Abstract
Protein lysine methyltransferases have important regulatory functions in cells, but mechanisms determining their activity and specificity are incompletely understood. Naturally, SETD2 introduces H3K36me3, but previously an artificial super-substrate (ssK36) was identified, which is methylated >100-fold faster. The ssK36-SETD2 complex structure cannot fully explain this effect. We applied molecular dynamics (MD) simulations and biochemical experiments to unravel the mechanistic basis of the increased methylation of ssK36, considering peptide conformations in solution, association of peptide and enzyme, and formation of transition-state (TS) like conformations of the enzyme-peptide complex. We observed in MD and FRET experiments that ssK36 adopts a hairpin conformation in solution with V35 and K36 placed in the loop. The hairpin conformation has easier access into the active site of SETD2 and it unfolds during the association process. Peptide methylation experiments revealed that introducing a stable hairpin conformation in the H3K36 peptide increased its methylation by SETD2. In MD simulations of enzyme-peptide complexes, the ssK36 peptide approached TS-like structures more frequently than H3K36 and distinct, substrate-specific TS-like structures were observed. Hairpin association, hairpin unfolding during association, and substrate-specific catalytically competent conformations may also be relevant for other PKMTs and hairpins could represent a promising starting point for SETD2 inhibitor development.
Similar content being viewed by others
Introduction
The methylation of histone and non-histone proteins, mainly at lysine and arginine residues, plays a key role in epigenetic regulation and cell signalling1,2,3. Histone lysine methylation has activating or repressive functions in the chromatin, depending on the position of the modified residue, the methylation state and the combination with other modifications4. Enzymes setting this modification are called protein lysine methyltransferases (PKMTs). One large family of PKMTs contains a conserved ~130 amino-acid SET (Su(var) 3-9, Enhancer of Zeste (E(z)) and Trithorax (trx)) domain, which forms the active site of the protein5. In the SET domain, the coenzyme S-adenosyl-L-methionine (SAM), which provides the activated methyl group, and the peptide containing the substrate lysine residue are located at opposing faces6. The lysine sidechain is bound into a hydrophobic tunnel allowing the ε-amino group of the lysine residue to approach the SAM methyl group in a deprotonated state7, eventually leading to a transfer of the methyl group in a bimolecular nucleophilic substitution (SN2) mechanism5,8.
The SET-domain containing protein 2 (SETD2, also called KMT3A) was first identified as huntingtin interacting protein 1 (HYPB, HIP-1)9. It has a size of 230 kDa corresponding to 2564 amino acids. SETD2 is the only PKMT known to introduce up to three methyl groups to lysine 36 of histone H3 (H3K36) in human cells10,11. H3K36me3 is enriched in the gene bodies of expressed genes since SETD2 is recruited by the elongating RNA Polymerase II9. Previous structural and kinetic studies have shown that an altered interaction of SETD2 with its peptide substrate can lead to strong biological effects. The K36M and K36I oncohistone mutants in histone variant H3.3 inhibit the methyltransferase activity of SETD2 because the methionine or isoleucine residue binds into the lysine binding tunnel of the active centre and thereby functions as a competitive enzyme inhibitor12,13. The inhibition of H3K36 PKMTs by the K36M/I oncohistones leads to massive perturbations of genome-wide H3K36me3 and H3K27me3 patterns and is frequently found in chondroblastomas14. Moreover, SETD2 frequently contains inactivating mutations in cancers15 and loss of SETD2 leads to global changes in DNA methylation patterns16.
Different structures of SETD2 in complex with H3K36 histone tail peptides and S-adenosyl-L-homocysteine (SAH) revealed that the peptide substrate is positioned in an extended conformation in a deep binding cleft in the catalytic SET domain of SETD2 where several contacts between the enzyme and the substrate peptide are formed17,18,19. Structure comparisons showed that the post-SET loop of SETD2 (amino acids 1692–1703) displays a dynamic behaviour that regulates autoinhibition17. In the state with no peptide bound in the SETD2 binding cleft, the post-SET loop is not resolved suggesting a flexibel behavior. Additionally, the autoinhibitory loop adopts a closed conformation and inserts R1670 into the active centre. This residue apparently functions as a placeholder and overlaps with H3K36M peptide in the SETD2-peptide complex, occupying the K36 access tunnel. An autoinhibitory function of equivalent loops was also observed for other PKMTs with different placeholder residues, such as serine in ASH1L or cysteine in NSD120. In crystal structures of PKMTs with bound peptide, the post-SET loop was observed in half opened and closed conformations covering the peptide in the active centre in a lid-like manner with the placeholder residues turned outwards. This indicates a dynamic opening and closing of this loop upon peptide binding and release17.
The substrate specificity of SETD2 for H3K36 has been previously mapped, revealing that the “natural” H3 residues were not the most preferred ones at many positions of the target sequence19. Based on this, an artificial peptide substrate was designed that contained the most favourable residues at each position (Fig. 1). It was shown that this 15 amino-acid long super-substrate peptide (ssK36), which differed at four positions from the original H3K36 (A31R, T32F, K37R and H39N) was methylated more than 100-fold faster than the corresponding natural H3K36 peptide. The crystal structure of the ssK36 peptide complexed to the SET domain of SETD2 was resolved, and subtle differences to the H3K36-SETD2 structure were observed, which hint towards the mechanism of the improved methylation of the ssK36 substrate19. The four amino acids altered in ssK36 establish different contacts compared to the canonical H3K36 residues, showing that ssK36-R31 forms an H-bond/salt bridge with SETD2-E1674, ssK36-F32 is bound into a pocket formed by SETD2-E1674 and SETD2-Q1676 and ssK36-R37 interacts with the backbone of SETD2-A1700. However, overall the ssK36- and H3K36-SETD2 complex structures are very similar, with an RMSD of both peptides of only 0.308 Å. Therefore, the crystal structures could not fully explain the huge enhancement in the methylation rate of ssK36.
In this work, a combination of molecular dynamics (MD) simulations and biochemical experiments were applied to identify the mechanisms responsible for the increased activity of SETD2 towards ssK36. Multiple steps of the catalytic cycle were investigated to examine the molecular processes explaining why SETD2 has such a strongly increased activity for the super-substrate peptide ssK36, viz. (a) the peptide conformation in solution, (b) the binding process of the peptide into the peptide binding cleft of SETD2 and (c) the approach of a SETD2-peptide complex towards catalytically competent conformations. Strikingly, we observed that ssK36 preferably adopts a hairpin conformation in solution with the target lysine in the middle of the loop facing outside, whereas the H3K36 peptide preferentially has an extended conformation. We next showed that peptides in a hairpin conformation have easier access to the active site of SETD2 compared to the extended conformation. These simulation results were validated by experimental FRET studies and peptide methylation studies with substrates exhibiting stable hairpin conformations. Moreover, in MD simulations of H3K36- and ssK36-SETD2 complexes, we observed increased numbers of the transition-state (TS)-like structures with ssK36. Our data reveal different dynamic interactions of both peptides with the SETD2 SET domain, which ultimately lead to substrate-specific catalytically competent conformations. Hence, by comparing the natural H3K36 peptide and the designed ssK36 in multiple steps of the catalytic cycle, the molecular mechanisms of the much higher catalytic activity of SETD2 towards ssK36 can be explained by an enhanced rate of association of the ssK36 peptide in a hairpin conformation and in better stabilization of TS-like conformations of the SETD2-ssK36 complex.
Results
Investigation of different conformational preferences of unbound H3K36 and ssK36
Our first aim was to find out if the conformation of the designed SETD2 super-substrate peptide ssK36 differs from that of the natural H3K36 peptide substrate. To observe potential conformational differences of both peptides in solution, each peptide was subjected to MD simulations in a water box for a total simulation time of 3.5 µs (50 replicates à 70 ns for each peptide). To generate a variety of random starting positions, each replicate had an independent equilibration phase of 10 ns preceding the following simulation. A total of 350,000 conformers from the MD simulations of H3K36 and ssK36 were processed by the clustering algorithm Enspara21 and distributed into clusters based on their conformational similarities measured as backbone atom root mean square deviation (RMSD). Each cluster was represented by a centroid structure, visualizing the peptide conformation, which most accurately characterises the corresponding cluster. To ensure a hypothesis-free clustering and to maximise the sampling space, the trajectories of both peptides were pooled before the clustering. Thereby, each conformation from either peptide had equal chances to be clustered with every other conformation.
Clustering into 2 groups revealed one cluster with an extended centroid structure and one with a hairpin-like bent conformation (Fig. 2a). Increasing the number of clusters led to three distinct centroid structures: one almost extended (similar to the one observed after clustering into two groups), one sharply bent with strong curvature centred at the target lysine residue and one mixture between the extended and hairpin conformation (Fig. 2b). The largest conformational differences between the centroid structures were observed between cluster 1 (extended) and cluster 2 (bent) (see Supplementary Table 1). Further increasing the number of clusters led to a splitting of the mixed clusters into sub-clusters, while the general extended and bent centroid structures for clusters 1 and 2 were maintained (Supplementary Fig. 1A). Repeating the clustering analysis with randomly selected subsets of the data (50%, 30% and 10%) led to similar centroid structures and comparable distributions of H3K36 and ssK36 among them indicating that the simulation time was sufficient to draw these conclusions (Supplementary Fig. 1B–E).
Next, it was determined how many conformations of the H3K36 or ssK36 simulations were assigned to the respective clusters. This analysis revealed that cluster 1 mainly consisted of conformations observed in simulations of the H3K36 peptide, while the majority of conformations in cluster 2 were produced in simulations with ssK36. Cluster 3 showed an almost equal contribution of H3K36 and ssK36 conformations. This distribution suggests that the H3K36 peptide preferably adopts an extended conformation, whereas the ssK36 peptide prefers a hairpin conformation with a loop at the position of the target lysine. To assess the statistical significance of the 2.2-fold hairpin preference of ssK36, clustering was conducted in three independent runs, which were analysed separately. Based on this, the preference of H3K36 to adopt an extended conformation and ssK36 to adopt a hairpin-like bent conformation was significant. t-test analysis of the results of the three independent MD analyses revealed p-values of 6.4 × 10−5 for the enrichment of H3K36 and ssK36 in clusters 1 and 2 in the two-state clustering (based on two-tailed t-test with equal variance). In the three-state clustering, p-values of 0.0036 and 0.0032 were obtained for the enrichment of H3K36 in cluster 1 and ssK36 in cluster 2. Additionally, we analysed the frequency of long-lasting hairpin conformations in the MD simulations of both peptides, defined as multiple consecutive MD simulation frames which are in hairpin conformation (Fig. 2d, e). This analysis revealed that ssK36 displayed 4.8-fold more hairpin conformations with long lifetimes compared to H3K36, again indicating that hairpin stabilization is stronger for ssK36.
A detailed analysis of the bent structures showed that the mutated amino acids in ssK36 are engaged in different intramolecular interactions, which stabilize the hairpin structure (Supplementary Fig. 2A–E). These interactions, among others, include hydrogen bonds of R31 with the backbone atoms of R40 and stacking of F32 and Y41 (Fig. 2c). This indicates that the different conformational preferences of H3K36 and ssK36 directly result from the four amino-acid exchanges in the ssK36 peptide (Supplementary Movie 1).
Experimental investigation of conformational preferences of the H3K36 and ssK36 peptides
The peptide simulations in solution revealed different conformational preferences for the H3K36 and ssK36 peptides. To challenge these simulation results experimentally, a FRET system was applied to determine the dynamic end-to-end distance distributions of both peptides in solution. For this, an EDANS fluorophore was attached to the C-terminus of the peptides and a Dabcyl quencher to the N-terminus (Dabcyl-peptide-EDANS). EDANS is excited at 340 nm and emits fluorescence at 490 nm. Due to FRET, the emission is partially quenched by Dabcyl depending on the average end-to-end distance and the Förster radius (R0) of the FRET pair. Hence, if fluorophore and quencher are in close proximity, more FRET occurs, and less fluorescent light is detected (Fig. 3a). The R0 of the EDANS/Dabcyl pair of fluorophores is 33 Å22, which is slightly longer than the average end-to-end distance of the peptides in the extended conformation of 27 Å. Hence, even for peptides in an extended conformation, FRET is expected to occur. To assess the dynamic structural properties of both peptides in the FRET experiments, the fluorescence intensity of both peptides was measured at multiple temperatures. Assuming a simple two-state equilibrium between the unfolded and hairpin peptide structures (U-H), the ΔH°’ of hairpin formation should be negative, because of more intramolecular interactions formed in the hairpin state. At the same time, ΔS°’ is expected to be negative as well, because of the reduced conformational freedom of the hairpin conformation. Ignoring the temperature dependence of both terms, with increasing temperature, the unfavourable TΔS term should cause a gradual shift of the equilibrium towards the unfolded conformation.
As shown in Fig. 3b, the intensity of Dabcyl-H3K36-EDANS was 33% higher than the intensity of Dabcyl-ssK36-EDANS at 5 °C. This difference suggests that the ssK36 peptide has a shorter average end-to-end distance. This result is in accordance with a preferential hairpin formation, which brings the quencher and fluorophore closer together, resulting in more FRET and less detectable fluorescence. As expected, the difference between H3K36 and ssK36 decreased with increasing temperature and completely disappeared at 95 °C indicating that the hairpin conformations have unfolded and no conformational differences of both peptides exist at this temperature due to the enhanced thermal movement. After normalisation to this endpoint, the differences between the two peptides were highly reproducible in two independent replicates of this experiment.
To test these observations and tackle the question, of whether the experimental data do indeed show the suggested different conformational preferences, two control systems were used. In one system, only the fluorophore but no quencher was attached to each peptide (Fig. 3c). Both peptides showed a 20-fold higher fluorescence due to the absence of FRET (Supplementary Fig. 3B–D). Moreover, the observed data showed no temperature-dependent differences in their fluorescence. This indicates that the effect, which was seen before, indeed is due to temperature-dependent conformational changes influencing the FRET efficiency.
In a second control experiment, the FRET peptides with quencher and fluorophore were used, but digested with Proteinase K before the measurement (Fig. 3d, for digestion control see Supplementary Fig. 4B). In this system, no conformational preferences are possible anymore. Again, a 12-fold higher overall fluorescence was observed, and no temperature-dependent differences between H3K36 and ssK36 were detected. This result confirms that the intact conformation of the peptides is necessary to observe the temperature-dependent FRET effects.
Simulation of the peptide association process
The observations in the peptide MD simulations and the solution FRET experiments suggested different conformational preferences for H3K36 and ssK36. To test whether these different conformations of both peptides influence their binding rate to SETD2, steered molecular dynamics (sMD) simulations were applied. sMD simulations use external forces in MD simulations to guide association processes. This accelerates processes that otherwise would be too slow to be modelled and concentrates the sampling along a specific, predefined reaction coordinate23. To be suitable for the sMD experiments, SETD2 was modelled in an open conformation, in which no peptide is bound, and the autoinhibitory post-SET loop (Q1676-K1703) is in a detached, open position. In this conformation, the placeholder residue R1670 points outwards, and it does not block the active site17 (Fig. 4a). Hence, this conformation represents a state in which a peptide substrate is able to dock into the binding cleft (Supplementary Fig. 5). During the sMD simulations, the loop was not anchored in the open conformation and simulations of the apoenzyme indicated that the loop falls back at timescales >500 ns without peptide. Hence the movement of the loop was slower than the association of the peptide in the sMD experiments, which prevented direct effects of spontaneous loop closure on the sMD simulations. Interestingly, loop closure was observed at shorter timescales after the peptide entered the binding cleft.
For sMD experiments, the H3K36 and ssK36 peptides were placed right above the open binding cleft, 30 Å away from the cofactor SAM with the K36 sidechain facing towards the SETD2 binding cleft. To accelerate the association process, a weak attractive force of 0.5 kJ/(mol × Å2) was applied between the Nε-atom of lysine 36 and the methyl group C-atom of the SAM (Fig. 4b). In order to define criteria describing a successful docking, the following geometric requirements for a transition-state (TS)-like conformation were derived from the SN2 geometry:
-
(1)
the distance between the lysine Nε and SAM methyl group C-atom is <4 Å.
-
(2)
the angle between the lysine Nε - lysine Cδ bond and the forming bond between lysine Nε and the SAM methyl group C-atom is in a 109° ± 30° range.
-
(3)
the angle between the lysine Nε-SAM methyl group C-atom and SAM methyl group C-atom-SAM S-atom bonds is in a range of 180° ± 30° (Fig. 4c).
One hundred sMD simulations of 50 ns were performed for each peptide, and the number of docking events monitored which fulfilled the success criteria in at least one snapshot. The analysis of the sMD simulations revealed that both peptides were able to establish SN2 TS-like conformations following this definition. The H3K36 peptide successfully docked into the active site in 40 of 100 simulations, whereas the ssK36 peptide docked successfully in 55 out of 100 simulations (Fig. 4e). An example of a successful docking event is provided in Supplementary Movie 2.
However, we identified a caveat in this experimental approach. Since lysine 36 is positioned in the middle of the peptide, movement of the peptide caused by pulling with the sMD force on this residue automatically induced the adoption of a hairpin conformation, because the K36 will move towards the SAM while the N- and C-termini of the peptide lag behind. Therefore, both peptides eventually formed hairpin conformations when approaching the active site of SETD2 (90% of H3K36 simulation replicates and 100% of ssK36 simulation replicates at least transiently showed a peptide end-to-end distance <15 Å, Supplementary Fig. 6). To preserve the different conformational preferences of the peptides during the sMD experiment, an additional repulsive force of 0.3 kJ/(mol × Å2) between the ends of the peptides was added to the system. This repulsive force increased with decreasing distance between N- and C-termini (N-C distance) and thereby counteracted the formation of a hairpin conformation during the association process (Fig. 4d, Supplementary Movie 3). With this approach, a direct comparison between the docking efficiency of the hairpin and the extended conformations was possible. 100 replicates of this sMD experiment showed that the number of successful dockings strongly decreased if the peptides were not able to approach SETD2 in a hairpin conformation (Fig. 4e). Overall, with the repulsive force, H3K36 docked only 11 times successfully and ssK36 18 times, corresponding to a 3.6-fold (H3K36) and 2.8-fold (ssK36) decrease in docking efficiency when compared to the unconstrained settings. This indicates that the hairpin formation heavily increased the chances of both peptides to successfully dock into the peptide binding cleft of SETD2. Moreover, in both settings, a higher number of productive docking events was observed with ssK36 than with H3K36. All the differences between ssK36 and H3K36 with and without repulsive force are highly significant (Supplementary Fig. 7). This finding underscores the higher intrinsic ability of the ssK36 peptide to adopt a hairpin conformation that is more productive in the association reaction.
Unfolding of hairpin conformation upon peptide binding to SETD2
The sMD experiments showed easier access of hairpin conformations into the active site of SETD2 compared to extended peptide conformations. However, crystal structures of SETD2 complexed with either H3K36 or ssK36 show both peptides bound in an extended conformation in the binding cleft in the SET domain (PDB: 5V21 for H3K36, PDB: 6VDB for ssK36)17,19. Therefore, the conformational changes during the sMD simulations were analysed in more detail to find out if, after the initial docking of the hairpin peptide into SETD2, transitions occurred between the hairpin and extended conformations. In this analysis, the crystal structures of the H3K36 or ssK36 peptides bound to SETD2 (PDB: 5V21 for H3K36, PDB: 6VDB for ssK36) were used as reference conformations for peptides in the fully extended state. The conformations of peptides observed in sMD simulations without repulsive force that reached a TS-like structure were compared to the reference conformations based on the backbone RMSD after positional optimisation by rigid body movement. In fact, 84% of ssK36 peptides reduced their RMSD to the extended reference conformation during successful docking events, as well as 68% of the H3K36 peptides, indicating that in most cases, the structures of the docked peptides approached the complex structure observed in the crystal structure analyses (Fig. 5a and Supplementary Fig. 8). It is possible that these numbers would further increase with longer simulation times. In many cases, the final structures after the sMD simulation showed a very good superposition with the extended peptide conformations observed in the crystal structure analysis, in particular at the residues surrounding K36 (Fig. 5b, c).
Since the peptides transiently adopted a hairpin conformation in almost all replicates of the sMD simulations (see above), the reduced RMSD between the peptide structures in the simulation and their crystal structure conformation implies an unfolding process, in which the hairpin structure opens up and the N-C distance increases (Fig. 5a and Supplementary Fig. 8). To monitor this process, the N-C distance of the peptides was determined during the sMD simulations leading to successful docking. For ssK36, 82% of the cases showed an increasing N-C distance during the simulation, as well as 85% of the H3K36 replicates. These analyses indicate that in many simulations during the docking process, both peptides unfold from a hairpin conformation into an extended conformation similar to the crystal structures (an example of this process is provided in Supplementary Movie 4). As expected, the RMSD to the extended reference conformation and N-C distance were highly anticorrelated during the simulations. Moreover, the increases in N-C distance were similar for both peptides indicating that if the transition between a hairpin and extended conformation takes place, both peptides behave similarly.
FRET analysis of peptide conformations during binding to SETD2
The analysis of the sMD simulations suggested that an unfolding of hairpin conformations occurs upon binding of the peptides to the active site of SETD2. To validate this observation experimentally, the H3K36 and ssK36 peptides with attached fluorophore and quencher were used to monitor the peptide conformation by FRET during the binding to SETD2 (Fig. 6a). Strikingly, the addition of SETD2 led to an increase in the fluorescence intensity of both peptides, but the extent of the intensity gain differed (Fig. 6b). The addition of SETD2 to H3K36 caused a 5.0% increase in intensity, while the intensity increased by 14.8% in the case of ssK36. This result suggests that dynamic hairpin conformations of both peptides are resolved during SETD2 binding since fluorophore and quencher are being separated. The finding that the addition of SETD2 caused a three-fold stronger increase in fluorescence of ssK36 than H3K36 can be connected to more hairpin conformations present in solution in the case of ssK36 and/or a more efficient binding of SETD2 to ssK36. To confirm that the intensity increase was caused by the interaction between quencher and fluorophore, peptides without quencher were used (Fig. 6c). Upon addition of SETD2, the intensity increased only slightly for both peptides, much less than for the peptides with the quencher attached (0.18% for EDANS-H3K36 and 1.2% for EDANS-ssK36).
Methylation experiments with stable hairpin substrates
Our data provide evidence for a previously unknown association pathway of peptides into SETD2, where the binding of a peptide is preferred in a hairpin conformation. During the binding process, the hairpin unfolds, and the peptide adopts the extended conformations seen in the structural studies. To investigate the effect of hairpin formation on the activity of SETD2 directly, we conducted SPOT peptide array methylation experiments with 15mer H3K36 and ssK36 peptides and H3K36(C-C) and ssK36(C-C) variants thereof, which contain two Cys residues at position 30 (P30C) and 43 (P43C) allowing them to form disulphide bonds under oxidative conditions. The disulphide bonds arrest the peptides in the hairpin conformation with K36 presented in the loop of the hairpin. The observed reaction rates (Fig. 6d, e) can be summarized as following:
-
(1)
H3K36(C-C) with chemically fixed hairpin conformation is methylated better than H3K36.
-
(2)
ssK36(C-C) with chemically fixed hairpin conformation is methylated worse than ssK36.
-
(3)
H3K36(C-C) and ssK36(C-C) are methylated almost equally.
H3K36 ≪ H3K36(C-C) ≈ ssK36(C-C) < ssK36
Our finding that the hairpin stabilized H3K36(C-C) is methylated better than the original H3K36 peptide clearly indicates that hairpin formation accelerates the reaction. However, the hairpin peptides H3K36(C-C) and ssK36(C-C) are methylated at a reduced rate when compared with ssK36, indicating that the unfolding of the peptide during complex formation is beneficial for methylation because it allows for the formation of additional contacts between SETD2 and the peptide. Finally, the observation that the hairpin stabilized forms of H3K36 and ssK36 are methylated at similar rates supports the notion that the hairpin formation potential is one of the critical differences between both peptides explaining large parts of their different methylation rates by SETD2.
MD simulation of the SETD2-peptide complexes
The SETD2 crystal structures with bound ssK36 and H3K36 peptides only resolve the ground state conformation of both complexes. Therefore, we used them as a starting point for MD simulations to investigate the interplay between protein and peptide in atomic detail over time and obtain more information about the dynamic processes leading to enzymatic catalysis (Fig. 7a, b). To derive a parameter that describes the likelihood of catalysis during the MD simulation, the criteria for an SN2-reaction TS-like structure as defined above were applied. In a total of 3 µs simulation time (15 simulations à 100 ns for two peptides), ssK36 established significantly more TS-like structures than H3K36. The complex of SETD2 with ssK36 was, on average 1117 times per simulation in a state, in which all TS criteria were fulfilled, and the SN2 reaction could take place. In contrast, the complex of SETD2 with H3K36 reached the TS-like conformation only 305 times on average per simulation (p-value 1.2 × 10−8, based on two-tailed t-test with equal variance) (Fig. 7c). Repeating the analysis with randomly selected subsets of the data (50%, 30% and 10%) led to similar ratios between H3K36 and ssK36 (Supplementary Fig. 9).
The increased number of TS-like conformations of ssK36 was accompanied by an increase in the lifetimes of these conformations. As shown in Fig. 7d, TS-like conformations established by H3K36 were mostly transient (only 13 events were identified in which SN2 criteria were fulfilled in 8 or more consecutive frames of the simulation). In contrast, the ssK36 peptide achieved long-lasting TS-like states efficiently (397 events fulfilled SN2 criteria in 8 or more consecutive frames). Overall, the ssK36 peptide established 30-fold more long-lasting TS-like conformations with SETD2 compared to H3K36.
Contact analysis of ssK36 and H3K36-SETD2 complexes
To identify the molecular mechanisms leading to the differing abilities of the H3K36- and ssK36-SETD2 complexes to reach TS-like structures, the contacts established between SETD2 and both peptides during the simulations were analysed. The analysis was based on distance criteria, and contacts were considered as established if the distance of a pair of heavy atoms from the peptide and SETD2 was below 4.5 Å. In each case, the fraction of time during which contact was established was analysed to create a contact profile. The resulting contact profiles for H3K36 and ssK36 were then contrasted and differences extracted (Fig. 8a). Previously, three characteristic differences were observed in the static crystal structures of SETD2-H3K36M and SETD2-ssK36M19: (1) ssK36-R31 interacts with E1674, (2) ssK36-F32 is placed in a pocket generated by E1674 and Q1676 and (3) ssK36-R37 interacts with the backbone of A1700. These effects were confirmed in the contact profiles observed in the MD simulations (Fig. 8a). Additionally, the contact profile displays a large difference at residue 39, which was not detected in the crystal structure analysis. At this position, H3 carries a histidine (H39) and ssK36 an asparagine (N39). In the ssK36-SETD2 complex, the Nδ-atom of N39 frequently interacts with the backbone atoms of SETD2 D1665 and Y1666 (Supplementary Fig. 10A). This could cause the backbone atoms of ssK36 N39-P43 to shift and move closer to SETD2 when compared to H3K36. This shift is further supported by the fact that ssK36-R40 is more involved in contact with SETD2, namely M1526 and Q1638, when compared to H3K36-R40 (Supplementary Fig. 10B).
As described above, characteristic differences in the established contacts between H3K36-SETD2 and ssK36-SETD2 were observed in the simulations, which are in good agreement with crystal structure analysis. However, contacts that stabilize catalytically competent conformations able to reach TS-like structures need to be distinguished from the overall contacts. Thus, a more focused view on the catalytically relevant contacts in TS-like conformations was prepared. The resulting contact profile displays where H3K36 and ssK36 bound differently to SETD2 in conformations that reached a TS-like structure. Shown are all contacts, which exhibited a change of over 35%, excluding neighbouring residues (Fig. 8b). This analysis revealed that N39 of ssK36 is engaged in different contacts compared to H39 in H3K36 including the preference of N39 to interact with the backbone atoms of Y1666 as observed before (Fig. 8a). This was also true for R40, as its contact preferences from the previous analysis were also observed in the TS-like conformations. Specific differences in the contact maps of catalytically competent conformations were observed for Y41: Y41 of ssK36 interacts with P1633, E1636 and T1653 of SETD2, whereas Y41 from H3K36 interacts with M1526 and Q1638. As a consequence, the C-terminal part of the ssK36 peptide is shifted towards SETD2 in the catalytically competent conformations when compared with H3K36 (Fig. 8c and Supplementary Fig. 11).
Exemplary snapshots of catalytically competent conformations are shown in Supplementary Fig. 10A–E. The H3K36 peptide shows altered TS-like structures near the target residue for methylation (K36) since V35 of H3K36 has more contact with V1695 than V35 of ssK36. Residue K37 of H3K36 forms different contacts with L1609 and D1665 compared to R37 of ssK36, which is more involved in contact with A1699. The alteration from T to F at position 32 also causes differences in catalytically competent conformations, as T32 of H3K36 interacts with K1673 while F32 of ssK36 interacts with I1602. Because of this, the N-terminal part of ssK36 moves closer to SETD2 in the catalytically competent conformations when compared with H3K36 (Fig. 8c and Supplementary Fig. 11), similarly as observed for the C-terminal part. Strikingly, in catalytically competent conformations the outer parts of the ssK36 peptide, namely residues A29–G33 and P38–P43, approached the reference point inside the protein (R1625), indicating that they come closer to SETD2. However, the middle part showed the opposite trend and slightly detached from SETD2, potentially giving more flexibility for K36 to orient itself (Fig. 8c and Supplementary Fig. 11).
All the peptide interacting residues identified in our work and in the structural analysis19 are fully conserved in an alignment of 64 representative mammalian SETD2 homologs (data not shown). We also inspected the literature for data on mutational studies of these residues (Supplementary Table 2)17,24. Strikingly, we observed that mutation of peptide interacting residues led to strong reductions in activity if peptide residues conserved between H3K36 and ssK36 are concerned, highlighting the essential roles of these interactions. However, mutations of Y1604 and T1637, which both contact residues in H3K36 that are altered in ssK36, led to an increase in H3K36 methylation, indicating that these regions are not ideal for catalysis in H3K36.
In summary, the different peptide sequences of H3K36 and ssK36 result in different catalytically competent conformations indicating that H3K36 and ssK36 promote catalysis via distinct, separate pathways using different contacts and interactions. According to the results of the MD simulations, the stabilization of catalytically competent conformations in H3K36 is less efficient and leads to fewer catalytically productive binding events. The four mutated residues in ssK36 cause a more efficient formation of catalytically competent conformations, which are different from those of H3K36, by establishing contacts only possible for ssK36, and this finally contributes to a higher enzymatic activity.
Discussion
PKMTs are essential enzymes, which modify lysine side chains in proteins by the addition of up to three methyl groups. The methylated lysine residues have important signalling roles in histones and non-histone proteins2,3. To distinguish different potential methylation substrates, PKMTs form contacts to the amino-acid residues surrounding the target lysine, which establish a specific readout of the amino acids sequence of the target peptide25. Here, we approached the mechanisms of the sequence-specific methylation of PKMT substrates using an artificially designed super-substrate peptide of SETD2 as a model system that had been identified before and shown to be methylated about 100-fold faster compared to the natural H3K36 peptide19. The solved crystal structures of SETD2 complexed with the H3K36M or ssK36M peptides17,18,19 represented important steps towards the understanding of SETD2’s substrate specificity by illustrating how H3K36M and ssK36M peptides bind into the active site of SETD2 and which contacts are established between SETD2 and the substrate peptides in each complex. However, despite the discovery of peptide-specific contacts, these structures were very similar overall, and they could not easily explain the 100-fold increase in the methylation rate of ssK36. One reason for this is that static crystal structures only capture the conformation of the ground state binding complex, and it is unknown to which extent this represents the catalytically competent conformations able to reach the TS of the enzymatic reaction. Moreover, complex structures do not describe the pathway of the association of the peptide to the enzyme, nor the different structures of the peptides in the solvent, which may affect the association reaction. Hence, critical questions regarding the substrate-specific activity of SETD2 remained unsolved.
Molecular dynamics simulations and protein modelling have the capacity to resolve steps and conformational distributions involved in protein-ligand association reactions and during enzymatic catalysis26,27. MD simulations combined with quantum mechanics have been applied to PKMTs to determine details about their catalytic mechanism and product specificities28,29,30,31,32. Moreover, MD simulations were applied to investigate conformational changes of PKMTs8,30,33,34 or their interaction with SAM and inhibitors33,35. Using MD simulations combined with biochemical FRET and peptide methylation experiments, in this study, we aimed to provide a comprehensive view of the role of the substrate peptide sequence in different steps critical for enzymatic turnover, viz. (1) the conformation of the substrate in solution, (2) the pathway of enzyme-substrate association and the conformational changes accompanying it and (3) the approach of the enzyme-substrate complex towards the TS of the methyl group transfer reaction.
Based on our data, the following model of the peptide binding process to SETD2 was developed (Fig. 9): The ssK36 peptide preferentially adopts hairpin conformation in solution, while H3K36 prefers to exist in an extended conformation (Fig. 9a). This difference is a direct result of the four introduced mutations because multiple peptide-specific contacts are established that stabilize the hairpin conformation of ssK36. The hairpin conformation of the ssK36 peptide in solution was confirmed by FRET experiments. Remarkably, the hairpin conformation presents K36 and the adjacent V35 in the loop region facing outside, suggesting that these residues could act as first contact points during the docking of the substrate into the SETD2 SET domain. sMD data indicated that hairpin conformations facilitate the entry of the peptide into the binding cleft of SETD2 when compared with extended peptide conformations suggesting that a transient hairpin conformation is needed during the initial docking of the substrate peptide to SETD2 (Fig. 9b). This result was also confirmed by peptide methylation experiments showing that H3K36 with artificially introduced hairpin conformation is methylated faster. After the formation of the initial SETD2-peptide complex mediated by loop residues V35 and K36, additional contacts between the peptide and SETD2 can then gradually spread towards C- and N-termini of the peptide in a zipper-like process. This leads to an unfolding of the hairpin and adoption of an extended peptide conformation as observed in the crystal structures of SETD2 complexed with either H3K36 or ssK36 (Fig. 9c). We found in the sMD simulations and FRET experiments that the N-C distance of the peptides increased during the peptide association process, when the RMSD of the conformations in the sMD and the crystal structures decreased, suggesting a gradual unfolding of the hairpin conformation for both peptides during the binding process. Preventing peptide unfolding reduced the methylation by SETD2, as seen in the methylation of ssK36 with chemically fixed hairpin conformation. The dynamic peptide association mechanism described in this work complements the understanding of the dynamic behaviour of the post-SET loop of the enzyme during peptide binding17.
Mechanistically, the preference for this association pathway may be related to the fact that SETD2 has an extended peptide binding cleft that can change between an open and a closed conformation in a peptide free state. In the hairpin conformation, K36 and V35 have maximum flexibility to position themselves and bind to their respective hydrophobic pockets in the SETD2 active site. Importantly, for this interaction, only the corresponding part of the binding cleft has to be in an open access state. The strong interaction of SETD2 with V35 and K36 could support long-lasting binding events of the peptide after the initial docking. During this phase, the transient opening of further parts of the binding cleft can lead to a stepwise formation of the other peptide-SETD2 contacts starting from the central part of the complex (V35 and K36) in a zipper-like process until the final stable complex is formed. In contrast to this stepwise process, direct binding of the peptide in an extended form would require a completely open binding cleft and this pathway is disfavoured for this reason.
This model is in agreement with several data from the literature: (1) The finding that hydrophobic residues at the V35 position are obligatory for substrate recognition by SETD219. (2) The key role of K36 in the binding of ssK36 to SETD2 is illustrated by the finding that the inhibition constant of the K36M mutant of ssK36 was only moderately (3.5-fold) improved as compared to the K36M mutant of H3K36, while the stimulation of ssK36 methylation was much stronger19. These results suggest that the outwards-faced V35 and K36 in the hairpin directly influence the binding process. (3) Previous investigations showed that the SET-domain containing PKMT SET7/9 had an increased methylation activity towards an artificially designed peptide with a disulphide-stabilized hairpin structure36. This could indicate that peptides with hairpin conformations, in general, have favourable catalytic properties for PKMT-catalysed peptide methylation.
In the next step of the enzymatic turnover cycle, the results from MD simulations of the SETD2-peptide complexes revealed a specific TS-like conformation for ssK36 that is stabilized more efficiently in SETD2-peptide complexes than the TS-like conformation of H3K36 (Fig. 9d). Our analysis confirmed findings from the previous crystal structure analysis19, but important additional contact differences were identified. The analysis of enzyme-peptide contacts in catalytically competent conformations observed in the MD simulations showed that H3K36 and ssK36 form distinct contact networks with the enzyme, indicating that methylation of both peptides proceeds through different TS-like conformations. The four introduced mutations formed unique enzyme contacts exclusively accessible for ssK36. Because of these contacts, the N- and C-terminal parts of ssK36 move closer to SETD2 when compared with H3K36. However, the central part of the peptide shows the opposite trend and slightly detaches from SETD2, potentially giving more flexibility for K36 to re-orient. This analysis raises the striking possibility that methylation of different peptide sequences by one PKMT may generally involve alternative substrate-specific conformations of the catalytically competent enzyme-peptide complex, which widens our understanding of the mechanism of this important group of enzymes.
Based on our data, the roughly 100-fold increase in methylation rate of ssK36 can be attributed to two distinct effects, the accelerated association due to preferred hairpin formation and the better stabilization of TS-like conformations. The finding that kinetic barriers during association and formation of TS-like conformations are lowered with ssK36, is in agreement with previous data showing that the KM-value of ssK36 is only marginally improved (1.4-fold), leaving most of the rate enhancement for kcat term (about 70-fold)19. The overall rate enhancement of ssK36 is in a very good agreement with the results of the MD simulations presented here because the 4.8-fold increase in the stable hairpin formation of ssK36 combined with the 30-fold increase in TS-like conformations with long lifetimes could explain an up to 140-fold increase in reaction rate. Currently, it is not possible to determine the minimal lifetimes of hairpin conformations and TS-like structures that are needed for productive association and catalysis. Hence, the 140-fold change represents an upper limit of the potential effect, because the differences in both properties are smaller if lifetimes were not considered. The sMD experiments support the proposed pathways of hairpin peptide conformation during the association process followed by the unfolding of the hairpin and positioning of the peptide in the SETD2 binding cleft. While they also qualitatively revealed improved efficiency of ssK36 in the association process, quantitative statements cannot be made, because the sMD approach includes external forces.
We conclude that the mechanistic principles of hairpin association and substrate-specific catalytic conformations discovered here shed new light on the catalytic mechanism of SETD2, an important enzyme in the physiology of human cells. They may apply to other PKMTs as well, thereby helping to understand the principles of catalysis of this large and highly relevant group of chromatin and protein-modifying enzymes with very important roles in cellular signalling. Moreover, the hairpin-based association mechanism may open new avenues for PKMT inhibitor design by using hairpin peptides as design scaffolds.
Experimental procedures
General settings and parameters in the molecular dynamics simulations
All molecular dynamics (MD) simulations were performed in OpenMM 7.4.237,38 utilizing the NVIDIA CUDA39 GPU platform. The systems were parameterised using the General Amber force field (GAFF) and AMBER 14 all-atom force field40,41,42. SAM was modelled based on the coordinates of SAH and parametrised using ANTECHAMBER from AmberTools (18.0)43. The non-bonded interactions were treated with a cut-off at 10 Å. Additionally, the Particle Mesh Ewald method44 was used to compute long-range Coulomb interactions with a 10 Å non-bonded cut-off for the direct space interactions. Energy minimisation of the system was performed until a 10 kJ/mole tolerance energy was reached. Simulations were run using a 2 fs integration time step. The Langevin integrator45 was used to maintain the system temperature at 300 K with a friction coefficient of 1 ps−1. The initial velocities were assigned randomly to each atom using a Maxwell–Boltzmann distribution at 300 K. A cubic water box with a 10 Å padding to the nearest solute atom was filled by water molecules using the tip4p-Ew model46. The ionic strength of 0.1 M NaCl was applied, by adding the corresponding number of Na+ and Cl− ions. Protonation states, equilibration protocols and other specifications for the individual system setups are described below. Production runs were performed under periodic boundary conditions, and trajectories were written every 10,000 steps (20 ps).
Simulation of peptides in solution
The peptide structures were retrieved from crystal structures of the complexed peptide with SETD2, PDB: 5V21 for the H3K36 peptide and PDB: 6VDB for the ssK36 peptide (Fig. 1a–c). Total number of atoms: 15753 for H3K36: 13 Cl− ions, 9 Na+ ions, volume of the box: 142,713 Å3; total number of atoms: 17,236 for ssK36: 15 Cl− ions, 10 Na+ ions, volume of the box: 159,179 Å3. Missing amino acids were modelled by the PyMOL (2.4.1) builder. Since the available crystal structures of SETD2 are complexed with K36M inhibitor peptides, M36 was mutated to K36 for both peptides using the PyMOL (2.4.1) mutagenesis tool. To equilibrate the solvent, a 5 ns pressure coupled equilibration with Monte Carlo barostat47 was performed at a pressure of 1 atm, which was followed by a 10 ns free equilibration without constraints. The equilibration steps were repeated for each simulation replicate to start the 70 ns production simulation with a variety of peptide starting positions.
Simulation of peptide association to SETD2
The structure of human SETD2 was retrieved from the Protein Data Base (PDB: 6VDB, all residue numbers in this work refer to this entry) and missing amino acids were modelled using PDBFixer48. The complexed peptide was deleted from the structure, and the centroid structures from the clustering of peptide conformations in solution, as described in the chapter Simulation Analysis, were placed 30 Å away from the binding cleft (distance between SAM methyl group and sidechain nitrogen of the peptide lysine 36). The target lysine was manually deprotonated as required for the SN2 mechanism7. The pKa values of SETD2 protein were calculated at pH 7 using PROPKA49,50 provided by the PDB2PQR server (version 2.0.0)51. The pKa values of peptide were assigned according to the AMBER ff14SB force field52. The Zn2+ ions were modelled using the cationic dummy atom method53,54,55. The cysteines 1499, 1501, 1516, 1520, 1529, 1533, 1539, 1631, 1678, 1680, 1685 were treated as unprotonated to ensure proper Zn2+ binding56. The protein charge was neutralised by adding 7 Cl− ions.
To model SETD2 in an open position, the post-SET loop (Q1691-K1703) was manually lifted upwards using PyMOL (2.4.1)57 based on the results described in Yang et al. 201615. In this conformation, the peptide binding cleft is no longer blocked by the post-SET loop and the autoinhibitory residue R1670 points outwards. The post-SET loop was not constrained in the open conformation. Simulations of the apoenzyme indicated that the loop falls back at timescales >500 ns without peptide, which did not interfere with the sMD experiments, which were conducted over 50 ns. However, in the sMD simulation replicates, contacts of the post-SET loop with the docked peptide were also observed to occur at shorter timescales.
The open position of SETD2 was then used for the sMD simulations23 (H3K36: total number of atoms 89,040, the volume of box 571,658 Å3; ssK36: total number of atoms 98,080, the volume of box 674,494 Å3). To equilibrate the solvent, a 5 ns pressure coupled equilibration with Monte Carlo barostat was performed at a pressure of 1 atm. The C-alpha (Cα) atoms of SETD2, the peptide and the SAM atoms were restrained with a force of 100, 100 and 5 kJ/mole × Å2, respectively. The restraints were taken off successively, starting with the SETD2 Cα restraints, followed by a 5 ns equilibration with the peptide and SAM still being restrained. Subsequently, the SAM and peptide restraints were removed as well, followed by 0.1 ns equilibration with no restraints. A distant dependent force of 0.5 × distance of centroid 1 (K37 atoms NZ, HZ1, HZ2) and centroid 2 (SAM atoms SD, CE, H10) (kJ/mol)/Å2) was used to pull the centre of mass (COM) of the lysine 36 sidechain nitrogen and its attached two hydrogen atoms, towards the COM of the SAM methyl group and its attached three hydrogen atoms. The sMD simulation was run for 100 replicates à 50 ns (total simulation time 5 µs).
To discriminate between the different conformational preferences of the peptides in the sMD experiment, an additional, distance-dependent repulsive force of −0.3 × distance centroid 1 (A29 atoms N, CA, C) and centroid 2 (P43 atoms CG, CD, OXT) (kJ/mol)/Å2) was added to the system. This repulsive force decreased with the distance of A29 and P43, and it pushed the peptide ends apart if they got in close proximity, thereby preventing the formation of a hairpin conformation.
MD simulation of SETD2-peptide complex conformations
The starting structures were retrieved from the Protein Data Base, PDB: 5V21 for SETD2 with the H3K36 peptide, PDB: 6VDB for SETD2 with the ssK36 peptide. Missing amino acids, M to K mutations, preparation of SAM and the Zn2+ ions was carried out as described in the previous section (H3K36: total number of atoms 70,956, the volume of the box 461,784 Å3; ssK36: total number of atoms 70,292, the volume of the box 440,548Å3). A 5 ns pressure coupled equilibration with Monte Carlo barostat was performed at a pressure of 1 atm. SETD2 and peptide C-alpha (Cα) atoms, as well as cofactor SAM atoms, were restrained with a force of 100 and 5 kJ/mole × Å2, respectively. The restraints were taken off successively, starting with the Cα restraints, followed by a 5 ns equilibration with only SAM restrained. Subsequently, the SAM restraints were removed as well, followed by 5 ns equilibration with no restraints. For production, 15 replicates à 100 ns were performed (total simulation time 1.5 µs).
Analysis of the MD simulation data
The data analysis was performed utilizing MDTraj (1.9.4)58, Enspara (0.1.1)21 and contact-map-explorer (0.7.1)59. The clustering of the peptide trajectories with Enspara was carried out using the k-hybrid algorithm based on backbone atom (Cα, C and N) root mean square deviation (RMSD). For the contact-map-explorer, a cut-off of 4.5 Å was used, and the next two neighbouring residues were ignored. A contact was counted if at least one heavy atom of a residue was in a 4.5 Å3 sphere of one heavy atom from another residue. All structures were visualized using PyMOL (2.4.1)57.
SETD2 cloning, expression and purification
The His6-tagged expression construct of SETD2 catalytic SET domain (amino acids 1347–1711, UniProt No: Q9BYW2) was expressed and purified as described previously19,60. In short, the plasmid encoding the His-tagged SETD2 SET domain was transformed into BL21 (DE3) Codon Plus cells and protein expression was induced by 0.2 mM IPTG at 17 °C for 16 h. Protein purification was done by affinity chromatography using Ni-NTA affinity agarose resin (Genaxxon bioscience). After washing the beads, the purified protein was eluted in elution buffer (220 mM imidazole, 30 mM KPI, 500 mM KCl, 0.2 mM DTT, 10% glycerol). Fractions containing SETD2 were pooled and dialysed in dialysis buffer (20 mM HEPES pH 7.2, 200 mM KCl, 0.2 mM DTT, 1 mM EDTA, 10% glycerol) for 3 h at 8 °C. Finally, the protein was aliquoted and flash frozen in liquid nitrogen and stored at – 80 °C. The purity of the protein preparation was analysed by sodium dodecyl sulfate–polyacrylamide gel electrophoresis (SDS-PAGE) using 16% gel stained with colloidal Coomassie brilliant blue (Supplementary Fig. 4A).
FRET analysis of peptide conformations and SETD2 binding kinetics
For the FRET experiments, the Jasco FP-8300 spectrofluorometer was used. The excitation was set to 340 nm, and the emission was measured at 490 nm. The excitation and emission bandwidths were 5 and 10 nm, respectively. Samples were stirred at 600 rpm. The peptides (Table 1) were obtained from JPT Peptide Technologies GmbH and dissolved in DMSO stock solutions at 5 mM. For the experiments, the peptides were diluted in 20 mM HEPES pH 7.2, 200 mM KCl, 1 mM EDTA and 10% glycerol to a final concentration of 10 µM. For control experiments, the peptides were diluted in 20 mM HEPES pH 7.2, 200 mM KCl and 10% glycerol to a concentration of 11 µM and 1/10 of the volume of a Proteinase K solution (100 µg/ml, dissolved in 20 mM HEPES pH 7, 100 mM NaCl and 10 mM MgCl2) was added and the mixture incubated for 1 h at 37 °C. The SETD2 binding kinetics were performed using 1 µM peptide dissolved in 20 mM HEPES pH 7.2, 200 mM KCl, 1 mM EDTA and 10% glycerol supplemented with 2 µM of SETD2 catalytic SET domain. Most measurements were performed at 26 °C, but for the analysis of peptide conformations, a temperature gradient from 5 to 95 °C in 10 °C steps was applied.
Peptide array methylation assay
Methylation of peptide SPOT arrays is a powerful method to assess the specificity of PKMTs61. Peptide arrays containing fifteen amino-acid long peptides were synthesized using the SPOT synthesis method with an Autospot peptide array synthesizer (Intavis AG, Köln, Germany), basically as described19. Briefly, the SPOT array membranes were pre-incubated in Incubation buffer (20 mM Tris/HCl pH 9, 1.5 mM MgCl2) for 5 min on a shaker. Thereafter, the membranes were incubated in methylation buffer supplemented with radioactively labelled SAM (PerkinElmer) and 1 μM SETD2 enzyme for 60 min on a shaker. Afterwards, the membranes were washed five times for 5 min in wash buffer (100 mM NH4HCO3, 1% SDS) and incubated in amplified NAMP100V (GE Healthcare) for 5 min. This was followed by exposure of the membranes to a HyperfilmTM high-performance autoradiography film (GE Healthcare) at −80 °C in the dark. The films were developed with an Optimax Typ TR machine after different exposure times. For quantification, the signal intensities were measured with the ImageJ software and analysed with Microsoft Excel.
Statistics
t-tests were conducted with Excel using the specified settings. P-values based on binomial distributions were calculated with Excel using the Binom.dist function.
Reporting summary
Further information on research design is available in the Nature Research Reporting Summary linked to this article.
Data availability
All biochemical data generated or analysed during this study are included in the published article and its supplementary files. Source data underlying plots shown in the figures and Supplementary Movies 1–4 are provided on DaRUS (https://doi.org/10.18419/darus-2508). All other data or sources are available from the corresponding author on reasonable request.
Code availability
MD simulations codes and analysis scripts are provided on DaRUS (https://doi.org/10.18419/darus-2508).
References
Allis, C. D. & Jenuwein, T. The molecular hallmarks of epigenetic control. Nat. Rev. Genet. 17, 487–500 (2016).
Jambhekar, A., Dhall, A. & Shi, Y. Roles and regulation of histone methylation in animal development. Nat. Rev. Mol. Cell Biol. 20, 625–641 (2019).
Cornett, E. M., Ferry, L., Defossez, P. A. & Rothbart, S. B. Lysine methylation regulators moonlighting outside the epigenome. Mol. Cell 75, 1092–1101 (2019).
Bannister, A. J. & Kouzarides, T. Regulation of chromatin by histone modifications. Cell Res. 21, 381–395 (2011).
Boriack-Sjodin, P. A. & Swinger, K. K. Protein methyltransferases: a distinct, diverse, and dynamic family of enzymes. Biochemistry 55, 1557–1569 (2016).
Qian, C. & Zhou, M. M. SET domain protein lysine methyltransferases: structure, specificity and catalysis. Cell Mol. Life Sci. 63, 2755–2763 (2006).
Zhang, X. & Bruice, T. C. Enzymatic mechanism and product specificity of SET-domain protein lysine methyltransferases. Proc. Natl Acad. Sci. USA 105, 5728–5732 (2008).
Chen, S. et al. The dynamic conformational landscape of the protein methyltransferase SETD8. Elife 8, e45403 (2019).
Sun, X. J. et al. Identification and characterization of a novel human histone H3 lysine 36-specific methyltransferase. J. Biol. Chem. 280, 35261–35271 (2005).
Edmunds, J. W., Mahadevan, L. C. & Clayton, A. L. Dynamic histone H3 methylation during gene induction: HYPB/Setd2 mediates all H3K36 trimethylation. EMBO J. 27, 406–420 (2008).
Eram, M. S. et al. Kinetic characterization of human histone H3 lysine 36 methyltransferases, ASH1L and SETD2. Biochim. Biophys. Acta 1850, 1842–1848 (2015).
Fang, D. et al. The histone H3.3K36M mutation reprograms the epigenome of chondroblastomas. Science 352, 1344–1348 (2016).
Lu, C. et al. Histone H3K36 mutations promote sarcomagenesis through altered histone methylation landscape. Science 352, 844–849 (2016).
Liu, Y. et al. Cryo-EM structure of SETD2/Set2 methyltransferase bound to a nucleosome containing oncohistone mutations. Cell Discov. 7, 32 (2021).
Kudithipudi, S. & Jeltsch, A. Role of somatic cancer mutations in human protein lysine methyltransferases. Biochim. Biophys. Acta 1846, 366–379 (2014).
Baubec, T. et al. Genomic profiling of DNA methyltransferases reveals a role for DNMT3B in genic methylation. Nature 520, 243–247 (2015).
Yang, S. et al. Molecular basis for oncohistone H3 recognition by SETD2 methyltransferase. Genes Dev. 30, 1611–1616 (2016).
Zhang, Y. et al. Molecular basis for the role of oncogenic histone mutations in modulating H3K36 methylation. Sci. Rep. 7, 43906 (2017).
Schuhmacher, M. K. et al. Sequence specificity analysis of the SETD2 protein lysine methyltransferase and discovery of a SETD2 super-substrate. Commun. Biol. 3, 511 (2020).
Huang, C. & Zhu, B. Roles of H3K36-specific histone methyltransferases in transcription: antagonizing silencing and safeguarding transcription fidelity. Biophys. Rep. 4, 170–177 (2018).
Porter, J. R., Zimmerman, M. I. & Bowman, G. R. Enspara: modeling molecular ensembles with scalable data structures and parallel computing. J. Chem. Phys. 150, 044108 (2019).
Arkin, M.R., Glicksman, M.A., Fu, H., Havel, J.J. & Du, Y. Inhibition of protein-protein interactions: non-cellular assay formats. In Assay Guidance Manual. (Eli Lilly & Company and the National Center for Advancing Translational Sciences, Bethesda, Maryland, 2004)
Yang, T. et al. Formation mechanism of ion channel in channelrhodopsin-2: molecular dynamics simulation and steering molecular dynamics simulations. Int. J. Mol. Sci. 20, 3780 (2019).
Zheng, W. et al. Sinefungin derivatives as inhibitors and structure probes of protein lysine methyltransferase SETD2. J. Am. Chem. Soc. 134, 18004–18014 (2012).
Del Rizzo, P. A. & Trievel, R. C. Molecular basis for substrate recognition by lysine methyltransferases and demethylases. Biochim. Biophys. Acta 1839, 1404–1415 (2014).
Chu, Y. & Guo, H. QM/MM MD and free energy simulation study of methyl transfer processes catalyzed by PKMTs and PRMTs. Interdiscip. Sci. 7, 309–318 (2015).
Brini, E., Simmerling, C. & Dill, K. Protein storytelling through physics. Science 370, eaaz3041 (2020).
Guo, H. B. & Guo, H. Mechanism of histone methylation catalyzed by protein lysine methyltransferase SET7/9 and origin of product specificity. Proc. Natl Acad. Sci. USA 104, 8797–8802 (2007).
Zhang, X. & Bruice, T. C. Catalytic mechanism and product specificity of rubisco large subunit methyltransferase: QM/MM and MD investigations. Biochemistry 46, 5505–5514 (2007).
Hu, P., Wang, S. & Zhang, Y. How do SET-domain protein lysine methyltransferases achieve the methylation state specificity? Revisited by Ab initio QM/MM molecular dynamics simulations. J. Am. Chem. Soc. 130, 3806–3813 (2008).
Xu, Q., Chu, Y. Z., Guo, H. B., Smith, J. C. & Guo, H. Energy triplets for writing epigenetic marks: insights from QM/MM free-energy simulations of protein lysine methyltransferases. Chemistry 15, 12596–12599 (2009).
Chu, Y., Yao, J. & Guo, H. QM/MM MD and free energy simulations of G9a-like protein (GLP) and its mutants: understanding the factors that determine the product specificity. PLoS ONE 7, e37674 (2012).
Yu, W. et al. Catalytic site remodelling of the DOT1L methyltransferase by selective inhibitors. Nat. Commun. 3, 1288 (2012).
Sun, J., Li, Z. & Yang, N. Mechanism of the conformational change of the protein methyltransferase SMYD3: a molecular dynamics simulation study. Int. J. Mol. Sci. 22, 7185 (2021).
Chen, S. et al. Substrate-differentiated transition states of SET7/9-catalyzed lysine methylation. J. Am. Chem. Soc. 141, 8064–8067 (2019).
Dhayalan, A., Kudithipudi, S., Rathert, P. & Jeltsch, A. Specificity analysis-based identification of new methylation targets of the SET7/9 protein lysine methyltransferase. Chem. Biol. 18, 111–120 (2011).
Eastman, P. P., Vijay S. OpenMM: a hardware independent framework for molecular simulations. Comput. Sci. Eng. 4, 34–39 (2010).
Eastman, P. et al. OpenMM 7: Rapid development of high performance algorithms for molecular dynamics. PLoS Comput. Biol. 13, e1005659 (2017).
Nvidia. Cuda Toolkit Documentation. Comp. A J. Comp. Educ. (2010). https://docs.nvidia.com/cuda/.
Copeland, R. A., Solomon, M. E. & Richon, V. M. Protein methyltransferases as a target class for drug discovery. Nat. Rev. Drug Discov. 8, 724–732 (2009).
Wang, J., Wolf, R. M., Caldwell, J. W., Kollman, P. A. & Case, D. A. Development and testing of a general amber force field. J. Comput. Chem. 25, 18 (2004).
Case, D. A. et al. AMBER 14. (University of California, San Francisco, 2014).
Wang, J., Wang, W., Kollman, P. A. & Case, D. A. Antechamber, an accessory software package for molecular mechanical calculations. J. Chem. Inf. Computer Sci. 222, 41 (2001).
Darden, T., York, D. & Pedersen, L. An N ⋅log(N) method for Ewald sums in large systems. J. Chem. Phys. 98, 4 (1993).
Bussi, G. & Parrinello, M. Accurate sampling using Langevin dynamics. Phys. Rev. E Stat. Nonlin Soft Matter Phys. 75, 056707 (2007).
Horn, H. W. et al. Development of an improved four-site water model for biomolecular simulations: TIP4P-Ew. J. Chem. Phys. 120, 9665–9678 (2004).
Faller, R. & de Pablo, J. J. Constant pressure hybrid Molecular Dynamics–Monte Carlo simulations. J. Chem. Phys. 116, 55–59 (2002).
Eastman, P. et al. OpenMM 4: a reusable, extensible, hardware independent library for high performance molecular simulation. J. Chem. Theory Comput. 9, 9 (2013).
Olsson, M. H. M., Søndergaard, C. R., Rostkowski, M. & Jensen, J. H. PROPKA3: consistent treatment of internal and surface residues in empirical pKa predictions. J. Chem. Theory Comput. 2, 13 (2011).
Sondergaard, C. R., Olsson, M. H., Rostkowski, M. & Jensen, J. H. Improved treatment of ligands and coupling effects in empirical calculation and rationalization of pKa values. J. Chem. Theory Comput. 7, 2284–2295 (2011).
Dolinsky, T. J., Nielsen, J. E., McCammon, J. A. & Baker, N. A. PDB2PQR: an automated pipeline for the setup of Poisson-Boltzmann electrostatics calculations. Nucleic Acids Res. 32, W665–W667 (2004).
Maier, J. A. et al. ff14SB: improving the accuracy of protein side chain and backbone parameters from ff99SB. J. Chem. Theory Comput. 11, 3696–3713 (2015).
Pang, Y. P., Xu, K., el Yazal, J. & Prendergast, F. G. Successful molecular dynamics simulation of the zinc-bound farnesyltransferase using the cationic dummy atom approach. Protein Sci. 9, 9 (2000).
Pang, Y.-P. Successful molecular dynamics simulation of two zinc complexes bridged by a hydroxide in phosphotriesterase using the cationic dummy atom method. Proteins 45, 7 (2001).
Oelschlaeger, P. S. & Rolf, D. Pleiss, Juergen. Modeling domino effects in enzymes: molecular basis of the substrate specificity of the bacterial metallo-beta-lactamases IMP-1 and IMP-6. Biochemistry 30, 12 (2003).
Cheng, X. & Zhang, X. Structural dynamics of protein lysine methylation and demethylation. Mutat. Res. 618, 102–115 (2007).
Schrödinger, L. L. C. The PyMOL Molecular Graphics System. Version: 2.4.1 (2015).
McGibbon, R. T. et al. MDTraj: a modern open library for the analysis of molecular dynamics trajectories. Biophys. J. 109, 1528–1532 (2015).
Swenson, D. E. H. & Roet, S. Contact Map Explorer. https://github.com/dwhswenson/contact_map. https://contact-map.readthedocs.io/en/latest/index.html. (2017).
Schuhmacher, M., Kusevic, D., Kudithipudi, S. & Jeltsch, A. Kinetic analysis of the inhibition of the NSD1, NSD2 and SETD2 protein lysine methyltransferases by a K36M oncohistone peptide. Chemistryselect 2, 9532–9536 (2017).
Bock, I. et al. Application of Celluspots peptide arrays for the analysis of the binding specificity of epigenetic reading domains to modified histone tails. BMC Biochem. 12, 48 (2011).
Acknowledgements
This work has been supported by the Deutsche Forschungsgemeinschaft under Germany’s Excellence Strategy EXC 2075 390740016 in PN2-5. M.S.K. was supported by the GERLS scholarship program funding program number 57311832 by the German Academic Exchange Service (DAAD) and the Egyptian Ministry of Higher Education.
Funding
Open Access funding enabled and organized by Projekt DEAL.
Author information
Authors and Affiliations
Contributions
P.S. conducted all experiments with help by M.C., S.W., M.S.K. and H.C. J.P. and A.J. supervised the work. P.S. and A.J. prepared the manuscript and figures. J.P. contributed to writing of the manuscript. All authors were involved in data analysis and interpretation and all authors approved the final version of the manuscript.
Corresponding authors
Ethics declarations
Competing interests
The authors declare no competing interests.
Peer review
Peer review information
Communications Chemistry thanks the anonymous reviewers for their contribution to the peer review of this work. Peer reviewer reports are available.
Additional information
Publisher’s note Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Supplementary information
Rights and permissions
Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.
About this article
Cite this article
Schnee, P., Choudalakis, M., Weirich, S. et al. Mechanistic basis of the increased methylation activity of the SETD2 protein lysine methyltransferase towards a designed super-substrate peptide. Commun Chem 5, 139 (2022). https://doi.org/10.1038/s42004-022-00753-w
Received:
Accepted:
Published:
DOI: https://doi.org/10.1038/s42004-022-00753-w
This article is cited by
-
Discovery of NSD2 non-histone substrates and design of a super-substrate
Communications Biology (2024)
-
Charakterisierung der Substratspezifität von Protein-Methyltransferasen
BIOspektrum (2023)
Comments
By submitting a comment you agree to abide by our Terms and Community Guidelines. If you find something abusive or that does not comply with our terms or guidelines please flag it as inappropriate.