Froze
Jameel
and
Matthias
Stein
*
Molecular Simulations and Design Group, Max Planck Institute for Dynamics of Complex Technical Systems, Sandtorstrasse 1, 39106 Magdeburg, Germany. E-mail: matthias.stein@mpi-magdeburg.mpg.de
First published on 19th July 2024
Calculating the Gibbs energies of binding of ligand-receptor systems with a thermochemical accuracy of ± 1 kcal mol−1 is a challenge to computational approaches. After exploration of the conformational space of the host, ligand and their resulting complexes upon coordination by semi-empirical GFN2 MD and meta-MD simulations, the systematic refinement through a multi-level improvement of binding modes in terms of electronic energies and solvation is able to give Gibbs energies of binding of drug molecules to CB[8] and β-CD macrocyclic receptors with such an accuracy. The accurate treatment of a small number of structures outperforms system-specific force-matching and alchemical transfer model approaches without an extensive sampling and integration.
For these blind predictions of ligand-receptor Gibbs energies of binding, macrocyclic containers such as cucurbit[n]urils (CB[n])11,12 and cyclodextrins (CDs)13,14 with unreleased experimental data are chosen.
Here, we systematically refine the Gibbs energies of binding from conformers generated through SQM sampling for the ‘drugs of abuse’ molecules to the CB[8] receptor of the SAMPL8 host–guest challenge. This challenge focused on binding of the CB[8] host to opioid drug molecules including fentanyl (G2), morphine (G3), ketamine (G5), and cocaine (G7) (see Fig. 1).9 It also included previously considered cycloheptanamine and cyclooctanamine molecules (G8 and G9). Experimental data were obtained from isothermal titration (ITC) and NMR spectroscopy.15 This set of SQM conformer–rotamers was used to investigate whether the mean absolute deviation of 3.16 kcal mol−1 from GFN2-xTB16 could be reduced using the suggested systematic refinement of both electronic energies and solvent description.5
In addition, we here present calculated Gibbs energies of binding of phenothiazine drug molecules to the β-cyclodextrin receptor, which was part of SAMPL9 challenge.10 Cyclodextrins are versatile and flexible receptors that can incorporate various types of molecules and modify their molecular properties. They also have applications in drug delivery. The Gilson group provided experimental thermodynamic data for different cyclodextrins and ligand molecules which were only later released and published.17 The amphiphile receptor centre with a hydrophobic cavity plus hydrophilic surface-exposed hydroxyl groups in complex with large and flexible ligands poses a further level of complexity to calculate Gibbs energies of binding.
The conformer-rotamer ensembles (CRE) for SAMPL8 and SAMPL9 ligand complexes with cucurbit[8]uril (CB[8]) and β-cyclodextrin (β-CD) hosts, respectively, were generated upon manually positioning the ligand inside the receptor. Ensembles of non-covalent binding poses were generated using GFN2-xTB with an automatic exploration of the low-energy molecular chemical space CREST.5,18 The CENSO workflow6 including different levels of quantum chemical refinement plus thermostatistical corrections and solvent modelling was as used to systematically refine the calculated Gibbs energies of binding.
Curcurubituril[8] is a rather rigid host with only a few conformers accessible.16 However, with certain force fields, cucurbituril hosts have been observed to collapse during MD simulations. The sampling of conformers of CB[8] receptor and receptor–ligand complexes showed that this is not the case for GFN2-xTB.16 A conformational search using an implicit solvation model in absence of any constraints gave only one single CB[8] host structure. The ligand molecules of SAMPL8 are rather small in size with only few rotatable bonds (Fig. 1). This leads to only 4–8 unique structures in the conformer–rotamer ensemble (CRE) of CB[8] in complex with large and rigid morphine (G3) and hydromorphone (G4), but up to 137 unique complex structures with the rather flexible fentanyl molecule (G2). The subsequent energetic ranking must thus be able to accurately calculate small energy differences between a large number of binding modes in order to give reliable Gibbs energies of binding. The CREs from our SAMPL8 GFN2-xTB/MetaMD/GBSA work16 were refined using a systematic improvement of description of electronic energies and solvation. We have used a three level approach with increasing refinement thresholds to reduce the number of structures to be considered at the next level (see Computational details).
The incremental increase in accuracy of electronic structure method, description of effect of solvation (see Computational details) and refined energy thresholds to omit higher lying structures significantly reduces the number of structures retained at leach level (see Fig. S2, ESI†). For example, for CB[8]·G3 (morphine) and CB[8]·G4 (hydromorphone) only one structure after ‘level 2’ is sufficient to give reliable Gibbs energies of binding (see below). Also for the flexible fentanyl (G2), when in complex with CB[8], a mere two remaining structures after ‘level 2’ give excellent calculated Gibbs energies of binding (see below). The largest decrease of tentative complexation structures is always seen when the level of DFT treatment is going from the fast and approximate B97-D3 with a small basis set to the meta-GGA r2SCAN-3c (see Fig. S1, ESI†).
Fig. 2 shows the deviation of calculated Gibbs energies of binding of the CB[8] receptor to ligands G1–G9 from experiment. The numbers reported are the Boltzmann-weighted averages of conformers at each level. The original GFN2 CREs had a mean absolute deviation (MAD) of 3.16 kcal mol−1 from experiment which is already close to the top-ranked force matching approach with a MAD of 2.03 kcal mol−1 in SAMPL8.9 Since calculations at ‘level 0’ are mere approximate single-point energies and not Gibbs energies of binding to remove high-lying complexes, they cannot be directly compared with experiment and are not discussed further (see Table S2 for numerical results, ESI†). A negative ΔΔGbind indicates an overbinding (too negative Gibbs energies) in Fig. 2. GFN2 systematically overestimates the Gibbs energies of binding (only for cyclic amines G8 and G9 an underestimation by 1–2 kcal mol−1 is seen). The composite mGGA method r2SCAN-3c at ‘level 1’ gives significantly better Gibbs energies of binding even for single-point calculations. This method was originally found to outperform hybrid functionals in terms of conformational energies at a significantly lower computational cost whereas non-covalent interactions are about as well described as with hybrid functionals.24 However, from Fig. 2 it becomes apparent that a structural re-optimization of GFN2 structures in combination with an improved description of solvation free energies (from ALPB to COSMO-RS) significantly reduces the deviation from experiment (MAD decreases from 4.6 kcal mol−1 at ‘level 1’ to 2.45 kcal mol−1 at ‘level 2’). This reduced MAD results in part from improved electronic energies (by 1.52 kcal mol−1) and solvation (by 0.64 kcal mol−1; see Table S2, ESI†). The hybrid meta-GGA PW6B95 at ‘level 3’ gives an additional reduction of MAD by ∼1 kcal mol−1 (see Table 1) and a final MSE of −0.6 kcal mol−1.
Fig. 2 Deviation of calculated Gibbs energies of binding from experiment (ΔΔGbind, in kcal mol−1) for G1 to G9 ligands to the CB[8] receptor. |
In the global statistical analysis of SAMPL8,9 there were 5 ligand-receptor CB[8] complexes which had a root mean square error of 4 kcal mol−1 or larger among all submissions. These were CB[8]·G1, CB[8]·G3, CB[8]·G4, CB[8]·G6, and CB[8]·G7 (see Fig. 1). The majority of methods tended to underestimate the Gibbs energies of binding for these systems, except for one with a Gibbs energy of binding ∼8 kcal mol−1 too large. Our level 2/level 3 results have a deviation from experiment of +0.5/−0.5 kcal mol−1 (G1); +3.2/−2.3 kcal mol−1 (G3); −3.2/−4.7 kcal mol−1 (G4); +4.1/−0.4 kcal mol−1 (G6); +2.8/−0.16 kcal mol−1 (for G7). This shows, that the CENSO refinement of a large number of GFN2 binding modes is competitive with and, in some instances, outperforming previous submissions to SAMPL8. Ligands G3 (morphine) and G4 (hydromorphone) appear to be intrinsically difficult to describe for any computational method. These are among the most complex ligand entities in SAMPL8 with multi-ring heterocycles, decorated by several functional groups and a protonated tertiary amines as part of a heterocycle. Due to their chemical environment these are notoriously difficult to describe for solvation models (see below). For ligand systems G1, G6, and G7 the extra computational cost to go from the meta-GGA type r2SCAN-3c (level 2) to the hybrid meta exchange-correlation functional PW6B95 (level 3) seems to be worth since the final MSE for these compounds is the best for those entries in SAMPL8.
For the CB[8] host, the overall top-performer in SAMPL8 so far have used classical bonding and non-bonding parameters obtained via QM force-matching (FM) methods, QM-derived atomic charges and fitted bonded parameters with a final MAD of 2.03 kcal mol−1.9,25 Derivation of QM charges and the molecular force matching was computationally expensive and required 10000s of DFT force calculations for each complex. As an alternative approach, with much less extensive sampling and a systematic refinement of QM interaction energies, our results with a MSE of −0.60 kcal mol−1 and a MAD of 1.82 kcal mol−1 outperform the FM and MD ansatz. Such an accuracy is achievable even when considering two to three orders fewer structures, depending on the level of refinement (see Fig. S2, ESI†).
The Gilson group found that β-CD binds to phenothiazine drug entities with good affinity and extended the investigation to phenothiazine derivatives. They possess favourable solubilities, and constitute a new class of molecule family that was never explored in any SAMPL challenge in the past. Experimental Gibbs energies of binding were obtained from ITC and NMR to characterize the non-covalent interactions and revealed the formation of 1:1 complexes.17 Gibbs energies of binding are in a very narrow range between −4.5 and −5.7 kcal mol−1. Chemical modifications at the heterocyclic core and/or aliphatic chain lengths increase the degree of conformational flexibility of the ligand; in combination with the flexible receptor this set represents a further level of challenge to computational approaches.
Whereas the CB[8] receptor was a rigid macrocyclic entity, the GFN2 conformational search of β-CD gave 56 unique conformers in the CRE, albeit some were high in energy and removed in subsequent QM refinement iteration steps. This shows that the iterative refinement procedure with increasing thresholds is an efficient way to filter out many high-lying conformers and to retain also few unique structures in a narrow energy window (after ‘level 3’ only two conformers were below the Boltzmann threshold of 99%). The SAMPL8 ‘drugs of abuse’ guests were small molecules with only a small number of unique conformers apart from G2 (see above). The free phenothiazines give rise to a larger number of unique conformers after CREST searches. However, the sequential QM refinement reduces the number of entries in a certain energy window above the minimum significantly by a factor of 5–10 (see Fig. S3, ESI†). For the phenothiazine-β-CD complexes, the conformational search also yielded more unique structures compared to SAMPL8 but most of them were removed during sequential refinement of electronic energies and solvation modelling.
Fig. 4 shows one example of the top-ranked pose of CPZ guest in complex with β-CD receptor. In general, the binding modes of highly ranked phenothiazine poses are in agreement with the structural interpretation of NMR studies. The β-CD receptor has two binding faces: the ‘primary’ is made up by seven primary alcohols (bottom of receptor in Fig. 4(left)), and the ‘secondary’ is consisting of fourteen alcohol groups on the other side of the receptor (top of Fig. 4(left)). Part of the phenothiazine moiety is located at the secondary face of the host and part of the drug penetrates deep into the host's cavity. Only the relatively bulky side-chains of TDZ and TFP were sufficiently locked to generate definite nuclear Overhauser effect (NOE) signals and to allow the definite assignment of an interaction with the secondary hydroxyl groups. For all phenothioazine ligands, binding poses in agreement with structural interpretation from NMR were obtained. They all reveal a bifurcated ammonium–hydroxyl interaction and an incorporation of the largely hydrophobic phenothiazine ring into the hydrophobic β-CD binding cavity (similar to Fig. 4).
The calculated Gibbs energy of binding of CPZ to β-CD (−6.7 kcal mol−1) is in good agreement with the experimental value of −5.4 kcal mol−1 (see Table S3, ESI†). In medicinal chemistry, introduction of a chlorine atom is frequently used to increase the lipophilicity of drug compounds.17 Promazine (PMZ) and chlorpromazine (CPZ) differ only in the replacement of a hydrogen atom by a chlorine, but chlorpromazine binds only slightly stronger than promazine (0.5 kcal mol−1 in experiment vs. 1.3 kcal mol−1 in calculations). This suggests that introducing the chlorine substituent is not significantly stabilizing ligand-receptor binding but may be beneficial for the drug's bioavailability. The calculated Gibbs energies of binding of all phenothiazine molecules at every level are given in Table S3 (ESI†).
Table 2 gives the analysis of errors of phenothiazine binding to β-CD. GFN2 is not able to give a binding of phenothiazine ligands to β-CD at all and the calculated Gibbs energy of binding is always positive (see Table S3 (ESI†)).
Semi-empirical methods, such as GFN2-xTB, have a poor performance in the description of ionic hydrogen bonds which are largely contributing to polarization.29 Such an underestimation of these strong hydrogen bonds can be assigned to the absence of polarization effects when using minimal valence basis sets in SQM.
As for the CB[8] receptor binding challenge, GFN2 generated structures are structurally very plausible but the deviation in energies from experiment is even larger. Calculations at level 0 and level 1 reduce the MSE and MAD significantly (see Table 2). Structural optimizations at level 2, however, do not lead to systematically lower errors for the SAMPL9 entries. High-level global hybrid meta-GGA XC functional DFT calculations generate very accurate Gibbs energies of binding with the targeted thermochemical accuracy (MSE + 0.4 kcal mol−1, MAD 0.7 kcal mol−1).
Fig. 5 shows that the MAD from experimental data can systematically be reduced when going from level 1 to 3.
Fig. 5 MAD from experiment in kcal mol−1 of calculated Gibbs energies of binding of phenothiazine drug molecules to β-CD. |
For β-CD phenothiazine binding, the best SAMPL9 submission was using an alchemical transfer model (ATM)10 with a proprietary ligand force field to give a MSE of −0.9 kcal mol−1 and a MAD of 1.6 kcal mol−1. In total, 64 individual alchemical Gibbs energy calculations and hundreds of nanoseconds of MD simulations needed to be performed obtain this accuracy. The combination of SQM exploration of the conformational space of ligands, receptors and complexes followed by refinement of electronic energies and solvation models is able to give results that are comparable to, or sometimes outperforming, the most accurate SAMPL9 submissions.
To refine the Gibbs energies of the resulting CREs, commandline energetic sorting (CENSO v.1.2.0)6 was used. At ‘level 0’, electronic energies of all the conformers were recalculated using the low-cost semi-empirical GGA-type density functional with long range dispersion corrections B97-D3(0)37,38 with a small def2-SV(P)39 basis set and the analytical linearized Poisson–Boltzmann (ALPB) solvation model.31 All conformers within 4 kcal mol−1 from the minimum were further considered for the next level. ‘level 0’ only served to eliminate unrealistic high-energy conformers.
At ‘level 1’, the Gibbs energies of all remaining conformers were calculated from single point energy calculations using the composite electronic structure method of meta-GGA type r2SCAN-3c,24,40 a large purpose-built def2-mTZVPP basis set41 and D4 dispersion corrections.42–44 The Gibbs energy threshold for this level was set to be 3.5 kcal mol−1.
Structures from ‘level 1’ were then re-optimized at ‘level 2’ using the same r2SCAN-3c functional with def2-mTZVPP basis sets and D4 dispersion corrections. The effect of solvents were included using DCOSMO-RS34 during the geometry optimizations. This step gave DFT-optimized structures of the conformers and enabled the removal of further non-unique conformers. The thermal corrections were, again, re-calculated using SPH calculations with GFN2-xTB. The Gibbs solvation energies were estimated using COSMO-RS v19.0.4(R 5514)35,45 with TZVPD_FINE parameters for SAMPL8 and TZVPD parameters for SAMPL9 calculations. Finally, conformers within 2.5 kcal mol−1 energy threshold were retained.
A final electronic energy refinement (‘level 3’) was carried out using the computationally demanding PW6B95 (6-parameter functional based on Perdew–Wang-91 exchange and Becke-95 correlation) global-hybrid meta-GGA density functional with dispersion corrections.38,46,47 and a large def2-TZVPD basis set.41 The solvent effects were obtained from COSMO-RS.
•Level 0: SP B97-D3(0)/def2-SV(P) + Esolv(GFN2-ALPB)
•Level 1: SP r2SCAN-3c(D4)/def2-mTZVPP + Esolv(GFN-ALPB) + GmRRHO(GNF2-ALPB-SPH)
•Level 2: OPT r2SCAN-3c(D4)/def2-mTZVPP/DCOSMO-RS + Gsolv(COSMO-RS) + GmRRHO(GFN2-ALPB-SPH)
•Level 3: SP PW6B95-D3(BJ)47/def2-TZVPD + Gsolv(COSMO-RS) + GmRRHO(GFN2-ALPB-SPH)
Since calculations at ‘level 0’ are mere energies of binding, they cannot be directly compared with experiments and are not discussed in the main text.
As an alternative to explicit molecular simulations, machine learning (ML) approaches are able to give Gibbs energies of binding. However, they require extensive network training on large datasets. For example, for the pillar[n]arene WP6,48 ML results trained on extensive experimental datasets were superior submissions to SAMPL9.49 For realistic or novel host–guest complexes,50 however, training data may sometimes be scarce. For example, the binding of phenothiazines to β-cyclodextrin was only recently investigated. Here, a ML framework to control the error of DFT calculations may be more appropriate.51
Footnote |
† Electronic supplementary information (ESI) available: Computational details, Gibbs energies of binding. See DOI: https://doi.org/10.1039/d4cp01529k |
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