Juliana
Murillo-López‡
a,
Kirill
Zinovjev‡
b,
Humberto
Pereira
c,
Andres
Caniuguir
d,
Richard
Garratt
c,
Jorge
Babul
d,
Rodrigo
Recabarren
a,
Jans
Alzate-Morales
a,
Julio
Caballero
*a,
Iñaki
Tuñón
*b and
Ricardo
Cabrera
*d
aCentro de Bioinformática y Simulación Molecular (CBSM), Facultad de Ingeniería, Universidad de Talca, 1 Poniente 1141, Talca, Chile. E-mail: jcaballero@utalca.cl
bDepartament de Química Física, Universitat de València, 46100 Burjassot, Spain. E-mail: ignacio.tunon@uv.es
cInstituto de Física de São Carlos, Universidade de São Paulo, São Paulo, Brazil
dDepartamento de Biología, Facultad de Ciencias, Universidad de Chile, Santiago, Chile. E-mail: ricabrer@uchile.cl
First published on 28th January 2019
Phosphofructokinases (Pfks) catalyze the ATP-dependent phosphorylation of fructose-6-phosphate (F6P) and they are regulated in a wide variety of organisms. Although numerous aspects of the kinetics and regulation have been characterized for Pfks, the knowledge about the mechanism of the phosphoryl transfer reaction and the transition state lags behind. In this work, we describe the X-ray crystal structure of the homodimeric Pfk-2 from E. coli, which contains products in one site and reactants in the other, as well as an additional ATP molecule in the inhibitory allosteric site adjacent to the reactants. This complex was previously predicted when studying the kinetic mechanism of ATP inhibition. After removing the allosteric ATP, molecular dynamic (MD) simulations revealed conformational changes related to domain packing, as well as stable interactions of Lys27 and Asp256 with donor (ATP) and acceptor (fructose-6-) groups, and of Asp166 with Mg2+. The phosphoryl transfer reaction mechanism catalyzed by Pfk-2 was investigated through Quantum Mechanics/Molecular Mechanics (QM/MM) simulations using a combination of the string method and a path-collective variable for the exploration of its free energy surface. The calculated activation free energies showed that a dissociative mechanism, occurring with a metaphosphate intermediate formation followed by a proton transfer to Asp256, is more favorable than an associative one. The structural analysis reveals the role of Asp256 acting as a catalytic base and Lys27 stabilizing the transition state of the dissociative mechanism.
X-ray structures of Pfk-2 with the F6P substrate (PDB ID: 3N1C) and with two MgATP2− (PDB ID: 3CQD) have been previously reported. There are few kinase structures in the Protein Data Bank (PDB) that are bound to both reactants and products, namely the xylulose kinase from Lactobacillus acidophilus (PDB ID: 3LL3), phosphoglycerate kinase from Homo sapiens (PDB ID: 2X15) and adenylate kinase from Plasmodium falciparum (PDB ID: 3TLX), which has not been associated to any publication, and, noteworthy, the Pfk-1 from E. coli with its reaction products.18 In this work, for the first time, we report the structure of a member of the ribokinase family (Pfk-2) solved with both reactants and products in the same crystal (PDB ID: 3UQD). Thus, this crystallographic structure could serve as a model to study the chemical reaction catalyzed by the enzyme, as it provides information not only about the position of each ligand at the beginning and the end of the phosphorylation reaction but also about the residues performing key interactions that could be relevant for the catalytic activity of the enzyme.
The ribokinase superfamily has been studied in terms of evolution, showing that the overall fold and reaction machinery are strongly conserved over a wide range of species and substrate specificities.19 In this family, the general chemical reaction consists of the ATP-dependent phosphorylation of a hydroxymethyl group in the substrates.13 Although the sequence similarities of these proteins are in the range of 18–22%,20 the alignment of different protein–ligand complexes reveals conserved regions that are important for catalysis and protein stabilization.14,21–24 These conserved regions have been targets of multiple studies, with Pfk-2 being the most studied phosphosugar kinase member at the biochemical and structural level.12,14,24–34 Noteworthy, the GXGD14,35 motif contains a highly conserved aspartate residue, for which the D256N mutation in Pfk-2 produced a striking 15000-fold decrease in the catalytic constant with no variation in the KM values for F6P or MgATP2−. This result indicates that Asp256 participates specifically in catalysis but not in substrate binding in Pfk-2.14 This residue has also been proposed to have a catalytic role in D-tagatose-6-P kinase (LacC), which is closely related to Pfk-2. In 2007, Miallau36et al. proposed a mechanism for LacC in which the side chain of the GXGD aspartate residue (Asp254) removes a proton from the substrate C1 hydroxyl group to activate the oxygen atom as a nucleophile, which then attacks the γ-phosphate of ATP to yield the phosphorylated product. Another residue involved in catalysis is present in the conserved “motif-I” located at the N-terminal region that ends with a lysine residue, as in 1-phosphofructokinase from E. coli (Lys41), LacC from S. aureus (Lys38) and ribokinase from Lactococcus lactis (Lys40).14,36 Thus, they also proposed that the nearby conserved lysine residue (Lys38) likely stabilizes the negative charge of the transition state.36 Following this reasoning, we present a mechanistic model for Pfk-2 in which the equivalent GXGD aspartate residue (Asp256) abstracts the proton from the substrate (see Fig. S1 in the ESI,† upper mechanism).
In general, two kinds of limiting mechanisms have been proposed for phosphoryl transfer reactions,4,37 which can be considered as the extremes across a spectrum of possible concerted (ANDN) mechanisms. On the one hand, in the associative or addition–elimination (AN + DN) mechanism, a nucleophilic attack occurs prior to the departure of the leaving group, and the reaction proceeds via a pentavalent phosphorane intermediate. If Pfk-2 performed this mechanism, the proton of the sugar phosphate substrate would be transferred to one of the non-bridging oxygen atoms of the phosphate group (see Fig. S1 in the ESI,† lower mechanism), decreasing its charge and favoring the approach to the nucleophile. On the other hand, in the dissociative or elimination–addition (DN + AN) mechanism, the reaction proceeds via an expansive transition state (TS) with metaphosphate character, where bond cleavage of the leaving group occurs prior to bond formation with the nucleophile. If the phosphoryl transfer of Pfk-2 followed this mechanism, the carboxylate group in a side chain would act as the base responsible for substrate deprotonation. In this case, the formal negative charges born by both the phosphate group and the nucleophile would then favor a dissociative mechanism. This same carboxylate group would then act as an acid to protonate the transferred phosphoryl group and thus regenerate the enzyme to its original state. This last step has been studied at the quantum mechanics/molecular mechanics (QM/MM) level in protein kinases, demonstrating its feasibility.38
In this work, we describe the crystallographic structure of Pfk-2 with products in one active site and reactants in the other, plus an additional MgATP2− positioned in the allosteric site adjacent to reactants. With this structure we performed an in-depth theoretical study of the phosphorylation reaction mechanism, using highly parallelized computational techniques. The comparison of the interactions observed in the crystal, and during MD simulations of the active sites containing reactants and products, allows the identification of a conformational change in the chain bearing the products that is essential for the reaction to take place. Furthermore, Lys27 adopts a better conformation for the reaction and Asp166 joins the coordination sphere of Mg2+, replacing a water molecule. QM/MM calculations were performed considering the effect of the protein environment and its flexibility.39 We determined that Pfk-2 follows a dissociative phosphorylation mechanism during catalysis, and we also clarified the role of some conserved residues within the ribokinase family, particularly those participating in enzyme catalysis.
All information related with the selected QM subsystem and computational methods used are described in the ESI.† Briefly, the AM1d-PhoT Hamiltonian43,44 was selected for the QM subsystem. The atoms included in the selected QM subsystem are represented in Fig. 1. QM/MM MD simulations were carried out in order to obtain the Minimum Free Energy Paths (MFEPs) by means of the on-the-fly string method.39,45,46 These MFEPs were obtained in the space of Collective Variables (CVs) that define the most important changes taking place during the chemical reaction (see Fig. 1). Once the converged MFEPs were determined, the corresponding potentials of mean force (PMFs) were obtained using the umbrella sampling method47 along the path CVs39,45 that define the progress of the system along these paths. This methodological combination has proven to be an efficient approach for studying the free energy landscapes of complex enzymatic reactions.39,48,49 Details related with the simulations performed are widely described on the ESI.†
As previously described for Pfk-2 and other ribokinase family members,21,29,36 the overall fold of the monomer consists of two domains, which perform different roles in substrate binding and oligomerization. The major domain is formed by a central β-sheet surrounded by α-helices, where a long furrow along the C-terminal edge of the sheet provides residues for the active site that contact F6P, ATP4− and Mg2+. The minor domain consists of a four-stranded β-sheet that acts as a lid over the active site and provides residues mainly involved in contacting F6P. This domain forms the monomer–monomer interface by orthogonal β-sheet packing, and shares part of the β3 strand with the complementary sheet in an arrangement called a β-clasp. The first half of β3 provides residues to the active and allosteric sites in the adjacent subunit of the dimer.31 It has been observed that the major and minor domains change their relative orientation upon substrate binding.26 For instance, whereas the chains in the crystal structure of the Pfk-2:F6P complex present variable relative orientations, in the Pfk-2:(MgATP)2 complex they adopt a fixed position. This induced fit upon sugar binding was also observed in the present structure, in which different relative orientations between domains are observed among the four monomers in the asymmetric unit.
In the active site bearing reactants the F6P molecule is oriented by electrostatic interactions between the 6-phosphate group and the positive charges of Arg90 and Arg29 (from the complementary chain) in a similar fashion as observed in the Pfk-2:F6P complex (PDB ID: 3N1C, chain D). In addition, hydroxyl groups OH3 and OH4 of the sugar phosphate sustained a bidentate coordination with the carboxylate group of Asp14 (as observed in Fig. 2a) that, although conserved in the Pfk-2:F6P complex, is somewhat pushed apart, decreasing the observed restraint on the torsion angle along the C3–C4 bond.31 As a consequence of the change in the sugar ring conformation, the Hydrogen Bond (HB) network around groups OH1, OH2 and OH3 is rearranged. Moreover, the oxygen atom of the hydroxyl group OH2 comes closer to the carboxylate oxygens of Asp256 (dO2(F6P):Oδ(Asp256) = 3.68 Å) than the oxygen atom of the group to be phosphorylated, OH1 (dO1(F6P):Oδ(Asp256) = 3.89 Å). Additionally, more solvent molecules can be found around the sugar phosphate, indicating more solvent accessibility than in the Pfk-2:F6P complex, consistent with a more open enzyme conformation. Moreover, Lys27 from the complementary chain is slightly displaced away from the 6-phosphate group and the fructose OH1. Regarding the substrate and inhibitor nucleotides, they are bound in a similar fashion as seen in the Pfk-2:(MgATP)2 complex.29 The β-phosphoryl group interacts with Asn187, whereas one Mg2+ ion is coordinated by oxygen atoms belonging to the β- and γ-phosphates (as seen in Fig. 2a) and through water molecules to Lys185, Glu190 and Asp166, similar to the Pfk-2:(MgATP)2 complex.29 The second Mg2+ ion belongs to the inhibitor MgATP2− and is coordinated with β- and γ-phosphoryl groups of ATPS and ATPA (as seen in Fig. 2a). Although the inhibitor MgATP2− forms π–π stacking with Tyr23, this nucleotide is displaced compared to the Pfk-2:(MgATP)2 complex29 because of the minor domain movement. Another important difference is that Lys27 is not able to interact with the γ-phosphate of the nucleotide, due to the interactions established with the 6-phosphate group of the sugar. These observations indicate a mutual negative effect of the binding of F6P and the allosteric MgATP2−.
In the active site containing the products (FBP and ADP, see Fig. 2b) only one Mg2+ ion has been found, and it forms the MgADP− product. The loop β13–α8 that surrounds the adenine moiety is slightly displaced towards the minor domain, according to the compaction of the whole subunit. Interactions with the 6-phosphate group are close to those described for the active site with reactants. However, HB interactions between the carboxylate oxygens of Asp14 and OH3 or OH4 hydroxyl groups of the sugar are strengthened, although without the constrained torsion observed in the Pfk-2:F6P complex.31 OH1 is closer to the Asp256 carboxylate group than OH2, similar to the disposition found in the Pfk-2:F6P complex. The guanidinium group of Arg105 is bound to the 1-phosphate group. The side chain nitrogen from Lys27 is tightly coordinated to phosphoryl groups 1 and 6.
Multiple sequence alignments of ribokinase family members show that a conserved lysine residue, associated with a catalytic role,21,36 is located at the N-terminus of the α1-helix29 belonging to the so-called “motif I,” with a conserved sequence XGKG. It has been stated that the combination of main-chain amide nitrogens and the conserved positively charged side-chains create an anion hole that helps to stabilize the transition state.21 For Pfk-2, this residue has been replaced by a glycine in the primary structure, mainly to make room for the OH2 group of the substrate.31 However, Lys27 of the complementary chain has its –NH3+ group at the same spatial location as the abovementioned conserved lysine side-chain.31 It is known that dimer formation is essential for catalysis in this family. In the case of Pfk-2, this seems to be due to the requirement of Lys27 from the complementary subunit to be present in the active site. The spatial location of this residue creates a charge-relay network that ultimately conducts the phosphorylation reaction. Some relevant distances and energy values are collected on the ESI (Tables S3 and S4†).
Interactions in the active sites of each complex seem to depend on the relative orientations of the domains, which in turn could be affected by the presence of the inhibitor MgATP2−, because it bridges the minor and major domains, stabilizing the overall conformation as we previously stated in Section 3.1. Thus, in order to assess changes in the level of compaction between both chains along the trajectory, we calculated the distance between the center of mass (COM) of the two domains (Fig. S3, see ESI†) using the VMD plug-in DisRg developed by Falsafi-Zadeh et al.50 These results showed that a closed conformation is favored in the product-containing chain.
After crystal packing relaxation, it is worthy to evaluate any change in the most relevant interactions within the active site. In this way, F6P conserved a very stable network of interactions with Arg90 and Asp14 residues that explains the recognition and affinity of this substrate in the active site (see Fig. S4 and S5, ESI†). Moreover, the interaction made with the conserved Asp256 residue (that belongs to the GXGD motif13,14) keeps stable during the entire MD simulation, although during the system construction, the PROPKA51 program determined that residue Asp256 in chain B should be protonated according to its chemical environment (Fig S5, ESI†). Additionally, the triphosphate moiety of MgATP2− performed stable interactions with Lys27, Lys185, Asn187 and Ser224 residues (Fig. S6 and S7, ESI†). Furthermore, the coordination sphere of Mg2+ keeps stable during the simulation; with the only change that Asp166 enters this coordination sphere replacing one water molecule with respect to the crystal structure. Finally, the distance between ligands in each chain was measured, revealing that in the reactants-containing chain, the distance between ligands constantly fluctuated approximately 5.2 Å, but in the case of the chain containing products, this distance was more stable and remained constant at an average value of 4.3 Å in the last 40 ns. Further details related with all these interactions are given in the ESI.†
To analyze the phosphoryl transfer pathway, we could have used either the active site with reactants, removing the inhibitor MgATP2−, or the active site with products. Considering that the monomer containing the reactants was initially prepared from an inhibited structure, some features seem to indicate that it could be further away from the catalytic conformation. The proximity between the phosphorous atom of the transferred phosphate group and the oxygen atom of the leaving ADP indicates a shorter path for phosphoryl transfer in the active site with products. The closed conformation observed in Pfk-2:F6P31 and Pfk-2:FBP:ADP complexes also argues in favor of this as the catalytic, and thus the best, conformation for QM/MM simulations of the reaction mechanisms.
In order to rationalize the different ordering between proton and phosphate transfers in the two converged mechanisms, we looked at the environment in which the process was taking place. Specifically, we analyzed the distance from Lys27 to the γ-phosphate group along the reaction pathway. In Fig. S10 in the ESI,† the evolution along the MFEPs of the distance between the nitrogen atom of the ε-amino group of Lys27 (NZ(Lys27)) and the phosphorous atom of the γ-phosphate of MgATP2− (Pγ(ATP)) for both converged pathways are depicted, together with the percentage of frames with a HB found between these two groups. We found that Lys27 assists the charge of the transferred phosphate in Path 1 establishing a close interaction with it. On the contrary, Lys27 has a minor role during the first stages of Path 2. Lys27 is found further away of the phosphate group during these first stages of the mechanism described by Path 2. Thus, the nature of the reaction mechanism is strongly coupled to the conformational diversity of the enzymatic active site and, in particular, to the electrostatic complementarity between the reacting fragments (the transferred phosphate group) and the protein (Lys27).
The plausible mechanisms for phosphate transfer reactions may be placed on a continuum between a completely associative mechanism and a completely dissociative one as described in the introduction. The nature of these mechanisms can be differentiated by the degree of bond formation and bond cleavage at the TS. In that sense, it is possible to construct a More O'Ferrall–Jencks52–54 diagram, choosing the bond orders (see ESI† for details)55 between the phosphorus atom of the transferred phosphate and either the donor or acceptor oxygen atoms as coordinates. Fig. 5 depicts the MFEPs projected on these bond orders, showing that phosphoryl transfer in Path 1 follows a dissociative-type mechanism. This is characterized by longer bond distances, required for the approach of the negatively charged phosphate to the hydroxyl group of the sugar. The sum of the distances of the phosphorous atom to both the acceptor and donor oxygens is always larger than 5.0 Å to reduce the electrostatic repulsion. Conversely, the phosphoryl transfer in Path 2 follows an associative-type mechanism, in which the phosphate transfer occurs with smaller distances to the donor and acceptor oxygen atoms. The proton is transferred to the γ-phosphate, reducing its charge and increasing the nucleophilicity of the O1 atom. This allows a closer approach between the reacting fragments. Accordingly, the TS in Path 2 appears considerably earlier than the TS in Path 1, in terms of the phosphorus distances to the leaving and nucleophilic oxygen atoms.
As we described in the Method section and ESI,† QM/MM simulations were performed using the AM1d-PhoT semiempirical Hamiltonian to describe the QM region. Although this semiempirical Hamiltonian was parameterized specifically to consider phosphate transfer reactions,43 a higher level of theory is required to obtain a precise estimation of energetics.59 Therefore, we corrected the converged strings by means of single point calculations on optimized geometries obtained at different values of the path CV coordinate s. For this purpose, we used the hybrid B3LYP/6-311++G**/OPLS Hamiltonian, and obtained the corrected free energy profiles, as depicted in Fig. 8. After this correction, the calculated free energy barriers were 21.0 and 55.2 kcal mol−1 for Paths 1 and 2, respectively. According to both the corrected and uncorrected free energy profiles, the preferred mechanism is the dissociative mechanism described by Path 1.
Fig. 8 Free energy profile for both paths, obtained with the string method and corrected at the B3LYP/6-311++G**/OPLS level. |
The free energy profile for this path is still 5.8 kcal mol−1 higher than the experimental value. The discrepancy with the experimentally derived value can also be partially reduced considering the zero-point energy correction to the activation free energy. Once the ZPE is included our best estimation of the activation free energy for the dissociative mechanism (Path 1) is 19.1 kcal mol−1. The remaining error is consistent with the observed reaction energy: although the experimental results show that the reaction is nearly thermoneutral,12 we found that in the corrected free energy profile the products where 4 kcal mol−1 higher than reactants. This could be due to an incomplete relaxation of the environment or inherent errors in our QM/MM description. As a further test we obtained the free energy profile after adding corrections with other functionals and/or basis sets (see Fig. S12†) obtaining results very similar to those presented here.
The larger free energy barrier obtained after corrections for Path 2 could be attributed to the limitations of the semiempirical Hamiltonian to describe this type of mechanisms. In a comparative QM/MM study of the catalytic mechanism of hairpin ribozyme with different quantum treatments,59 the authors concluded that when a non-bridging oxygen atom of the phosphate group acts as the base that activates the nucleophile, the AM1d-PhoT Hamiltonian predicts that proton transfer precedes phosphate transfer in a clearly asynchronous reaction pathway, just as was found in our case. However, at higher theoretical levels (either using density functional theory or ab initio approaches) the reaction proceeds in the reverse order, with the phosphate transfer preceding the proton transfer. Thus, semiempirical structures appear in high-energy regions of the Potential Energy Surface (PES) obtained at better levels of theory, explaining the large barrier obtained in the corrected free energy profile for Path 2. However, it is worth noting that though the AM1d-PhoT method doesn't correctly describe the structures for Path 2, the obtained activation energy is expected to resemble similar values when higher QM levels are used, as was observed in the previous cited study in hairpin ribozyme,59 where AM1d-PhoT still could reproduce the energetics in reasonable agreement with respect to higher level QM data. This would mean that the energy barrier obtained for Path 2 at a higher QM level should lie not far from 35 kcal mol−1. In fact, QM/MM studies at a DFT level in protein kinase A (PKA)17,60 have shown that potential energy barriers for the associative mechanism are within a range of 25–35 kcal mol−1. Instead, when the reaction takes place with proton transfer to another base (Asp256 in our case), the PES obtained at higher levels of theory shows that the reaction proceeds through a less asynchronous pathway, where the phosphate transfer precedes proton transfer. This is precisely the kind of mechanism described by Path 1 in our AM1d-PhoT/MM treatment.
In order to further investigate the relative energetics of Paths 1 and 2 and the possible dependence with respect to the chosen computational level, we performed an exploration of the potential energy surface at the B3LYP/MM level. In particular, we carried out a relaxed B3LYP/MM scan along the tightness coordinate (the distance between the donor and acceptor oxygen atoms, O3β–O1) for structures where the phosphorous atom is equidistant to both oxygens. In this scan we moved the system from the dissociative pathway region (where the tightness coordinate takes values of around 5 Å) to the associative one (with values of about 4 Å for the tightness coordinate), see Fig. S11.† Our results clearly demonstrate that the associative pathway (Path 2) presents relative energies that would be 15–20 kcal mol−1 larger than for the dissociative mechanism (Path 1), in good agreement with the difference observed between the activation free energies. We are thus confident that the representation of the reaction mechanism provided by Path 1 obtained from our QM/MM simulations correctly reproduces the main characteristics of the reaction between F6P and ATP catalyzed by Pfk-2.
Altogether, these characteristics prompted us to select the subunit containing products for QM/MM calculations: the ligands and residues in the active site were better oriented and the subunit conformation was in the closed state needed for the enzymatic reaction to take place. The exploration of the phosphoryl transfer mechanism with the string method showed that the preferred path in Pfk-2 is a dissociative mechanism where Asp256 acts as a general base. After phosphorylation of F6P, Asp256 acts as an acid to protonate the transferred phosphoryl group, recovering in this way the original state of the enzyme. During this process, Lys27 from the complementary chain stabilizes the transition state, forming a HB contact with the γ-phosphate during transfer. A second path was also obtained in which the phosphorylation is mainly associative, following a non-concerted mechanism, with the proton transfer preceding the phosphate transfer. However, this mechanism was found to be unfavorable due to a prohibitively high free energy barrier.
The methodology used in this work opens the possibility to study other members of the ribokinase family since relevant information regarding the kinetic mechanism of Pfk-2 is provided. In addition, the specific roles of Asp256 and Lys27 residues, which belong to the conserved enzymatic machinery of the family, were clarified. Furthermore, the reported crystal structure could serve as a model to reconstruct the active sites of other members of the family, as it provides detailed information about the relative position and specific interactions of both reactants and products embedded in their corresponding chemical environment.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c9sc00094a |
‡ These authors contributed equally. |
This journal is © The Royal Society of Chemistry 2019 |