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molecular-dynamics

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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name molecular-dynamics 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. license MIT metadata {"version":"1.1","skill-author":"Kuan-lin Huang"} Molecular Dynamics Overview 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: OpenMM ( https://openmm.org/ ): High-performance MD simulation engine with GPU support, Python API, and flexible force field support MDAnalysis ( https://mdanalysis.org/ ): Python library for reading, writing, and analyzing MD trajectories from all major simulation packages Installation: conda install -c conda-forge openmm mdanalysis nglview # or uv pip install openmm mdanalysis When to Use This Skill Use molecular dynamics when: Protein stability analysis : How does a mutation affect protein dynamics? Drug binding simulations : Characterize binding mode and residence time of a ligand Conformational sampling : Explore protein flexibility and conformational changes Protein-protein interaction : Model interface dynamics and binding energetics RMSD/RMSF analysis : Quantify structural fluctuations from a reference structure Free energy estimation : Compute binding free energy or conformational free energy Membrane simulations : Model proteins in lipid bilayers Intrinsically disordered proteins : Study IDR conformational ensembles Core Workflow: OpenMM Simulation 1. System Preparation from openmm.app import * from openmm import * from openmm.unit import * import sys def prepare_system_from_pdb ( pdb_file, forcefield_name= "amber14-all.xml" , water_model= "amber14/tip3pfb.xml" ): """ Prepare an OpenMM system from a PDB file. Args: pdb_file: Path to cleaned PDB file (use PDBFixer for raw PDB files) forcefield_name: Force field XML file water_model: Water model XML file Returns: pdb, forcefield, system, topology """ # Load PDB pdb = PDBFile(pdb_file) # Load force field forcefield = ForceField(forcefield_name, water_model) # Add hydrogens and solvate modeller = Modeller(pdb.topology, pdb.positions) modeller.addHydrogens(forcefield) # Add solvent box (10 Å padding, 150 mM NaCl) modeller.addSolvent( forcefield, model= 'tip3p' , padding= 10 *angstroms, ionicStrength= 0.15 *molar ) print ( f"System: {modeller.topology.getNumAtoms()} atoms, " f" {modeller.topology.getNumResidues()} residues" ) # Create system system = forcefield.createSystem( modeller.topology, nonbondedMethod=PME, # Particle Mesh Ewald for long-range electrostatics nonbondedCutoff= 1.0 *nanometer, constraints=HBonds, # Constrain hydrogen bonds (allows 2 fs timestep) rigidWater= True , ewaldErrorTolerance= 0.0005 ) return modeller, system 2. Energy Minimization from openmm.app import * from openmm import * from openmm.unit import * def minimize_energy ( modeller, system, output_pdb= "minimized.pdb" , max_iterations= 1000 , tolerance= 10.0 ): """ Energy minimize the system to remove steric clashes. Args: modeller: Modeller object with topology and positions system: OpenMM System output_pdb: Path to save minimized structure max_iterations: Maximum minimization steps tolerance: Convergence criterion in kJ/mol/nm Returns: simulation object with minimized positions """ # Set up integrator (doesn't matter for minimization) integrator = LangevinMiddleIntegrator( 300 *kelvin, 1 /picosecond, 0.004 *picoseconds) # Create simulation # Use GPU if available (CUDA or OpenCL), fall back to CPU try : platform = Platform.getPlatformByName( 'CUDA' ) properties = { 'DeviceIndex' : '0' , 'Precision' : 'mixed' } except Exception: try : platform = Platform.getPlatformByName( 'OpenCL' ) properties = {} except Exception: platform = Platform.getPlatformByName( 'CPU' ) properties = {} simulation = Simulation( modeller.topology, system, integrator, platform, properties ) simulation.context.setPositions(modeller.positions) # Check initial energy state = simulation.context.getState(getEnergy= True ) print ( f"Initial energy: {state.getPotentialEnergy()} " ) # Minimize simulation.minimizeEnergy( tolerance=tolerance*kilojoules_per_mole/nanometer, maxIterations=max_iterations ) state = simulation.context.getState(getEnergy= True , getPositions= True ) print ( f"Minimized energy: {state.getPotentialEnergy()} " ) # Save minimized structure with open (output_pdb, 'w' ) as f: PDBFile.writeFile(simulation.topology, state.getPositions(), f) return simulation 3. NVT Equilibration from openmm.app import * from openmm import * from openmm.unit import * def run_nvt_equilibration ( simulation, n_steps= 50000 , temperature= 300 , report_interval= 1000 , output_prefix= "nvt" ): """ NVT equilibration: constant N, V, T. Equilibrate velocities to target temperature. Args: simulation: OpenMM Simulation (after minimization) n_steps: Number of MD steps (50000 × 2fs = 100 ps) temperature: Temperature in Kelvin report_interval: Steps between data reports output_prefix: File prefix for trajectory and log """ # Add position restraints for backbone during NVT # (Optional: restraint heavy atoms) # Set temperature simulation.context.setVelocitiesToTemperature(temperature*kelvin) # Add reporters simulation.reporters = [] # Log file simulation.reporters.append( StateDataReporter( f" {output_prefix} _log.txt" , report_interval, step= True , potentialEnergy= True , kineticEnergy= True , temperature= True , volume= True , speed= True ) ) # DCD trajectory (compact binary format) simulation.reporters.append( DCDReporter( f" {output_prefix} _traj.dcd" , report_interval) ) print ( f"Running NVT equilibration: {n_steps} steps ( {n_steps* 2 / 1000 : .1 f} ps)" ) simulation.step(n_steps) print ( "NVT equilibration complete" ) return simulation 4. NPT Equilibration and Production def run_npt_production ( simulation, n_steps= 500000 , temperature= 300 , pressure= 1.0 , report_interval= 5000 , output_prefix= "npt" ): """ NPT production run: constant N, P, T. Args: n_steps: Production steps (500000 × 2fs = 1 ns) temperature: Temperature in Kelvin pressure: Pressure in bar report_interval: Steps between reports """ # Add Monte Carlo barostat for pressure control system = simulation.context.getSystem() system.addForce(MonteCarloBarostat(pressure*bar, temperature*kelvin, 25 )) simulation.context.reinitialize(preserveState= True ) # Update reporters simulation.reporters = [] simulation.reporters.append( StateDataReporter( f" {output_prefix} _log.txt" , report_interval, step= True , potentialEnergy= True , temperature= True , density= True , speed= True ) ) simulation.reporters.append( DCDReporter( f" {output_prefix} _traj.dcd" , report_interval) ) # Save checkpoints simulation.reporters.append( CheckpointReporter( f" {output_prefix} _checkpoint.chk" , 50000 ) ) print ( f"Running NPT production: {n_steps} steps ( {n_steps* 2 / 1000000 : .2 f} ns)" ) simulation.step(n_steps) print ( "Production MD complete" ) return simulation Trajectory Analysis with MDAnalysis 1. Load Trajectory import MDAnalysis as mda from MDAnalysis.analysis import rms, align, contacts import numpy as np import matplotlib.pyplot as plt def load_trajectory ( topology_file, trajectory_file ): """ Load an MD trajectory with MDAnalysis. Args: topology_file: PDB, PSF, or other topology file trajectory_file: DCD, XTC, TRR, or other trajectory """ u = mda.Universe(topology_file, trajectory_file) print ( f"Universe: {u.atoms.n_atoms} atoms, {u.trajectory.n_frames} frames" ) print ( f"Time range: 0 to {u.trajectory.totaltime: .0 f} ps" ) return u 2. RMSD Analysis def compute_rmsd ( u, selection= "backbone" , reference_frame= 0 ): """ Compute RMSD of selected atoms relative to reference frame. Args: u: MDAnalysis Universe selection: Atom selection string (MDAnalysis syntax) reference_frame: Frame index for reference structure Returns: numpy array of (time, rmsd) values """ # Align trajectory to minimize RMSD aligner = align.AlignTraj(u, u, select=selection, in_memory= True ) aligner.run() # Compute RMSD R = rms.RMSD(u, select=selection, ref_frame=reference_frame) R.run() rmsd_data = R.results.rmsd # columns: frame, time, RMSD return rmsd_data def plot_rmsd ( rmsd_data, title= "RMSD over time" , output_file= "rmsd.png" ): """Plot RMSD over simulation time.""" fig, ax = plt.subplots(figsize=( 10 , 4 )) ax.plot(rmsd_data[:, 1 ] / 1000 , rmsd_data[:, 2 ], 'b-' , linewidth= 0.5 ) ax.set_xlabel( "Time (ns)" ) ax.set_ylabel( "RMSD (Å)" ) ax.set_title(title) ax.axhline(rmsd_data[:, 2 ].mean(), color= 'r' , linestyle= '--' , label= f'Mean: {rmsd_data[:, 2 ].mean(): .2 f} Å' ) ax.legend() plt.tight_layout() plt.savefig(output_file, dpi= 150 ) return fig 3. RMSF Analysis (Per-Residue Flexibility) def compute_rmsf ( u, selection= "backbone" , start_frame= 0 ): """ Compute per-residue RMSF (flexibility). Returns: resids, rmsf_values arrays """ # Select atoms atoms = u.select_atoms(selection) # Compute RMSF R = rms.RMSF(atoms) R.run(start=start_frame) # Average by residue resids = [] rmsf_per_res = [] for res in u.select_atoms(selection).residues: res_atoms = res.atoms.intersection(atoms) if len (res_atoms) > 0 : resids.append(res.resid) rmsf_per_res.append(R.results.rmsf[res_atoms.indices].mean()) return np.array(resids), np.array(rmsf_per_res) 4. Protein-Ligand Contacts def analyze_contacts ( u, protein_sel= "protein" , ligand_sel= "resname LIG" , radius= 4.5 , start_frame= 0 ): """ Track protein-ligand contacts over trajectory. Args: radius: Contact distance cutoff in Angstroms """ protein = u.select_atoms(protein_sel) ligand = u.select_atoms(ligand_sel) contact_frames = [] for ts in u.trajectory[start_frame:]: # Find protein atoms within radius of ligand distances = contacts.contact_matrix( protein.positions, ligand.positions, radius ) contact_residues = set () for i in range (distances.shape[ 0 ]): if distances[i]. any (): contact_residues.add(protein.atoms[i].resid) contact_frames.append(contact_residues) return contact_frames Force Field Selection Guide System Recommended Force Field Water Model Standard proteins AMBER14 ( amber14-all.xml ) TIP3P-FB Proteins + small molecules AMBER14 + GAFF2 TIP3P-FB Membrane proteins CHARMM36m TIP3P Nucleic acids AMBER99-bsc1 or AMBER14 TIP3P Disordered proteins ff19SB or CHARMM36m TIP3P System Preparation Tools PDBFixer (for raw PDB files) from pdbfixer import PDBFixer from openmm.app import PDBFile def fix_pdb ( input_pdb, output_pdb, ph= 7.0 ): """Fix common PDB issues: missing residues, atoms, add H, standardize.""" fixer = PDBFixer(filename=input_pdb) fixer.findMissingResidues() fixer.findNonstandardResidues() fixer.replaceNonstandardResidues() fixer.removeHeterogens( True ) # Remove water/ligands fixer.findMissingAtoms() fixer.addMissingAtoms() fixer.addMissingHydrogens(ph) with open (output_pdb, 'w' ) as f: PDBFile.writeFile(fixer.topology, fixer.positions, f) return output_pdb GAFF2 for Small Molecules (via OpenFF Toolkit) # For ligand parameterization, use OpenFF toolkit or ACPYPE # uv pip install openff-toolkit from openff.toolkit import Molecule, ForceField as OFFForceField from openff.interchange import Interchange def parameterize_ligand ( smiles, ff_name= "openff-2.0.0.offxml" ): """Generate GAFF2/OpenFF parameters for a small molecule.""" mol = Molecule.from_smiles(smiles) mol.generate_conformers(n_conformers= 1 ) off_ff = OFFForceField(ff_name) interchange = off_ff.create_interchange(mol.to_topology()) return interchange Best Practices Always minimize before MD : Raw PDB structures have steric clashes Equilibrate before production : NVT (50–100 ps) → NPT (100–500 ps) → Production Use GPU : Simulations are 10–100× faster on GPU (CUDA/OpenCL) 2 fs timestep with HBonds constraints : Standard; use 4 fs with HMR (hydrogen mass repartitioning) Analyze only equilibrated trajectory : Discard first 20–50% as equilibration Save checkpoints : MD runs can fail; checkpoints allow restart Periodic boundary conditions : Required for solvated systems PME for electrostatics : More accurate than cutoff methods for charged systems Additional Resources OpenMM documentation : https://openmm.org/documentation.html MDAnalysis user guide : https://docs.mdanalysis.org/ GROMACS (alternative MD engine): https://manual.gromacs.org/
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