Int J Med Sci 2020; 17(13):2031-2039. doi:10.7150/ijms.46231 This issue
1. Institute for Computational Science and Technology, Ho Chi Minh City, Vietnam.
2. VNUHCM-University of Technology, Ho Chi Minh City, Vietnam.
The PB2 protein of the influenza virus RNA polymerase is a major virulence determinant of influenza viruses. It binds to the cap structure at the 5' end of host mRNA to generate short capped RNA fragments that are used as primers for viral transcription named cap-snatching. A large number of the compounds were shown to bind the minimal cap-binding domain of PB2 to inhibit the cap-snatching machinery. However, their binding in the context of an extended form of the PB2 protein has remained elusive. A previous study reported some promising compounds including azaindole and hydroxymethyl azaindole, which were analyzed here to predict binding affinity to PB2 protein using the steered molecular dynamics (SMD) and molecular mechanics Poisson-Boltzmann surface area (MM-PBSA) methods. The results show that the rupture force (Fmax) value of three complexes is in agreement with the binding free energy value (ΔGbind) estimated by the MM-PBSA method, whereas for the non-equilibrium pulling work (Wpull) value a small difference between A_PB2-4 and A_PB2-12 was observed. The binding affinity results indicate the A_PB2-12 complex is more favorable than the A_PB2-4 and A_PB2-16 complexes, which means the inhibitor (12) has the potential to be further developed as anti-influenza agents in the treatment of influenza A.
Keywords: Azaindole (4 and 16), hydroxymethyl azaindole (12), protein_PB2, SMD, MM-PBSA
Both seasonal and pandemic influenza have been causing severe illness and death for both humans and farm animals . The virus variants have emerged and posed a constant threat to human health. Changes in viral genes often result in viral evolutionary advantages, such as the degree of virulence and the more efficient replication and transmissibility of the virus .
There has been four main influenza A pandemics, including the H1N1 Spanish flu (1918), the H2N2 Asian flu (1957), the H3N2 Hong Kong flu (1968), and the H1N1 swine flu (2009) [3,4]. These have been examples of fast transmission of animal influenza viruses to humans . Although vaccination could prevent influenza for 70-90% of healthy adults [6,7], it is only effective against a limited range of strains and it practically has no effect against new and potentially pandemic strains [8-10]. Therefore, the development of effective drugs against influenza is currently considered as a high priority by different governmental and international agencies, especially by pharmaceutical industries at the worldwide scale.
The influenza virus is an enveloped virus, in which the outer layer is a lipid membrane, which is taken from the host cell where the virus multiplies [11,12]. A glycoprotein is a type of protein molecule linked to sugar. When it is located in a cell membrane, it helps to identify and communicate with the cell. The cell uses the glycoproteins embedded in the plasma membrane to get the oligosaccharides on the outside of the cell, which is typically decorated with different oligosaccharides such as hemagglutinin (HA) [13,14] and neuraminidase (NA) . The NA protein is actually the target of the antiviral drugs Relenza and Tamiflu [16,17]. Additionally, the M2 protein is also a membrane protein and is a target of the antiviral Adamantanes (including Amantadine and Rimantadine) [18,19]. However, the long-term effectiveness of these drugs is a matter of great concern due to the emergence of drug-resistant strains of the virus. Thus, there is an urgent need for new agents to prevent and treat the influenza virus infection, especially in high-risk groups and during pandemic influenza.
Some previous studies showed that some small molecule inhibitors were able to make novel targets in the influenza life cycle against [20-30]. The genome of the influenza virus includes eight different ribonucleoprotein complexes that enclose eight viral genomic RNA segments. Similarly to other negative-stranded RNA viruses, the viral RNA polymerase of influenza virus is always packaged in the infectious virion as a complex with the nucleoprotein [31-34]. The RNA-dependent RNA polymerase of influenza virus is composed of the PA, PB1, and PB2 subunits. A heterotrimeric polymerase is required for RNA transcription and replication that take place in the nucleus during influenza virus infection .
The influenza virus is based on a cap-snatching mechanism to accomplish its transcription . Following the entrance of the ribonucleoprotein complexes into the nucleus, the 5' cap of the host pre-mRNA in the nucleus is captured by the cap-binding domain of PB2 . Together with 10-13 nucleotides downstream, the 5' cap is subsequently cleaved off by the N-terminal cap-dependent endonuclease of PA . This 5'-capped oligonucleotide is used as the primer for initiation of the viral transcription by PB1 . This process is called as a “cap-snatching” mechanism, which allows the endonuclease to cleave the 5' caps from host RNAs, and then the latter act as transcription primers . Clearly, the PB2 subunit is linked to the initiation of viral transcription and is known as a cap-binding protein [40-42]. According to recent studies, a cap-primer-dependent in vitro RNA synthesis is affected by the PB2 gene and, therefore, a series of in vitro inhibitors has supported such role for PB2 . monoclonal antibodies specific for the PB2 subunit have interfered with the initiation step of mRNA-primed transcription in vitro , and antibodies monospecific for the C terminus of PB2 have inhibited cap snatching and cap-dependent transcription in vitro but not cap-binding . Moreover, antibodies directed to the region from positions 300 to 550 in PB2 inhibited cap snatching and partially affected cap recognition [46,47]. However, the activities of both transcription and cap-dependent endonuclease have required the presence of all three subunits of the polymerase and the RNA template [48, 49].
To elucidate some crucial molecular determinants for the interaction of some inhibitors with PB2 protein of influenza A (protein_PB2), the binding affinity of the azaindole (4&16) and hydroxymethyl azaindole (12) for PB2 protein was predicted. For this purpose, the different theoretical methods including steered molecular dynamics (SMD) [50-52] and Molecular Mechanics Poisson-Boltzmann Surface Area (MM-PBSA) [53,54] were used to compute the binding affinities of these inhibitors for protein_PB2.
The 3D structures of the complexes were taken from Protein Data Bank with PDB ID: 5JUN (A_PB2-4) , 5BUH (A_PB2-12) and 5F79 (A_PB2-16) . The 2D structures of the inhibitors (4), (12) and (16) are shown in Figure 1. The inhibitor topologies and coordinate files were generated by using Swiss Param .
The simulation processes of complexes were conducted by using CHARMM 27 force field  implemented in the GROMACS 5.1.2 package  at absolute temperature 300 K. The TIP3P water model  was used in all simulation systems. All distance bonds within the proteins were constrained by the Linear Constraint Solver (LINCS) algorithm . The electrostatic and van der Waals interactions were used to depict non-bonded interactions, with the non-bonded interaction pair-list being updated every 10 fs using a cutoff of 1.4 nm. The Particle Mesh Ewald truncation method  was used to treat the long-range electrostatic interactions. From these structures, short 2 ns MD simulations were performed in the NVT ensemble, which were followed by 3 ns NPT simulation. The leap-frog algorithm  was used to integrate the equations of motion with the time step set to 2 fs for the MD simulations.
Caver 3.0  package was used to determine the pulling pathway through the widest tunnel as this minimizes the occurrence of collisions between the inhibitor and protein_PB2 during the simulation. Then the Caver 3.0 and PyMOL  packages were employed to rotate the protein_PB2 in such a way that the inhibitor unbinding pathway is along the z-axis (Figure 1).
In the Steered Molecular Dynamics (SMD) simulation [50-52], each of the inhibitor-protein_PB2 complexes was placed in a triclinic box of 6nm × 6nm × 14 nm to have enough space to pull the inhibitor out of the binding site. The three-dimensional coordinates of the center of the complex were 3nm × 3nm × 3 nm. The complexes were immersed in a salt solution with a concentration of 0.15 M of sodium and chloride to neutralize the total charge.
The pulling force is measured according to the following equation:
where is the force constant, is the pulling velocity, is the pulling direction normal, and are the positions of protein at time and initial time, respectively. During the simulations, the spring constant value was set to 600 kJ/ (mol.nm2) (approximately 1020 pN/nm), which is a typical value used in atomic force microscope (AFM) experiments . The complete dissociation of the inhibitor from the binding pocket of protein_PB2 was reached during 500 ps for three complexes with pulling velocity set at = 0.005 nm/ps.
In order to calculate the relative binding affinities of the complexes using the SMD simulation, the non-equilibrium pulling work profile was used to evaluate a scoring function to rank the binding affinities between the inhibitor and protein. The non-equilibrium pulling work is approximately defined as follows:
where is the non-equilibrium pulling work of external force , and is the number of steps in the SMD simulation, is the inhibitor displacement in step i, here the centers of mass (COM) of the inhibitors were employed to measure the inhibitor displacement.
To estimate binding free energy between the inhibitors and protein_PB2, each snapshot extracted from the equilibrium MD simulation was used to estimate the binding free energy using the MM-PBSA method. The binding free energy of the inhibitor-protein is computed by this approach as follows [53,54]:
where and are contributions of electrostatic and vdW energies, respectively . and are non-polar and polar solvation energies . Here, derived from the electrostatic potential between solute and solvent was determined using the continuum solvent approximation . It is the change of electrostatic energy from transferring solute in a continuum medium, from a low solute dielectric constant (ε = 2) to a higher one with water without salt (ε = 78.45). Using a grid spacing of 0.1 Å, the APBS package  was implemented for numerical solution of the corresponding linear Poisson-Boltzmann equation. The nonpolar solvation term was approximated as linearly dependent on the solvent accessible surface area (SASA), derived from Shrake-Rupley numerical method  integrated in the APBS package. = γSASA + β, where γ = 0.0072 kcal/mol.Å2 and β = 0 . The entropic contribution is determined using the normal mode approximation .
The contact networks between the inhibitors and protein_PB2 were determined by using the LigPlot and PyMOL packages [65,74]. The root mean square deviation (RMSD), the number of hydrogen bond (H-bond) and the number of contacts (NC) were calculated by the “gmx_mpi hbond” and “gmx_mpi mindist” tools in the GROMACS package. The standard errors of the mean (E) are approximately estimated as follows:
Where N is the number of snapshots, xi is a quantity at each snapshot, and is the average value of xi.
In order to indicate the stability of the systems including A_PB2-4, A_PB2-12, and A_PB2-16, the RMSD time profiles calculated for protein_PB2's backbone and the inhibitor's heavy atoms are shown in Figure 2A & B for every analyzed system. The RMSD values reveal that the three systems reached equilibrium after 250 ns when the RMSD values start fluctuating around about 0.3 nm and 0.45 nm for the backbone of protein_PB2 and around 0.1 nm for the inhibitor's heavy atoms in all cases. The snapshots collected from the last 100 ns of MD simulations were used to calculate the binding free energy through the MM-PBSA method.
a) z-direction of the inhibitor (16) exiting the binding pocket of protein_PB2, and b) 2D structures of the inhibitors (4), (12), and (16).
RMSD time profiles for a) the backbone of protein_PB2 in the three complexes and b) the heavy atoms of three inhibitors. c) the contact network between three inhibitors and protein_PB2. Residues shown in yellow form H-bonds (cyan lines) with the ligands.
The number of H-bonds (a) and the number of NC (b) formed between protein_PB2 and the inhibitors are presented as a function of SMD simulation time.
The contact network has an important role in stabilizing energetically favored inhibitors. Figure 2C displays the contact network between three inhibitors and protein_PB2. By analyzing the interfaces we found the following interactions:
The H-bond between the inhibitors and protein_PB2 has an important role in the binding affinity of the complexes. Therefore, the average H-bond occupancies (during the last 100 ns of the MD simulations) were also calculated to determine the contribution of each residue at the interfaces in each complex. The results indicate that the Phe323, Phe325, His357, Glu361, Phe363, Lys376, and Phe404 residues are involved in the formation of a H-bond network in the three complexes (Table 1). Most of the residues forming the contact network with three inhibitors are the Phe aromatic residues. That means the Phe residues can have a key role in interactions with the inhibitors and lead to the change of the binding affinity of the inhibitors for protein_PB2.
Average occupancies of H-bonds between the inhibitors and protein_PB2 in the three A_PB2-4, A_PB2-12, and A_PB2-16 complexes, determined from the last 100 ns of the MD simulations
|Residue||Inhibitor (4)||Inhibitor (12)||Inhibitor (16)|
|Phe323 (O)||0.1873 (N4)||0.0055 (N1)||0.0044 (F2)|
|Phe325 (O)||0.0431 (N4)||0.1101 (F2)||0.0112 (N5)|
|Arg332 (N)||0.4688 (N2, F1, O)|
|Ser337 (O)||0.0019 (N)|
|His357 (N)||0.6012 (O1, O2)||0.2155 (N2, O, F1, F2)||0.0377 (O1, F2)|
|Glu361 (O)||0.5202 (N5)||0.8033 (N1, O)||0.5010 (N1)|
|Phe363(O)||0.0323(N4)||0.0795 (N1)||0.2188 (N1)|
|Lys376 (N)||0.4432 (N4)||0.1113 (N, O)||0.6212 (N)|
|Phe404 (O)||0.2261 (F1)||0.2278 (O)||0.0220 (N)|
|Gln406 (N)||0.0110 (N5)||0.0060 (N, N2, F1, F2)|
|Asn429 (N)||0.2032 (N6, O1, F1)||0.5721 (F1, N5)|
|Met431 (O)||0.0032 (N4)|
|His432 (N)||0.0731 (O1)|
Additionally, in order to describe the unbinding process of the inhibitor-protein_PB2 complexes, the H-bond (r < 0.35nm) and the NC (r < 0.6nm) are determined as a function of simulation time (Figure 3A & B). At the bound state, there are three H-bonds formed between inhibitors (4) and (16) and protein_PB2, while there are only 2 H-bonds between inhibitor (12) and protein_PB2. At the unbound state, the number of H-bonds decreases to 0 for all three complexes. Likewise, the NC value also helps follow the unbinding process of the inhibitor-protein_PB2 complexes. There are roughly 1125 NCs formed between the three inhibitors and protein_PB2 at the bound state, which decrease to 0 NCs after 400 ps for inhibitor (4), after 425 ps for inhibitor (16) and after 450 ps for inhibitor (12) at the unbound state. Although the NC and the number of H-bonds of the A_PB2-16 complex are greater than those of the A_PB2-4 and A_PB2-12 complexes, the NC and the number of H-bonds of the A_PB2-16 complex reach 0 faster than those of the A_PB2-4 and A_PB2-12 complexes.
Binding affinity is widely used to evaluate and rank order strength of biomolecular interactions in biological systems. In this research, to make a full understanding of the binding mechanism of these inhibitors to protein_PB2, we estimated the binding affinity of the azaindole (4&16) and hydroxymethyl azaindole (12) to protein_PB2.
The SMD is used as a method to study the unbinding process of small molecules (the inhibitors) from a large molecule (protein_PB2) and is capable of rank the compounds binding a same target protein according to their relative binding affinities . The pulling force profile is started as a function of time (shown in Figure 4A). The Fmax has an important role to indicate the dissociation between protein_PB2 and the inhibitors. Here the pulling force profile is able to show the division of two consecutive stages: During the first stage, the pulling force continuously increased until the inhibitors started to dissociate from protein_PB2, and the external force reached the Fmax value when the H-bonds are broken. During the second stage, the pulling force started to decrease as the inhibitors are exiting the binding pocket of protein_PB2. In more detail, the largest pulling force of the A_PB2-12 complex (Fmax = 477.50 pN, t=220 ps) is larger than those of the A_PB2-4 complex (Fmax = 462.42 pN, t=170 ps) and the A_PB2-16 complex (Fmax = 315.86 pN, t=125 ps), respectively. Overall, the variation of pulling force profiles among the inhibitor-protein_PB2 complexes could be attributed to the binding site of protein_PB2. Moreover, the evolution of the steering force during the inhibitor displacement first showed a linear behavior which then became nonlinear before the Fmax value was reached (seen from Figure 4B). At this point, the inhibitor is still located in the binding pocket. After obtaining the Fmax value, the force value decreased steeply and fluctuated around zero value (beginning at 2.25 nm), when the inhibitor detached from the protein_PB2 along the pulling direction.
(a) Force vs time and (b) force vs displacement profiles. (c) Pulling work-time profile.
Binding affinity values of three inhibitors for protein_PB2, estimated from the MM-PBSA method and SMD simulations
|ΔEelec (kcal/mol)||ΔEvdW (kcal/mol)||ΔGsur (kcal/mol)||ΔGPB (kcal/mol)||-TΔS (kcal/mol)||ΔGbind (kcal/mol)||Fmax (pN)||Wpull (kcal/mol)|
The non-equilibrium pulling work (Wpull) is also used to predict the relative binding affinity of protein_PB2-inhibitor systems (eq. 2). As seen from Figure 4C, the Wpull rapidly increased as the pulling force does, until the inhibitors come out from the binding pocket of protein_PB2. It reached a stable value when the inhibitors lost their non-bonded contacts with protein_PB2 (corresponding to 50 kcal/mol for (16), 60 kcal/mol for (12) and 65 kcal/mol for (4)). However, note that small fluctuations occur, which can be neglected. All three systems reach a stable state after 250 ps.
In this work, the MM-PBSA method is also used to estimate the binding free energies and makes possible to indicate the contribution of each energy component to the inhibitor's potency. As seen in Table 2, the contribution of different energy components to the ΔGbind indicates that the electrostatic energy (ΔEelec) has a more important role than the vdW energy (ΔEvdW). The changes in the nonpolar solvation energy (ΔGsur) values significantly contributed to the difference of the ΔGbind among the complexes. The entropy (-TΔS) of the A_PB2-12 complex is larger than those of the A_PB2-4 and A_PB2-16 complexes. The loss of polar solvation energy (ΔGPB) is compensated by the remaining components of the ΔGbind in these systems.
Specifically, the ΔEelec obtained from the complex formation compensates the loss in ΔGPB. Here, the ΔEelec of the A_PB2-12 complex (-16.43 kcal/mol) is more negative than those of both remaining complexes (-7.63 kcal/mol for the A_PB2-4 complex, and -7.71 kcal/mol for the A_PB2-16 complex). The ΔGvdW values of the three complexes (ranged from -1.86 to -3.60 kcal/mol) do not lead to the difference of their ΔGbind values. Conversely, the ΔGsur values of these complexes significantly contribute to the difference of their ΔGbind values (ranged from -6.95 to -4.41 kcal/mol). The entropy contribution (-TΔS) of the A_PB2-12 complex (7.36 kcal/mol) is greater than those of the A_PB2-4 and A_PB2-16 complexes (0.52 kcal/mol for the A_PB2-4 complex, and 0.49 kcal/mol for the A_PB2-16 complex). Clearly, the OH group of inhibitor (12) is not only yielded to a more negative value of electrostatic energy but also contributed to making a fairly large entropic energy. Here, the -TΔS value of the A_PB2-12 complex contributed appreciably to the change of the binding free energy while this energy component has a negligible impact on the binding free energy to two remaining complexes. Finally, the ΔGbind of the A_PB2-12 complex (-12.70 kcal/mol) is lower than that of both remaining complexes (-10.04 kcal/mol for the A_PB2-4 complex, and -6.44 kcal/mol for the A_PB2-16 complex). The results indicate that the affinity of inhibitor (12) bound for protein_PB2 is stronger than that of inhibitors (4) and (16). Moreover, our calculations reveal that the Fmax of three complexes is in good agreement with the ΔGbind value, while the Wpull value has a small difference between A_PB2-4 and A_PB2-12. In short, the inhibitor (12) has the potential to be further developed as anti-influenza agents in the treatment of influenza A.
In the present theoretical study, we applied the SMD and MM-PBSA methods to predict the binding affinity of three inhibitors for protein_PB2. A number of interesting results emerged from our work, which can be summarized as follows:
Supplementary parameterization scheme.
We sincerely thank Prof. Mai Suan Li from the Institute of Physics, Polish Academy of Science, Poland; for supporting and valuable comments. This research was funded by the Department of Science and Technology - Ho Chi Minh City (HCMC - DOST), and the Institute for Computational Science and Technology (ICST) at Ho Chi Minh City, Vietnam under Contract No.14/2018/HĐ-KHCNTT. The computing resources were provided by the Institute for Computational Science and Technology at Ho Chi Minh City, Vietnam.
HN conceived the experiment. TP and HN conducted the experiment. TP, HLN, TP-T and HN analyzed the results. HN wrote the paper. All authors reviewed the manuscript.
The authors have declared that no competing interest exists.
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Corresponding author: E-mail: hung.nvorg.vn (H.N).