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September 22, 2021 14:55
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{ | |
"cells": [ | |
{ | |
"cell_type": "code", | |
"execution_count": 1, | |
"id": "970ed216", | |
"metadata": {}, | |
"outputs": [ | |
{ | |
"name": "stderr", | |
"output_type": "stream", | |
"text": [ | |
"Warning: importing 'simtk.openmm' is deprecated. Import 'openmm' instead.\n" | |
] | |
} | |
], | |
"source": [ | |
"import time\n", | |
"import os\n", | |
"import pickle\n", | |
"\n", | |
"from simtk.openmm import XmlSerializer\n", | |
"from simtk import openmm\n", | |
"from simtk.openmm import app, unit\n", | |
"import openmmtools" | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"id": "269645ac", | |
"metadata": {}, | |
"source": [ | |
"# Check computation time for setUseDispersionCorrection(True) for only the NonbondedForce that contains nonalchemical atoms, but not the CustomNonbondedForce that contains alchemical atoms" | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"id": "378e7055", | |
"metadata": {}, | |
"source": [ | |
"Use long-range env" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 9, | |
"id": "09632b1e", | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"with open('rbd_ace2_example/rbd_ace2_hybrid_system.xml', 'r') as f:\n", | |
" system = XmlSerializer.deserialize(f.read())\n", | |
"with open('rbd_ace2_example/rbd_ace2_state.xml', 'r') as f:\n", | |
" state = XmlSerializer.deserialize(f.read())" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 10, | |
"id": "0848171e", | |
"metadata": { | |
"scrolled": true | |
}, | |
"outputs": [ | |
{ | |
"data": { | |
"text/plain": [ | |
"[<openmm.openmm.MonteCarloBarostat; proxy of <Swig Object of type 'OpenMM::MonteCarloBarostat *' at 0x2b04dbf2eed0> >,\n", | |
" <openmm.openmm.CustomBondForce; proxy of <Swig Object of type 'OpenMM::CustomBondForce *' at 0x2b04dbf2e1b0> >,\n", | |
" <openmm.openmm.HarmonicBondForce; proxy of <Swig Object of type 'OpenMM::HarmonicBondForce *' at 0x2b04dbf2e0f0> >,\n", | |
" <openmm.openmm.CustomAngleForce; proxy of <Swig Object of type 'OpenMM::CustomAngleForce *' at 0x2b051d42dba0> >,\n", | |
" <openmm.openmm.HarmonicAngleForce; proxy of <Swig Object of type 'OpenMM::HarmonicAngleForce *' at 0x2b051d42de10> >,\n", | |
" <openmm.openmm.CustomTorsionForce; proxy of <Swig Object of type 'OpenMM::CustomTorsionForce *' at 0x2b051d42d8d0> >,\n", | |
" <openmm.openmm.PeriodicTorsionForce; proxy of <Swig Object of type 'OpenMM::PeriodicTorsionForce *' at 0x2b051d42dcf0> >,\n", | |
" <openmm.openmm.NonbondedForce; proxy of <Swig Object of type 'OpenMM::NonbondedForce *' at 0x2b051d42d120> >,\n", | |
" <openmm.openmm.CustomNonbondedForce; proxy of <Swig Object of type 'OpenMM::CustomNonbondedForce *' at 0x2b051d42da80> >,\n", | |
" <openmm.openmm.CustomBondForce; proxy of <Swig Object of type 'OpenMM::CustomBondForce *' at 0x2b051d42dc90> >]" | |
] | |
}, | |
"execution_count": 10, | |
"metadata": {}, | |
"output_type": "execute_result" | |
} | |
], | |
"source": [ | |
"system.getForces()" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 11, | |
"id": "aacc7cd7", | |
"metadata": {}, | |
"outputs": [ | |
{ | |
"data": { | |
"text/plain": [ | |
"True" | |
] | |
}, | |
"execution_count": 11, | |
"metadata": {}, | |
"output_type": "execute_result" | |
} | |
], | |
"source": [ | |
"system.getForce(7).getUseDispersionCorrection()" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 12, | |
"id": "a2eda49f", | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"system.getForce(8).setUseLongRangeCorrection(False)" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 13, | |
"id": "b48b609f", | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"# Set up integrator\n", | |
"integrator = openmmtools.integrators.LangevinIntegrator(temperature=300 * unit.kelvin, \n", | |
" collision_rate=1 / unit.picoseconds, \n", | |
" timestep=4 * unit.femtoseconds)\n" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 14, | |
"id": "8e72cca6", | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"# Set up context\n", | |
"platform_name = 'CUDA'\n", | |
"platform = openmm.Platform.getPlatformByName(platform_name)\n", | |
"if platform_name in ['CUDA', 'OpenCL']:\n", | |
" platform.setPropertyDefaultValue('Precision', 'mixed')\n", | |
"if platform_name in ['CUDA']:\n", | |
" platform.setPropertyDefaultValue('DeterministicForces', 'true')\n", | |
"context = openmm.Context(system, integrator, platform)\n", | |
"context.setPeriodicBoxVectors(*state.getPeriodicBoxVectors())\n", | |
"context.setPositions(state.getPositions())\n", | |
"context.setVelocitiesToTemperature(300 * unit.kelvin)" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 15, | |
"id": "8381169b", | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"nsteps = 100\n", | |
"initial_time = time.time()\n", | |
"for step in range(nsteps):\n", | |
" context.setParameter('lambda_sterics_insert', (step + 1) * 0.01)\n", | |
" integrator.step(1)\n", | |
"elapsed_time = (time.time() - initial_time) * unit.seconds" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 16, | |
"id": "6ec993d7", | |
"metadata": {}, | |
"outputs": [ | |
{ | |
"data": { | |
"text/plain": [ | |
"Quantity(value=8.10090708732605, unit=second)" | |
] | |
}, | |
"execution_count": 16, | |
"metadata": {}, | |
"output_type": "execute_result" | |
} | |
], | |
"source": [ | |
"elapsed_time" | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"id": "8bbdd964", | |
"metadata": {}, | |
"source": [ | |
"# Check computation time for setLongRangeCorrection(True) for both CustomNonbondedForces" | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"id": "277b2307", | |
"metadata": {}, | |
"source": [ | |
"Use long-range env" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 14, | |
"id": "9e939bce", | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"with open('rbd_ace2_example/rbd_ace2_hybrid_system.xml', 'r') as f:\n", | |
" system = XmlSerializer.deserialize(f.read())\n", | |
"with open('rbd_ace2_example/rbd_ace2_state.xml', 'r') as f:\n", | |
" state = XmlSerializer.deserialize(f.read())" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 16, | |
"id": "4f66d4b3", | |
"metadata": {}, | |
"outputs": [ | |
{ | |
"data": { | |
"text/plain": [ | |
"True" | |
] | |
}, | |
"execution_count": 16, | |
"metadata": {}, | |
"output_type": "execute_result" | |
} | |
], | |
"source": [ | |
"system.getForce(7).getUseDispersionCorrection()" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 15, | |
"id": "0c8fc258", | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"system.getForce(8).setUseLongRangeCorrection(True)" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 17, | |
"id": "2bae6f98", | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"# Set up integrator\n", | |
"integrator = openmmtools.integrators.LangevinIntegrator(temperature=300 * unit.kelvin, \n", | |
" collision_rate=1 / unit.picoseconds, \n", | |
" timestep=4 * unit.femtoseconds)\n" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 18, | |
"id": "881624d3", | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"# Set up context\n", | |
"platform_name = 'CUDA'\n", | |
"platform = openmm.Platform.getPlatformByName(platform_name)\n", | |
"if platform_name in ['CUDA', 'OpenCL']:\n", | |
" platform.setPropertyDefaultValue('Precision', 'mixed')\n", | |
"if platform_name in ['CUDA']:\n", | |
" platform.setPropertyDefaultValue('DeterministicForces', 'true')\n", | |
"context = openmm.Context(system, integrator, platform)\n", | |
"context.setPeriodicBoxVectors(*state.getPeriodicBoxVectors())\n", | |
"context.setPositions(state.getPositions())\n", | |
"context.setVelocitiesToTemperature(300 * unit.kelvin)" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 19, | |
"id": "aadbe82a", | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"nsteps = 100\n", | |
"initial_time = time.time()\n", | |
"for step in range(nsteps):\n", | |
" context.setParameter('lambda_sterics_insert', (step + 1) * 0.01)\n", | |
" integrator.step(1)\n", | |
"elapsed_time = (time.time() - initial_time) * unit.seconds" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 20, | |
"id": "57ee6d31", | |
"metadata": {}, | |
"outputs": [ | |
{ | |
"data": { | |
"text/plain": [ | |
"Quantity(value=36.05855202674866, unit=second)" | |
] | |
}, | |
"execution_count": 20, | |
"metadata": {}, | |
"output_type": "execute_result" | |
} | |
], | |
"source": [ | |
"elapsed_time" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": null, | |
"id": "8c22e1d5", | |
"metadata": {}, | |
"outputs": [], | |
"source": [] | |
}, | |
{ | |
"cell_type": "markdown", | |
"id": "e26b353e", | |
"metadata": {}, | |
"source": [ | |
"# Check computation time for setLongRangeCorrection(True) for both CustomNonbondedForces (and with Peter's fix)" | |
] | |
}, | |
{ | |
"cell_type": "markdown", | |
"id": "99e6326c", | |
"metadata": {}, | |
"source": [ | |
"Use long-range-peter env" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 2, | |
"id": "f3c7ac6d", | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"with open('rbd_ace2_example/rbd_ace2_hybrid_system.xml', 'r') as f:\n", | |
" system = XmlSerializer.deserialize(f.read())\n", | |
"with open('rbd_ace2_example/rbd_ace2_state.xml', 'r') as f:\n", | |
" state = XmlSerializer.deserialize(f.read())" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 3, | |
"id": "64722b8a", | |
"metadata": {}, | |
"outputs": [ | |
{ | |
"data": { | |
"text/plain": [ | |
"True" | |
] | |
}, | |
"execution_count": 3, | |
"metadata": {}, | |
"output_type": "execute_result" | |
} | |
], | |
"source": [ | |
"system.getForce(7).getUseDispersionCorrection()" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 4, | |
"id": "408abbbe", | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"system.getForce(8).setUseLongRangeCorrection(True)" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 5, | |
"id": "13c8b1ce", | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"# Set up integrator\n", | |
"integrator = openmmtools.integrators.LangevinIntegrator(temperature=300 * unit.kelvin, \n", | |
" collision_rate=1 / unit.picoseconds, \n", | |
" timestep=4 * unit.femtoseconds)\n" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 6, | |
"id": "7d428b9f", | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"# Set up context\n", | |
"platform_name = 'CUDA'\n", | |
"platform = openmm.Platform.getPlatformByName(platform_name)\n", | |
"if platform_name in ['CUDA', 'OpenCL']:\n", | |
" platform.setPropertyDefaultValue('Precision', 'mixed')\n", | |
"if platform_name in ['CUDA']:\n", | |
" platform.setPropertyDefaultValue('DeterministicForces', 'true')\n", | |
"context = openmm.Context(system, integrator, platform)\n", | |
"context.setPeriodicBoxVectors(*state.getPeriodicBoxVectors())\n", | |
"context.setPositions(state.getPositions())\n", | |
"context.setVelocitiesToTemperature(300 * unit.kelvin)" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 7, | |
"id": "f542945d", | |
"metadata": {}, | |
"outputs": [], | |
"source": [ | |
"nsteps = 100\n", | |
"initial_time = time.time()\n", | |
"for step in range(nsteps):\n", | |
" context.setParameter('lambda_sterics_insert', (step + 1) * 0.01)\n", | |
" integrator.step(1)\n", | |
"elapsed_time = (time.time() - initial_time) * unit.seconds" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": 8, | |
"id": "23a2999c", | |
"metadata": {}, | |
"outputs": [ | |
{ | |
"data": { | |
"text/plain": [ | |
"Quantity(value=12.859097957611084, unit=second)" | |
] | |
}, | |
"execution_count": 8, | |
"metadata": {}, | |
"output_type": "execute_result" | |
} | |
], | |
"source": [ | |
"elapsed_time" | |
] | |
}, | |
{ | |
"cell_type": "code", | |
"execution_count": null, | |
"id": "973923ff", | |
"metadata": {}, | |
"outputs": [], | |
"source": [] | |
} | |
], | |
"metadata": { | |
"kernelspec": { | |
"display_name": "Python 3 (ipykernel)", | |
"language": "python", | |
"name": "python3" | |
}, | |
"language_info": { | |
"codemirror_mode": { | |
"name": "ipython", | |
"version": 3 | |
}, | |
"file_extension": ".py", | |
"mimetype": "text/x-python", | |
"name": "python", | |
"nbconvert_exporter": "python", | |
"pygments_lexer": "ipython3", | |
"version": "3.8.12" | |
} | |
}, | |
"nbformat": 4, | |
"nbformat_minor": 5 | |
} |
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