Dynamin-related proteins (DRPs) are large multidomain GTPases required for diverse membrane-remodeling events. DRPs self-assemble into helical structures, but how these structures are tailored to their cellular targets remains unclear. We demonstrate that the fungal DRP Vps1 primarily localizes to and functions at the endosomal compartment. We present crystal structures of a Vps1 GTPase–bundle signaling element (BSE) fusion in different nucleotide states to capture GTP hydrolysis intermediates and concomitant conformational changes. Using cryoEM, we determined the structure of full-length GMPPCP-bound Vps1. The Vps1 helix is more open and flexible than that of dynamin. This is due to further opening of the BSEs away from the GTPase domains. A novel interface between adjacent GTPase domains forms in Vps1 instead of the contacts between the BSE and adjacent stalks and GTPase domains as seen in dynamin. Disruption of this interface abolishes Vps1 function in vivo. Hence, Vps1 exhibits a unique helical architecture, highlighting structural flexibilities of DRP self-assembly.
Dynamin-related proteins (DRPs) are large multidomain GTPases that play central roles in membrane fission and fusion events throughout the cell (Praefcke and McMahon, 2004; Hoppins et al., 2007; Ferguson and De Camilli, 2012). DRPs are vital for many cellular functions that depend on membrane remodeling including endocytosis, intracellular trafficking, mitochondrial dynamics, and energy homeostasis. Mutations in DRPs are associated with aging as well as several human diseases including neurodegeneration, optic atrophy, and Charcot Marie Tooth type 2A (Faelber et al., 2013).
All DRPs remodel membranes using a similar general mechanism: coordinated self-assembly coupled with GTP hydrolysis–dependent conformational changes (Chappie and Dyda, 2013; Antonny et al., 2016). The general mechanism of action of DRPs has been extensively studied for both fission DRPs such as dynamin and fusion DRPs such as Mfn1/Fzo1 as well as more distant members of the family including the bacterial dynamin-like proteins, Mx proteins, and atlastins (Low and Löwe, 2006; Low et al., 2009; Chappie et al., 2010, 2011; Bian et al., 2011; Byrnes and Sondermann, 2011; Faelber et al., 2011; Ford et al., 2011; Gao et al., 2011; Byrnes et al., 2013; Fröhlich et al., 2013; Reubold et al., 2015; Qi et al., 2016; Alvarez et al., 2017; Cao et al., 2017; Francy et al., 2017). Due to the functional versatility of DRPs and their ubiquity within cellular environments, considerable interest exists in understanding how specific DRPs are tailored for their particular functional niche and cellular targets.
Vps1 is a conserved fungal DRP that was originally identified in screens designed to capture mutants that are deficient in sorting of carboxypeptidase Y (CPY) to the vacuole (Rothman and Stevens, 1986; Vater et al., 1992). Δvps1 cells exhibit major defects in vacuolar dynamics and cargo transport to the vacuole (Raymond et al., 1992). Vps1 has been implicated in both vacuolar fusion and fission (Peters et al., 2004) as well as in regulation of peroxisome abundance and division, late endosome-to-vacuole trafficking, endocytosis, and retrograde trafficking from the endosomes and vacuoles (Kuravi et al., 2006; Smaczynska-de Rooij et al., 2010, 2012; Hayden et al., 2013; Chi et al., 2014; Arlt et al., 2015). Despite the clear importance of Vps1 for regulating fundamental yeast cellular processes, no structural analysis of Vps1 has been reported to date.
By sequence homology, Vps1 shares three structural domains with dynamin 1: a catalytic GTPase domain, a three-helix bundle termed the bundle signaling element (BSE), and an all-helical Stalk formed by three helices from the Middle domain and one from the GTPase Effector Domain (GED; Fig. 1; Chappie and Dyda, 2013). The BSE, formed by two helices that flank the GTPase and a helix from the C-terminal part of GED, is an intramolecular signaling module that transmits hydrolysis-dependent conformational changes from the GTPase domain to the rest of the molecule, while the Stalk mediates self-assembly and higher-order oligomerization (Gao et al., 2010, 2011; Faelber et al., 2011; Ford et al., 2011). Dynamin, uniquely, has a pleckstrin homology (PH) domain between its middle and GED as well as a C-terminal proline- and arginine-rich domain (PRD). The dynamin PH domain preferentially interacts with membranes containing phosphatidylinositol-(4,5)-bisphosphate and plays a critical function in membrane recruitment, regulation of self-assembly, and, by penetrating the membrane, fission (Achiriloaie et al., 1999; Ramachandran et al., 2009; Kenniston and Lemmon, 2010). The PRD contains numerous interaction motifs for multiple binding partners and is required for dynamin recruitment to its sites of action. Vps1 lacks both a PH and a PRD. These differences, therefore, necessitate alternative membrane recruitment mechanisms for Vps1. Vps1 and other non-dynamin DRPs have two features absent in dynamin: Insert A and Insert B. Insert A is an insertion of 25–50 residues of unknown function within the GTPase domain. Insert B is a stretch of ∼75 nonconserved residues that replaces the PH and is predicted to be of low complexity. How these Vps1 features affect its structure and function remains unclear.
To address these outstanding questions, we performed an extensive functional, biochemical, and structural characterization of Vps1. We show that Vps1 preferentially associates with the endosomal compartment and is required for its dynamics and morphology. We crystallized minimal GTPase-BSE fusion constructs of Vps1 in different nucleotide states to capture intermediates of the Vps1 GTP hydrolysis cycle. We show via cryoEM that Vps1 self-assembles into helices that are more flexible and fenestrated than those generated by dynamin. Using a pseudoatomic model generated by combining our crystal structures with our reconstruction of the Vps1 helical assembly, we identified a novel interface between adjacent GTPase domains. Disruption of this interface abrogates Vps1 function in vivo. Furthermore, the Vps1 helical assembly lacks the lateral contacts between its BSEs and adjacent GTPases and Stalks that are observed in pseudoatomic models of the dynamin assembly. These structural adaptations contribute to the more open helical architecture of Vps1 and may help Vps1 to remodel a wider range of potential templates. Collectively, our data reveal specific structural adaptations to the basic DRP machine that accommodate its unique functional requirements.
Vps1 localizes to and functions at the endosomal compartment
Cells lacking Vps1 (Δvps1) exhibited altered vacuolar morphology and dynamics when compared with WT cells (strain W303A; Fig. S1 A and Videos 1 and 2; Raymond et al., 1992; Peters et al., 2004) as assessed by visualizing the vacuolar membrane using either the lipophilic dye FM 4–64 (Vida and Emr, 1995) or by using genomically-integrated EGFP-tagged vacuolar membrane protein Vph1. W303A cells had dynamic and flexible vacuoles that frequently exhibited fusion and fission events. By contrast, the vacuolar compartment in Δvps1 cells consisted of static spherical components that were often clustered (Videos 1 and 2). Δvps1 cells also exhibited significant defects in endosomal function and morphology (Hayden et al., 2013; Lukehart et al., 2013). Snc1 is a v-SNARE required for fusion of vesicles from the TGN with the plasma membrane but is itself recycled via the endosomal compartment (Lewis et al., 2000). Steady-state localization of Snc1 was disrupted in Δvps1 cells: Snc1 was mislocalized to the vacuolar membrane, whereas in WT cells, it was primarily found on the plasma membrane (Fig. S1 B; Saimani et al., 2017). In WT cells, Tlg2, a t-SNARE used as a late endosomal marker, was punctate throughout the cytosol, whereas in Δvps1 cells, Tlg2 was mislocalized to the vacuolar membrane (Fig. S1 C). Remaining Tlg2 puncta appeared to be associated with the vacuolar membrane.
The endosomal compartment is enriched in phosphatidylinositol 3-phosphate (PI3P; Gillooly et al., 2000). Some PI3P is also found on the vacuolar membrane and is particularly enriched at the vertex junctions of docked vacuoles, where it plays an important role in vacuolar fusion (Fratti et al., 2004). We examined the localization of PI3P in WT and Δvps1 cells using the GFP-tagged FYVE domain from mammalian EEA1 as a probe (Burd and Emr, 1998). We observed highly dynamic FYVE puncta in WT cells (Fig. 2 A and Video 3). A diffuse FYVE signal was also detected throughout the vacuolar membrane. In Δvps1 cells, the PI3P signal lost its dynamic nature and was enriched to the cluster adjacent to the vacuole, representing the defective endosomal compartment (Fig. 2 A and Video 4).
Some aspects of endosomal function did not appear to be disrupted in Δvps1 cells. The multivesicular body (MVB) biogenesis pathway was intact in Δvps1 cells, as determined by examining the localization of carboxypeptidase S tagged with EGFP (Cps1-EGFP; Fig. S1 D). Cps1-EGFP did not accumulate in the endosomal compartment in Δvps1 cells, whereas it did in cells lacking Vps4, which is known to cause a defect in MVB biogenesis (Fig. S1 D; Shestakova et al., 2010).
Vps1 tagged with EGFP using a linker customized to include a stretch of 10 asparagine residues was fully functional and rescued the known growth defect of Δvps1 cells at 37°C (Fig. S2 A; Rothman et al., 1990). Vps1 generally had a diffuse cytosolic localization with highly dynamic foci that concentrated at vacuolar vertex junctions (Fig. 2 B). Deletion of Vps4, which is required for disassembly of ESCRT-III filaments and therefore proper endosomal function (Schöneberg et al., 2017), resulted in the expected Class E morphology of the endosomal compartment, with endosomes extensively stacked together adjacent to the vacuole (Babst et al., 1997; Finken-Eigen et al., 1997). In Δvps4 cells, Vps1 clustered around the class E compartment (Fig. 2 B). Furthermore, we observed significant endosomal localization for Vps1 based on colocalization with endosomal puncta labeled with FYVE (Fig. 2 C). 67.8 ± 4.9% of Vps1 puncta were associated with PI3P puncta (n = 181). We also observed some Vps1 enrichment within developing buds that was not associated with PI3P (not depicted). Taken together, these data indicate that Vps1 primarily concentrates within the endosomal compartment.
Self-assembly and coordinated GTP hydrolysis are necessary for the function of other DRPs. Stalk mutants, such as G397D in rat dynamin 1 and G385D in Dnm1, are defective in self-assembly and impair function (Ingerman et al., 2005; Ford et al., 2011). Mutants like K44A in human dynamin 1 lack efficient catalytic turnover and act as dominant negatives in vivo, trapping the helical assembly in a hyperconstricted prefission state (Damke et al., 1994; Sundborger et al., 2014). To determine the effect of Vps1 oligomerization and hydrolysis on endosomal function, we introduced point mutations into Vps1 at analogous positions (G436D and K42A). Vps1 G436D produced stable dimers in solution as assessed by size-exclusion chromatography (SEC) coupled to multiangle light scattering (MALS; SEC-MALS; Fig. S2 B). Like all other vps mutants, Vps1 is required for trafficking and maturation of CPY (Stevens et al., 1982). Cells lacking Vps1 exhibited a defect in maturation of CPY (Fig. 2 D). Expression of WT Vps1 in Δvps1 cells fully rescued this defect, whereas expression of either Vps1 K42A or Vps1 G436D did not. When tagged with EGFP, all expressed Vps1 K42A appeared to concentrate in defined intense spots adjacent to the vacuole (Fig. 2 E). The Vps1 K42A puncta formed at endosomal sites based on colocalization with those formed by mCherry-FYVE (Fig. S2 C). Strikingly, overexpression of Vps1 K42A in Δvps1 cells resulted in formation of extended filaments that appeared tangentially attached to the vacuolar compartment (Fig. S2 D). By contrast, Vps1 G436D-EGFP was diffuse and did not form puncta (Figs. 2 E and S2 C) as expected for a higher-order assembly-deficient DRP. Δvps1 cells expressing either mutant retained the vacuolar morphology observed in Δvps1 cells (Fig. 2 E). Expression levels for Vps1-EGFP and Vps1 K42A-EGFP in Δvps1 cells were comparable, while levels for Vps1 G436D-EGFP were slightly elevated (Fig. S2 E). Hence, the defects observed were not due to variations in expression levels of the mutants. When Vps1 K42A was overexpressed in WT cells, the vacuolar morphology seen in Δvps1 cells was induced (Fig. S2 F). By contrast, overexpression of Vps1 G436D in WT cells did not exhibit a dominant-negative phenotype. These data indicate Vps1 has a major endosomal function that depends on Vps1 assembly and hydrolysis.
Biochemical characterization of Vps1
As attempts to purify Saccharomyces cerevisiae Vps1 were unsuccessful, we sought an alternative source of Vps1 that was more amenable to purification and characterization. We therefore screened other fungal VPS1 genes for the ability to rescue the growth defect of Δvps1 cells at 37°C. VPS1 from Chaetomium thermophilum fully rescued the Δvps1 phenotype (Fig. 3 A). We purified C. thermophilum Vps1 fused to maltose-binding protein (MBP) after transient expression in Expi293F cells. The protein exhibited GTP hydrolysis with a basal activity of 1.52 hydrolysis events per minute, comparable with that observed for rat dynamin 1 (3.05 min−1; Fig. S3 A). The presence of dioleoyl phosphatidyl serine (DOPS) liposomes minimally stimulated Vps1 (3.05 min−1), while dynamin 1 was robustly stimulated to a turnover of 41.3 min−1 (Fig. S3 A; Warnock et al., 1995; Stowell et al., 1999; Ford et al., 2011). Removal of the MBP tag did not significantly alter these rates (no liposomes, 2.0 min−1; DOPS, 3.3 min−1; Fig. S3 B and not depicted). Substitution of lipid nanotubes containing phosphoserine (PS) and PI3P for DOPS liposomes similarly showed only minimal stimulation of Vps1 GTPase activity (absence, 2.0 min−1; presence, 3.6 min−1), whereas dynamin 1 was again robustly stimulated (presence, 39.6 min−1; not depicted). Vps1 was, however, able to assemble into helical structures on these nanotubes (Fig. 3 B). Hence, the absence of significant lipid stimulation of GTP hydrolysis by Vps1 is not due to an inability of Vps1 to self-assemble on lipid templates.
We next purified and characterized the hydrolysis of a minimal GTPase-BSE construct from C. thermophilum Vps1 (hereafter Vps1 GG), comparable with the minimal GG construct previously used for dynamin 1 (Chappie et al., 2009, 2010, 2011). Dynamin 1 GG dimerizes in the presence of GDP.AlF4−, and this change can be monitored by SEC (Fig. S3 C; Chappie et al., 2010). Vps1 GG only exhibited a shift to a faster-migrating species on SEC with GDP.AlF4− but not when preincubated with GMPPCP, GTPγS, or GDP (Fig. S3 D). SEC-MALS confirmed that Vps1 GG dimerized only in the presence of GDP.AlF4− (Fig. 3 C). Vps1 GG exhibited basal GTPase activity of 1.1 min−1 with an apparent KM of 60 µM, as assessed using a colorimetric phosphate release assay (Fig. 3 D; Leonard et al., 2005). This hydrolysis activity was not stimulated by DOPS liposomes (not depicted). Since GTP hydrolysis by rat full-length dynamin 1 is robustly stimulated by liposomes (Fig. S3 A), assembly is required for GTP hydrolysis (especially stimulated hydrolysis). Full-length Vps1 assembled (see above) but exhibited only modest lipid-stimulated GTP hydrolysis. This difference in stimulated GTP hydrolysis rates may allow Vps1 to assemble into longer and more persistent structures.
The crystal structures of Vps1 GG bound to GMPPCP, GDP.AlF4−, and GDP
To characterize the catalytic cycle of Vps1, we crystallized Vps1 GG in complex with GMPPCP, GDP.AlF4−, and GDP, respectively (Figs. 4 and S4 A). Vps1 GG in complex with GMPPCP (hereafter GGGMPPCP) crystallized with two complete nucleotide-bound GG dimers in the asymmetric unit, which superposed with root mean square (r.m.s.) deviations of Cα residues of 0.55 Å; Fig. S4 B). The dimers were formed by the GMPPCP-bound GTPase domains and buried a surface area of 2,486 Å2 (Fig. 4 A). Each GTPase bound one GMPPCP in a deep pocket (Fig. 4 B) that was closed off at the dimer interface by the other monomer. In the binding pocket, an Mg2+ ion was coordinated by the side-chain hydroxyl groups of Ser57 in the P loop and Thr77 in Switch 1 as well as the β- and γ-phosphates of the nucleotide. The β-phosphate also formed a hydrogen bond with the side chain of Lys56. The guanosine base was coordinated by the side chain of Asp242 in G4 and was also contacted in trans by the side chain of Asp245 from the G4 loop of the dimer partner. Switches 1 and 2 were also both well ordered (Fig. 4 C). The BSEs in this structure were in the fully extended open conformation (Fig. 4 A). However, the close approach of neighboring molecules related by noncrystallographic symmetry induced local disorder in the CGED helix of the BSE of molecule D (Fig. S4 B). Consequently, the structural model for this BSE was less complete.
Vps1 GG in complex with GDP.AlF4− (GGGDP.AlF4-; Fig. 4 D) also crystallized with two complete GG dimers in the asymmetric unit, which superposed with r.m.s. deviations of Cα residues: 0.68 Å (Fig. S4 C). The GTPases formed the same canonical interface with an inaccessible area of 2,586 Å2. We observed density for GDP, AlF4−, along with an additional density peak that was coordinated by the side chain of Ser43 in the P loop, the main chain carbonyl oxygens of Gly72 and Gly74 at the top of Switch 1, a β-phosphate oxygen, and a fluorine within the AlF4− moiety. We interpret this density as a sodium ion based on the presence of a sodium ion in the equivalent position of the dynamin 1 GG structure in complex with GDP.AlF4− (Fig. 4, E and F; Chappie et al., 2010). Surprisingly, the BSEs in this structure were also in the fully extended, open conformation (Fig. 4 D). As for GGGMPPCP, the CGED helix of molecule D was disordered (Fig. S4 C).
Both GGGMPPCP and GGGDP.AlF4- structures had additional interpretable density N-terminal to the NGTPase helix. C. thermophilum Vps1 has a unique N-terminal extension of 19 amino acids. This packs against the core of the GTPase domain (Fig. S4 D). The function of this extension remains unknown, but its presence is required to produce abundant soluble protein.
Furthermore, we determined the structure of a similar Vps1 GG construct in complex with GDP (hereafter GGGDP; Figs. 4 C and S4 A). GGGDP crystallized with a single molecule in the asymmetric unit. A crystallographic twofold axis generated the same GTPase dimer around the nucleotide binding sites with a buried interface of 2,637 Å2 (Fig. 4 G). The bound GDP was contacted by Lys56 in the P loop, which formed a hydrogen bond with the β-phosphate and the main chain amide nitrogens of Ser53, Ser54, Gly55, K56, and Ser57 (Fig. 4, H and I). Switches 1 and 2 were unusually well ordered for a GDP-bound GTPase structure due to stabilization by the dimer interface. Switch 1, however, was pulled away from the active site, which allowed several waters to enter. The BSEs in this structure were disordered (Fig. 4 G), perhaps due to steric clashing imposed by the crystal symmetry or due to the construct used. Refined density for each nucleotide is shown (Fig. 4 J).
GGGDP showed overall deviations of Cαs of 1.73 Å and 1.93 Å with GGGMPPCP and GGGDP.AlF4-, respectively. Structural superpositions revealed several nucleotide-dependent conformational changes within the GTPase domain (Fig. 5). First, there was a significant shift in Switch 1 with a maximum movement at Gln73 of 7.3 Å compared with GGGMPPCP (Fig. 5 A) and 8.2 Å with respect to GGGDP.AlF4- (Fig. 5 B). These Switch 1 movements resulted in a shift of ∼2.8 Å at the base of α1 within the core GTPase fold (see Fig. S5 for a sequence alignment that details the nomenclature for the structural elements within GG). This movement was transmitted to and amplified at the loop between β2B and β3 at the base of the core β-sheets of the GTPase fold: His162 moved 7.4 Å compared with the GGGMPPCP and 6.8 Å compared with the GGGDP.AlF4-. The shift in this loop resulted in movements at the bases of all the sheets in this region. β2A and αB were pulled toward the repositioned β2B (Fig. 5 C). These movements together resulted in a shift in the position of the loop between β2A and αB (the αB loop; 3.1 Å). Interestingly, this lies adjacent to Insert A, most of which we observed in our GGGMPPCP and GGGDP structures. A morph of the movements of the Cαs present in both GGGMPPCP and GGGDP is shown in Video 5. This movement also destroys an alignment of four hydrophobic residues observed in GGGMPPCP- and GGGDP.AlF4--bound structures: Tyr126 (in β2A–αB loop), Trp114 (in β2A), Tyr159 (in β2B), and Ile86 (in β2; Fig. 5 D). Together, these residues form a “hydrophobic ridge.” When GGGMPPCP and GGGDP.AlF4- were compared, small additional rotations in the Switch 1 region and the P loop were observed, which may have fine-tuned the conformation of the catalytic site for hydrolysis (Video 6).
Vps1 GGGMPPCP crystallized with the BSEs in the open conformation, as did dynamin 1 GG bound to GMPPCP (Chappie et al., 2011). Comparison of the structures (Fig. S6 A) demonstrated that while the GTPase cores superpose well (overall core r.m.s. deviation, 1.17 Å), differences concentrate within the BSEs. In Vps1 GGGMPPCP, the BSEs were rotated further away from the GTPase core than the BSEs in the dynamin-GMPPCP structure, resulting in a further opening out of the BSEs. The largest rotation was observed for the CGED helix, where the helix rotated out a further 22.1° compared with the dynamin structure (Fig. S6 B). The NGTPase helix rotated an additional 20.5°, while the CGTPase helix rotated 16.9°. The result of this opening out was that the distance between comparable residues at the base of CGED was 137.2 Å in Vps1 GG and 126.6 Å in the dynamin structure.
When compared with Vps1 GGGDP, both Vps1 GGGMPPCP and Vps1 GGGDP.AlF4- underwent a Switch 1 movement that was transmitted to the bases of the β-sheets, the β2A–αB loop, and the αB helix. Dynamin GGGMPPCP behaved analogously to Vps1 GGGMPPCP and underwent a comparable Switch 1 movement (Fig. S6 C; Chappie et al., 2011; Anand et al., 2016). The conformation of dynamin 1 GGGDP.AlF4-, however, was similar to that of dynamin 1 GGGDP (Fig. S6 D; Chappie et al., 2010). This is because this GDP.AlF4−-bound structure crystallized with the BSEs in the closed conformation rather than the extended and open conformation we observed for Vps1 GGGDP.AlF4-. The open BSE conformation was previously observed only with a GG construct for Arabidopsis thaliana DRP1A bound to GDP.AlF4− (Yan et al., 2011).
The cryoEM structure of full-length Vps1
To obtain mechanistic insight into self-assembly of Vps1, we characterized full-length Vps1 fused to MBP using EM. In the nucleotide-free state, Vps1 was heterogeneous and formed curved filaments (Fig. 6 A). Addition of GDP resulted in formation of rings with outer diameter 41.2 ± 1.9 nm (mean ± SD) and lumenal diameter 17.2 ± 1.6 nm. When viewed side-on, we observed short stacks of rings or short helices (Fig. 6 A). Addition of GDP.AlF4− also yielded rings and short stacks (outer diameter 43.6 ± 3.5 nm; lumenal diameter 20.9 ± 2.9 nm). By contrast, incubation with GMPPCP produced extended helices of uniform diameter of 39.3 ± 2.2 nm (Fig. 6 A). The GMPPCP-bound Vps1 tubes exhibited structural flexibility, which may represent an inherent ability of Vps1 to accommodate a range of templates of varying geometry. Nevertheless, these tubes were suitable for structural characterization by cryoEM (Fig. S7 A).
We determined the structure of the full-length Vps1 helical assembly assembled in the presence of GMPPCP to a global resolution of 11 Å using cryoEM and helical reconstruction (Fig. S7, A and B; He and Scheres, 2017). The helical tube had a lumenal diameter of 19.1 nm and an outer diameter of 42.4 nm (Fig. S7 C). The tube was right-handed, 1-start, and had 14.9 subunits per turn with a pitch of 157 Å. The different domains of Vps1 are readily distinguishable in the density map (Fig. 6 B). Removal of the MBP tag after assembly by incubation with PreScission protease did not affect the helical assemblies (Fig. S7 D).
Comparison of our helical reconstruction of Vps1 with that of GMPPCP-bound dynamin 1 ΔPRD assembled on DOPS (Chappie et al., 2011) revealed several striking differences (Fig. 6, C–H). First, the Vps1 helix had an increased pitch (157 Å) compared with that of dynamin1 ΔPRD (99 Å; Fig. 6, C and D). This was due primarily to the increased tilt of the BSEs themselves in the Vps1 helix (−37° to a plane perpendicular to the helical axis compared with 7° for dynamin 1 ΔPRD; Fig. 6, E and F). This generated the longer “arms” seen in the T view (Fig. 6, C and D). Second, the Vps1 helix had an increased tilt of the stalks and GTPases relative to a plane perpendicular to the helical axis in the Vps1 assembly (14.5° for Vps1 compared with 7.5° for dynamin 1 ΔPRD; Fig. 6, E and F). The Vps1 helical assembly had a more “open” architecture than dynamin 1 ΔPRD as a consequence of these differences. The Vps1 helix consisted of 14.9 subunits per turn with an outer diameter of 424 Å compared with 13.2 subunits per turn and 400 Å for dynamin 1 ΔPRD (Fig. 6, G and H). No density was visible for the region that would be occupied by Insert B, within the lumen of the helix, likely due to the conformational flexibility of the low-complexity sequence that comprises Insert B, whereas the positions of the PH domains adjacent to the lipid were clear in the case of the dynamin 1 assembly (Fig. 6 H). In addition, no density was visible for the C-terminal MBP tag.
In contrast with dynamin, the BSE density in Vps1 made no contacts or interfaces with the densities for either Stalks or neighboring GTPase domains. The GTPase dimerization interface was readily discernible as expected for a GMPPCP-bound structure. We also identified a new second interface between adjacent GTPase domains (Fig. S7 E), which appeared to stabilize the open helical configuration of the Vps1 assembly.
A pseudoatomic model for Vps1
To understand the observed structural differences in our Vps1 reconstruction more fully, we generated a pseudoatomic model for the full-length Vps1 helix. Crystal structures of the Vps1 GGGMPPCP dimer and the Stalk dimer from rat dynamin 1 ΔPRD (Ford et al., 2011) were sequentially docked as independent rigid units into the helical reconstruction (Fig. 7 A). Overall identity and similarity between C. thermophilum Vps1 and rat dynamin 1 across the stalk were 34% and 55%, respectively. Vps1 GGGMPPCP fit well into the globular, bilobal density on the outer surface of the helix, with the BSEs being placed into the thin rods of density connecting the GTPases to the stalks. The Stalk dimer easily fit into the Stalk density. The full helix was generated by applying the helical parameters to the positioned dimers, followed by a local optimization. The fit did not generate any steric clashes and required no additional manipulation to the atomic models (Fig. 7, B–G). Small gaps present between the tops of the Stalks and the ends of the BSEs could readily be accounted for by the residues missing in the docked models: seven amino acids between the end of the CGTPase helix and the start of the Stalk and 10 amino acids between the end of the Stalk and the CGED helix. Small protrusions of unfilled density remained at the bases of the stalks and were likely the start and end of the disordered Insert B sequence (Fig. 7 D). An additional small patch of unfilled density adjacent to the CGED helix likely arose from the linker connecting Vps1 and MBP (Fig. 7 F).
Within the Stalk, Interface 3 at the bases of the stalks (facing the helix lumen) were formed as predicted from the linear filaments observed in the dynamin 1 ΔPRD and MxA crystals (Gao et al., 2010, 2011; Faelber et al., 2011; Ford et al., 2011) and in models of helical assemblies generated on the bases of these structures. This positioned the tight L2 loop between helices α1C2 and α2 in the stalk, where the assembly-deficient mutations G436D (Vps1) and G397D (rat dynamin 1) are found, which is presumably the molecular basis for the assembly deficiency (Fig. S2, B and C). Furthermore, the “sticky patch,” which forms Interface 1 (Ford et al., 2011) between adjacent Stalk dimers, was again formed (Fig. 7 E). The fit also reinforced the observation from the density that the BSEs do not form any additional contacts with either the Stalks or adjacent GTPase domains, which is in contrast with what has been observed in dynamin crystal structures and in a model for the helical assembly (Chappie et al., 2011; Faelber et al., 2011; Reubold et al., 2015).
As predicted by the model, mutation of residues in either C. thermophilum Vps1 Interface 1 or Interface 2 disrupted Vps1 function as determined using both growth assays and by assessing vacuolar morphology (Fig. S8, A and B). By contrast, mutation of a residue not known to be involved in either Stalk interface or any other interactions (C. thermophilum Vps1 K498E) behaved as did WT C. thermophilum Vps1 when assessed using either assay.
We observed a novel interface formed by GTPases from adjacent rungs on the helix (Fig. 7 G). This interface was formed by close approach of the β2A–αB loops (the αB loops) and Insert A from adjacent GTPase domains. The αB loop underwent significant nucleotide-dependent conformational changes as observed in our crystal structures (Fig. 5 A), and hence formation of this interface may be context dependent. The close approach of adjacent Insert A in this interface may also be important for the formation or stability of this interface. Comparison of the residues that comprise the αB loops from several different DRP family members (Fig. S5) as well as variations in Insert A sequence demonstrates several differences in the solvent-facing residues that could contribute an additional layer of regulation on helix formation. We term this interface the αB interface.
Disruption of the αB interface abrogates Vps1 function in vivo
We mutated the αB loop and the surface-facing residues on the αB helix as a control in both C. thermophilum Vps1 and S. cerevisiae Vps1. Expression of C. thermophilum or S. cerevisiae Vps1 bearing a mutated αB loop did not rescue growth of Δvps1 cells at 37°C nor rescue the defect in vacuolar morphology (Fig. 8, A–D). By contrast, mutation of the surface-facing residues on the αB helix, which are not predicted to be involved in the formation of this interface, behaved like WT Vps1. Furthermore, while S. cerevisiae Vps1-EGFP rescued CPY maturation in Δvps1 cells, Vps1 bearing a mutated αB loop did not (Fig. S8 C).
DRPs are mechanochemical enzymes that are responsible for numerous membrane-remodeling events within the cell. How the general fundamental features of DRP function are adapted to specific cellular targets and functions is an area of outstanding interest. In this study, we extensively characterized the fungal DRP Vps1. Vps1 preferentially assembles at the endosomal compartment and regulates its function. We present crystal structures of minimal Vps1 GG constructs in different nucleotide states that capture several steps of the catalytic pathway and reveal unique features on the GTPase domain that are determinants of a novel biologically important interface that forms during Vps1 helical self-assembly. We show by cryoEM that assembled full-length Vps1 has a looser packing when compared with the helix formed by dynamin 1 that may provide it with appropriate flexibility to accommodate its preferred cellular template. Pseudoatomic modeling that combined our crystallographic and EM structures identified a novel, biologically important interface that forms during Vps1 helical self-assembly.
Our data show that Vps1 self-assembly is required for its function at the endosomal compartment. Vps1 G436D, the equivalent of the assembly-defective dynamin mutation G397D, cannot rescue endosomal function, as assessed using several assays. Conversely, expression of Vps1 K42A, the equivalent of dynamin K44A, which can be trapped in a hyperconstricted prefission state, results in formation of few large assemblies within the cell that are invariably associated with the endosomal compartment. Although Vps1 has been reported to act at several sites within the cell, trapped Vps1 assemblies are always localized to the endosomal compartment. Hence, the primary site of action of Vps1 is the endosomal compartment. It is possible that Vps1 can be recruited to and assemble at other sites within the cell but that the K42A mutation, for unknown reasons, preferentially becomes trapped at the endosome.
The helical reconstruction of the GMPPCP-bound Vps1 assembly revealed a more open and looser helix than that observed for GMPPCP-bound dynamin 1. Structural comparison showed significant differences in the orientation of the BSEs in the assembled helices. These changes resulted in the increased pitch of the Vps1 helix and the concomitant additional space between adjacent rungs. The BSEs in Vps1 also did not appear to engage in any interfaces, unlike in models for helically assembled dynamin and in the linear dynamin filaments captured in the crystal structures. Strikingly, Drp1 assembled on nanotubes exhibits a pitch of ∼130 nm, approximately intermediate between what is observed for dynamin and Vps1 (Francy et al., 2017). Since Vps1, dynamin 1, and Drp1 all exhibit different pitches and overall architectures and are known to function at different cellular targets, it is of course tempting to speculate that the helical architectures of DRPs have been extensively customized for their appropriate cellular targets.
Vps1 GTPase domains interact across the rungs of the helical assembly at two distinct interfaces. The first is the canonical head-to-head dimerization interface that has been observed in all DRP assemblies and brings the active sites together for reciprocal stimulation of catalytic turnover. The second, which we term the αB interface, arises from the close approach of the αB loops and Insert A in neighboring subunits. The likely function of this interface is to further stabilize the open architecture of the Vps1 assembly. Disruption of this interface abrogated Vps1 function in vivo. Our GG crystal structures showed that this region exhibits significant nucleotide-dependent conformational changes. The function of Insert A remains unknown. It is present in all DRPs with the exception of dynamin. It is not conserved among Vps1 family members and ranges in length from 27 residues in C. thermophilum Vps1 to 47 residues in S. cerevisiae Vps1. However, our pseudoatomic model revealed close approach of Insert A from adjacent GTPase domains in the αB interface. We therefore speculate that Insert A may be required to form or stabilize this interface.
One striking difference between Vps1 and dynamin 1 is the robust stimulation of dynamin GTPase activity observed in the presence of liposomes, whereas stimulation of Vps1 by liposomes is minimal. Several possibilities may account for this difference. First, dynamin self-assembles into helical polymers with or without lipid substrate regardless of nucleotide triphosphate load, but its GTPase activity is only stimulated in the presence of negatively charged phospholipids. The dynamin PH domain is critical for regulation and facilitation of lipid-stimulated GTP hydrolysis. We only observed helical assembly of Vps1 on preformed nanotubes and not on liposomes similar to those that have typically been used to stimulate dynamin GTPase activity. Instead of a PH domain, Vps1 has Insert B. Insert B may have a differing lipid preference when compared with the PH domain or may be a site for posttranslational modifications, regulating targeting to or avidity for lipids. Second, different patterns of BSE or noncanonical GTPase–GTPase interactions in assembled Vps1 compared with dynamin may result in the observed differences between Vps1 and dynamin. Indeed, the architecture of assembled Vps1 lacks additional contacts between the extended BSEs and neighboring Stalks/GTPases, whereas models of assembled dynamin do predict additional contacts. These may contribute to formation of a hydrolysis-competent conformation of GTPase domains of assembled dynamin.
Vps1 can assemble on lipid nanotubes containing PI3P. One avenue for future enquiry is to determine the lipid-bound structure of Vps1 and to determine how lipid binding affects the general architecture of Vps1 helical assemblies. Although our current structure is full-length, Insert B is disordered. Since Insert B would be lipid facing in a lipid-bound helix, its function is likely to mediate lipid interaction either directly or indirectly. In addition, we observed that deletion of Insert B prevented self-assembly even in the absence of lipids (unpublished data). In cells, Vps1 ΔInsB had a diffuse cytosolic distribution, and purified Vps1 ΔInsB could not assemble even in the absence of lipids. Therefore, Insert B is likely required both for lipid interaction and for Vps1 helical assembly.
Collectively, our study provides insight into the mechanistic determinants in Vps1 that tailor it for the generation of open and flexible helices, which are likely to be required for its endosomal functions. Various DRPs like Dnm1 and Drp1 more closely resemble Vps1 than dynamin in that they have an Insert A and B and lack PH and PRD domains. This study therefore has important implications for defining the mechanistic and structural relationships among dynamin family members and underscores the fundamental principles of helix assembly in these proteins.
Materials and methods
Yeast genetic manipulation and molecular biology
Strains of S. cerevisiae used in this study are listed in Table S1. Gene deletions were generated in W303A/α diploids by homologous recombination using appropriate cassettes amplified from pFA6a-kanMX6, pFA6a-His3MX6, or pFA6-natMX4 (Longtine et al., 1998; Goldstein and McCusker, 1999) flanked with a sequence (30 nt) proximal to the coding sequence of the target gene. Diploids were subsequently sporulated by starvation in SPO (1% potassium acetate, 0.1% yeast extract, and 0.05% glucose) medium for 2 d. Following manual tetrad dissection, knockout haploids were extensively validated. Deletion strains were generated at 30°C with the exception of Δvps1::NAT, where all construction stages from sporulation onwards were conducted at room temperature.
YPD (2% yeast extract, 1% peptone, and 2% glucose supplemented with L-tryptophan and adenine) was used for routine growth. Synthetic complete (yeast nitrogen base, ammonium sulfate, 2% glucose, and amino acids) or synthetic defined (yeast nitrogen base, ammonium sulfate, 2% glucose, and appropriate amino acid dropout) media were used before microscopy or to maintain plasmid selection as required. Cells were induced to sporulate by overnight incubation in YPA (2% potassium acetate, 2% peptone, and 1% yeast extract) followed by incubation in SPO.
Select plasmids used in the course of this study are detailed in Table S2. S. cerevisiae VPS1 was amplified from W303A/α genomic DNA, prepared using the Yeast DNA Extraction kit (Thermo Fisher Scientific). C. thermophilum VPS1 was amplified from C. thermophilum cDNA (Amlacher et al., 2011). All constructs were generated by splicing by overlap extension and Gibson assembly. C. thermophilum VPS1 was fused at its C terminus to MBP and cloned into pcDNA3.1+ for expression in mammalian cells. The following GG constructs were used: pET-15b PreScission–C. thermophilum VPS1 GG, where residues 355–668 of the VPS1 coding sequence were replaced with an AGAGA linker and pET-15b C. thermophilum VPS1 G-EGFP-G, where residues 359–668 of the VPS1 coding sequence were replaced with a cassette consisting of an AG–PreScission site–EGFP–PreScission site–GA construct.
Analysis of growth by serial dilution
Following overnight growth in appropriate media, cells were diluted and regrown to mid-logarithmic phase in YPD at 30°C (OD600 0.6–0.8). Cells were then diluted to 0.5 OD600/ml, and fivefold serial dilutions were made in water. 2 µl of each dilution was spotted onto YPD plates, after which the cells were incubated at 30 or 37°C for 2 or 3 d before imaging.
Protein extracts for Western blotting were obtained as described previously (Millen et al., 2009). In brief, cells were lysed on ice by resuspension in 1 ml ice-cold H2O supplemented with 150 µl 1.85 M NaOH and 7.5% (vol/vol) β-mercaptoethanol. Protein was precipitated by addition of 150 µl 50% (wt/vol) TCA. Pellets were washed twice with acetone, resuspended in 150 µl 1× SDS-PAGE buffer, and incubated for 30 min at 30°C followed by 2 min at 95°C. Antibodies used were as follows: anti-PGK1 (ab113687; Abcam), anti-CPY (ab34636; Abcam), and anti-EGFP (ab290; Abcam). Labeled secondary antibodies were IRDye 680RD goat anti-rabbit antibody (926-68171; LI-COR Biosciences) and IRDye 680RD goat anti-mouse (926-68070; LI-COR Biosciences). These were detected using the Odyssey system (LI-COR Biosciences). Bands were integrated and quantified using the Fiji distribution of ImageJ (National Institutes of Health; Schindelin et al., 2012).
Preparation of yeast for microscopy
Cells were grown overnight in YPD or synthetic defined medium appropriately supplemented to maintain plasmid selection. Cells were then diluted in YPD and grown to mid-logarithmic phase. Vacuolar membranes were stained with 10 µM FM 4–64 (Thermo Fisher Scientific) for 45 min followed by washing and incubation in YPD medium without dye for 1 h. Cells were plated onto No. 1.5 glass-bottomed cover dishes (MatTek Corporation) previously treated with 15 µl of 2 mg/ml concanavalin A (Sigma-Aldrich).
Confocal microscopy and image analysis
Confocal images were acquired on a Nikon A1 confocal microscope with a Plan Apochromat 100× oil objective. NIS Elements Imaging software (Nikon) was used to control acquisition. Images were further processed using Fiji or NIS Elements.
Protein expression and purification
Full-length C. thermophilum Vps1 was expressed in mammalian cells using the Expi293 Expression System (Invitrogen). Cells were transfected with plasmid DNA encoding a C. thermophilum Vps1-MBP fusion construct following the recommended protocol. 48 h after transfection, cells were washed twice with ice-cold PBS, and the pellet was resuspended in HNG buffer (50 mM Hepes/KOH, pH 8, 500 mM NaCl, and 5% glycerol) supplemented with 5 mM MgCl2, 10 mM β-mercaptoethanol, 1% Tween-20, 0.3% NP-40, 50 µg/ml DNase I, and the Halt Protease Inhibitor Cocktail (Thermo Fisher Scientific). After incubation at 4°C for 1 h, the lysate was homogenized using a Dounce homogenizer. The resulting homogenate was centrifuged at 21,000 g for 30 min at 4°C. The supernatant was incubated with amylose agarose resin (New England Biolabs) for 1 h at 4°C. The beads were extensively washed with HNG, then with HNG supplemented with an additional 500 mM NaCl, and then HNG again. The protein was then eluted using HNG supplemented with 100 mM maltose and protease inhibitor cocktail. The protein was concentrated and flash frozen for long-term storage at −80°C until use.
C. thermophilum Vps1 GG and C. thermophilum Vps1 G-EGFP-G were expressed overnight at 21°C by IPTG induction in BL21 cells grown in 2×TY. Cells were pelleted, washed, and resuspended in TN buffer (20 mM Tris/Cl, pH 8.0, 150 mM NaCl, and 1.93 mM β-mercaptoethanol). After homogenization using an Emulsiflex-C3 (Avestin), lysates were clarified by centrifugation at 142,000 g for 45 min at 4°C. Clarified lysates were applied to Ni-IDA beads in batch (Macherey Nagel). The beads were extensively washed and loaded into a column, and then protein was eluted in TN with a gradient to 250 mM imidazole. Peak fractions were pooled and dialyzed against TN to remove imidazole. Both proteins were then digested with PreScission protease at room temperature: in the case of C. thermophilum Vps1 GG, to remove the N-terminal tags, and in the case of C. thermophilum Vps1 G-EGFP-G, to excise the EGFP. C. thermophilum Vps1 GG was further purified by anion exchange chromatography and SEC, equilibrated in 5–20 mM Hepes, pH 7.4, 150 mM NaCl, and 1.93 mM β-mercaptoethanol using a Superdex 200 16/60 column (GE Healthcare). Following cleavage, C. thermophilum Vps1 G-EGFP-G was rebound to Ni-IDA (to remove cleaved EGFP), eluted, and dialyzed. Purification was completed as for C. thermophilum Vps1 GG. Proteins were concentrated and flash frozen in liquid nitrogen until use. Rat dynamin 1 (with a PreScission site engineered at the start of the PRD) was expressed in BL21(DE3) pLysS (Promega) cells as an N-terminal His6 fusion using the pET-15b vector. Protein expression was induced as for Vps1 GG. Cells were resuspended in 20 mM Tris/Cl, pH 8.0, 500 mM NaCl, and 1.93 mM β-mercaptoethanol and then were lysed, clarified, and bound to Ni-IDA. Protein was subsequently dialyzed and passed over ion exchange and size exclusion as for Vps1 GG using Tris/Cl, pH 8.0, 500 mM NaCl, and 1.93 mM β-mercaptoethanol as a running buffer. The protein was then concentrated, supplemented with glycerol to 10%, and frozen for long-term storage.
Human dynamin 1 GG was expressed in Escherichia coli as an MBP fusion and purified as described previously (Chappie et al., 2009) via amylose affinity, anion exchange following removal of the tag by PreScission protease cleavage, and SEC. The protein was dialyzed into a final buffer of 20 mM Hepes, pH 7.5, 150 mM KCl, 4 mM MgCl2, 2 mM EGTA, and 1 mM DTT during the final SEC step on a Superdex 75 10/300 GL column. Peak SEC fractions were collected, concentrated to 100–200 µl, flash frozen in aliquots, and stored at −80°C.
Preparation of liposomes and nanotubes
Liposomes were made from 100% DOPS, and nanotubes were made from 40% D-galactosyl-β-1,1' N-nervonoyl-D-erythro-sphingosine, 40% DOPS, and 20% PI3P (Avanti). Lipids in chloroform were mixed in a glass tube with methanol added to keep the solution clear in the case of nanotubes containing PI3P. The mixtures were dried using a stream of nitrogen gas and were dessicated for at least 30 min. Liposomes and nanotubes were rehydrated in 20 mM Hepes/NaOH, pH 7.4, and 150 mM NaCl to a lipid concentration of 0.5 mg/ml. DOPS liposomes were subsequently extruded through a 1-µm Nucleopore membrane (Whatman).
Continuous GTPase assays using the GTP regenerating system were performed as previously described (Ingerman and Nunnari, 2005) with the exception that reaction mixes without GTP were preincubated at 37°C for 10 min before addition of GTP to a final concentration of 1 mM. Reactions contained 142.5 mM NaCl, 7.5 mM KCl, and 5 mM MgCl2 and were conducted at pH 7.0.
The colorimetric GTPase assay used to determine the kinetic parameters for Vps1 GG was performed using the malachite green phosphatase assay kit (Echelon Biosciences). Reactions contained 142.5 mM NaCl, 7.5 mM KCl, and 5 mM MgCl2 and were performed at pH 7.0. Reactions were preincubated at 37°C for 10 min before addition of GTP at various final concentrations. Samples were withdrawn at several time points, and reactions were stopped by addition of EDTA, pH 8.0, to a final concentration of 100 mM. Malachite green reagent was added in accordance with the manufacturer’s guidelines, and absorbance was determined after 30 min at 630 nm. Amount of phosphate released was determined using a standard curve. Kinetic parameters were calculated numerically by fitting data to the Hill Equation using a nonlinear least squares method as implemented in Prism (GraphPad Software).
Vps1 GG or dynamin 1 GG (19 µM) were preincubated where indicated in the absence or presence of the relevant nucleotide or nucleotide analogue (2 mM) for 1 h at 37°C. Samples were then loaded onto a Superdex 75 10/300 column preequilibrated in a running buffer of 20 mM Hepes, pH 7.4, 150 mM NaCl, 5 mM MgCl2, 2 mM EGTA, and 1.93 mM β-mercaptoethanol, and elution volumes were recorded and compared. Gel filtration standards (Bio-Rad) were run in the same buffer.
Purified S. cerevisiae Vps1 G436D (4.0 mg/ml) was subjected to SEC using a Superdex 200 10/300 GL equilibrated in SEC-MALS buffer (20 mM Hepes, pH 7.5, 150 mM NaCl, 5.0 mM MgCl2, 2.0 mM EGTA, and 2.0 mM β-mercaptoethanol). C. thermophilum Vps1 GG (2.5 mg/ml) and Vps1 GG K56A (4.0 mg/ml) were subjected to SEC using a Superdex 75 10/30 equilibrated in SEC-MALS buffer. Nucleotide-dependent oligomerization was assessed by incubating with various nucleotides at 2.0 mM for 1 h at 37°C followed by centrifugation at 13,000 g for 10 min before SEC-MALS analysis. The gel filtration column was coupled to a static 18-angle light-scattering detector (DAWN HELEOS-II) and a refractive index detector (Optilab T-rEX; Wyatt Technology). Data were collected continuously at a flow rate of 0.5 ml/min. Data analysis was performed using the program Astra VI. Monomeric BSA (6.0 mg/ml; Sigma-Aldrich) was used for normalization of the light-scattering detectors and data quality control.
Prior to crystallization, C. thermophilum Vps1 GG (73 µM) was preincubated with 1 mM β,γ-methyleneguanosine 5′-triphosphate (GMPPCP; Sigma-Aldrich) for 1 h at room temperature in 5 mM Hepes, pH 7.4, 150 mM NaCl, 5 mM MgCl2, and 1.93 mM β-mercaptoethanol. Crystals were obtained by hanging drop vapor diffusion at room temperature, by equilibration of droplets of 5–6 µl containing 18.25–36.5 µM protein and 0.5 mM GMPPCP against a reservoir of 400 µl containing 14% PEG 4000, 0.2 M sodium acetate, and 0.1 M Tris/Cl, pH 8.7–9.0. Crystals appeared after 24–48 h. Crystals were cryoprotected by sequential transfer through solutions of the crystallization condition supplemented with 0.5 mM GMPPCP and increasing concentrations of PEG 400 to a final concentration of 15%. C. thermophilum Vps1 GG bound to GDP.AlF4− was generated by incubating 25 or 50 µM protein in 5 mM Hepes, pH 7.4, 150 mM NaCl, 5 mM MgCl2, and 1.93 mM β-mercaptoethanol with 2 mM GDP, to which NaF was added sequentially with vortexing to a final concentration of 20 mM, and to which AlCl3 was added to a final concentration of 2 mM. The sample was then passed through a cellulose filter of 0.22-µm pore size before setup. Crystals were grown by vapor diffusion using 5-µl droplets containing 12.5 or 25 µM protein and 1 mM GDP.AlF4− against a reservoir of 400 µl containing 5–10% PEG 8000, 20% glycerol, and 0.08 M MES, pH 5.6–6.2, at room temperature. Crystals appeared after 24 h. Crystals required no additional cryoprotection and were flash cooled in liquid nitrogen for storage. Crystals of C. thermophilum Vps1 GG bound to GDP were obtained by preincubation of protein with 2.3 mM GDP in 5 mM Hepes, pH 7.4, 150 mM NaCl, 5 mM MgCl2, and 1.93 mM β-mercaptoethanol. Crystals were grown by vapor diffusion at room temperature against a reservoir of 400 µl containing 14–19% PEG 4000, 0.07–0.1 M trisodium citrate, and 20% isopropanol using 5-µl droplets containing 12.5 or 25 µM protein with 1.15 mM GDP, and crystals appeared after 24–48 h. Crystals were cryoprotected by transfer to a solution containing 18% PEG 4000, 0.07 M trisodium citrate, and 20% isopropanol, and then substitution of the solution took place with the same supplemented with increasing amounts of PEG 400 to a final concentration of 10%. Cryoprotected crystals were flash cooled in liquid nitrogen for storage.
Crystallographic data collection, structure determination, and refinement
Reflection data for C. thermophilum GGGMPPCP crystals were collected at 100K at ID-22 at the Advanced Photon Source (Argonne National Laboratory, Lemont, IL) at a wavelength of 1 Å using an Eiger detector. Crystals were monoclinic and belonged to spacegroup P21 with cell axes a = 83.03, b = 120.18, c = 85.04 Å, and β = 120.22°. A dataset was collected using a single crystal to minimum Bragg spacings of 2.26 Å. The Vps1 GGGDP.AlF4- crystals were also monoclinic (spacegroup P21) with cell dimensions a = 69.04, b = 121.16, c = 104.73 Å, and β = 90.62°. Reflection data were collected to a resolution of 3.1 Å. GGGDP crystals belonged to spacegroup R32 and had cell dimensions a = b = 84.98 and c = 271.50 Å. A complete dataset was collected to a resolution of 2.13 Å. Reflection data were indexed and integrated using iMOSFLM (Battye et al., 2011). All data were scaled using Aimless (Evans, 2006) from the CCP4 suite of crystallographic software (Collaborative Computational Project, Number 4, 1994). Data collection statistics are shown in Table S3.
The GGGMPPCP structure was solved by molecular replacement using Phaser (McCoy et al., 2007) as implemented in Phenix (Adams et al., 2010). The structure of Homo sapiens dynamin 1 GG bound to GMPPCP (PDB ID 3ZYC; Chappie et al., 2011) was used as a search model. Two complete dimers were present in the asymmetric unit. GGGDP.AlF4- was solved using a chain A from 3ZYC as the search model. Four copies were placed, which together created the two dimers within the asymmetric unit. GGGDP was solved using chain A from the structure of dynamin 1 GG bound to GDP.AlF4− (PDB ID 2X2E; Chappie et al., 2010). The structure had a single molecule within the asymmetric unit.
All models were completed and improved by iterative rounds of refinement using phenix.refine (Afonine et al., 2012) and COOT (Emsley et al., 2010). The structures were refined using restrained coordinate and individual B factor refinement together with parameter refinement for translation/libration/screw (TLS) groups identified using the Phenix interface. Early rounds incorporated simulated annealing. Refinement statistics and final model geometries are shown in Tables S4 and S5. Densities for the CGED helices of molecules D in both the GGGMPPCP and GGGDP.AlF4- structures were weak. All images were made using Pymol 188.8.131.52 (Schrödinger, Inc.) and UCSF Chimera (Pettersen et al., 2004). Coordinates and structure factors for GGGMPPCP, GGGDP.AlF4-, and GGGDP have been deposited in the Protein Data Bank with PDB IDs 6DEF, 6DJQ, and 6DI7, respectively.
To induce formation of Vps1 assemblies, Vps1 was diluted into assembly buffer (20 mM MES, pH 5.5, 1 mM MgCl2, and 2 mM EGTA) to yield final NaCl and protein concentrations of ∼150 mM and 0.5–1 mg/ml, respectively. Samples were incubated for the indicated periods of time.
Sample aliquots (3 µl) were adsorbed to glow-discharged 400-mesh carbon-coated copper grids and stained with 2% uranyl formate. Images were recorded on a TF20 electron microscope (FEI) equipped with a field emission gun at the indicated magnification on a 4,000 × 4,000 Gatan Ultrascan charge-coupled device camera.
3 µl of 0.5 mg/ml tubes were applied on the carbon side of glow-discharged holey R2/1 Quantifoil grids (Quantifoil Micro Tools GmbH), manually blotted from the back side, and then plunge frozen in liquid ethane using a homemade manual plunger. Images were collected at the Electron Bio-Imaging Centre at Diamond Light Source under low-dose conditions (∼40 e−/Å2 total) using a Titan Krios 300-kV microscope equipped with a Schottky X field emission gun and a Gatan Quantum energy filter with K2 Summit detector. Videos (6,426; each with 40 frames) were collected using EPU software (FEI) at a nominal magnification of 98,000 (1.06 Å/pixel) with under focus values ranging from 1.5 to 3.5 µm.
Image processing and helical reconstruction
Video frames were aligned using UCSF MotionCor2 (Zheng et al., 2017), and the resulting aligned videos were used for contrast transfer function estimation using CTFFIND4 (Rohou and Grigorieff, 2015). Micrographs were subsequently used for helical reconstruction using RELION 2.0 (He and Scheres, 2017). Helical segments were boxed using EMAN 2.0 e2helixboxer.py (Tang et al., 2007), and Fourier transforms from individual tubes or 2D class averages generated using SPRING (Desfosses et al., 2014) were used to estimate the helical parameters. A small dataset with 953 segments (500-pixel box size) was used in iterative helical real space reconstruction (IHRSR; implemented in SPIDER; Egelman, 2007; Shaikh et al., 2008) to refine the helical parameters, which converged to a rotation angle of 24.07° and a 10.48 Å rise. The full dataset containing 29,692 segments (600-pixel box size [scaled to 400], 90.41% overlap between neighboring boxes, and interbox distance 6× helical rise) was used in the helical processing workflow in RELION 2.0. The segments were analyzed by 2D classification, and classes showing clear structural details were selected for further processing (26,485 segments correspond with ∼158,000 subunits). The first round of refinement, using a featureless cylinder (400 pixels in diameter; low pass filtered to 30 Å), resulted in a map with resolution of 16.7 Å. This was used as an initial reference for the subsequent rounds of refinement, which resulted in a final density map at 11 Å after B-factor sharpening and application of a soft-edged mask. Further 3D classification did not reveal distinguishable 3D classes. The final EM map has been deposited with the EM Databank with ID code 7874.
Online supplemental material
Fig. S1 shows characterization of endosomal trafficking in Δvps1 cells. Fig. S2 shows characterization of the Vps1 K42A and G436D mutants. Fig. S3 shows biochemical characterization of Vps1. Fig. S4 shows the structures of Vps1 GG bound to GMPPCP, GDP.AlF4−, and GDP. Fig. S5 shows DRP GG alignments. Fig. S6 shows further comparison of Vps1 GG and dynamin 1 GG structures. Fig. S7 shows details of the cryoEM reconstruction of full-length C. thermophilum Vps1 assembly bound to GMPPCP. Fig. S8 shows validation of the Stalk interfaces of the Vps1 helical assembly. Table S1 shows yeast strains used in this study. Table S2 shows cell biology–related plasmids used in this study. Table S3 shows crystallographic data collection and processing. Table S4 shows refinement. Table S5 shows model geometry. Video 1 shows vacuoles in W303A cells. Video 2 shows vacuoles in Δvps1 cells. Video 3 shows localization of GFP-FYVE in W303A cells. Video 4 shows localization of GFP-FYVE in Δvps1 cells. Video 5 shows morph between GGGMPPCP and GGGDP. Video 6 shows morph between GGGMPPCP and GGGDP.AlF4-.
C. thermophilum cDNA, GFP-SNC1, and GFP-TLG2 were gifts from Ed Hurt (University of Heidelberg, Heidelberg, Germany) and Allyson O’Donnell (University of Pittsburgh, Pittsburgh, PA). We thank Willam Furey, Simon Watkins, and the Center for Biological Imaging (University of Pittsburgh, Pittsburgh, PA), and we thank Yuriy Chaban and Daniel Clare at Diamond Light Source (Didcot, UK). We thank the beamline staffs at the Southeast Regional Collaborative Access Team (SER-CAT) and the Northeastern Collaborative Access Team (NE-CAT) at the Advanced Photon Source (APS). All final reflection data were collected at the SER-CAT 22-ID beamline at the APS (Argonne National Laboratory, Lemont, IL). Supporting institutions may be found at www.ser-cat.org/members.html. Preliminary data for GGGMPPCP were collected on NE-CAT beamline 24-ID-C under the General User Proposal GUP-51113 (PI: J.S. Chappie), which is funded by the National Institute of General Medical Sciences from the National Institutes of Health (P41 GM103403).
The Pilatus 6M detector on the 24-ID-C beamline is funded by a National Institutes of Health Office of Research Infrastructure Programs High-End Instrumentation grant (S10 RR029205). This research used resources of the APS, a US Department of Energy (DOE) Office of Science User Facility operated for the Department of Energy Office of Science by Argonne National Laboratory under contract number DE-AC02-06CH11357. Use of the APS was supported by the US Department of Energy, Office of Science, Office of Basic Energy Sciences under contract number W-31-109-Eng-38. We acknowledge Diamond Light Source for access and support of the CryoEM facilities at the UK National Electron Bio-Imaging Centre funded by the Wellcome Trust, Medical Research Council, and Biotechnology and Biological Sciences Research Council (proposal EM14856-13). This study was supported by the National Institutes of Health (grants GM120102 to M.G.J. Ford and GM082251 to P. Zhang) and the UK Wellcome Trust Investigator Award 206422/Z/17/Z (to P. Zhang). J.S. Chappie is a Nancy and Peter Meinig Investigator in the Life Sciences.
The authors declare no competing financial interests.
Author contributions: N.V. Varlakhanova designed and performed experiments, analyzed and interpreted data, and wrote and revised the manuscript; F.J.D. Alvarez designed and performed experiments, analyzed and interpreted data, and revised the manuscript; T.M. Brady, B.A. Tornabene, and C.J. Hosford performed experiments; J.S. Chappie and P. Zhang provided conceptual advice, analyzed data, and revised the manuscript; M.G.J. Ford conceived the project, designed and performed experiments, analyzed and interpreted data, and wrote and revised the manuscript.
N.V. Varlakhanova and F.J.D. Alvarez contributed equally to this paper.