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Add scVelo RNA velocity analysis workflow and IQ-TREE reference documentation
- Introduced a comprehensive RNA velocity analysis pipeline using scVelo, including data loading, preprocessing, velocity estimation, and visualization. - Added a script for running RNA velocity analysis with customizable parameters and output options. - Created detailed documentation for IQ-TREE 2 phylogenetic inference, covering command syntax, model selection, bootstrapping methods, and output interpretation. - Included references for velocity models and their mathematical framework, along with a comparison of different models. - Enhanced the scVelo skill documentation with installation instructions, use cases, and best practices for RNA velocity analysis.
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scientific-skills/molecular-dynamics/SKILL.md
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scientific-skills/molecular-dynamics/SKILL.md
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---
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name: molecular-dynamics
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description: Run and analyze molecular dynamics simulations with OpenMM and MDAnalysis. Set up protein/small molecule systems, define force fields, run energy minimization and production MD, analyze trajectories (RMSD, RMSF, contact maps, free energy surfaces). For structural biology, drug binding, and biophysics.
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license: MIT
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metadata:
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skill-author: Kuan-lin Huang
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---
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# Molecular Dynamics
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## Overview
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Molecular dynamics (MD) simulation computationally models the time evolution of molecular systems by integrating Newton's equations of motion. This skill covers two complementary tools:
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- **OpenMM** (https://openmm.org/): High-performance MD simulation engine with GPU support, Python API, and flexible force field support
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- **MDAnalysis** (https://mdanalysis.org/): Python library for reading, writing, and analyzing MD trajectories from all major simulation packages
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**Installation:**
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```bash
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conda install -c conda-forge openmm mdanalysis nglview
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# or
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pip install openmm mdanalysis
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```
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## When to Use This Skill
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Use molecular dynamics when:
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- **Protein stability analysis**: How does a mutation affect protein dynamics?
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- **Drug binding simulations**: Characterize binding mode and residence time of a ligand
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- **Conformational sampling**: Explore protein flexibility and conformational changes
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- **Protein-protein interaction**: Model interface dynamics and binding energetics
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- **RMSD/RMSF analysis**: Quantify structural fluctuations from a reference structure
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- **Free energy estimation**: Compute binding free energy or conformational free energy
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- **Membrane simulations**: Model proteins in lipid bilayers
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- **Intrinsically disordered proteins**: Study IDR conformational ensembles
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## Core Workflow: OpenMM Simulation
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### 1. System Preparation
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```python
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from openmm.app import *
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from openmm import *
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from openmm.unit import *
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import sys
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def prepare_system_from_pdb(pdb_file, forcefield_name="amber14-all.xml",
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water_model="amber14/tip3pfb.xml"):
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"""
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Prepare an OpenMM system from a PDB file.
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Args:
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pdb_file: Path to cleaned PDB file (use PDBFixer for raw PDB files)
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forcefield_name: Force field XML file
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water_model: Water model XML file
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Returns:
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pdb, forcefield, system, topology
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"""
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# Load PDB
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pdb = PDBFile(pdb_file)
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# Load force field
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forcefield = ForceField(forcefield_name, water_model)
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# Add hydrogens and solvate
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modeller = Modeller(pdb.topology, pdb.positions)
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modeller.addHydrogens(forcefield)
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# Add solvent box (10 Å padding, 150 mM NaCl)
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modeller.addSolvent(
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forcefield,
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model='tip3p',
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padding=10*angstroms,
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ionicStrength=0.15*molar
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)
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print(f"System: {modeller.topology.getNumAtoms()} atoms, "
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f"{modeller.topology.getNumResidues()} residues")
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# Create system
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system = forcefield.createSystem(
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modeller.topology,
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nonbondedMethod=PME, # Particle Mesh Ewald for long-range electrostatics
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nonbondedCutoff=1.0*nanometer,
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constraints=HBonds, # Constrain hydrogen bonds (allows 2 fs timestep)
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rigidWater=True,
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ewaldErrorTolerance=0.0005
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)
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return modeller, system
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```
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### 2. Energy Minimization
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```python
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from openmm.app import *
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from openmm import *
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from openmm.unit import *
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def minimize_energy(modeller, system, output_pdb="minimized.pdb",
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max_iterations=1000, tolerance=10.0):
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"""
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Energy minimize the system to remove steric clashes.
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Args:
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modeller: Modeller object with topology and positions
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system: OpenMM System
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output_pdb: Path to save minimized structure
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max_iterations: Maximum minimization steps
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tolerance: Convergence criterion in kJ/mol/nm
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Returns:
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simulation object with minimized positions
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"""
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# Set up integrator (doesn't matter for minimization)
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integrator = LangevinMiddleIntegrator(300*kelvin, 1/picosecond, 0.004*picoseconds)
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# Create simulation
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# Use GPU if available (CUDA or OpenCL), fall back to CPU
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try:
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platform = Platform.getPlatformByName('CUDA')
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properties = {'DeviceIndex': '0', 'Precision': 'mixed'}
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except Exception:
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try:
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platform = Platform.getPlatformByName('OpenCL')
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properties = {}
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except Exception:
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platform = Platform.getPlatformByName('CPU')
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properties = {}
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simulation = Simulation(
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modeller.topology, system, integrator,
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platform, properties
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)
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simulation.context.setPositions(modeller.positions)
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# Check initial energy
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state = simulation.context.getState(getEnergy=True)
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print(f"Initial energy: {state.getPotentialEnergy()}")
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# Minimize
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simulation.minimizeEnergy(
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tolerance=tolerance*kilojoules_per_mole/nanometer,
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maxIterations=max_iterations
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)
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state = simulation.context.getState(getEnergy=True, getPositions=True)
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print(f"Minimized energy: {state.getPotentialEnergy()}")
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# Save minimized structure
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with open(output_pdb, 'w') as f:
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PDBFile.writeFile(simulation.topology, state.getPositions(), f)
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return simulation
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```
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### 3. NVT Equilibration
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```python
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from openmm.app import *
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from openmm import *
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from openmm.unit import *
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def run_nvt_equilibration(simulation, n_steps=50000, temperature=300,
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report_interval=1000, output_prefix="nvt"):
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"""
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NVT equilibration: constant N, V, T.
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Equilibrate velocities to target temperature.
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Args:
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simulation: OpenMM Simulation (after minimization)
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n_steps: Number of MD steps (50000 × 2fs = 100 ps)
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temperature: Temperature in Kelvin
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report_interval: Steps between data reports
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output_prefix: File prefix for trajectory and log
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"""
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# Add position restraints for backbone during NVT
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# (Optional: restraint heavy atoms)
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# Set temperature
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simulation.context.setVelocitiesToTemperature(temperature*kelvin)
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# Add reporters
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simulation.reporters = []
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# Log file
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simulation.reporters.append(
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StateDataReporter(
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f"{output_prefix}_log.txt",
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report_interval,
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step=True,
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potentialEnergy=True,
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kineticEnergy=True,
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temperature=True,
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volume=True,
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speed=True
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)
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)
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# DCD trajectory (compact binary format)
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simulation.reporters.append(
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DCDReporter(f"{output_prefix}_traj.dcd", report_interval)
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)
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print(f"Running NVT equilibration: {n_steps} steps ({n_steps*2/1000:.1f} ps)")
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simulation.step(n_steps)
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print("NVT equilibration complete")
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return simulation
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```
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### 4. NPT Equilibration and Production
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```python
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def run_npt_production(simulation, n_steps=500000, temperature=300, pressure=1.0,
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report_interval=5000, output_prefix="npt"):
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"""
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NPT production run: constant N, P, T.
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Args:
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n_steps: Production steps (500000 × 2fs = 1 ns)
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temperature: Temperature in Kelvin
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pressure: Pressure in bar
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report_interval: Steps between reports
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"""
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# Add Monte Carlo barostat for pressure control
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system = simulation.context.getSystem()
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system.addForce(MonteCarloBarostat(pressure*bar, temperature*kelvin, 25))
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simulation.context.reinitialize(preserveState=True)
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# Update reporters
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simulation.reporters = []
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simulation.reporters.append(
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StateDataReporter(
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f"{output_prefix}_log.txt",
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report_interval,
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step=True,
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potentialEnergy=True,
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temperature=True,
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density=True,
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speed=True
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)
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)
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simulation.reporters.append(
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DCDReporter(f"{output_prefix}_traj.dcd", report_interval)
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)
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# Save checkpoints
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simulation.reporters.append(
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CheckpointReporter(f"{output_prefix}_checkpoint.chk", 50000)
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)
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print(f"Running NPT production: {n_steps} steps ({n_steps*2/1000000:.2f} ns)")
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simulation.step(n_steps)
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print("Production MD complete")
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return simulation
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```
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## Trajectory Analysis with MDAnalysis
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### 1. Load Trajectory
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```python
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import MDAnalysis as mda
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from MDAnalysis.analysis import rms, align, contacts
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import numpy as np
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import matplotlib.pyplot as plt
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def load_trajectory(topology_file, trajectory_file):
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"""
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Load an MD trajectory with MDAnalysis.
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Args:
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topology_file: PDB, PSF, or other topology file
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trajectory_file: DCD, XTC, TRR, or other trajectory
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"""
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u = mda.Universe(topology_file, trajectory_file)
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print(f"Universe: {u.atoms.n_atoms} atoms, {u.trajectory.n_frames} frames")
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print(f"Time range: 0 to {u.trajectory.totaltime:.0f} ps")
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return u
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```
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### 2. RMSD Analysis
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```python
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def compute_rmsd(u, selection="backbone", reference_frame=0):
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"""
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Compute RMSD of selected atoms relative to reference frame.
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Args:
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u: MDAnalysis Universe
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selection: Atom selection string (MDAnalysis syntax)
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reference_frame: Frame index for reference structure
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Returns:
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numpy array of (time, rmsd) values
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"""
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# Align trajectory to minimize RMSD
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aligner = align.AlignTraj(u, u, select=selection, in_memory=True)
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aligner.run()
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# Compute RMSD
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R = rms.RMSD(u, select=selection, ref_frame=reference_frame)
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R.run()
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rmsd_data = R.results.rmsd # columns: frame, time, RMSD
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return rmsd_data
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def plot_rmsd(rmsd_data, title="RMSD over time", output_file="rmsd.png"):
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"""Plot RMSD over simulation time."""
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fig, ax = plt.subplots(figsize=(10, 4))
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ax.plot(rmsd_data[:, 1] / 1000, rmsd_data[:, 2], 'b-', linewidth=0.5)
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ax.set_xlabel("Time (ns)")
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ax.set_ylabel("RMSD (Å)")
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ax.set_title(title)
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ax.axhline(rmsd_data[:, 2].mean(), color='r', linestyle='--',
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label=f'Mean: {rmsd_data[:, 2].mean():.2f} Å')
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ax.legend()
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plt.tight_layout()
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plt.savefig(output_file, dpi=150)
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return fig
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```
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### 3. RMSF Analysis (Per-Residue Flexibility)
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```python
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def compute_rmsf(u, selection="backbone", start_frame=0):
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"""
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Compute per-residue RMSF (flexibility).
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Returns:
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resids, rmsf_values arrays
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"""
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# Select atoms
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atoms = u.select_atoms(selection)
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# Compute RMSF
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R = rms.RMSF(atoms)
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R.run(start=start_frame)
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# Average by residue
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resids = []
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rmsf_per_res = []
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for res in u.select_atoms(selection).residues:
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res_atoms = res.atoms.intersection(atoms)
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if len(res_atoms) > 0:
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resids.append(res.resid)
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rmsf_per_res.append(R.results.rmsf[res_atoms.indices].mean())
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return np.array(resids), np.array(rmsf_per_res)
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```
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### 4. Protein-Ligand Contacts
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```python
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def analyze_contacts(u, protein_sel="protein", ligand_sel="resname LIG",
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radius=4.5, start_frame=0):
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"""
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Track protein-ligand contacts over trajectory.
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Args:
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radius: Contact distance cutoff in Angstroms
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"""
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protein = u.select_atoms(protein_sel)
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ligand = u.select_atoms(ligand_sel)
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contact_frames = []
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for ts in u.trajectory[start_frame:]:
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# Find protein atoms within radius of ligand
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distances = contacts.contact_matrix(
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protein.positions, ligand.positions, radius
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)
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contact_residues = set()
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for i in range(distances.shape[0]):
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if distances[i].any():
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contact_residues.add(protein.atoms[i].resid)
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contact_frames.append(contact_residues)
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return contact_frames
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```
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## Force Field Selection Guide
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| System | Recommended Force Field | Water Model |
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|--------|------------------------|-------------|
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| Standard proteins | AMBER14 (`amber14-all.xml`) | TIP3P-FB |
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| Proteins + small molecules | AMBER14 + GAFF2 | TIP3P-FB |
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| Membrane proteins | CHARMM36m | TIP3P |
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| Nucleic acids | AMBER99-bsc1 or AMBER14 | TIP3P |
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| Disordered proteins | ff19SB or CHARMM36m | TIP3P |
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## System Preparation Tools
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### PDBFixer (for raw PDB files)
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```python
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from pdbfixer import PDBFixer
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from openmm.app import PDBFile
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def fix_pdb(input_pdb, output_pdb, ph=7.0):
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"""Fix common PDB issues: missing residues, atoms, add H, standardize."""
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fixer = PDBFixer(filename=input_pdb)
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fixer.findMissingResidues()
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fixer.findNonstandardResidues()
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fixer.replaceNonstandardResidues()
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fixer.removeHeterogens(True) # Remove water/ligands
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fixer.findMissingAtoms()
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fixer.addMissingAtoms()
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fixer.addMissingHydrogens(ph)
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with open(output_pdb, 'w') as f:
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PDBFile.writeFile(fixer.topology, fixer.positions, f)
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return output_pdb
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```
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### GAFF2 for Small Molecules (via OpenFF Toolkit)
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```python
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# For ligand parameterization, use OpenFF toolkit or ACPYPE
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# pip install openff-toolkit
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from openff.toolkit import Molecule, ForceField as OFFForceField
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from openff.interchange import Interchange
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def parameterize_ligand(smiles, ff_name="openff-2.0.0.offxml"):
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"""Generate GAFF2/OpenFF parameters for a small molecule."""
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mol = Molecule.from_smiles(smiles)
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mol.generate_conformers(n_conformers=1)
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off_ff = OFFForceField(ff_name)
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interchange = off_ff.create_interchange(mol.to_topology())
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return interchange
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```
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## Best Practices
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- **Always minimize before MD**: Raw PDB structures have steric clashes
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- **Equilibrate before production**: NVT (50–100 ps) → NPT (100–500 ps) → Production
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- **Use GPU**: Simulations are 10–100× faster on GPU (CUDA/OpenCL)
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- **2 fs timestep with HBonds constraints**: Standard; use 4 fs with HMR (hydrogen mass repartitioning)
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- **Analyze only equilibrated trajectory**: Discard first 20–50% as equilibration
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- **Save checkpoints**: MD runs can fail; checkpoints allow restart
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- **Periodic boundary conditions**: Required for solvated systems
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- **PME for electrostatics**: More accurate than cutoff methods for charged systems
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## Additional Resources
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- **OpenMM documentation**: https://openmm.org/documentation.html
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- **MDAnalysis user guide**: https://docs.mdanalysis.org/
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- **GROMACS** (alternative MD engine): https://manual.gromacs.org/
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- **NAMD** (alternative): https://www.ks.uiuc.edu/Research/namd/
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- **CHARMM-GUI** (web-based system builder): https://charmm-gui.org/
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- **AmberTools** (free Amber tools): https://ambermd.org/AmberTools.php
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- **OpenMM paper**: Eastman P et al. (2017) PLOS Computational Biology. PMID: 28278240
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- **MDAnalysis paper**: Michaud-Agrawal N et al. (2011) J Computational Chemistry. PMID: 21500218
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