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gmx_MMPBSA calculates binding free energies from molecular dynamics trajectories using MM/PBSA (Molecular Mechanics/Poisson-Boltzmann Surface Area) and MM/GBSA (Molecular Mechanics/Generalized Born Surface Area) methods. Developed by Valdés-Tresanco and colleagues, it bridges GROMACS simulations with AMBER's MMPBSA.py engine, enabling end-state free energy calculations for protein-ligand, protein-protein, and protein-nucleic acid complexes.
These methods estimate binding affinity by calculating the free energy difference between bound and unbound states. The calculation combines molecular mechanics energies (van der Waals, electrostatic) with implicit solvation models, offering a balance between the speed of empirical scoring functions and the accuracy of rigorous alchemical methods.
Binding free energy () is computed from snapshots extracted from an MD trajectory:
Each term comprises several energy components:
| Component | Description |
|---|---|
| Van der Waals interactions (Lennard-Jones potential) | |
| Coulombic electrostatic interactions | |
MM/PBSA solves the Poisson-Boltzmann equation for electrostatic solvation, providing higher accuracy but at greater computational cost. MM/GBSA uses analytical Generalized Born approximations, running faster while maintaining reasonable accuracy for ranking compounds.
| Model | Description |
|---|---|
GB-HCT (igb=1) | Hawkins-Cramer-Truhlar model, fast but less accurate |
GB-OBC1 (igb=2) | Onufriev-Bashford-Case model, variant 1 |
GB-OBC2 (igb=5) | OBC variant 2, recommended for most applications |
GB-Neck (igb=7) | Improved treatment of interstitial regions |
GB-Neck2 (igb=8) | Further refinements to neck region calculations |
The OBC2 model (igb=5) provides a good balance of accuracy and speed for protein-ligand systems.
ProteinIQ provides cloud-based access to gmx_MMPBSA, eliminating the need to configure AMBER, GROMACS, or compute environments locally.
| Input | Description |
|---|---|
MD Trajectory file | GROMACS trajectory (.xtc, .trr) or multi-model PDB. Contains atomic coordinates across simulation frames. |
Topology file | GROMACS topology (.tpr or .top). Defines force field parameters and system topology. |
Index file | Optional GROMACS index file (.ndx). Specifies receptor and ligand atom groups. Auto-detected if omitted. |
Input parameter file | Optional gmx_MMPBSA input file. Overrides settings with custom parameters. |
| Setting | Description |
|---|---|
Calculation method | MM/GBSA (faster, suitable for screening), MM/PBSA (more accurate), or Both for comparison |
Energy decomposition | When enabled, calculates per-residue energy contributions to identify key binding site residues |
| Setting | Description |
|---|---|
Start frame | First frame to analyze (1-indexed) |
End frame | Last frame to analyze. Use -1 to include all frames |
Frame interval | Analyze every nth frame. Set to 2 or higher to reduce computation for long trajectories |
| Setting | Description |
|---|---|
Salt concentration | Ionic strength in molar (default 0.15 M, physiological conditions) |
GB model | Generalized Born variant for MM/GBSA. GB-OBC2 (igb=5) recommended |
Results include total binding free energy with component breakdown:
| Column | Description |
|---|---|
DELTA TOTAL | Net binding free energy (kcal/mol). More negative indicates stronger binding. |
VDWAALS | Van der Waals contribution |
EEL | Electrostatic energy (gas phase) |
EGB or EPB | Polar solvation (GB or PB method) |
ESURF or ENPOLAR | Nonpolar solvation (surface area term) |
When energy decomposition is enabled, per-residue contributions identify which amino acids drive binding.
| (kcal/mol) | Interpretation |
|---|---|
| < −15 | Very strong binding |
| −10 to −15 | Strong binding (nanomolar range) |
| −5 to −10 | Moderate binding |
| > −5 | Weak binding |
These values should be interpreted as relative rankings rather than absolute affinities. MM/PBSA and MM/GBSA excel at comparing similar ligands binding to the same target, but absolute values carry significant uncertainty.
The single-trajectory approach used here assumes identical conformations for complex, receptor, and ligand. This reduces noise but misses conformational reorganization effects. Results depend heavily on the quality and length of the MD simulation—short simulations with poor sampling produce unreliable energies.
Entropy contributions are not calculated by default due to computational cost and large uncertainties. For charged ligands, electrostatic and polar solvation terms often exhibit significant cancellation, amplifying small errors. Results should guide compound prioritization rather than predict absolute binding constants.
| Polar solvation energy (PB or GB model) |
| Nonpolar solvation, proportional to solvent-accessible surface area |
| Conformational entropy (optional, computationally expensive) |