The SiRHP-SiRFP interaction is highly sensitive to cryogenic TEM (cryo-EM) preparation
We determined the structure of the SiRFP/SiRHP dimer from three modified, minimal dimers, each of which is named by the change to SiRFP and its resulting molecular weight (Table S1). First, we truncated SiRFP to remove the N-terminal Fld domain (SiRFP-43/SiRHP). This is an inactive dimer, as the Fld domain is required for electron transfer. Nevertheless, the two subunits bind tightly and is the most simplified complex between SiRFP and SiRHP19. Second, we truncated both SiRFP’s N-terminal octamerization domain as well as the linker between the Fld and FNR domains to create a monomeric SiRFP that can be locked in an open position (SiRFP-60D/SiRHP)20. Third, we generated a variant of monomeric SiRFP-60 lacking reactive cysteines into which we engineered a disulfide bond between the Fld and FNR domains (SiRFP-60X/SiRHP)21.
Each variant is highly sensitive to traditional blotting plunge-freezing methods for cryo-EM preservation. To overcome this sensitivity, we combined the protection of a high critical micelle concentration, fluorinated lipid, fos-choline-8 (FF8, Creative Biolabs, Shirley, NY, USA )22, with the blot-free, rapid plunging afforded by the chameleon system (SPT Labtech, Melbourn, UK)23. This cryo-EM sample preparation helped us to retain each intact complex within near ideal ice thickness and avoid denaturation at the air water interface (Fig. S1). The smallest complex (SiRFP-43/SiRHP) showed well-aligned 2D class averages, however the 3D structure revealed structural anisotropy, either due to its small size/asymmetric geometry or from a preferred orientation, that limited high-resolution analysis despite the absence of mobile elements (Figs. S1A and S2). SiRFP-60D/SiRHP showed moderate-resolution density (3.54 Å) for the SiRFP FNR domain and SiRHP, however the N-terminal Fld domain was not visible (Figs. S1B and S3A). The 2.84 Å-resolution structure of SiRFP-60X/SiRHP revealed the most detail for SiRFP’s Fld and FNR domains, despite a lack of density for the linker between SiRFP’s domains in the highest-resolution reconstruction (Figs. 1A, S1C, and S3B). High resolution features for each of the cofactors in both subunits supported this reported resolution (Fig. S4). Therefore, we analyzed the SiRFP-SiRHP interface for this construct in detail.
SiRFP-SiRHP binding
The SiR dodecameric holoenzyme is composed of oligomers of the dimers discussed here and is about 800 kDa in mass. Despite this large mass, the binding interface between the minimal SiRFP/SiRHP dimer is small, reaching the surface area of 1,138 Å2 relative to the overall surface of 43,610 Å2. SiRHP alone has a solvent-exposed surface of 25,680 Å2. SiRFP-60X alone has a solvent-exposed surface of 21,930 Å2. That is, for a large complex only about 2.6% of the solvent-exposed surface is buried upon subunit binding. This is consistent with hydrogen-deuterium exchange data on the complex that reveals single, short peptides from each subunit that become occluded upon binding3, the sequences of which predicted the interface would be dominated by hydrophobic interactions (Fig. 1B).
The interface is governed by the N-terminus of SiRHP. The structure of this region is previously uncharacterized as it is proteolytically removed in the X-ray crystal structure of E. coli SiRHP24. These 80 amino acids follow the topology helix 1 - loop - helix 2 - turn - helix 3 - b-strand 1 - helix 4 - loop - b-strand 2 (Fig. 1C). Only amino acids from the turn, helix 4, and surrounding loops directly interact with SiRFP. The regions that are N-terminal to the interface interact with domain 1 or the N-terminal half of the parachute domain (i.e. the first sulfite or nitrite reductase repeat (S/NiRR)24,25), breaking SiRHP’s pseudo two-fold symmetry (Figs. 1A and S5A). An extension to the parachute domain that is not ordered in the original crystal structure, from amino acids 184–209, helps to hold the N-terminus in place (Fig. S5A). Those that are N-terminal to the interface approach the distal active site, but do not contribute significantly to anion or siroheme binding as they are held back by interactions to SiRFP, discussed below. Moving N-terminally along the peptide, it then turns back to form the loop that binds a pocket in SiRFP before moving away from SiRFP. The N-terminal most amino acids reach all the way to the other side of SiRHP, interacting with the N-terminus of the a-helix (h11) that precedes the linker that joins the two S/NiRRs and mimics the siroheme binding site (Fig. S5B)24.
The central interaction that pegs the subunits together is a p-cation interaction between h-Lys27 from SiRHP (for simplicity, amino acids from SiRHP will be designated with the prefix “h-“) and f-His258 from SiRFP (similarly, amino acids from SiRFP will be designated with the prefix “f-“) (Figs. 1D and E). This interaction is buttressed by f-Phe496 and f-Val500, which have previously been shown essential for SiRFP-SiRHP binding13. Further hydrophobic and p-stacking interactions dominate the interface. For example, h-Leu40 inserts into a pocket in SiRFP formed between f-b-sheet 17 and f-a-helix 18, which includes f-Phe496. h-Ile65 Cg2 sits 3.3 Å from the plane of f-Arg250’s guanidinium group (Figs. 1D and F), which is rotated 90o from its position in free SiRFP20. h-Gln72Cg also packs into a pocket formed by the backbone atoms of f-Ile247, f-Thr248, and f-Gly249, pinned in place by the h-Ile65/f-Arg250 and h-Lys73/f-His258 interactions. Farther from the interface, there is another stacking interaction between the guanidinium group from h-Arg63 and the h-Phe437 aromatic ring that stabilized the deformed helix that includes h-Ile65 (Figs. 1D and G). h-Phe437 is adjacent, through h-A443, to SiRHP’s iron-sulfur cluster. In this way, the binding interface between SiRFP and SiRHP reaches to the SiRHP active site through a network of hydrophobic interactions (Fig. S6).
Neither ionic interactions nor hydrogen bonds play a direct role in the interface, but rather stabilize the amino acids and structural elements that mediate the interface (Figs. 1C, D and S6). For example, a hydrogen bond network from f-Thr404Og through f-Tyr498OH and finally to f-His258Nd1 position its imidazole ring for the interaction with h-Lys73. An ionic interaction between h-Lys127Nz and h-Asp38Od2 reach across the loop, presenting h-Leu40 to project into SiRFP’s pocket. An additional ionic interaction between h-Asp61d1 and h-Arg66NHd also stabilize the deformed helix that contains h-Ile65 and turn it towards f-Arg250.
The SiRHP interaction with SiRFP differs from SIR interaction with ferredoxin
g-proteobacteria couple a diflavin reductase, SiRFP, to SiRHP. In contrast, other organisms like Zea mays and Mycobacteria tuberculosis use a ferredoxin (Fd) as their reductase partner15,17. In Z. mays SIR, Fd bridges SIR’s C-terminal domain 2 to a loop between the first two b-strands (amino acids Asp110 to Asn118), positioning the Fd iron-sulfur cluster near the SIR metal sites26. The interaction is bolstered by en face stacking between Fd Tyr37 and SIR Arg324 (Fig. 2A).
In SiRHP, the equivalent element between the structurally conserved b-strands 1 and 2 is considerably longer, stretching from h-Asp62 to h-Arg77 and containing a short helix from h-Arg63 to h-Glu71 (Fig. 2B). This loop contains the critical residues h-Gln72 and h-Lys73 that anchor the interaction with SiRFP’s FNR domain, which faces away from where Fd binds to the Z. mays homolog (Fig. 2C). Further, the arginine in SIR that stacks with Fd Tyr37 is not conserved in SiRHP – the equivalent position is h-Gly262, despite the structural conservation of the loop between b-strands 7 and 8 that contributes to siroheme binding (Fig. 2D).
The SiRHP active site loop is locked in its closed conformation
When bound to SiRFP, SiRHP’s anion binding loop (h-Asn149 to h-Arg153) is in its closed position, held in place by a long, through-space interaction between h-Arg53 and h-Asn149 (Fig. 3A). h-Arg53 is, in turn, held in place by stacking between its guanidinium group and h-Tyr58. The ring of h-Tyr58 subsequently sits over the methyl group on the siroheme pyrroline A ring. The only other new protein/siroheme interaction identified in this now complete structure of SiRHP is an ionic bond between h-Gln60 and the propionyl group from siroheme pyrroline ring B. The siroheme is saddle-shaped, as in free SiRHP and unlike in dissimilatory SIR27–30. h-Arg153 is flipped away from the bound phosphate. The other three anion binding amino acids, h-Arg83, h-Lys215, and h-Lys217, remain largely unchanged from free SiRHP (Figs. 3A-C)24.
This conformation differs from the various redox and anion-bound structures of free SiRHP24,31–33. In the phosphate-bound, free SiRHP structure that lacks the N-terminal 80 amino acid extension24, the loop is flipped open such that h-Ala146-h-Ala148 are disordered (Fig. 3B). Upon reduction and sulfite binding, h-Arg153 flips over to interact with the smaller anion and the loop becomes ordered32. h-Asn149 points away from the active site. In this way, SiRFP binding to SiRHP, with the ordering of SiRHP’s N-terminus, induces an intermediate structure with elements of both the oxidized, phosphate bound and the reduced, sulfite bound conformations (Fig. 3D).
In the original SiRHP X-ray crystal structure, the siroheme iron is significantly domed above the siroheme nitrogens, indicative of an oxidized Fe3+ (Fig. 3B)24. Subsequent chemical reduction experiments show the doming flattens upon conversion to Fe2+, commensurate with release of the phosphate to allow substrate binding (Fig. 3B)32. Contemporary X-ray diffraction experiments show that this reduction is beam-induced, but within the constraints of the crystal the phosphate remains bound to the siroheme iron in the active site33. In this cryo-EM structure, the siroheme iron appears to be in the plane of the siroheme nitrogens, suggesting that it has also been reduced by the electron beam. The central density for the phosphate is 3.5 Å from the siroheme iron and its pyramidal shape is rotated such that the oxygen-iron bond is broken (Figs. 3A and S4C).
SiRFP is highly mobile
Although the 2D class averages in all three datasets appeared to show little orientation preference with discernable features, further analysis revealed each to have unique properties related to the SiRFP variant used to generate the dimer (Table S1, Figs. S1-3).
SiRFP-43/SiRHP (107 kDa in mass): The 2D class averages for SiRFP-43/SiRHP appeared to show high-resolution features, however the initial 3D models were poorly aligned, likely due to a combination of small mass, preferred orientation, and limitations in grid preparation, so the refined volume did not achieve high resolution despite its simplified form. 3D variability analysis in CryoSPARC34 did not reveal significant conformational mobility, however orientation analysis and calculation of the 3DFSC35 showed the particles harbored a preferred orientation (Fig. S2). Nevertheless, the absence of SiRFP’s Fld domain did not alter the SiRFP-SiRHP interaction.
SiRFP-60D/SiRHP (123 kDa): As with SiRFP-43/SiRHP, this dimer showed 2D class averages with high-resolution features for the core of the dimer (Figs. S1B and S3A). Nevertheless, the initial models were of inconsistent structure, so we checked for heterogeneity using “3D variability” in CryoSPARC, which revealed a distinctive degree of movement in the Fld domain. To better understand the degree of flexibility for the Fld domain from the SiRFP-60D/SiRHP dimer, we performed both “3D flex” in CryoSPARC as well as “heterogenous refinement” in cryoDRGN36 with the particles from refinement on the main heterodimer body. This analysis, anchored on the SiRFP-FNR/SiRHP dimer, identified a dramatic movement of SiRFP’s Fld domain relative to the FNR domain, swinging 20o between the most compact and most open forms (Video S1 and Fig. 4A). The density for the linker joining the domains is not visible. In its most compact conformation, the Fld domain reaches the canonical “closed” conformation in which the Fld domain tucks into a cavity in the FNR domain (Fig. 4B). In the most open conformation, the Fld domain assumes a different position to that seen in the “open” conformation determined by X-ray crystallography of the same monomeric variant and the average solution envelope determined from SANS, intermediate between the fully opened and closed conformations (Fig. 4C)19,20.
SiRFP-60X/SiRHP (124 kDa): The Fld and FNR domains are covalently linked in this dimer, thus restricting the swinging domain motion of the Fld domain seen in the SiRFP-60D/SiRHP dimer. No preferred orientation was identified either in 2D or 3D analysis (Fig. S3B). Nevertheless, there is no density for the linker between the Fld and FNR domains in the highest-resolution reconstruction, which suggests that the 36 amino acid linker is exceptionally dynamic but allows SiRFP’s two domains to come into close contact to catch them in a crosslink. Locking the Fld and FNR domains in the closed conformation resulted in the most stable variant for high-resolution analysis (2.84 Å), discussed above.
With further classification of the SiRFP-60X/SiRHP structure, a sub-class of ~ 20,000 particles (10% of the particles used for highest resolution reconstruction for this dataset) emerged that revealed the linker between the two domains. The linker runs from the C-terminal end of the Fld domain (amino acid f-Ser207) to the N-terminal end of the FNR domain (amino acid f-Ile226) (Fig. 4D). There is neither defined secondary structure nor contact with either of the SiRFP domains, thus the linker is not constrained in a single conformation across the entire ensemble of particles even when the domains are crosslinked. The highly mobile nature of these 36 amino acids explains how the Fld domain can reposition for contact with the oxidase partner, SiRHP, presumably to mediate electron transfer.