own account.
You can see command line arguments for this driver using the following command from the top level of this repositry:
python ELECTRIC/ELECTRIC.py --help
Here is the help information for the command line arguments:
usage: ELECTRIC.py [-h] -mdi MDI -snap SNAP -probes PROBES
[--nengines NENGINES] [--equil EQUIL]
[--stride STRIDE] [--byres BYRES] [--bymol]
required arguments:
-mdi MDI flags for mdi (default: None)
-snap SNAP The file name of the trajectory to analyze. (default:
None)
-probes PROBES Atom indices which are probes for the electric field
calculations. For example, if you would like to
calculate the electric field along the bond between
atoms 1 and 2, you would use -probes "1 2". (default:
None)
optional arguments:
-h, --help show this help message and exit
--nengines NENGINES This option allows the driver to farm tasks out to
multiple Tinker engines simultaneously, enabling
parallelization of the electric field analysis
computation. The argument to this option **must** be
equal to the number of Tinker engines that are launched
along with the driver. (default: 1)
--equil EQUIL The number of frames to skip performing analysis on at
the beginning of the trajectory file (given by the -snap
argument) For example, using --equil 50 will result in
the first 50 frames of the trajectory being skipped.
(default: 0)
--stride STRIDE The number of frames to skip between analysis
calculations. For example, using --stride 2 would result
in analysis of every other frame in the trajectory.
(default: 1)
--byres BYRES Flag which indicates electric field at the probe atoms
should be calculated with electric field contributions
given per residue. If --byres is indicated, the argument
should be followed by the filename for a pdb file which
gives residues. (default: None)
--bymol Flag which indicates electric field at the probe atoms
should be calculated with electric field contributions
given per molecule. (default: False)
The driver will output a file called proj_totfield.csv. This is a CSV file which contains data on the projected electric field at the point between each probe atom due to each fragment , depending on input (--byres for by residue, --bymol for by molecule, or by atom if neither argument is given.). Each column will contain a header which indicates which probe atoms the measurement is between, followed by the frame number, while the rows will be the electric field at the mean location between the probe atoms due to a particular fragment
Consider the example (bench5), which was run with the following command:
python ${DRIVER_LOC} -probes "1 40" -snap bench5.arc -mdi "-role DRIVER -name driver -method TCP -port 8022" --bymol
Here, we have set the probe atoms to be atoms 1 and 40, and we have indicated we want the the electric field between the probe atoms based on contributions by molecule. Headers will be "i and j - frame n. Where i and j are the atom indices of the probes, and n is the frame number.
For the example, headers are:
"1 and 40 - frame 0"
"1 and 40 - frame 1"
"1 and 40 - frame 2"
"1 and 40 - frame 3"
"1 and 40 - frame 4"
Since this calculation was run using --bymol, there are 216 rows, one for each molecule in the system.
The first entry, column 1 and 40 - frame 0, header molecule 1, gives the projected total electric field at the midway point between atom 1 and atom 40 due to molecule 1. The electric field has been projected along the vector which points from atom 1 to atom 40. The projection will always be along the vector from atom 1 to atom 2. You can reverse the sign of the number if you would like the vector to point the opposite way.
A sample script which calculates the time average for each probe pair is given in the directory sample_analysis.