Abstract
Pseudopilins form the central pseudopilus of the sophisticated bacterial type 2 secretion systems. The crystallization of the EpsI:EpsJ pseudopilin heterodimer from Vibrio vulnificus was greatly accelerated by the use of nanobodies, which are the smallest antigen-binding fragments derived from heavy-chain only camelid antibodies. Seven anti-EpsI:EpsJ nanobodies were generated and co-crystallization of EpsI:EpsJ nano-body complexes yielded several crystal forms very rapidly. In the structure solved, the nanobodies are arranged in planes throughout the crystal lattice, linking layers of EpsI:EpsJ heterodimers. The EpsI:EpsJ dimer observed confirms a right-handed architecture of the pseudopilus, but, compared to a previous structure of the EpsI:EpsJ heterodimer, EpsI differs 6° in orientation with respect to EpsJ; one loop of EpsJ is shifted by ~5 Å due to interactions with the nanobody; and a second loop of EpsJ underwent a major change of 17 Å without contacts with the nanobody. Clearly, nanobodies accelerate dramatically the crystallization of recalcitrant protein complexes and can reveal conformational flexibility not observed before.
Keywords: General secretory pathway, Pseudopilins, Single-chain antibody, Crystallization chaperones
1. Introduction
Of all the bottlenecks of structure determinations through X-ray crystallography, arguably, the most critical is the actual production of crystals. Thus far, numerous techniques have been developed to circumvent this major obstacle. Natural partner proteins can greatly improve the probability of obtaining crystals by stabilizing the protein of interest, and by creating additional crystal contact surfaces. However, not all proteins have natural partners with whom they interact strongly, or these partners are not yet known, therefore alternative binders has been explored, including “Designed Ankyrin Repeat Proteins” (DARPins) (Huber et al., 2007; Stumpp and Amstutz, 2007), and a diversity of antibody domains, in particular Fab's (Kovari et al., 1995) and single-chain Fv's (Essen et al., 2003; Hunte and Michel, 2002).
The occurrence of bona fide antibodies devoid of light chains in camelidae (Hamers-Casterman et al., 1993) is at the origin of major new developments in antibody technology (Muyldermans et al., 2001). These so-called heavy-chain antibodies bind antigens solely with one single variable domain, referred to as VHH or nanobody (Nb). The single-domain antigen-binding fragments are smaller (~12–15 kDa) and have several advantages compared to their larger antibody counterparts in terms of stability (Perez et al., 2001; van der Linden et al., 1999), expression yield, protease resistance, solubility (Whitlow et al., 1993) and cost (Wolfson, 2006).
The nanobodies in the crystal structures available so far exhibit the classical immunoglobulin fold, with a scaffold of nine anti-parallel β-strands forming two sandwiching β-sheets. At the time of this study, there are structures reported of 22 protein camelid nano-body complexes (De Genst et al., 2004, 2005, 2006; Decanniere et al., 1999, 2001; Desmyter et al., 2001, 2002, 1996; Dolk et al., 2005; Dumoulin et al., 2003; Koide et al., 2007; Loris et al., 2003; Spinelli et al., 2006; Tegoni et al., 1999; Tereshko et al., 2008; Transue et al., 1998). Of all the protein-nanobody complexes, only two proteins had no previous available structure prior to solving the complex with the nanobody: MazE and phage p2 RBP (Loris et al., 2003; Spinelli et al., 2006). While the purpose of the VHH of the VHH:phage p2 RBP structure was to identify the receptor-binding site, the VHH:MazE structure, in which only 44 of the 98 amino acids of MazE were ordered, is the only case reported in which the nanobody was used for stabilization and crystallization of a novel protein.
The nanobody antigen-binding loops have a more diverse repertoire than the canonical antigen-binding loops seen in traditional human and mouse antibodies (Decanniere et al., 2000). Each nanobody has three hypervariable loops, called complementarity determining regions (CDRs), which are apposed to each other and often interact with the antigen. For nanobodies, the CDR3 commonly makes the most contacts with the antigen which is likely due to its exceptional length (16–18 amino acids versus typically 9 amino acids in mouse and 12 amino acids in human antibodies) and sequence variability (Muyldermans et al., 2001; Revets et al., 2005). Interestingly, not all three CDRs need to interact with the antigen for binding to occur. The current study focuses on the complex of a nanobody with a heterodimer from a protein secretion system. Many pathogenic bacteria secrete a diversity of proteins, including bacterial toxins, from the periplasm into the extracellular milieu via an intricate, two-membrane spanning, multi-protein machinery called the “Type 2 Secretion System” (T2SS) or the “General Secretory Pathway” (Cianciotto, 2005; Filloux, 2004; Overbye et al., 1993; Sandkvist et al., 1997; Tauschek et al., 2002). The T2SS is also referred to as the “Extracellular Protein Secretion” (Eps) system in Vibrio species (Sandkvist et al., 1997). In Vibrio cholerae, the causative agent of cholera, the T2SS protein machinery translocates the ~85 kDa cholera toxin and several unrelated proteins in their folded state into the lumen of the gut (Bortoli-German et al., 1994; Cianciotto, 2005; Connell et al., 1995; Hardie et al., 1995; Hirst and Holmgren, 1987; Pugsley, 1992; Sandkvist, 2001b).
In Vibrio species the T2SS is assembled from 11 different proteins, many of these being present in multiple copies (Filloux, 2004; Sandkvist, 2001a; Sandkvist et al., 2000). The T2SS can be thought of as consisting of three major components: (i) the “secretin” EpsD, which forms a protein-conducting pore in the outer membrane; (ii) the “pseudopilins” in the periplasm (EpsG, EpsH, EpsI, EpsJ, and EpsK) assembled into a filamentous “pseudopilus”; and (iii) the “inner membrane platform”. In our attempts to enhance the understanding of the architecture and functioning of the T2SS machinery we have solved previously crystal structures of several T2SS proteins (Johnson et al., 2006; Korotkov and Hol, 2008; Korotkov et al., 2006; Yanez et al., 2008a, 2008b).
Importantly, unraveling three-dimensional structures of the T2SS secretion machinery also assists in understanding aspects of the Type 4 Pilus Biogenesis (T4PB) system (Filloux, 2004; Hobbs and Mattick, 1993; Peabody et al., 2003). The pilins and pseudopilins share a highly variable Type 4a Pilin fold which consists of a long N-terminal α-helix, a variable region, and a conserved C-terminal β-sheet (Craig and Li, 2008). In the T2SS, EpsG is called the “major” pseudopilin because it is the predominant protein component of the pseudopilus. EpsH, EpsI, EpsJ and EpsK are present in lesser amounts and are therefore known as the “minor” pseudopilins. These proteins are thought to form the piston-like pseudopilus that pushes the secreted proteins out of the bacteria and/or may function as a plug for the outer membrane pore (Filloux et al., 1998; Mattick and Alm, 1995; Sandkvist, 2001a; Sauvonnet et al., 2000).
The EpsI:EpsJ heterodimer had previously proven to be very difficult to crystallize, requiring a combination of species variation, surface entropy reduction mutagenesis, and N- and C-terminal truncations (Yanez et al., 2008b). Here we report how nanobodies assisted in obtaining crystals almost immediately of a variant of the heterodimer which had never given a crystal hit before. It appears that the nanobody promoted crystal formation by forming layers of nanobodies interspersed by layers of EpsI:EpsJ heterodimers.
2. Materials and methods
2.1. Cloning, expression, and purification of EpsI and EpsJ
Soluble domains of Vibrio vulnificus EpsI and EpsJ, with the first 24 residues of both chains truncated, were obtained as previously described in Yanez et al. (2008b). Briefly, EpsI:EpsJ, with the EpsI containing an N-terminal TEV-cleavable hexahistidine (His6) tag, were cloned into pCDF-NT, a modified pCDFDuet-1 vector (Novagen). The proteins were co-expressed in Escherichia coli BL21(DE3) (Novagen) cells that were grown at 30 °C until A600 = 0.6, induced with 0.5 mM IPTG. After 4 h of expression at 25 °C, the cells were harvested, lysed using French press, and centrifuged at 20,000g for 40 min to clarify the lysate. The EpsI:EpsJ protein complex was purified with IMAC using Ni-NTA resin (Qiagen), TEV His6 cleavage, followed by an additional pass through the Ni-NTA resin. Finally a Superdex 75 HR10/30 size-exclusion column (GE Health-care), equilibrated in 20 mM Tris-HCl (pH 7.8), 250 mM NaCl, 1 mM EDTA was utilized as a final polishing step.
2.2. Nanobody generation
A llama (Lama glama) was injected several times with in total 2 mg of purified EpsI:EpsJ complex. The immunization, library construction and selection have been performed following standard procedures (Conrath et al., 2001), with minor modifications: total RNA was extracted from the peripheral blood lymphocytes (Chom czynski and Sacchi, 1987), 50 lg of total RNA was used to prepare cDNA using SuperScript II (Invitrogen) and a dN6 primer according to the manufactures instruction. Finally, all selected nanobody genes were cloned in a pHEN6 vector for expression with a Histag in E. coli (Conrath et al., 2001).
2.3. Solid-phase ELISA
Maxisorb 96-well plates (Nunc) were coated with EpsI:EpsJ complex preparations overnight at 4 °C at 1 μg/ml in sodium bicarbonate buffer pH 8.2. Residual protein binding sites in the wells were blocked for 2 h at room temperature with 2% milk in PBS. Detection of antigen-bound nanobodies was performed with a mouse anti-haemaglutinin-decapeptide-tag (clone 16B12, BAbCO) or a mouse anti-histidine-tag (Serotec), as appropriate. Subsequent detection of the mouse anti-tag antibodies was done with an alkaline phosphatase anti-mouse-IgG conjugate (Sigma), respectively. The absorption at 405 nm was measured 15 min after adding the enzyme substrate p-nitrophenyl phosphate.
2.4. EpsI:EpsJ and nanobody complex formation
The purified EpsI:EpsJ complex was incubated with the purified nanobody (Nb11) at room temperature for 30 min. The EpsI:EpsJ:Nb11 complex was then concentrated to 10 mg/ml and then separated from uncomplexed proteins via size-exclusion column chromatography, and concentrated to 8–10 mg/ml for crystallization experiments.
2.5. Crystallization
After mixing 1 μl of the EpsI:EpsJ:Nb11 protein solution with 1 μl of precipitant, plate-like crystals of EpsI:EpsJ:Nb11 grew readily in several conditions from the Index Screen (Hampton Research). While many crystals did not yield adequate diffraction, the best diffracting crystals came from 25% PEG 3350, 0.1 M ammonium sulfate, and 0.1 M Bis-Tris, pH 5.5. Crystals were cryo-protected with the mother liquor plus 1% PEG 400. Remarkably, 5% PEG 400, other PEGs, and glycerol destroyed the diffraction power of these crystals. Crystals were flash-frozen in liquid nitrogen and sent for data collection at SSRL beamline 9-2.
2.6. Structure determination
Data sets were collected at the 9-2 beamline of the Stanford Synchrotron Radiation Laboratory (SSRL) on a MarUSA MarMosaic-325 CCD detector. Data extending to 2.58 Å were processed with XDS (Kabsch, 1993).
The EpsI:EpsJ:Nb11 structure was solved using a multi-step procedure that included molecular replacement and model building. Phaser (McCoy et al., 2007) was used for molecular replacement using EpsI:EpsJ (Yanez et al., 2008b) as a search model for EpsI:EpsJ, and the antibody 2B2X (Clark et al., 2006; 72.4% amino acid sequence identity) after removal of the CDR regions as a search model for the nanobody. Although Phaser did not find a solution for the nanobody, the best EpsI:EpsJ solution from Phaser was used for further density modification (DM) in CCP4 (Collaborative Computational Project, 1994). The density maps obtained by density modification were submitted into RESOLVE (Terwilliger, 2004) for automatic model building. After RESOLVE built two substantial β-strands of the nanobody (Tyr32-Arg38 and Ala96-Arg107), superposition of 2B2X was possible using the SSM superpose command of the graphics program Coot (Emsley and Cowtan, 2004). The superimposed 2B2X molecule was merged into the same model as EpsI:EpsJ and subjected to rigid body and restrained refinement in REFMAC5 (Murshudov et al., 1997). CNS annealing was employed in the initial stages (Brünger et al., 1998), followed by rounds of REFMAC with TLS refinement with seven TLS groups for each chain of EpsI and EpsJ as determined by the TLS motion determination (TLSMD) server (Painter and Merritt, 2006). REFMAC refinement with medium main-chain and medium side-chain NCS restraints was alternated with manual model building with Coot. The stereochemical quality of the model was verified using Molprobity (Lovell et al., 2003) and PROCHECK (Laskowski et al., 1993). Final structure determination and refinement statistics are listed in Table 1.
Table 1.
V. vulnificus Epsl:EpsJ:Nb11 | |
---|---|
Data set | |
Wavelength (Å) | 1.12709 |
Space group | P1 |
a (Å) | 46.8 |
b (Å) | 67.4 |
c (Å) | 128.6 |
α | 96.7° |
β | 91.6° |
γ | 90.2° |
Unique reflections | 49,095 |
Resolution (Å) | 20–2.58 (2.68–2.58)b |
Completeness (%) | 90.0 (71.0) |
Redundancy | 2.0 (2.0) |
Rmerge (%) | 12.9 (59.1) |
I/σ | 14.8 (2.7) |
Wilson B-factor (Å2) | 55.1 |
Refinement a | |
Resolution (Å) | 20–2.58 |
Reflections used | 44,423 |
Heterotrimers per unit cell | 4 |
Residues per unit cell | 1397c |
Atoms | 11,238 |
Waters per unit cell | 156 |
Chloride ion per unit cell | 4 |
Rwork (%) | 23.2 |
Rfree (%) | 27.9 |
R.m.s.d bond lengths (Å2) | 0.006 |
R.m.s.d. bond angles (°) | 0.849 |
B-average (Å2) | 66.0 |
EpsI | 66.6 |
Epsj | 66.0 |
Nb11 | 65.4 |
B-water (Å2) | 62.9 |
Ramachandran | |
Most favored | 97.1% |
Additionally allowed | 2.7% |
Disallowed | 0.2% |
Refinement statistics are based on Refmac5 values.
Values in parentheses refer to outer shell.
A total of 1397 out of 1636 residues were built into the electron density for the final EpsI:EpsJ:Nb11 model. Parts of the N- and C-termini were not present in the electron density and were omitted from the model. Poor electron density was observed for several loop regions, therefore the following residues were not included in the final structure: EpsI Pro55 and Leu86 in chain A, Lys56, Gln83, and Pro84 in chain D. Leu58, Thr81-Leu85 and Ala99 in chain G; for Epsj Glu69-Pro70 in chain B, Gly67-Pro70 and Gln102-Phe103 in chain E, Glu69-Ser71 in chain H, and Asn66-Glu69 and Pro104-Arg105 in chain K; in Nb11 only Va112-Gln13 in chain L.
3. Results
3.1. VHH library construction and selection of specific binders
The VHH repertoire of the library resulting from the immunization was expressed on phages following procedures and selection of phage particles expressing an EpsI:EpsJ binding VHH as detailed in Section 2. A clear enrichment was observed after three consecutive rounds of selection on solid-phase coated antigen. Twice 48 randomly chosen colonies—after the second and third round—were grown for expression of their VHH as soluble protein. Of the crude periplasmic extracts tested in an ELISA, 46 were shown to be specific towards the EpsI:EpsJ complex. After HinfI/RFLP and sequence analysis on the VHH genes amplified from the clones positive in ELISA, 11 different nanobodies against the EpsI:EpsJ complex were identified. Seven of these were expressed and purified.
3.2. EpsI:EpsJ:nanobody complexes in solution
A complex of N-terminally histidine-tagged, N-terminally truncated EpsI(25–117):EpsJ(25–217) from V. vulnificus (hereafter referred to as “EpsI” and “EpsJ”, respectively) was incubated with each of the seven nanobodies in a 1:1 molar ratio to test complex formation in vitro. For four of the seven nanobodies this was successful according to native gel analysis (Fig. 1B). These four ternary EpsI:EpsJ:nanobody complexes were subsequently prepared, purified and subjected to crystallization trials. The protein–nanobody complex of EpsI:EpsJ with NbEpsIJ-11 (hereafter called Nb11) yielded well-diffracting crystals very rapidly. Throughout the remainder of the study, the residue numbering referred to in the text corresponds to the continuous numbering in the PDB file as seen at the top of the sequence alignment in Fig. 1A. To translate this residue numbering of the nanobody to the standard ImMuno-GeneTics (IMGT) numbering for immunoglobulins (Lefranc, 2005; Lefranc et al., 2003), refer to the lower line of the sequence alignment in Fig. 1A.
3.3. Structure solution
The EpsI:EpsJ:Nb11 crystals belong to space group P1, with four copies of the EpsI:EpsJ:Nb11 heterotrimer per unit cell, containing 1397 well-defined amino acids out of 1636 residues in total (Fig. 2A). The EpsI:EpsJ:Nb11 structure was refined to an Rwork = 23.2% and Rfree = 27.9% with good geometry (Table 1). The Cα carbons of the four EpsI:EpsJ:Nb11 heterotrimers per cell can be superimposed with pairwise root mean square deviations (RMSD) between 0.5 and 0.6 Å. Since these structures are so similar, one trimer (consisting of Chain A for EpsI, Chain B for EpsJ and Chain C for Nb11) will be the main ternary complex analyzed in the rest of this report.
3.4. The structure of Nb11 and its CDRs
The four nanobody molecules per triclinic unit cell are very similar in structure with RMSD's ranging from 0.1 to 0.4 Å for 109–111 Cα atoms. Overall, the structure of Nb11 follows the classical immunoglobulin scaffold seen in other nanobody structures to date. Comparison of the Nb11 structure with the VH domain of the closest structural neighbor 1IGT, an intact IgG2a monoclonal antibody (Harris et al., 1997), shows that the major regions of difference involve CDR3 (Supplementary Figure S2). The closest nano-body DALI match among nanobodies of known structure is 1ZVH (De Genst et al., 2006) with a sequence identity of 63%, and an RMSD of 1.5 Å (Supplementary Figure S2).
The CDRs in our structure appear to display excellent electron density, allowing an evaluation of the CDR conformations to see if they adopt one of the canonical types that have been previously defined (Al-Lazikani et al., 1997; Chothia and Lesk, 1987; Chothia et al., 1992). The conformations of both of CDR1 and CDR2 from Nb11 can be classified as canonical type 1 in their respective hypervariable region repertoires.
CDR3 in Nb11 consists of Ala96-Asp106 and changes its direction at the point where β-strand F begins, by ~130°, and terminates prior to the beginning of strand G (Figs. 2B, 3 and 4B). The conformations of CDR3 are more difficult to classify since CDR3's are longer and more variable than CDR1 and CDR2. In one study conformations of CDR3's were separated into β-hairpins with either a kinked base, a kinked base with an additional bulge, or an extended base (Shirai et al., 1996). A more recent CDR3 classification divides structures into three classes based on the “torso” and “head”: (1) torso with a β-bulge; (2) torso with regular β-sheet hairpin rather than β-bulge structure; (3) short regions that form short hairpins (Morea et al., 1998). The torso is formed by a two-stranded anti-parallel β-sheet composed of the first five and last six residues of the loop. All residues not in the torso make up the head of the CDR3 loop (Decanniere et al., 1999). The Nb11 structure seen here adheres to the torso with a β-bulge class in an extreme manner, with CDR3 folding over the framework and directing its β-strands perpendicular to the CDR1 and CDR2 β-strands (Fig. 4, Supplementary Figures S2B and C).
3.5. EpsJ:Nb11 interactions
The EpsJ:Nb11 interface buries 1461 Å2 solvent accessible surface, close to the average of 1554 Å2 buried surface for antibody-protein complexes (Jones and Thornton, 1996). The tightness of the interface can be judged with the gap volume index which is a measure of the complementarity of surfaces (Jones and Thornton, 1996). In the case of the of the EpsJ:Nb11 interface, the gap volume index is 2.6 Å, which is below the average gap volume index of 3.0 Å for antibody-protein complexes (Jones and Thornton, 1996). EpsJ buries 731 Å2 in the EpsJ:nanobody interface which is ~8% of its total accessible protein surface involving 26 interface residues in EpsJ (interactions are described in the Supplementary Text). The interacting residues on EpsJ are all from the first β-sheet of the so-called “variable region” that includes strands β1–β5.
A total of 22 residues from Nb11 are engaged in contacts with EpsJ (Figs. 1A and 4B; Supplementary Table 1). CDR1 and CDR2 make rather minor contacts, burying 121 Å2 and 87 Å2, respectively. CDR3 buries 478 Å2 surface area, providing the majority of the interface. CDR3 serves as the primary binding loop to EpsJ by burying itself into an extensive pocket formed by the βA–βB, β4–bβ and β1–β5 loops of EpsJ (Fig. 4). This EpsJ pocket contains several charged residues that are complementary with the charged residues on CDR3, as described in the Supplementary Text.
4. Discussion
4.1. The EpsI:EpsJ:Nb11 complex reveals structural changes that may be relevant to pseudopilus function
It is of interest to compare EpsI, EpsJ as well as the EpsI:EpsJ heterodimer in our current structure (Fig. 2B) with those of the V. vulnificus EpsI:EpsJ structure described by Yanez et al. (2008b) since this is the first time the effect of nanobody binding on a heterodimer can be evaluated.
The two structures of EpsI from these two studies superimpose with an RMSD of 0.7 Å for 75 equivalent Cα atoms. The major differences reside in flexible loops with the largest divergence at Asn57 with a shift of 3.8 Å for the Ca atoms between the two structures.
The EpsJ molecule in the current structure superimposes with EpsJ in the previous structure of Yanez et al. (2008b), with an RMSD of 0.9 Å for 152 equivalent Cα atoms, but this requires ignoring two loops which are very different in conformation:
-
(i)
In the heterodimer without nanobody, the β2–β3 loop is in an extended conformation in all four EpsJ molecules, whereas this loop in is bent by almost 90° in all four EpsJ molecules of the current EpsI:EpsJ:nanobody crystals (Fig. 3). At the Cα of Gln100, the loop deviates by more than 16 Å if we compare both complexes. The functional implications of this dramatic change in conformation of the β2–β3 loop in the two crystal forms remain unclear but might indicate structural changes pseudopilins are likely to undergo during assembly into a pseudopilus or during transport of secreted proteins out of the cell by the T2SS.
-
(ii)
The β4–β5 loop (Trp125-Val137) with a largest difference of 4.8 Å at the position of Pro128 (Fig. 3). This β4–β5 loop difference is probably due to interactions of the loop with the nanobody in the EpsI:EpsJ:Nb11 structure, with the nanobody causing these residues to adopt an altered and well-defined conformation in the ternary complex (Figs. 3 and 4; Supplementary Text). In contrast, several residues (Ala132-Gly133) from this loop are highly flexible in the previous EpsI:EpsJ structure (Yanez et al., 2008b).
Our new structure allows a comparison of the entire EpsI:EpsJ heterodimer in the current EpsI:EpsJ:Nb11 ternary complex (Fig. 2B) with the V. vulnificus EpsI:EpsJ heterodimer described by Yanez et al. (2008b). When excluding the two major deviating loops in EpsJ discussed above, the two heterodimers can be superimposed with an RMSD of 1.1 Å for 218 equivalent Cα atoms. In both structures, the arrangement of EpsI and EpsJ corresponds with a right-handed nature of the T2SS pseudopilus (Korotkov and Hol, 2008; Yanez et al., 2008b), a key element of the T2SS for which right-handed and left-handed arrangements have been proposed (Craig et al., 2006; Köhler et al., 2004). The orientation of EpsI versus EpsJ differs by approximately 6° in the two heterodimers (Fig. 3). This flexibility might be important during the assembly and/or functioning of the dynamic piston-like pseudopilus in the central periplasmic space of the T2SS.
4.2. Nanobodies can promote crystal growth in multiple ways
Yanez et al. (2008b) recently described the difficulties which had to be overcome to obtain suitable crystals for the structure determination of the EpsI:EpsJ heterodimer. Compared to the approximately 10 months and 17 protein variants it had taken to start from EpsI:EpsJ and to arrive at well-diffracting crystals of the mutated and truncated form, crystallization of wild-type N-terminally truncated EpsI:EpsJ in complex with nanobody Nb11 merely took 15 days. A total of 192 crystallization conditions were tested. Only optimization of the cryoprotectant was required.
Several of the four nanobodies shown to bind to EpsI:EpsJ (Fig. 1B) gave crystals with both N- and C-terminal His6-tagged EpsI:EpsJ; however the crystals with Nb11 that lead to structure determination were the best diffracting and required no optimization. Interestingly, the most robust crystal producing complex contained an EpsI variant with a cleaved N-terminal His6-tag. This variant of EpsI:EpsJ had formerly, without Nb11, given no crystal hits whatsoever. Clearly, the addition of a nanobody converted a protein that was very difficult to crystallize into a complex which could be crystallized to diffraction quality within days.
Crystal contacts between nanobodies from neighboring EpsI:EpsJ:Nb11 heterotetramers bury 464 Å2 solvent accessible surface, involving 10 residues from each nanobody (Figs. 1A and 4B). Essentially all these contacts are provided by framework side chains. Fig. 5 shows how Nb11 assists in crystal packing: layers of nanobodies contacting each other traverse the crystal linking layers of EpsI:EpsJ heterodimers.
It is of interest to compare the way by which nanobody Nb11 promotes crystallization of the V. vulnificus EpsI:EpsJ heterodimer with the way by which another nanobody, NbGspD-7, facilitated crystal formation of the flexible periplasmic domain of the T2SS secretin GspD (“peri-GspD”) as described by Korotkov et al., in press. In the latter case, NbGspD-7 generates a compact heterotetramer formed by two nanobodies and two peri-GspD chains. Even though NbGspD-7 also engages in crystal contacts with adjacent tetramers, the main effect of this nanobody on the crystal growth in this case is most likely a decrease of the conformational freedom of its target protein with a concomitant increase of the crystallization probability.
These two cases of substantial acceleration of crystal growth of two recalcitrant proteins are therefore achieved mainly by “gluing” in the case of Nb11 and by “freezing” in the case of NbGspD-7. Future studies are needed to evaluate which of these modes of operation will be predominant in general. Both nanobodies accelerated crystal growth dramatically and this bodes well for future applications of nanobodies as “crystallization chaperones”.
5. Protein Data Bank accession codes
The atomic coordinates and structure factors have been deposited in the RCSB Protein Data Bank and are available under accession code 3CFI.
Supplementary Material
Acknowledgments
We thank Jürgen Bosch, Stewart Turley, and Jan Abendroth for help and valuable discussions. We thank Nele Buys for the selection, expression and purification of the nanobodies. We are indebted to the support staff of beamline 9-2 of the SSRL for assistance during data collection. Portions of this research were carried out at the Stanford Synchrotron Radiation Laboratory (SSRL), supported by the Department of Energy and by NIH. This work was supported by Grant AI34501 from the NIH, by the Howard Hughes Medical Institute (HHMI) to W.G.J.H., and University of Washington's Molecular Biophysics Training Grant (5 T32 GM008268-19) from the NIH. This work was also supported by the Belgian Government under the framework of the Interuniversity Attraction Poles (I.A.P. P6/19).
Footnotes
Appendix A. Supplementary data Supplementary data associated with this article can be found in the online version, at doi:10.1016/j.jsb.2008.11.008.
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