Solution of multiple open and substrate-bound closed structures by cryo-EM
Advances in cryo electron microscopy (cryoEM) allow the structural determination of conformational states recalcitrant to the crystallography23–26, thus we used cryoEM to examine the conformational states of PreP in the absence of substrate (apo-PreP). We first used differential scanning fluorimetry (DSF) to optimize the unfolding entropy and unfolding and dissociation enthalpy of human PreP (Extended data Fig. 2)27. Apo-PreP grids were then prepared by Vitrobot and a dataset of 2,626 micrographs collected at a 300 kV on a Titan Krios at various ice thicknesses to overcome orientation bias and/or denaturation by exposure to the air-water interface (Table 1, Extended Fig. 3,4). Apo-PreP grids were then prepared by Vitrobot and a dataset of 2,626 micrographs collected at 300 kV on a Titan Krios. During processing, we observed that the predominant classes contained particles only half the expected size of PreP (Fig. 1A, Extended data Fig. 3). Following 3D classification of 411,000 particles, four classes were obtained (Extended data Fig. 3). The two major classes, comprising ~ 208,000 and ~ 118,000 particles, displayed an intact PreP-N domain but a denatured PreP-C domain and were refined to 4.2 Å (Fig. 1B, Extended data Fig. 4,5). The third class, comprised of 50,000 particles and refined to 4.5 Å, was found to contain full-length PreP adopting a partial open conformation that we designate pO (Fig. 1B, Extended data Fig. 3). The final class, of ~ 34,000 particles, was comprised of nearly full-length PreP particles adopting an open conformation was refined to 5.3 Å (Extended data Fig. 3).
It has previously been demonstrated that the vast majority of particles derived from diverse proteins or protein complexes (90%) are adsorbed to the air-water interface28. Extensive studies have shown that many proteins are denatured rapidly upon exposure to the air-water interface29. Therefore, we hypothesized that the extensive denaturation of the PreP-C domain described above resulted from denaturation at the air-water interface. To explore this possibility, we used fiducial-less cryo electron tomography (cryoET) to examine the distribution of PreP particles within the vitrified ice. This analysis of the Vitrobot prepared grids revealed that nearly all PreP particles were adsorbed to the air-water interface (Fig. 1C, Extended data Fig. 6, Movie 1). Approximately ~ 88% of particles had half of the anticipated size in our cryoET analysis, consistent with that a majority of 3D classes (80%) having a denatured PreP-C domain (Fig. 1C, Extended data Fig. 6A). Interestingly, while PreP-N and PreP-C share a highly similar structure, PreP-N has an additional β-hairpin (Extended data Fig. 6B). This β-hairpin extends from an α-helix that binds the catalytic zinc ion and interacts with the α-helical hairpin that links PreP-N and PreP-C. This unique structure likely makes PreP-N more stable than PreP-C (Extended data Fig. 6B). Together, our data indicate that PreP-C preferentially denatured during the vitrification process, either by the repetitive exposure to air-water interface and/or shear force caused by filter blotting (Extended data Fig. 6C)30.
We hypothesized that if the amount of time the sample spent on the grid prior to vitrification (dwell time) could be significantly reduced, PreP denaturation would likewise be reduced. Spotiton, a novel method of vitrifying samples using a piezo electric dispensing head to deliver sample droplets onto a self-blotting nanowire grid, has been shown to significantly reduce the dwell time of particles at the air-water interface prior to vitrification30–33. We employed this technique to prepare grids using a 133 millisecond dwell time (compared to 1–2 seconds for Vitrobot) by chameleon34, a commercial version of Spotiton developed by SPT Labtech via the National Center for CryoEM Access and Training (NCCAT) general user program 2. An apo-PreP dataset of 3,012 micrographs was processed to yield about 363,000 particles from well-defined 3D classes from these grids. Following 2D and 3D classification, all classes were found to contain full-length PreP particles, and no denaturation was observed (Fig. 1D, 1E, Table 1, Extended data Fig. 7,8). 3D classification of PreP particles revealed three distinct open state structures of PreP. They were refined to an open state (O) and two partially open states (pO1 and pO2) with resolution of 4 Å, 3.7 Å, 3.9 Å, respectively. Structural models of these three states were then built and refined (Table 1, Extended data Fig. 5B-D, 8, Movie 2). Two substrate-bound PreP cryoEM structures were also determined. We also optimized PreP in the presence of a five-fold molar excess of Aβ 1–40 by DSF. Grids were prepared by chameleon, and a dataset of 3,483 micrographs was processed to yield about 175,000 particles from a well-defined 3D class that was refined to a partially closed (pC) state of PreP at 3.3 Å resolution (Fig. 1F, Table 1; Extended data Fig. 5E,9,11). A similar approach was used to obtain a Coulomb potential map for PreP in complex with a model presequence peptide from human citrate synthase (27 aa long, CS27)35, resulting in a pC state PreP at 4.6 Å resolution (Fig. 1G, Table 1; Extended data Fig. 10,11). Structural models of these substrate-bound PreP were then built and refined (Table 1, Extended data Fig. 5E,11, Movie 3). We define the substrate-bound PreP cryoEM structures as pC state to differentiate from the closed (C) state crystal structures of PreP that were solved in the presence or absence of Ab6.
Structural analysis of apo- and substrate-bound PreP reveal key states in PreP catalytic cycle and the molecular basis for substrate recognition
Comparison of the five cryoEM structures derived from the apo- and substrate-bound PreP reveals three key conformational states based on the degree of opening of the catalytic chamber: open (O), partially open (pO), and partially closed (pC). Apo-PreP has three states, O, pO1, and pO2 that are distinct from each other with the two pO states being slightly more open than the pC or C states (Fig. 2A, Extended data Fig. 12, Table S1). Aβ- and citrate synthase presequence (CS27)-bound PreP structures in the pC state are nearly identical to each other and are slightly more open than crystal structures of apo or Ab-bound PreP6 (Fig. 2A, Extended data Fig. 12, Table S1). Of these structures, the pO, pC, and C states of PreP have a small variation in the degree of opening, making their chamber inaccessible to substrate binding. Thus, only PreP open state has a large enough opening to capture its peptide substrates and release the proteolytic products.
Two major differences exist between these structures. The first is mediated by the rigid body displacement between PreP-N and PreP-C domains, whereby the two halves of this chamber-containing protease open up, similar to a clamshell (Fig. 2A-C, Extended data Fig. 12, Movie 4, Table 1). The displacement results in a difference in the distance, angle, and contacts between these domains. Most noticeably, both the distance and angle between PreP-N and PreP-C in PreP open state is substantially larger than the rest of states while the buried surface between PreP-N and PreP-C is much reduced compared to the others. The displacement between PreP-N and PreP-C is most likely driven by the entropically favorable rigid body motion. We also observed major conformational rearrangements in two additional regions, switch A (aa 174–225) and switch C (aa 506–550) (Fig. 2A-C; Extended data Fig. 12, Movie 4). Switch A contains two α-helices that have residues for the binding of substrate and catalytic zinc ion (Fig. 2A). The helix-turn-helix motif of the switch C region joins PreP-N and PreP-C and makes extensive contacts with an extended β-hairpin within the long a-helix of the switch A region, allowing the switch A and C region move jointly with the displacement between PreP-N and PreP-C (Fig. 2A).
3D classification revealed that the majority of PreP particles (~ 74%) were in the partially open pO states, indicating that PreP in the absence of substrate prefers to be in a state inaccessible to substrate binding. We then used size exclusion chromatography (SEC) in-line with small angle X-ray scattering (SAXS) to further assess how the distribution of PreP conformational states in solution is influenced by the presence of Aβ and presequence from citrate synthase (CS27) under physiological buffer conditions (Fig. 2D, Extended data Fig. 13, Table 2). SAXS is a highly effective technique to eliminate structural models that do not produce calculated scattering patterns that fit the experimental scattering profile36. SEC-SAXS also reduces large aggregates that contaminated our previously reported SAXS profile of PreP6. Consistent with the cryoEM data, the SEC-SAXS data confirms that PreP alone in solution is also preferred in a pO state (~ 63%), instead of the open state (~ 37%) (Extended data Table 2). The fact that PreP in solution prefers the pO state rather than the open state is logical because the transition from the pO states to O state loses substantial buried surface (650–940 Å2) and a network of hydrogen bonds and salt bridges, and thus is energetically unfavorable (Extended data Table S1). The presence of CS27 significantly reduced the Rg value from 31.5 Å to 30.8 Å, leading PreP to be mostly in the closed state (~ 82%) (Extended data Table 2). However, the presence of Aβ only slightly reduced the Rg and Dmax values. This is consistent with that only a subtle conformational switch occurs between pO and pC states (Fig. 2D, Extended data Fig. 13, Table 1), whereby substrate-binding promotes domain closure.
Together, our data leads to the hypothesis that PreP undergoes the following conformational switch during the catalytic cycle (Fig. 2E): PreP is predominantly in the partial open state at the resting condition. The transition from the pO states to O state allows the capture of substrate, and thus is a key state in the catalytic cycle. Upon opening, peptides that are rich in positively charged residues are attracted to the negatively charged, catalytic chamber of PreP-N which can further select for its substrates based on their size and conformational compatibility within the chamber (Fig. 2F)6. The catalytic site of PreP undergoes minimal conformational change, and thus is poised to carry out proteolysis (Fig. 2G). After proteolysis, the closed to open transition allows the release of proteolytic products to initiate the next catalytic cycle.
Mechanism for the conformational switches between PreP open and closed states in the presence and absence of substrates
The comparison of PreP cryoEM structures reveals the molecular basis for the equilibrium between partially open and open state in the absence of substrate. PreP has three regions that undergo substantial conformational switches, defined as switch A, B, and C (Fig. 3A). As discussed above, switch A and C move together with rigid body displacement between PreP-N and PreP-C (Fig. 2A, 3A). The switch A and C regions in the pO states have lower resolution and higher thermal B factors than the rest of PreP structures (Fig. 3B). In comparison, the resolution and thermal B factors of these regions in the open and substrate-bound states are not profoundly different from the rest of protein (Fig. 3B). Together, this is indicative of high conformational dynamics within these regions. As switch A contains residues involved in substrate peptide binding and catalytic zinc ion coordination, such high dynamic would render pO state catalytically incompetent. The presence of substrate stabilizes switch A, and thus, the residues for substrate binding and catalysis, allowing the catalytic reaction. This suggests that PreP uses the substrate-assisted catalysis as a mechanism for the substrate selection. This is because amyloid peptides have the high propensity to unfold and form a b-strand, which can then form the cross-b-sheet with other amyloid peptides. The catalytic cleft of PreP selectively binds the b-strand of substrate peptide after such peptide is unfolded inside the catalytic chamber. Only peptides that tend to unfold and form the b-strand can stabilize PreP’s catalytic cleft, leading to catalysis.
PreP switch B (aa 421–436, within PreP-N) represents a rotation of an α-helix when the PreP open state is compared with the rest of conformational states (pO, pC, or C) (Fig. 3C,3D; Extended data Movie 5). The rotation of switch B is particularly noticeable at residue M436, which rotates ~ 60o to transit through the hydrophobic pocket formed by Y450 and L467 (Fig. 3C,3D). This allows a rigid body rotation of PreP-C in relationship to PreP-N (Fig. 2E, 3E). Such a rotation maintains the interactions between switch B and PreP-C, e.g., the contacts of E432 with R675 and that of H430 with N676 and the main chains of aa residues 642 and 643. Thus, there should be minimal energetic barrier for such rotation to allow the rapid shift between PreP partially open and open states driven by the entropically favorable rigid body motion between PreP-N and PreP-C.
The rotation of switch B also offers the molecular basis for PreP’s substrate-induced conformational switch and substrate selectivity. Switch B has hydrophobic residues L428 and I432 that, together with the surrounding residues, form a substrate binding exosite distal to the catalytic zinc ion (~ 28–33Å away) (Fig. 3F, Extended data Movie 5). This exosite is highly hydrophobic and is shown to bind Aβ residues that are away from the preferred cleavage sites of Aβ (aa 19/20 or aa 20/21) (Fig. 3F)6. The interaction of the exosite with the hydrophobic residues of substrate would favor the closed state and thus promote the open to closed transition (Fig. 3E). Furthermore, this in part explains why PreP prefers to degrade peptide substrates that are rich in hydrophobic residues, e.g., presequences and Aβ.
Our structural analysis predicts the conformational dynamics of switch A and C and substrate-induced stabilization of three switch regions. To test this, we utilized peptide amide hydrogen deuterium exchange (HDX) mass spectrometry, which is a powerful tool to probe protein conformational dynamics because it allows evaluation of comparative solvent accessibility throughout the protein36–41. As expected, a reduced HDX was observed in segments in both PreP-N and PreP-C that are involved in the substrate binding (e.g., aa 91–141, aa 703–720, aa 892–903, and aa 931–940). We also observed reduced HDX of both switch A and C regions and, to a lesser degree, switch B when two different PreP substrates, Aβ and citrate synthase presequence (CS27) were present, which confirmed our prediction (Fig. 3G, Extended data Fig. 14–16). To probe how the interface between PreP-N and PreP-C controls the equilibrium between the pO and O states, we carried out structure-guided mutagenesis in this region at positions predicted to weaken the interaction between PreP-N and PreP-C. We found that two point mutations, D367A and Q637A modestly increased the catalytic activity of PreP (Fig. 3H). Thus, destabilization of this interface enhances, rather than diminishes, PreP’s enzymatic activity, presumably through increasing the ease with which PreP can transition through the key conformational states of its catalytic cycle.