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. Author manuscript; available in PMC: 2018 Jan 1.
Published in final edited form as: J Comput Aided Mol Des. 2016 Sep 22;31(1):1–19. doi: 10.1007/s10822-016-9974-4

Table 2.

Summary of computational methods in all SAMPL5 host-guest submissions

Method Conformational sampling Energy model Solvent model SAMPL5 Refs.
OAH/OAMe
    APR-OPC (C, E) MD; docking GAFF/RESP OPC [41]
    APR-TIP3P (C, E) MD; docking GAFF/RESP TIP3P [41]
    BEDAM (C, I) MD OPLS-2005 AGBNP2 [54]
    DFT/TPSS-ca (Q, I) Manual DFT-D3 (TPSS functional) COSMO-RS [55]
    DFT/TPSS-na (Q, I) Manual DFT-D3 (TPSS functional) COSMO-RS [55]
    DLPNO-CCSD(T)a (Q, I) Manual DLPNO-CCSD(T) COSMO-RS [55]
    Metadynamics (C, E) Funnel metadynamics GAFF/RESP TIP3P [56]
    MMPBSA-GAFF (C, I) MD GAFF/RESP PBSA; TIP3P [56]
    MMPBSA-OPLSb (C, I) MD OPLS/RESP PBSA; TIP3P [56]
    MovTyp-1 (C, I) Mixed torsion/low mode KECSA 1 Implicit [40]
    MovTyp-2 (C, I) Mixed torsion/low mode KECSA 2 Implicit [40]
    TI/BARc (C, E) MD; docking CGenFF TIP3P [57]
    TI-psc (C, E) MD; docking CGenFF TIP3P [57]
    TI-rawc (C, E) MD; docking CGenFF TIP3P [57]
    HBARd (C, E) MD; docking CGenFF TIP3P [57]
    HBAR-psd (C, E) MD; docking CGenFF TIP3P [57]
    HBAR-ps1d (C, E) MD; docking CGenFF TIP3P [57]
    HBAR-ps2d (C, E) MD; docking CGenFF TIP3P [57]
    SOMD-1e (C, E) MD GAFF/RESP TIP3P [58]
    SOMD-2 (C, E) MD GAFF/RESP TIP3P [58]
    SOMD-3 (C, E) MD GAFF/RESP TIP3P [58]
    SOMD-4 (C, E) MD GAFF/RESP TIP3P [58]
CBClip
    BAR-ab-initiof (C, E) MD CGenFF TIP3P [59]
    BAR-dockf (C, E) MD; docking CGenFF TIP3P [59]
    TI-ab-initiof (C, E) MD CGenFF TIP3P [59]
    TI-BARf (C, E) MD; docking CGenFF TIP3P [59]
    TI-dockf (C, E) MD; docking CGenFF TIP3P [59]
    BEDAM (C, I) MD OPLS-2005 AGBNP2 [54]
    MovTyp-1 (C, I) Mixed torsion/low mode KECSA 1 Implicit [40]
    MovTyp-2 (C, I) Mixed torsion/low mode KECSA 2 Implicit [40]
    SOMD-1e (C, E) MD GAFF/RESP TIP3P [58]
    SOMD-2 (C, E) MD GAFF/RESP TIP3P [58]
    SOMD-3 (C, E) MD GAFF/RESP TIP3P [58]
    SOMD-4 (C, E) MD GAFF/RESP TIP3P [58]

APR attach-pull-release approach [60], OPC “optimal” 3-charge, 4-point rigid water model [61]; TIP3P transferable interaction potential three-point [47]; BEDAM binding energy distribution analysis method [62]; DLPNO-CCSD(T) domain based, local pair natural orbital-coupled-cluster single double and perturbative triple excitations [63]; DFT-D3 density functional theory with the latest dispersion corrections [64]; MovTyp Movable Type method [53]; SOMD single topology relative free energy calculations performed with Sire/OpenMM6.3 software [65, 66]; BAR Bennett acceptance ratio [50]; TI thermodynamic integration [49, 67]; GAFF generalized AMBER force field [68]; CGenFF CHARMM generalized force-field [69]; RESP restrained electrostatic potential [70]; OPLS-2005 optimized potentials for liquid simulations 2005 force field [71, 72]; KECSA knowledge-based and empirical combined scoring algorithm [73]; AGBNP2 analytical generalized born plus non-polar 2 [74]; COSMO-RS conductor-like screening model for real solvents [75]; MMPBSA molecular mechanics Poisson Boltzmann/solvent accessible surface area [52]. The classifications of the energy model: quantum (Q) or classical (C), as well as the solvent model: implicit (I) or explicit (E) are listed in parentheses following the name of each method

a

DLPNO-CCSD(T) and DFT/TPSS-n (n indicates neutralized) used neutralized hosts, yet fully charged guests. DFT/TPSS-c (c indicates charged) used both fully charged hosts and guests

b

The MMPBSA-OPLS approach was only used to generate predictions for the OAMe subset

c

TI was used to compute binding affinities in both TI-raw and TI-ps. Lowest values of the computed binding free energies were reported in TI-raw. In TI-ps, possible corrections were added through calculating the relative pKa/pKb of the ligands to known analogs

d

Binding free energies in HBAR submission were computed by Hamiltonian replica exchange method (HREM) combined with the BAR method. The protonation state correction was used in HBAR-ps, HBAR-ps1 and HBAR-ps2. Results from the neutralized-only systems were reported as HBAR-ps1 and those from systems at the experimental ionic strength were reported as HBAR-ps2. TI/BAR prediction only reported binding affinities for the OAH subset based on the averaged results computed by TI and HREM/BAR for each guest

e

All SOMD predictions were produced based on single topology relative free energy calculations combined with multistate Bennet acceptance ratio (MBAR) method, but with different protocols. SOMD-1: No corrections; SOMD-2: includes a correction term for long-range dispersion interactions; SOMD-3: same as SOMD-2, but a correction term for the use of the flat-bottom distance restraints was also applied to bring the decoupled guest to a standard concentration; SOMD-4: same as SOMD-3 but with an additional correction term for electrostatic energies

f

Predictions were generated by either TI (labeled with TI-) or HREM/BAR (label by BAR-). Also the starting structures were obtained by quantum calculations (labeled with “ab initio”) or docking (labeled with “dock”). TI/BAR reported the lowest binding affinity from either method