Abstract
Site Identification by Ligand Competitive Saturation (SILCS) is a molecular simulation approach that uses diverse small solutes in aqueous solution to obtain functional group affinity patterns of a protein or other macromolecule. This involves employing a combined Grand Canonical Monte Carlo (GCMC)-molecular dynamics (MD) method to sample the full 3D space of the protein, including deep binding pockets and interior cavities from which functional group free energy maps (FragMaps) are obtained. The information content in the maps, which include contributions from protein flexibilty and both protein and functional group desolvation contributions, can be used in many aspects of the drug discovery process. These include identification of novel ligand binding pockets, including allosteric sites, pharmacophore modeling, prediction of relative protein-ligand binding affinities for database screening and lead optimization efforts, evaluation of protein-protein interactions as well as in the formulation of biologics-based drugs including monoclonal antibodies. The present article summarizes the various tools developed in the context of the SILCS methodology and their utility in computer-aided drug design (CADD) applications, showing how the SILCS toolset can improve the drug-development process on a number of fronts with respect to both accuracy and throughput representing a new avenue of CADD applications.
Introduction
In recent decades, computer simulations have become an important tool in the drug discovery and development process, making a central contribution to CADD. This includes predicting and understanding the binding of drug candidates to a target macromolecule, typically a protein, to make predictions that lead the drug development process as well as help facilitate the interpretation of results from experimental studies. CADD has benefited from the advancement of more accurate force field parameters, novel conformational and solute sampling algorithms, machine learning practices, computer hardware, in particular graphics processing units (GPU), and sophisticated software.
Current CADD methods provide trade-offs between accuracy and computational time requirements. For example, free energy perturbation (FEP) methods are widely used for computing protein-ligand relative binding affinities, often within an accuracy of less than 1 kcal/mol. However, these calculations demand large computational resources to achieve their level of accuracy. In the context of FEP, approaches such as Bennett Acceptance Ratio (BAR),1 multistate BAR,2 thermodynamic integration (TI),3 weighted histogram analysis method (WHAM),4, 5 and multisite lambda dynamics6–8 offer improved accuracy in determination of absolute or relative binding affinities in the treatment of congeneric series of ligands. Alternatively, ligand docking methods require minimal computational time with the compromise of decreased accuracy. Accordingly, there is a need for alternate CADD methods that maintain the accuracy of FEP-based methods but at a significantly lower computational cost. Such capabilities would allow for CADD to better lead the drug development process by allowing for predictions to improve various drug properties to be made on a time scale faster than experimental procedures. For example, if it is possible to synthesize and experimentally validate 100 compounds per week as part of a medicinal chemistry campaign, then CADD methods should be able to produce accurate predictions at a 10- to 100-fold faster rate to effectively expedite the drug optimization process.
Towards achieving the required accuracy and speed to lead the drug discovery process, the co-solvent or mixed molecular dynamics (MD) approaches offer great potential.9 These methods typically involve MD simulations of a protein in aqueous solution in which additional “co-solvents” are mixed in with the aqueous solution. The co-solvent molecules, or solutes, are small, with molecular weights below 150 daltons, and represent different chemical functionalities. This results in the identification of druggable binding sites, and vital molecular interactions occurring in protein-ligand binding sites which comprises plenty of information useful for qualitative and quantitative analysis for high affinity ligands. Typically, these approaches using a single solute molecule, such as isopropanol or phenol that includes hydrogen bond donor and acceptor capability as well as apolar functional groups. Some of the well-known co-solvent methods includes MDmix,10–13 MixMD,14–22 probe-based MD,23–26 and the works from Yang and Wang.27–30 Many other research labs have also come up with similar ideas and applied them to their target of interest.31–47 While these methods employ different force fields and solute molecules with different concentrations, their ultimate objective is to map the affinity patterns of functional groups on the targeted protein surface. Ghanakota and Carlson48 present an outstanding review paper discussing in detail the different co-solvent methods along with their applications on a variety of targets. However, the usage of a single, or even a few, solute molecules in the simulation systems limit the types of functional groups being considered.
Historically, the first example of considering multiple solutes in the context of CADD was reported in 1985 by Goodford in the program GRID.49 In that approach, multiple solutes (water, methyl group, amine nitrogen, carboxy oxygen, and hydroxyl) were employed to map protein surfaces resulting in visual energy contour grids depicting favorable interaction sites. This information content was then used to design compounds having similar chemical groups matching the energy contours. Subsequently, other methods such as multiple copy simultaneous search (MCSS)50, multiple protein structure (MPS) and FTMap51, 52 were developed and applied to varieties of macromolecules. However, these approaches applied limited representations of the aqueous environment through the use of various continuum solvent models as well as no or limited treatment of protein flexibility.
Towards better addressing the various issues with CADD technologies discussed above the idea of SILCS (Site Identification by Ligand Competitive Saturation) was conceptualized in the year 2008 by Olgun Guvench and Alex MacKerell with their first article on this method published in 2009 examining BCL-6 oncoprotein.53 The initial implementation of SILCS involved two solutes, propane and benzene in aqueous solution using extensive MD simulations, with the water used to map the hydrogen bond donor and acceptor functional group maps, termed FragMaps, in addition to aliphatic and aromatic distributions. In that initial implementation, a repulsive potential between the apolar solutes was implemented to avoid their aggregation, thereby allowing for the use of multiple solutes in the simulation system. Progressively, Raman et al.54, 55 extended the SILCS method to additional solutes (e.g. 8 solutes at 0.25 M including benzene, propane, methanol, formamide, acetaldehyde, imidazole, acetate and methylammonium) as well as converting the FragMaps to free energy distributions that could be used to estimate ligand binding affinities as well as rapidly allow for the relaxation of complex, drug-like ligands in the field of the FragMaps using a Monte-Carlo algorithm (see details below).
Another important contribution to the SILCS methodology was developed by Lakkaraju et al.56 The approach combined the Grand Canonical ensemble-based Monte Carlo (GCMC) sampling with MD, yielding GCMC-MD, for enhancing the overall sampling of the solute molecules and water. Using GCMC, facilitated with an enhanced sampling oscillating chemical potential approach, helps to improve the sampling of the solutes and water, especially in deep or fully occluded ligand binding pockets as found in nuclear and G-protein coupled receptors.57 This greatly increased the range of proteins and other macromolecules accessible to the SILCS technology.
Development of the GCMC-MD methodology was followed by a number of further developments of the SILCS technology. Yu et al.58, 59 developed an automated pharmacophore generation protocol that could be used in large-scale database screening using programs such as Pharmer.60 As alluded to above, tools were developed so the SILCS FragMaps could be utilized in various contexts such as SILCS-MC docking,61 taking advantage of the ability to rapidly calculate protein-ligand relative binding affinities,61, 62 SILCS-Hotspots63 was developed to facilitate identification of novel allosteric binding sites on proteins. An interesting extension was the application of SILCS for calculating protein-protein interactions (PPI).64 This technology was then combined with the ability of the SILCS-MC to rapidly dock ligands to all possible binding sites on a protein leading to the development of SILCS-Biologics.65, 66 This approach allows for evaluation of excipients in biologics formulation including the formulation of monoclonal antibodies (mAb).
The remainder of this review focuses on various aspects of the SILCS technology. Details of the methodology are included in the Computational Details section. That section includes a discussion of the computational demands of the SILCS “pre-computed ensemble” approach that allows it to lead the drug discovery process in medicinal chemistry campaigns. This is followed by information on the various tools based on the SILCS technology and their application in a variety of contexts. That section includes a summary of validation studies, testing the efficacy of the technology for predicting protein-ligand absolute or relative binding affinities for a benchmark of eight protein targets with diverse set of ligands.62 The predicted accuracy for relative binding affinities was less than 1 kcal/mol achieving a similar level of accuracy as that obtained from alchemical FEP methods with significantly lower computational cost. The final section presents potential future developments and applications of SILCS, including its utilization for modelling large macromolecular contexts and its use in studies on RNA.
Computational Details
A. SILCS Simulations
SILCS simulations are initially performed to pre-compute an ensemble of the solutes, water and protein conformations, yielding the SILCS FragMaps, which are used for the subsequent SILCS calculations. The approach was developed to allow for competition between all the solutes and water for the entire region occupied by the target macromolecule. The simulation systems consist of a protein or other macromolecule and randomly distributed solute molecules at a concentration of 0.25 M immersed in an aqueous solution of 55 M water. The most common solute molecules include benzene, propane, methanol, formamide, dimethyl ether, methylammonium, imidazole, and acetate in the standard version of the SILCS methodology. The solutes represent apolar (aromatic and aliphatic) groups, hydrogen bond donors and acceptors, and charged functional groups. Moreover, alternate solute molecules such as fluoroethane, trifluoroethane, chloroethane, fluorobenzene, chlorobenzene, and bromobenzene may be considered for accommodating halogen atoms, along with the dimethyl ether and methanol, in the halogen “SILCS-X” version.62
The SILCS simulation protocol includes a hybrid oscillating excess chemical potential (μex) grand-canonical Monte Carlo and molecular dynamics (GCMC-MD) approach in order to improve the overall sampling of the solute molecules and water. The GCMC moves comprise molecular translations, molecular rotations, and insertion or deletion of the solutes and water. All these moves are accepted or rejected based on the Metropolis criteria. The use of the oscillating μex involves altering μex to attain adequate solute insertion acceptance rates, representing an enhanced solute sampling approach. Further details of the GCMC method can be accessed in our previous work.61, 62 The MD simulations provide additional conformational sampling of the protein, solutes and water in the NPT ensemble at a system temperature and pressure of 298 K and 1 atm, respectively. The backbone alpha carbon atoms of the protein are typically restrained with a force constant of 0.12 kcal mol−1 Å-2. The timestep for the MD simulation is 2 fs with periodic boundary conditions. The simulation box size is extended 15 Å beyond the proteins in all three dimensions. For transmembrane proteins, in the SILCS-Membrane tool, the principal axis of the protein is aligned with the bilayer normal (z-axis) and relocates the protein to the center of the bilayer. The GCMC-MD simulations are performed in a sequential manner for a total of 126 cycles, composed of 26 equilibration cycles in which the solutes and water are redistributed on the simulation system followed by 100 production cycles. Each cycle involves 200,000 GCMC steps, 5,000 steps of steepest descent minimization, 100-ps equilibration MD, and a 1-ns production MD simulation. The SILCS simulation protocol recommends ten independent simulations for each target in order to obtain adequately converged ensembles of the distributions of the solutes and water and the conformations of the protein. The force field parameters for the protein, solute molecules and ligands are obtained from the additive CHARMM36m and CHARMM general force field (CGenFF).67–70 The GCMC code and additional workflows were initially developed in the MacKerell laboratory combined with various GROMACS71 utilities, which is also used for the MD simulations. In addition to studies of soluble proteins, the SILCS-Membrane module is available that allows for SILCS simulations of proteins, such as GPCRs and transporters, in an explicit membrane environment. The SILCS Software Suite is available from SilcsBio LLC and is free to not-for-profit researchers.
B. FragMap Construction
From the SILCS GCMC-MD simulations probability distributions of the solutes and water are calculated. The 100 1-ns production MD trajectories from each of the 10 independent simulations, yielding a total of 1 microsecond of MD, are used for producing FragMaps by binning selected atoms of the solute molecules into 1 Å x 1 Å x 1 Å cubic volume elements (voxels). The resulting occupancies are then normalized for the number of simulation snapshots and for the concentration of the solute atoms in the bulk solution. The bulk concentration is typically based on the average number of solute atoms relative to total number of water molecules at a 55 M concentration but may also be calculated based on an assumed concentration of 0.25 M or based on the total volume of the simulation system.72 The normalized occupancies are then converted to grid free energy (GFE) values by using the Boltzmann transformation. Therefore, GFE is an atom-based score representing free energy of the functional groups represented by the solutes relative to being in the bulk aqueous solution. Accordingly, the GFE FragMaps can assume both negative and positive free energies indicating favorable and unfavorable interactions with the protein, respectively, with zero kcal/mol indicating a free energy equivalent to being in aqueous solution. Along with the FragMaps, an “exclusion map” is generated based on regions not sampled by water or any solute molecules during the entire production run. This accounts for the conformational flexibility of the protein indicating the extent to which ligands binding to the protein can penetrate under the traditional solvent accessible surface. Thus, once the SILCS simulations are completed and the FragMaps and exclusion maps calculated, the protein structure itself is no longer used for subsequent SILCS calculations, though the structures used to initiate the simulations and from the SILCS MD simulations themselves are available for visualization and other purposes.
Regarding classification of solute molecules and associated GFE FragMaps, there are four main atom classification schemes (ACS): Generic Apolar Scale (GAS21), Generic Apolar Scale with Halogens (GAX21), Specific Standard (SS21), and Specific Halogen (SX21). In the Generic ACS, several “specific” FragMap types are grouped together to yield “generic” FragMaps. The formamide nitrogen (FORN) and imidazole donor nitrogen (IMIH) voxel distributions were merged to yield a generic hydrogen bond donor (GEND) FragMap, while formamide oxygen (FORO), dimethyl ether oxygen (DMEO), and imidazole acceptor nitrogen (IMIN) distributions are combined into a generic hydrogen bond acceptor (GENA) FragMap. Generic FragMaps also include apolar FragMaps based on the carbons of benzene and propane, heterocycle carbons of imidazole (GEHC), and methanol oxygen (MEOO) distributions. The charged functional groups include a methylammonium nitrogen (MAMN) atom type for positively charged groups, and an acetate oxygens (ACEO) atom type for negatively charged groups. In the Specific ACS, all specific FragMaps are used, supplemented by generic maps. Additionally, both the Generic and Specific ACS can be supplemented with the halogen FragMaps obtained from SILCS-X simulations.62
The convergence of the FragMaps is verified by calculating a metric named the overlap coefficient between the first five (1 to 5) and the remaining five (6 to 10) independent SILCS simulations. Higher values (ranges between 0 to 1) of OC confirm the convergence of the FragMaps. Additional details regarding the calculation of FragMaps, overlap coefficient, GFE, and ACS can be found in these references.55, 61, 62 The FragMaps obtained from the SILCS simulations can be used in a qualitative manner to assist ligand design by visualizing 3D regions where fragments can be placed and linked to make drug-like molecules or ligands can be modified by adding or removing functional groups for improving binding affinity and specificity. An example of the PTP1B FragMaps visualization is shown in Figure 1A where the FragMaps are overlaid on the crystal structure of the protein (PDB 2QBS). As shown, a variety of FragMaps occupy the active site of the protein (dotted oval). In addition, the distribution of FragMaps around the entire protein indicates the potential presence of additional putative binding sites on the protein; such sites may potentially act as allosteric binding sites. Figure 1B shows the FragMaps overlaid on the ligand from the PTP1B crystal structure at the binding site. The apolar FragMaps clearly replicate the presence of both aromatic rings. The representation of hydrogen bond donor and acceptor maps shows the possibility of such groups in that region. In addition, the carboxylate groups of the crystal ligand are accurately captured by the ACEO FragMaps as shown on the left side of the figure. The acetate group makes multisite interactions with the surrounding protein residues including lysine and arginine, along with waters. This example shows the capability of SILCS FragMaps in capturing prominent molecular interactions or binding hotspots that can be further utilized for several CADD approaches as shown in the later sections of this article. The FragMaps and exclusion maps can be readily visualized using Pymol73 or visual molecular dynamics (VMD)74 program as well as in other programs as the maps may be supplied in CCP4 format traditionally used for visualization of electron densities.
Figure 1:
(A) FragMaps shown for PTP1B overlaid on the crystal structure (PDB 2QBS) along with co-crystal ligand in the binding pocket. (B) FragMaps overlaid on the protein PTP1B ligand crystal conformation with the portion of the protein occluding the binding pocket view omitted. The co-crystal ligand structure is shown in CPK representation. For figures A and B, carbon, nitrogen, oxygen, sulfur and bromine atoms are shown in cyan, blue, red, yellow and pink, respectively. The FragMaps color are GENN or APOLAR (green), GENA (red), GEND (blue), MEOO (tan), MAMN (cyan), and ACEO (orange). FragMaps isocontour surfaces are displayed for apolar, charged, hydrogen bonding donor and acceptor groups at a cutoff of −1.2, −1.5, −0.9, and −0.9 kcal/mol. (C) Different SILCS atom classification schemes for the same ligand. Atom types GENA, GEND, PRPC, BENC, DMEO, FORN, GEHC, ACEC, BRBX and NCLA are shown in red, blue, yellow, green, magenta, light blue, brown, orange, pink, and white respectively.
C. SILCS Toolset
The SILCS toolset comprises a number of applications (Figure 2) based on the FragMaps obtained from the SILCS simulations. Most of these applications are quantitative in nature, providing information that may be used for various aspects of drug development as well as macromolecular modelling. These include the ability to perform spatial and conformational sampling of ligands ranging from fragment molecules to drug-like molecules to larger molecules such as polypeptides, oligonucleotides and oligosaccharides, termed SILCS-MC. This technology is the foundation for additional tools including SILCS-Hotspots for allosteric site identification and SILCS-Biologics for use in the formulation of mAbs and other protein-based drugs. To facilitate database screening, SILCS may be used to create Pharmacophores, termed SILCS-Pharm. In addition, SILCS-PPI allows for the mapping of protein-protein interactions (PPI) including the full range of possible interactions between protein partners. Details of these methods and associated applications are presented below.
Figure 2:
SILCS applications based on the FragMaps obtained by running SILCS simulations.
D. Computational Requirements of the SILCS Method
Central to the utility of the SILCS toolset is the huge computational efficiency of the method. This is based on the SILCS approach being based on the use of a pre-computed ensemble of the solute, water, and protein conformations. This pre-computed ensemble, in the form of the SILCS FragMaps and exclusion map, is then used for all the calculations associated with the SILCS toolset. Thus, once the initial SILCS simulations are completed, subsequent calculations take on the order of seconds to hours. For example, SILCS-MC using an exhaustive docking approach may require on the order of minutes on a single core per ligand, whereas a local pose refinement calculation, analogous to FEP methods, requires only seconds. SILCS-PPI calculations are more demanding but still only require on the order of hours. This speed allows for large number of ligands to be evaluated against all possible binding sites on a protein in a matter of hours on a multicore small computer cluster. Concerning the initial SILCS simulations, their computational demands are based on the systems size. In the context of a cluster of 10 GPUs, (e.g. NVIDIA 2080TI GPUs on 8 core Ryzen CPUs or on the cloud such as AWS) for a small protein such as Mcl-1 or Bcl-xL (35–40K atoms) the calculation is completed within one day while a GPCR with full membrane representation (~140,000 atoms) requires approximately 3.5 days. Thus, while the initial SILCS simulations require a significant amount of time, once the SILCS FragMaps are available, they may be used for the full range of SILCS toolset in a rapid, and accurate manner.
Applications of SILCS Toolset in CADD
A. SILCS-MC Docking
SILCS FragMaps can be utilized to perform rapid ligand docking and compute approximate ligand binding affinities. To calculate the binding free energies, each non-hydrogen atom of the ligand is either classified as one of the FragMap types or assigned as non-classified. All hydrogens are non-classified. The Cartesian coordinates of each classified atom are then used to determine its overlap with a FragMap voxel, with that atom being assigned the GFE value of the voxel. Atoms that are non-classified are assigned a GFE of zero. The Ligand Grid Free Energy (LGFE) is simply the sum of its individual atomic GFEs, which SILCS uses as an approximation of the ligand binding free energy. LGFEs are only approximations of binding free energy due to the lack of additional factors, such as the entropy loss of combining multiple smaller fragments into a larger ligand. The SILCS exclusion map, voxels for which no solute or water atoms were sampled during the simulations, acts as the protein surface and imposes an energetic penalty to prevent the ligand from penetrating into the protein. Figure 1C details the FragMap classifications for an example PTP1B ligand using all four atom classification schemes.
The SILCS-MC docking procedure involves a series of energy minimization, Markov chain Monte Carlo, and simulated annealing steps to determine the lowest LGFE pose of the ligand. The initial ligand pose used by SILCS-MC can either be generated randomly (“exhaustive” or “docking” protocol) or taken from a predetermined set of coordinates (“local” or “pose refinement” protocol). For the docking protocol, the ligand is randomly placed within a sphere of a given radius (ligand placement radius, rLP) centered at a user-determined coordinate. Previous work has shown the docking protocol to generally perform better than the pose refinement protocol, though at more computational expense.61 For each docking or pose refinement, multiple SILCS-MC runs are used for each ligand to improve sampling and convergence of the LGFEs. There are several advantages to the SILCS-MC docking procedure for computing ligand binding affinities compared to current alchemical FEP75–77 methods. First, while some knowledge of the location of the binding pocket is needed to seed to the docking simulations, the exhaustive protocol negates the need for detailed crystal structure coordinates of the parent ligand. Second, each ligand binding affinity and binding pose is independent of any other ligand, so there is no need to perform many relative binding affinity calculations as is required by FEP methods, especially with cycle-closure corrections.78 Lastly, LGFE approximates the ligand’s absolute binding free energy, so no experimental data is necessary for computing such quantities, though that data can be used to improve SILCS absolute binding free energies as is done for FEP methods.62
In a recent study, SILCS-MC docking was performed for all four classification schemes, as detailed in Figure 1C on a collection of 8 target proteins. Multiple ligand-placement radii were used for the exhaustive protocol: 1, 2, 5 and 10 Å such that a total of 16 models were run for each protein (four ligand-placement radii for each of the four classification schemes). Several performance metrics were used to compare the computed binding free energies to experimental values, including mean unsigned error (MUE), Pearson’s correlation coefficient (R), and percent correct (PC). The best performing model across multiple target proteins according to this metric was SX21 using the exhaustive protocol with rLP = 5 Å,62 such that this was assigned as the default protocol for SILCS-MC docking if no experimental data is available. If some experimental data is available, the best performing model can be chosen for further testing and model optimization. For these purposes, PC (representing rank-ordering of ligands) was chosen as the desired performance metric. Performance of SILCS for PTP1B ligands79 is shown in Figure 3 and Table 1 for a full set of 48 ligands as well as a smaller curated set of 23 ligands first used by Wang et al. with the FEP+ method78 and subsequently used by other groups to test AMBER GPU-TI,80 Flare81 FEP, and pmx82 (GROMACS utility). The SILCS results for PTP1B compare favorably to these published FEP based approaches that used the smaller ligand set, even when all 48 ligands are used. The Default model performs similarly to Flare FEP81 (PC = 0.78) and pmx82 (PC = 0.68 to 0.76), while the Best PC model approaches the AMBER GPU-TI80 results (PC = 0.814). Among these methods, only FEP+78 (PC = 0.844) surpasses the performance of SILCS-Best PC. When all 8 targets were considered, the SILCS-MC method is similarly competitive with the FEP methods, though at a computational savings of more than 300 fold.62 Moreover, ML optimization of the SILCS model proves to be a particularly powerful tool not currently available to FEP methods, producing an average percent correct score of 0.82, surpassing FEP+’s performance of 0.78 with the OPLS 2.1 force field.62, 78
Figure 3:
Computed versus experimental ΔG for 23 (upper) and 48 (lower) PTP1B ligands for various SILCS models: Default, Best PC, and ML-Optimization based on the PC for the 23- and 48-ligand sets were performed independently.
Table 1:
Performance of SILCS for 23 and 48 PTP1B ligands using Default, Best PC, and ML-Optimized models.
| Model | ACS | rLP | Ligands | MUE | R | PC |
|---|---|---|---|---|---|---|
| Default | SX21 | 5 | 23 | 0.707 | 0.650 | 0.761 |
| Best PC | GAS21 | 5 | 23 | 0.642 | 0.781 | 0.828 |
| ML-Opt | SX21* | 5 | 23 | 0.622 | 0.865 | 0.895 |
| Default | SX21 | 5 | 48 | 0.880 | 0.753 | 0.755 |
| Best PC | GAS21 | 5 | 48 | 0.936 | 0.790 | 0.804 |
| ML-Opt | GAS21* | 5 | 48 | 0.903 | 0.815 | 0.810 |
indicates parameters were optimized using the Bayesian-MCSA procedure; rLP is the ligand placement radius, in units of Å; MUE is the mean unsigned error, in units of kcal/mol; R is Pearson’s correlation coefficient; PC is percent correct.
A machine learning (ML) procedure, Bayesian Markov State Monte Carlo Simulated Annealing (Bayesian-MCSA) allows for improvements in the predictability of the SILCS-MC method when experimental information is available. In the published study, the ML approach was used to further optimize the weighting of each FragMap as it contributes to the atomic GFE values.61 Using a set of ligand binding poses generated from non-optimized SILCS-MC docking simulations, FragMaps weights were adjusted via Bayesian-MCSA while ligand coordinates were fixed in order to optimize the PC metric. This optimization procedure was performed on five different training sets, each composed of 80% of the available 48 ligands to produce five different PC-optimized models for each ACS (20 total models). Each new model was then used for new SILCS-MC docking on all 48 ligands, with the best performing model (as determined by PC) chosen as the “ML-Optimized” model. While the PC-based ML-optimized model only marginally improves the performance for the full 48-ligand set, for the smaller, curated set of 23 ligands, the performance of SILCS surpasses that of FEP+. A particular advantage of the Bayesian ML SILCS method is the use of the FragMaps as priors such that the optimization may be undertaken with small training sets of ligands as previously reported.
While SILCS-MC can supply information on changes in ligand affinity upon chemical modification at an accuracy competitive with computationally demanding FEP methods, it offers additional information on the contributions of individual atoms in the ligand to the changes in affinity that are not accessible to FEP methods. Atomic GFE values can be used to guide lead optimization by detailing how different moieties in a ligand contribute to the change in binding affinity. Figure 4 details a modification between two PTP1B ligands where a cyclopentyl group is added in order to occupy a hydrophobic pocket. While the new group contributes favorably to binding affinity, its addition shifts the other moieties into less favorable positions, reducing their favorable contributions, thereby limiting the overall gain in affinity. This can be observed in the summed GFE score of −2.19 kcal/mol for the full cyclopentyl group, whereas the GFE score for other rings and nitrogen atom becomes less favorable. Overall, this modification results in a computed ΔΔGSILCS score of −1.0 kcal/mol, matching well with the ΔΔGExpt value of −0.87 kcal/ mol. The FragMaps in this pocket further suggest that acetate groups flanking both ends of the ligand may be a new direction for further optimization. Such detail could not be extracted from typical FEP-based methods. The results for PTP1B exemplify the information content of SILCS that is not accessible in other CADD binding affinity methods.
Figure 4:
LGFE and GFE moiety contributions between two PTP1B ligands where a cyclopentyl group is added onto a terminal amine group. Atomic GFE contributions for the constituent groups are shown in units of kcal/mol. While the cyclopentyl group contributes favourably to the binding free energy, other constituent groups are moved into less favorable positions, reducing the overall gain in free energy upon addition of the cyclopentyl group. FragMap contours are the same as those in Figure 1.
B. SILCS-Pharm
Pharmacophore modelling is a widely used CADD approach that is based on the types and spatial relationship of functional groups that are crucial for interactions of ligands with the protein target.83 The resulting pharmacophore models can be used to quickly screen against a database to identify ligands with functional groups that match the required features and its performance is often superior to ligand docking based virtual screening (VS).84 SILCS FragMaps at negative GFE values represent the favorable binding regions for the respective functional groups on a given target. When the desired binding site on the target is confirmed, SILCS-Pharm converts these favorable FragMaps into pharmacophore features using a clustering approach with the resulting target-based pharmacophore used for VS.58, 59
Generation of pharmacophore features from GFE FragMaps by SILCS-Pharm involves four key steps. The first step is selection of voxels at a user assigned GFE cutoff for each type of FragMap within the user-defined binding region. All significant voxels which have more favorable GFE values than the cutoff value are selected within the binding pocket and then used in the second step for clustering. For each FragMap type, voxels that are adjacent to each other are put into the same cluster and form a FragMap feature. At the third step, FragMap features are converted into pharmacophore features. Since there are multiple FragMap types, while pharmacophore feature types need to be generic for VS purposes, FragMap features are then combined and generalized into pharmacophore features for practical use. After generation of the pharmacophore features in the third step, they are prioritized according to their feature GFE (FGFE) values. Since GFE represents the binding strength of a fragment atom at a given position, FGFE, which is the sum over GFEs of all voxels within a FragMap feature cluster, can be used to quantify the significance of a pharmacophore feature.59 In addition to the normal pharmacophore features, volume constraints that define the shape of the binding region are constructed based on the SILCS exclusion map. Compared to the traditional volume restraints that are built from a rigid structure, use of exclusion map introduces target flexibility in the definition of the binding site shape in a pharmacophore model and thus can help to lower the number of false negatives in a VS.59 At the last step, final pharmacophore hypotheses (i.e., models) are generated by combining selected pharmacophore features for use in VS. Typically, a given binding site will contain 5 to 10 pharmacophore features, numbers that are too large for VS as the number of ligands that match to type and location of large numbers of feature become vanishingly small. Accordingly, the user can select a small set of features, typically 4, to comprise an individual pharmacophore hypothesis for VS. The users can further select features to be included in the final hypotheses with the help of external information such as chemical structures of known binders. Models containing 4 features gave the best performances in general according to our test using the targets from the DUD database.85 In practice, multiple pharmacophore hypotheses are selected for a given binding site and each used for individual VS. The top ranked compounds, for example, 10K per hypothesis, are then pooled and subjected to SILCS-MC pose refinement from which the LGFE scores are used for final ranking and selection of compounds for experimental testing.86
In our previous study, SILCS pharmacophore models were tested in VS using the DUD data sets for eight protein targets including HIVPR, Fxa, DHFR, FGFr1, P38 MAP, ADA, ER and AmpC.59 Enrichment results of SILCS-Pharm on the eight targets were compared with docking results using available docking programs including DOCK,87 AutoDock,88 and AutoDock Vina.89 Better enrichment results were observed in general for SILCS-Pharm models when compared to the docking results along with significantly lower computational costs. One example is shown in Figure 5 for the protein target ER. As shown in Figure 5A, apolar (green meshes) and hydrogen bonding donor (blue meshes) and acceptor (red meshes) FragMaps are seen in the binding pocket of ER. SILCS-Pharm followed by user intervention produced a four-feature pharmacophore model as shown in Figure 5B composed of three hydrophobic features (green) and one joint hydrogen bonding donor and acceptor feature (cyan). This pharmacophore model is consistent with the crystal binding mode of a ligand from PDB entry 3ERT as shown in Figure 5B. When we tested this model against DUD data set for ER, an early stage enrichment factor (EF1) of 14.3 and an area under the curve (AUC) of 0.81 were achieved, where these values were 6.0 and 0.64 for AutoDock 4 which yielded the best results among all tested docking methods.59
Figure 5:
(A) FragMaps at the binding pocket of ER (PDB: 3ERT) with apolar, hydrogen bonding donor and acceptor FragMaps contoured at −1.5, −0.8 and −0.8 kcal/mol and (B) the pharmacophore model generated using SILCS-Pharm from our previous study.59 Apolar pharmacophore features are colored in green and hydrogen bonding donor and acceptor joint feature is colored in cyan. Crystal binding mode of a ligand in PDB entry 3ERT is also overlaid on the pharmacophore model.
C. SILCS-Hotspots
Two areas of particular interest to drug discovery are the identification of novel allosteric binding sites and the use of fragment-based drug design (FBDD). FBDD is a promising methodology to develop novel ligands that target macromolecules.90–93 Instead of using large, drug-like compounds for screening, FBDD first identifies small fragments that bind to a set of binding “hotspots”. Once the hotspots and promising fragments are identified, chemists design larger, more drug-like molecules either by linking them or adding R-groups to a scaffold that can capture the fragment-protein interaction.94, 95 With respect to allosteric binding sites, while such sites have long been exploited for therapeutic agents, interest in identifying such sites has recently increased. Allosteric sites offer the possibility of improved specificity, especially against targets with common substrates, and to minimize side effects with targets that participate in biochemically essential pathways. In such targets, either positively or negatively modulating the activity may be preferable to completely inhibiting the protein activity. Towards identification of allosteric sites, it’s important to account for binding pockets that are not evident in experimental protein structures as well as being amenable to targeting by drug-like molecules.
SILCS-Hotspots is an extension of the SILCS-MC methodology designed to identify fragment binding hotspots that are spatially distributed across the global protein structure including both surface and interior binding sites.63 It is performed by comprehensively partitioning the full 3D space of the protein into a collection of overlapping regions into which each fragment is docked a minimum of 1000 times using SILCS-MC. Once the fragments have been docked on the entire protein, two rounds of spatial clustering for the individual fragments and the overall fragment types are undertaken from which the final hotspots are identified. Accordingly, the method not only identifies sites but also a collection of fragments occupying those sites. This approach has been applied to a set of ~90 mono and bicyclic rings present in drug molecules96 and the Astex MiniFrag90 set, though user-supplied fragment libraries may be employed. In addition, the methodology can be applied to larger drug-like molecules to identify their binding sites. As SILCS-Hotspots use SILCS FragMaps, which are computed from GCMC-MD simulations with an enhanced sampling strategy, the method can identify a large number of sites on the target protein, including many sites not accessible in crystal structures. SILCS-Hotspots has successfully recapitulated the location of known drug-like molecules in both allosteric and orthosteric binding sites on diverse proteins targets including the nuclear receptor, kinases, enzyme, and GPCRs63 as well as successfully leading to the identification of novel ligand binding and allosteric sites.86, 97
An example is presented in Figure 6 for Androgen receptor (PDB 2AM9). The figure shows potential binding hotspots on the protein surface as van der Waals spheres and are colored based on the average LGFE scores of the fragments occupying each site binding pose. The SILCS-Hotspots method successfully identified the orthosteric binding site, which is occluded and is not accessible in a typical MD simulation. The identification of the internal orthosteric binding site was possible due to GCMC sampling performed during the SILCS simulation where solute molecules are removed/inserted anywhere in the simulation system. This and the use of the SILCS exclusion maps allows for the fragments to be docked into the interior orthosteric site. In addition, a known allosteric site was identified by the SILCS-Hotspots method. In the figure, flufenamic acid, an allosteric modulator, from the crystal structure PDB:2PIX is overlaid on the SILCS FragMaps and Hotspots calculated using PDB:2AM9. Notably, this allosteric site is not discoverable using other static pocket detection algorithms, such as FTMap52 or Fpocket,98 because the pocket is closed in the crystal structure used for the SILCS simulations (PDB:2AM9) indicating the ability of the SILCS approach to identify deep and occluded pockets. This illustrates the importance of accounting for protein dynamics in finding allosteric pockets.
Figure 6:
SILCS-Hotspots results on Androgen Receptor. Shown are the SILCS Hotspots as VDW spheres colored by average LGFE score (red, most favorable to blue, least favorable) along with the SILCS FragMaps at −1.2 kcal/mol (see Figure orthosteric and allosteric pocket in legend). The orthosteric site is occluded and is not visible in the solvent accessible surface representation of the receptor.
For both identification of allosteric sites and FBDD our analysis indicates the importance of considering all hotspots, versus just the most favorable sites. For FBDD to work successfully, it is essential to identify fragment binding sites that are spatially adjacent such that fragments occupying those sites may be linked to create drug-like ligands. Current experimental and computational approaches typically can identify only a limited number of fragment sites as well as use a limited number of fragment types. These limitations are particularly challenging as fragments that are of utility for FBDD alone may have binding affinities in the high mM range, making them inaccessible to experimental methods. Importantly, SILCS-Hotspots largely overcomes such limitations.
D. SILCS-PPI
Computational identification of protein-protein interactions (PPI) is challenging due to the large dimensionality of the docking process as well as the need to take into account protein flexibility. SILCS FragMaps, by accounting for protein flexibility and offering grid-based GFE distributions, were therefore investigated for use in PPI, leading to the SILCS-PPI protocol.64 A variety of protein-docking algorithms have been developed99 with a large portion adopting global searching algorithms that utilize fast Fourier transforms (FFT).100 The FFT approach expedites the sampling process but requires a scoring function expressed on 3D grids. Since SILCS GFE FragMaps are naturally expressed on 3D grids, our SILCS-PPI protocol adapted the FFT-based algorithm to address the PPI prediction problem. Superior to classic FFT-based PPI prediction methods, the FragMap free energy grids contain intrinsic contributions from protein flexibility and desolvation effects. To take advantage of these grids for PPI docking, the probability distributions of sidechains were extracted from the SILCS simulations, yielding protein probability grids (PPG). The PPG are then assigned to the corresponding FragMap types, such that the spatial overlap of the FragMaps of the receptor protein with the PPG of the ligand protein acts as a rapid, grid-based estimation of the binding between the proteins. Notably, complementary information from the receptor and ligand proteins may be considered as part of the scoring function, from which the correlations between protein A and B are evaluated through FFT for both pairs. That is, FragMaps of protein A with PPGs of protein B and PPGs of protein A with FragMaps of protein B are all being considered. The docking score is summed over all FragMap types and the best score will be found for the PPI pose, which has maximized matches between FragMaps and PPGs of protein A and B.
SILCS-PPI was tested using eight protein-protein complexes mainly from the protein docking benchmark 5.0101 covering a variety of protein types. Competitive performance by SILCS-PPI was observed when compared with three other commonly used PPI docking methods include ZDOCK,102 RosettaDock,103 and ClusPro.104 Moreover, as SILCS-PPI does global docking and samples the entire receptor surface, alternative PPI binding orientations can be also being considered, with the top 2000 orientations generated by default. The validity of alternative binding poses was confirmed by experimental crystal contacts in some of the test cases. While SILCS-PPI in the context of a single PPI calculation is computationally expensive due to the need to perform the SILCS simulations, once the FragMaps are available, they can be used for additional PPI calculations with other proteins as well as for use in the context of the range of SILCS tools.
E. SILCS-Biologics
Protein therapeutics are an increasingly common drug class that leverages the inherent specificity of proteins, including mAbs, for their targets.105–108 However, protein therapeutic typically require a concentrated protein formulation, which can lead to aggregation, precipitation, and degradation due to self-association of the therapeutic molecule.109–112 Minimizing these issues is important to allow for the drug to be delivered intravenously (IV) and to maintain the integrity of the drug during storage. Excipients are small molecules other than the active pharmaceutical ingredients that are added to the formulation of the therapeutic to improve the stability, bioavailability, and manufacturability.113–115 It has been shown that certain excipients can increase stability and lower viscosity of the protein therapeutics significantly. However, the selection of the excipient often relies on experimental trial and error due to a lack of methodologies to rationally select excipients.
The need for improved approaches for protein formulations led to the development of SILCS-Biologics.65, 66 The approach combines SILCS-PPI64 and SILCS-Hotspots63 to discover excipients and rationally select excipients using a data-science and machine learning approach. The SILCS-Biologics workflow provides a set of features for each excipient from the SILCS-PPI and SILCS-Hotspots calculations and then identifies features that are most responsible for experimental physico-chemical data, such as the stability or viscosity of a protein therapeutic. SILCS-Biologics has been successfully applied to the National Institute of Standards and Technology mAb (NISTmAb)116, 117 along with the CNTO607118 mAb. CNTO607 is a model mAb to examine PPIs and NISTmAb was used to examine excipient−protein interactions taking advantage of the experimental data available on that system.118 Features from SILCS-Biologics based on the NISTmAb Fab for the different excipients include the distribution of binding sites and number of sites for each excipient, predicted affinity of excipients, competition of excipients, and the relation of the interactions to predicted PPI encompassing the entire protein surface. From the validation study, a range of SILCS-Biologics derived data was shown to be predictive against various experimental data. Specifically, the number of favorable excipient binding sites that are involved in predicted PPIs correlate with experimentally determined viscosity for a range of excipients including amino acids and sugars. In addition, a combination of the number of binding sites and the predicted binding affinity is indicated to be predictive of relative protein stability.
Figure 7 shows how chemically similar excipients may lead to differential interaction with a protein therapeutic. In the figure, the Fab domain of the NIST antibody structure is shown in surface representation. The surface of the protein is colored based on the likelihood of being involved in self-PPI (blue (low probability) to red (high probability)). We hypothesize that large amounts of PPI of the protein drug with itself (self-PPI) in a protein therapeutic lead to aggregation and higher viscosity. The figure also shows the binding hotspots of arginine (A) and lysine (B), two chemically similar excipients, on the Fab domain. Although having very similar chemical structures, they show differences in their interaction patterns. The detailed knowledge of how these excipients interact at the surface of the protein therapeutic combined with their self-PPI pattern provides a depth of knowledge to the formulation scientists to select the best excipients that can reduce aggregation in the sample. In addition to qualitative exploration, SILCS-Biologics is of utility for quantitative and predictive excipient design. Comparison of arginine, trehalose, and sucrose with the NISTmAb Fab, all of which give the highest viscosity, indicates that higher viscosities are associated with a low number of predicted binding sites, with lower binding affinity of arginine, leading to its anomalously high impact on viscosity. Such analysis indicates the potential for the SILCS-Biologics approach to be of utility in the rational design of excipients during biologics formulation.
Figure 7:
Different distribution of excipients, (A) Arginine and (B) Lysine, on the surface of the Fab domain of the NIST antibody. The surface of the Fab domain is colored based on PPI preference, where the residues are predicted to be involved in PPI are colored in red with regions approaching zero PPI in blue. Reprinted (adapted) with permission from Molecular Pharmaceutics. Copyright 2020 American Chemical Society.
Applications with other co-solvent Methods
Similar to the SILCS applications, other co-solvent based methods have shown potential in the context of different CADD applications. Table 2 summarizes most of the available co-solvent methods and their published applications for CADD purposes. Details of the different methods may vary based on the number and type of co-solvents, sampling approach, force field parameters, and calculations of the distribution of co-solvents. However, the ultimate gain from using such approaches generally is to identify biologically relevant sites on the protein surfaces and using that information in rational drug design. In spite of the technical differences, most of the approaches successfully report identification of crucial binding positions including active and allosteric sites for a diverse collection of proteins indicating a general utility of co-solvent approaches. However, the major success of these methods is their utilization in computing protein-ligand relative binding affinities, hit identification, and lead optimization. Prominently, the methods MDmix, MixMD, and pMD have shown several such capabilities for drug design against a range of protein targets. All of these studies indicate the general utility of co-solvent methods and it is always encouraging to see how different labs leverage such methodologies in innovative applications.
Table 2:
Summary of the other co-solvent based methods and their applications in the context of CADD.
| Method/Authors | Targeted Applications |
|---|---|
| MDmix | Detecting binding sites and druggability prediction10, water displaceability prediction and interaction maps of protein binding sites,11 protein-ligand docking and computing binding affinities,12 and pharmacophore modeling13 |
| MixMD | Identifying binding sites,17, 19, 22 Mapping hotspots,15, 16 co-solvent on/off rate kinetics and allosteric binding sites,21 predicting displaceable water sites,18 free energies and entropies of binding sites20 |
| pMD | Identification of ligands binding site including active and allosteric binding sites in proteins,23 and membrane bound drug targets (pMD-membrane)24, 26 |
| Caflisch and co-workers | On-off rates and binding affinities of co-solvent,44 and water displaceability by co-solvents45 |
| Yang and Wang co-workers | Finding binding hotspots,27–30 and druggable protein conformations119 |
| Tan and co-workers | Identifying halogen and hydrophobic binding sites for ligand design,38–40, 120 and multiple ligand mapping MD36 |
| Fabritiis and co-workers | Predicting protein cryptic sites46 |
| Bahar and co-workers | Druggability assessment of allosteric proteins,41 and pharmacophore modeling121 |
| Cosolvent Analysis Toolkit | Hotspot identification37 |
| Favia and co-workers | Revealing cryptic ligand binding pockets32 |
| Lill and co-workers | Identify binding location of different functional group and rank-ordering of ligands34, 47 |
| EXPROPER | Ligand binding of proteins and hotspot locations35 |
| Uehara & Tanaka | Multiple druggable protein conformations31 |
| ColDock | Generating protein-ligand docking structures42 |
| Fragment dissolved MD | Identifying binding sites43 |
Future Directions and Summary
While the SILCS toolset has a significant number of capabilities, ongoing efforts involve new concepts and applications based on the use of the pre-computed FragMaps. An interesting avenue is the impact of inclusion of the explicit treatment of electronic polarization in the calculation of the FragMaps using the Drude polarizable force field. The first study moving in this direction involved a diverse set of targets and ligands using the SILCS framework with comparison to the results from the additive force field.122 Usage of the Drude polarizable force field produces better hydrogen bond donor or acceptor FragMaps including halogen atoms and results in better docking scores as compared to scores of the additive force field. An extension of the SILCS-MC docking approach is in progress to include water-mediated interactions between the protein and ligands for more accurately predicting relative binding affinities and better understanding the contributions of individual water molecules to ligand binding. Another ongoing development is focused on improving the sampling efficiency of the GCMC simulations by enhancing insertion and deletion probabilities via two main approaches: (i) implementing biases into the GCMC procedure, and (ii) implementing a new, more adaptive oscillating-μex algorithm. The biases are built on the work of Woo et al.123 by implementing a cavity-biased search algorithm and a conformational bias. These two biases select the optimal insertion points and conformations and orientations for each fragment. These efforts are being performed in conjunction with an extended oscillating-μex algorithm that responds more strongly and directly to changes in solute concentrations, leading to greater sampling of the solutes in the GCMC simulation and ultimately a more dynamic physicochemical environment around the target protein. While the introduction of biasing methods in GCMC led to increased computational costs, efforts to port the GCMC code to GPUs show promise to significantly improve the speed of these aspects of the SILCS simulations. These advances are also showing significant progress in the application of SILCS to RNA molecules, an emerging class of drug targets. In the end, our laboratory is committed to implementing and validating useful computational tools to facilitate multiple aspects of the drug development process.
Among different co-solvent based methods, SILCS developments have made tremendous progress in the last decade, broadening the types of applications and applying them to a variety of protein targets. The primary advantage over other co-solvent methods is the utilization of multiple solutes in the SILCS simulations, allowing for the calculations of FragMaps for a broad range of chemical functional groups. Once available, the FragMaps may be used in a variety of contexts as described above in the overview of the SILCS toolset. Examples of interesting application of the methods have included the identification of host-based antivirals with the potential to treat a wide range of RNA viruses including influenza, coronaviruses and filoviruses,86 the development of a model to predict hERG blockade,124 an important problem in drug development, through SILCS simulations of the hERG channel itself, design of lipopolysaccharide analogs targeting TLR4,125 and the modelling of interaction of IgG antibodies with the protein Endoglycosidase S2.126 In an interesting variation of the SILCS approach, it was utilized to study the permeability of small drug molecules across phospholipid bilayers and their free energy profiles.72 Notable application by other laboratories include using SILCS to facilitate the design of covalent inhibitors127 and the optimization of kinase inhibitors.128 Overall, these various applications further indicate the utility of the SILCS approach indicating it to be a platform approach of wide utility beyond just being used for site identification by ligand competitive saturation.
Acknowledgements
This work was supported by NIH grant R44GM109635 and R35GM131710 and the Samuel Waxman Cancer Research Foundation. The authors acknowledge computer time and resources from the Computer-Aided Drug Design (CADD) Center at the University of Maryland, Baltimore.
Footnotes
Conflicts of interest
ADM Jr. is co-founder and Chief Scientific Officer of SilcsBio LLC.
References
- 1.Bennett CH, J. Comp. Phys, 1976, 22, 245–268. [Google Scholar]
- 2.Shirts MR and Chodera JD, J. Chem. Phys, 2008, 129, 124105. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 3.Kirkwood JG, J. Chem. Phys, 1935, 3, 300–313. [Google Scholar]
- 4.Kumar S, Bouzida D, Swendsen RH, Kollman PA and Rosenberg JM, J. Comput. Chem, 1992, 13, 1011. [Google Scholar]
- 5.Kumar S, Rosenberg JM, Bouzida D, Swendsen RH and Kollman PA, J. Comp. Chem, 1995, 16, 1339–1350. [Google Scholar]
- 6.Hayes RL, Armacost KA, Vilseck JZ and Brooks III CL, J. Phys. Chem. B, 2017, 121, 3626–3635. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 7.Vilseck JZ, Armacost KA, Hayes RL, Goh GB and Brooks III CL, J. Phys. Chem. Lett, 2018, 9, 3328–3332. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 8.Raman EP, Paul TJ, Hayes RL and Brooks III CL, J. Chem. Theory Comput, 2020, 16, 7895–7914. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 9.Bissaro M, Sturlese M and Moro S, Drug Discov. Today, 2020, 25, 1693–1701. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 10.Seco J, Luque FJ and Barril X, J. Med. Chem, 2009, 52, 2363–2371. [DOI] [PubMed] [Google Scholar]
- 11.Alvarez-Garcia D and Barril X, J. Med. Chem, 2014, 57, 8530–8539. [DOI] [PubMed] [Google Scholar]
- 12.Arcon JP, Defelipe LA, Modenutti CP, López ED, Alvarez-Garcia D, Barril X, Turjanski A. n. G. and Martí MA, J. Chem. Inf. Model, 2017, 57, 846–863. [DOI] [PubMed] [Google Scholar]
- 13.Arcon JP, Defelipe LA, Lopez ED, Burastero O, Modenutti CP, Barril X, Marti MA and Turjanski AG, J. Chem. Inf. Model, 2019, 59, 3572–3583. [DOI] [PubMed] [Google Scholar]
- 14.Lexa KW and Carlson HA, J. Am. Chem. Soc, 2011, 133, 200–202. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 15.Lexa KW and Carlson HA, J. Chem. Inf. Model, 2013, 53, 391–402. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 16.Ung PM, Ghanakota P, Graham SE, Lexa KW and Carlson HA, Biopolymers, 2016, 105, 21–34. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 17.Graham SE, Leja N and Carlson HA, J. Chem. Inf. Model, 2018, 58, 1426–1433. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 18.Graham SE, Smith RD and Carlson HA, J. Chem. Inf. Model, 2018, 58, 305–314. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 19.Ghanakota P and Carlson HA, J. Phys. Chem. B, 2016, 120, 8685–8695. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 20.Ghanakota P, DasGupta D and Carlson HA, J. Chem. Inf. Model, 2019, 59, 2035–2045. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 21.Chan WK, DasGupta D, Carlson HA and Traynor JR, J. Comput. Chem, 2021, 42, 2170–2180. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 22.Smith RD and Carlson HA, J. Chem. Inf. Model, 2021, 61, 1287–1299. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 23.Prakash P, Hancock JF and Gorfe AA, Proteins: Struct. Funct. Bioinf, 2015, 83, 898–909. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 24.Sayyed-Ahmad A and Gorfe AA, J. Chem. Theory Comput, 2017, 13, 1851–1861. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 25.Sayyed-Ahmad A, Curr. Top. Med. Chem, 2018, 18, 2278–2283. [DOI] [PubMed] [Google Scholar]
- 26.Prakash P, Sayyed-Ahmad A and Gorfe AA, PLoS Comput. Biol, 2015, 11, e1004469. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 27.Yang C-Y and Wang S, ACS Med. Chem. Lett, 2010, 1, 125–129. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 28.Yang C-Y and Wang S, ACS Med. Chem. Lett, 2011, 2, 280–284. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 29.Yang C-Y and Wang S, ACS Med. Chem. Lett, 2012, 3, 308–312. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 30.Yang C-Y, PloS one, 2015, 10, e0118671. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 31.Uehara S and Tanaka S, J. Chem. Inf. Model, 2017, 57, 742–756. [DOI] [PubMed] [Google Scholar]
- 32.Kimura SR, Hu HP, Ruvinsky AM, Sherman W and Favia AD, J. Chem. Inf. Model, 2017, 57, 1388–1401. [DOI] [PubMed] [Google Scholar]
- 33.Schmidt D, Boehm M, McClendon CL, Torella R and Gohlke H, J. Chem. Theory Comput, 2019, 15, 3331–3343. [DOI] [PubMed] [Google Scholar]
- 34.Yang Y, Mahmoud AH and Lill MA, J. Chem. Inf. Model, 2018, 59, 38–42. [DOI] [PubMed] [Google Scholar]
- 35.Yanagisawa K, Moriwaki Y, Terada T and Shimizu K, J. Chem. Inf. Model, 2021, 61, 2744–2753. [DOI] [PubMed] [Google Scholar]
- 36.Tan YS and Verma CS, J. Chem. Theory Comput, 2020, 16, 6633–6644. [DOI] [PubMed] [Google Scholar]
- 37.Zariquiey FS, de Souza JV and Bronowska AK, Sci. Rep, 2019, 9, 1–14. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 38.Tan YS, Śledź P, Lang S, Stubbs CJ, Spring DR, Abell C and Best RB, Angew. Chem, 2012, 124, 10225–10228. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 39.Tan YS, Spring DR, Abell C and Verma C, J. Chem. Inf. Model, 2014, 54, 1821–1827. [DOI] [PubMed] [Google Scholar]
- 40.Tan YS, Spring DR, Abell C and Verma CS, J. Chem. Theory Comput, 2015, 11, 3199–3210. [DOI] [PubMed] [Google Scholar]
- 41.Bakan A, Nevins N, Lakdawala AS and Bahar I, J. Chem. Theory Comput, 2012, 8, 2435–2447. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 42.Takemura K, Sato C and Kitao A, J. Phys. Chem. B, 2018, 122, 7191–7200. [DOI] [PubMed] [Google Scholar]
- 43.Privat C, Granadino-Roldán JM, Bonet J, Tomas MS, Perez JJ and Rubio-Martinez J, Phys. Chem. Chem. Phys, 2021, 23, 3123–3134. [DOI] [PubMed] [Google Scholar]
- 44.Huang D and Caflisch A, ChemMedChem, 2011, 6, 1578–1580. [DOI] [PubMed] [Google Scholar]
- 45.Huang D, Rossini E, Steiner S and Caflisch A, ChemMedChem, 2014, 9, 573–579. [DOI] [PubMed] [Google Scholar]
- 46.Martinez-Rosell G, Lovera S, Sands ZA and De Fabritiis G, J. Chem. Inf. Model, 2020, 60, 2314–2324. [DOI] [PubMed] [Google Scholar]
- 47.Mahmoud AH, Yang Y and Lill MA, J. Chem. Theory Comput, 2019, 15, 3272–3287. [DOI] [PubMed] [Google Scholar]
- 48.Ghanakota P and Carlson HA, J. Med. Chem, 2016, 59, 10383–10399. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 49.Goodford PJ, J. Med. Chem, 1985, 28, 849–857. [DOI] [PubMed] [Google Scholar]
- 50.Miranker A and Karplus M, Proteins: Struct. Funct. Bioinf, 1991, 11, 29–34. [DOI] [PubMed] [Google Scholar]
- 51.Kozakov D, Grove LE, Hall DR, Bohnuud T, Mottarella SE, Luo L, Xia B, Beglov D and Vajda S, Nat. Protoc, 2015, 10, 733–755. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 52.Ngan CH, Bohnuud T, Mottarella SE, Beglov D, Villar EA, Hall DR, Kozakov D and Vajda S, Nucleic Acids Res, 2012, 40, W271–W275. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 53.Guvench O and MacKerell AD Jr, PLoS Comput. Biol, 2009, 5, e1000435. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 54.Raman EP, Yu W, Guvench O and MacKerell AD, J. Chem. Inf. Model, 2011, 51, 877–896. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 55.Raman EP, Yu W, Lakkaraju SK and MacKerell AD Jr., J. Chem. Inf. Model, 2013, 53, 3384–3398. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 56.Lakkaraju SK, Raman EP, Yu W and MacKerell AD Jr., J. Chem. Theory Comput, 2014, 10, 2281–2290. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 57.Lakkaraju SK, Yu W, Raman EP, Hershfeld AV, Fang L, Deshpande DA and MacKerell AD Jr., J. Chem. Inf. Model, 2015, 55, 700–708. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 58.Yu W, Lakkaraju SK, Raman EP and MacKerell AD Jr., J. Comput. Aided Mol. Des, 2014, 28, 491–507. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 59.Yu W, Lakkaraju SK, Raman EP, Fang L and MacKerell AD Jr., J. Chem. Inf. Model, 2015, 55, 407–420. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 60.Koes DR and Camacho CJ, J. Chem. Inf. Model, 2011, 51, 1307–1314. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 61.Ustach VD, Lakkaraju SK, Jo S, Yu W, Jiang W and MacKerell AD Jr., J. Chem. Inf. Model, 2019, 59, 3018–3035. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 62.Goel H, Hazel A, Ustach VD, Jo S, Yu W and Mackerell A, Chem. Sci, 2021, 12, 8844–8858. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 63.MacKerell AD Jr, Jo S, Lakkaraju SK, Lind C and Yu W, Biochim. Biophys. Acta, Gen. Subj, 2020, 1864, 129519. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 64.Yu W, Jo S, Lakkaraju SK, Weber DJ and MacKerell AD Jr, Proteins: Struct. Funct. Bioinf, 2019, 87, 289–301. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 65.Jo S, Xu A, Curtis JE, Somani S and MacKerell AD, Mol. Pharm, 2020, 17, 4323–4333. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 66.Somani S, Jo S, Thirumangalathu R, Rodrigues D, Tanenbaum LM, Amin K, MacKerell AD Jr and Thakkar SV, J. Pharm. Sci, 2021, 110, 1103–1110. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 67.Vanommeslaeghe K, Hatcher E, Acharya C, Kundu S, Zhong S, Shim J, Darian E, Guvench O, Lopes P, Vorobyov I and Mackerell AD Jr., J. Comput. Chem, 2010, 31, 671–690. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 68.Vanommeslaeghe K and MacKerell AD Jr., J. Chem. Inf. Model, 2012, 52, 3144–3154. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 69.Vanommeslaeghe K, Raman EP and MacKerell AD Jr., J. Chem. Inf. Model, 2012, 52, 3155–3168. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 70.Yu W, He X, Vanommeslaeghe K and MacKerell AD Jr, J. Comput. Chem, 2012, 33, 2451–2468. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 71.Van der Spoel D, Lindahl E, Hess B, Groenhof G, Mark AE and Berendsen HJC, J. Comput. Chem, 2005, 26, 1701–1718. [DOI] [PubMed] [Google Scholar]
- 72.Lind C, Pandey P, Pastor RW and MacKerell AD Jr, J. Chem. Theory Comput, 2021, 17, 3188–3202. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 73.DeLano WL, CCP4 Newsletter on protein crystallography, 2002, 40, 82–92. [Google Scholar]
- 74.Humphrey W, Dalke A and Schulten K, J. Mol. Graph, 1996, 14, 33–38. [DOI] [PubMed] [Google Scholar]
- 75.Williams-Noonan BJ, Yuriev E and Chalmers DK, J. Med. Chem, 2018, 61, 638–649. [DOI] [PubMed] [Google Scholar]
- 76.Cournia Z, Allen B and Sherman W, J. Chem. Inf. Model, 2017, 57, 2911–2937. [DOI] [PubMed] [Google Scholar]
- 77.Cournia Z, Allen BK, Beuming T, Pearlman DA, Radak BK and Sherman W, J. Chem. Inf. Model, 2020, 60, 4153–4169. [DOI] [PubMed] [Google Scholar]
- 78.Wang L, Wu Y, Deng Y, Kim B, Pierce L, Krilov G, Lupyan D, Robinson S, Dahlgren MK, Greenwood J, Romero DL, Masse C, Knight JL, Steinbrecher T, Beuming T, Damm W, Harder E, Sherman W, Brewer M, Wester R, Murcko M, Frye L, Farid R, Lin T, Mobley DL, Jorgensen WL, Berne BJ, Friesner RA and Abel R, J. Am. Chem. Soc, 2015, 137, 2695–2703. [DOI] [PubMed] [Google Scholar]
- 79.Wilson DP, Wan Z-K, Xu W-X, Kirincich SJ, Follows BC, Joseph-McCarthy D, Foreman K, Moretto A, Wu J and Zhu M, J. Med. Chem, 2007, 50, 4681–4698. [DOI] [PubMed] [Google Scholar]
- 80.Song LF, Lee T-S, Zhu C, York DM and Merz KM Jr, J. Chem. Inf. Model, 2019, 59, 3128–3135. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 81.Kuhn M, Firth-Clark S, Tosco P, Mey AS, Mackey MD and Michel J, J. Chem. Inf. Model, 2020, 60, 3120–3130. [DOI] [PubMed] [Google Scholar]
- 82.Gapsys V, Pérez-Benito L, Aldeghi M, Seeliger D, Van Vlijmen H, Tresadern G and de Groot BL, Chem. Sci, 2020, 11, 1140–1152. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 83.Yang S-Y, Drug Discov. Today, 2010, 15, 444–450. [DOI] [PubMed] [Google Scholar]
- 84.Leach AR, Gillet VJ, Lewis RA and Taylor R, J. Med. Chem, 2010, 53, 539–558. [DOI] [PubMed] [Google Scholar]
- 85.Huang N, Shoichet BK and Irwin JJ, J. Med. Chem, 2006, 49, 6789–6801. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 86.Weston S, Baracco L, Keller C, Matthews K, McGrath ME, Logue J, Liang J, Dyall J, Holbrook MR, Hensley LE, Jahrling PB, Yu W, MacKerell AD Jr and Frieman MB, Proc. Nat. Acad. Sci, 2020, 117, 30687–30698. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 87.Ewing TJ, Makino S, Skillman AG and Kuntz ID, J. Comput. Aided Mol. Des, 2001, 15, 411–428. [DOI] [PubMed] [Google Scholar]
- 88.Morris GM, Huey R, Lindstrom W, Sanner MF, Belew RK, Goodsell DS and Olson AJ, J. Comput. Chem, 2009, 30, 2785–2791. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 89.Trott O and Olson AJ, J. Comput. Chem, 2010, 31, 455–461. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 90.O’Reilly M, Cleasby A, Davies TG, Hall RJ, Ludlow RF, Murray CW, Tisi D and Jhoti H, Drug Discov. Today, 2019, 24, 1081–1086. [DOI] [PubMed] [Google Scholar]
- 91.Rathi PC, Ludlow RF, Hall RJ, Murray CW, Mortenson PN and Verdonk ML, J. Med. Chem, 2017, 60, 4036–4046. [DOI] [PubMed] [Google Scholar]
- 92.Lolli G and Caflisch A, ACS Chem. Biol, 2016, 11, 800–807. [DOI] [PubMed] [Google Scholar]
- 93.Zhu J and Caflisch A, J. Med. Chem, 2016, 59, 5555–5561. [DOI] [PubMed] [Google Scholar]
- 94.Jahnke W, Erlanson DA, Mannhold R, Kubinyi H and Folkers G, Fragment-based approaches in drug discovery, Wiley Online Library, 2006. [Google Scholar]
- 95.Erlanson DA, McDowell RS and O’Brien T, J. Med. Chem, 2004, 47, 3463–3482. [DOI] [PubMed] [Google Scholar]
- 96.Taylor RD, MacCoss M and Lawson AD, J. Med. Chem, 2014, 57, 5845–5859. [DOI] [PubMed] [Google Scholar]
- 97.Gomes AA, da Silva GF, Lakkaraju SK, Guimarães BG, MacKerell AD Jr and Magalhães M. d. L. B., J. Chem. Inf. Mod, 2021, 61, 1931–1941. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 98.Schmidtke P, Le Guilloux V, Maupetit J and Tufféry P, Nucleic Acids Res, 2010, 38, W582–W589. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 99.Huang S-Y, Drug Discov. Today, 2014, 19, 1081–1096. [DOI] [PubMed] [Google Scholar]
- 100.Katchalski-Katzir E, Shariv I, Eisenstein M, Friesem AA, Aflalo C and Vakser IA, Proc. Nat. Acad. Sci. U.S.A, 1992, 89, 2195–2199. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 101.Vreven T, Moal IH, Vangone A, Pierce BG, Kastritis PL, Torchala M, Chaleil R, Jiménez-García B, Bates PA and Fernandez-Recio J, J. Mol. Biol, 2015, 427, 3031–3041. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 102.Pierce BG, Hourai Y and Weng Z, PloS one, 2011, 6, e24657. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 103.Gray JJ, Moughon S, Wang C, Schueler-Furman O, Kuhlman B, Rohl CA and Baker D, J. Mol. Biol, 2003, 331, 281–299. [DOI] [PubMed] [Google Scholar]
- 104.Comeau SR, Gatchell DW, Vajda S and Camacho CJ, Nucleic Acids Res, 2004, 32, W96–W99. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 105.Ecker DM, Jones SD and Levine HL, MAbs, 2015, 7, 9–14. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 106.Kintzing JR, Interrante MVF and Cochran JR, Trends Pharmacol. Sci, 2016, 37, 993–1008. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 107.Mullard A, Nat. Rev. Drug Discov, 2017, 16, 73–76. [DOI] [PubMed] [Google Scholar]
- 108.Walsh G, Nat. Biotechnol, 2010, 28, 917–924. [DOI] [PubMed] [Google Scholar]
- 109.Mueller C, Altenburger U and Mohl S, J. Pharm. Pharmacol, 2018, 70, 666–674. [DOI] [PubMed] [Google Scholar]
- 110.Cauchy M, D’aoust S, Dawson B, Rode H and Hefford MA, Biologicals, 2002, 30, 175–185. [DOI] [PubMed] [Google Scholar]
- 111.Huus K, Havelund S, Olsen HB, van de Weert M and Frokjaer S, Biochem, 2005, 44, 11171–11177. [DOI] [PubMed] [Google Scholar]
- 112.Shire SJ, Curr. Opin. Biotechnol, 2009, 20, 708–714. [DOI] [PubMed] [Google Scholar]
- 113.Kamerzell TJ, Esfandiary R, Joshi SB, Middaugh CR and Volkin DB, Adv. Drug Delivery Rev, 2011, 63, 1118–1159. [DOI] [PubMed] [Google Scholar]
- 114.Roberts CJ, Trends Biotechnol, 2014, 32, 372–380. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 115.Roberts CJ, Das TK and Sahin E, Int. J. Pharm, 2011, 418, 318–333. [DOI] [PubMed] [Google Scholar]
- 116.Dong Q, Liang Y, Yan X, Markey SP, Mirokhin YA, Tchekhovskoi DV, Bukhari TH and Stein SE, MAbs, 2018, 10, 354–369. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 117.Schiel JE, Turner A, Mouchahoir T, Yandrofski K, Telikepalli S, King J, DeRose P, Ripple D and Phinney K, Anal. Bioanal. Chem, 2018, 410, 2127–2139. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 118.Teplyakov A, Obmolova G, Wu S-J, Luo J, Kang J, O’Neil K and Gilliland GL, J. Mol. Biol, 2009, 389, 115–123. [DOI] [PubMed] [Google Scholar]
- 119.Kalenkiewicz A, Grant BJ and Yang C-Y, Biology, 2015, 4, 344–366. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 120.Tan YS, Reeks J, Brown CJ, Thean D, Ferrer Gago FJ, Yuen TY, Goh ETL, Lee XEC, Jennings CE and Joseph TL, J. Phys. Chem. Lett, 2016, 7, 3452–3457. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 121.Lee JY, Krieger JM, Li H and Bahar I, Protein Sci, 2020, 29, 76–86. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 122.Goel H, Yu W, Ustach VD, Aytenfisu AH, Sun D and MacKerell AD, Phys. Chem. Chem. Phys, 2020, 22, 6848–6860. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 123.Woo H-J, Dinner AR and Roux B, J. Chem. Phys, 2004, 121, 6392–6400. [DOI] [PubMed] [Google Scholar]
- 124.Mousaei M, Kudaibergenova M, MacKerell AD Jr and Noskov S, J. Chem. Inf. Model, 2020, 60, 6489–6501. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 125.Ernst O, Khan MM, Oyler BL, Yoon SH, Sun J, Lin F-Y, Manes NP, MacKerell AD Jr, Fraser ID and Ernst RK, Msystems, 2021, 6, e00306–00321. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 126.Aytenfisu AH, Deredge D, Klontz EH, Du J, Sundberg E and MacKerell AD Jr, PLoS Comput. Biol, 2021, 17, e1009103. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 127.Zhang H, Jiang W, Chatterjee P and Luo Y, J. Chem. Inf. Model, 2019, 59, 2093–2102. [DOI] [PMC free article] [PubMed] [Google Scholar]
- 128.Li G, Zhang W, Xie Y, Li Y, Cao R, Zheng G, Huang N and Zhou Y, J. Chem. Inf. Model, 2020, 60, 3287–3294. [DOI] [PubMed] [Google Scholar]







