Open Access Article
Santiago
Sosa
ab,
Andrés H.
Rossi
a,
Alan M.
Szalai
b,
Sebastián
Klinke
ac,
Jimena
Rinaldi
a,
Ana
Farias
a,
Paula M.
Berguer
a,
Alejandro D.
Nadra
d,
Fernando D.
Stefani
be,
Fernando A.
Goldbaum
ac and
Hernán R.
Bonomi‡
*a
aFundación Instituto Leloir, IIBBA-CONICET, Av. Patricias Argentinas 435, (C1405BWE) Ciudad Autónoma de Buenos Aires, Argentina. E-mail: hbonomi@leloir.org.ar
bCentro de Investigaciones en Bionanociencias (CIBION)-CONICET, Godoy Cruz 2390 (C1425FQD), Ciudad Autónoma de Buenos Aires, Argentina
cPlataforma Argentina de Biología Estructural y Metabolómica PLABEM, Av. Patricias Argentinas 435 (C1405BWE) Ciudad Autónoma de Buenos Aires, Argentina
dDepartamento de Fisiología, Biología Molecular y Celular, Departamento de Química Biológica and IQUIBICEN-CONICET, Facultad de Ciencias Exactas y Naturales, Universidad de Buenos Aires, Ciudad Universitaria, Pabellón 2 (C1428EHA), Ciudad Autónoma de Buenos Aires, Argentina
eDepartamento de Física, Facultad de Ciencias Exactas y Naturales, Universidad de Buenos Aires, Pabellón 1 Ciudad Universitaria (C1428EHA), Ciudad Autónoma de Buenos Aires, Argentina
First published on 21st February 2019
Engineering oligomeric protein self-assembly is an attractive approach to fabricate nanostructures with well-defined geometries, stoichiometry and functions. The homodecamer Brucella Lumazine Synthase (BLS) is a highly stable and immunogenic protein nanoparticle (PNP). Here, we engineered the BLS protein scaffold to display two functions in spatially opposite regions of its structure yielding a Janus-like nanoparticle. An in silico analysis of the BLS head-to-head dimer of homopentamers shows major inter-pentameric interactions located in the equatorial interface. Based on this analysis, two BLS protomer variants were designed to interrupt pentamer self-dimerization and promote heteropentameric dimers. This strategy enabled us to generate a decameric particle with two distinct sides formed by two independent pentamers. The versatility of this new self-assembly nanofabrication strategy is illustrated with two example applications. First, a bifunctional BLS bearing Alexa Fluor 488 fluorophores on one side and sialic acid binding domains on the other side was used for labelling murine and human cells and analyzed by flow cytometry and confocal microscopy. Second, multichromophoric FRET nanoparticles were fabricated and characterized at the single molecule level, showing discrete energy transfer events. The engineered BLS variants constitute a general platform for displaying two functions in a controlled manner within the same PNP with potential applications in various areas such as biomedicine, biotechnology and nanotechnology.
Proteins are highly versatile and present diverse self-organized arrangements. Protein oligomerization depends on the primary peptide sequence as well as external conditions such as pH, temperature, ionic strength and the presence of ligands. The quaternary structure is intimately related to protein functions with a huge diversity in nature. An analysis of the quaternary arrangements of the Protein Data Bank (PDB) entries (https://www.rcsb.org/) classified by the OLIGAMI database1 reveals that approximately 47% of the catalogued proteins are monomeric and that most of the remaining form low copy number oligomers, mainly dimers (30.9%), trimers (4.6%), tetramers (8.7%) and hexamers (2.9%). In some special cases proteins form bigger complexes of, for example, 10, 12, 24 or 60 subunits. Interestingly, most of the latter structures are homopolymeric and present a high degree of symmetry.
Protein nanoparticles (PNPs) are a special subset of supramolecular protein assemblies. The PNP hallmark is a symmetric, either oligomeric or multimeric repetitive structure, sometimes conferring enhanced stability (e.g. chemical, mechanical or thermal)2,3 and high immunogenicity.4 Most of these particles derive from viral scaffold proteins such as virus-like proteins (VLPs), but some non-viral proteins, such as ferritins or small heat shock proteins, also belong to this particular protein class.5,6 In some cases, these arrangements form molecular cages able to entrap, for example, small molecules, nucleic acids7 or multiple proteins8 within their structure. These characteristics make PNPs very attractive models for bio- and nanotechnological developments. By combining protein engineering and chemical manipulation of PNPs, it has been possible to develop novel systems with potential applications in a wide range of fields including vaccine platforms,5,9 nanomedicine,10 cargo delivery11 and nanomaterials.6
The oligomeric state of polypeptides can be altered by manipulating either the external physicochemical conditions, its primary sequence or by producing chemical modifications to the scaffold. Engineering protein modules to control molecular self-assembly is a current new challenging and technologically relevant nanofabrication approach.12,13 Mutations may be predicted in a target sequence in order to produce a desired effect in an oligomer. Due to the complex nature of the protomer–protomer interaction networks and their difficulty to be accurately predicted, this strategy is particularly well suited for protein ensembles for which their molecular structure is available.
The lumazine synthase (LS, EC 2.5.1.78) enzyme, also known as RibH, belongs to the riboflavin biosynthetic pathway found in plants and microorganisms.14 The LS tertiary structure is highly conserved across taxa, even in very distant primary sequences. Strikingly, very subtle changes in the tertiary structure give rise to radically different quaternary assemblies (Fig. S1†): the Type-I LS or RibH/RibH1 group is composed of pentamers and icosahedrons, while the Type-II LS or RibH2 group encompasses only decamers.15,16 In all known LS variants, pentamers act always as the basic building blocks of these molecules. Interestingly, the icosahedral Type-I LSs have been extensively used as a model of protein cages for multiple purposes, recently reviewed by Azuma et al.17
The Brucella spp. Lumazine Synthase (BLS) is a homodecamer (Type-II LS) formed by the head-to head association of two homopentamers.15,18 BLS plays a key role in the Brucella infectious process,19 shows high thermal and chemical stability20 and elicits a strong immunogenic response in different animal models.21–27 Its disordered N-termini (first 8–10 residues of all chains) allow to genetically fuse polypeptides without affecting its structural properties, giving rise to chimeric constructs. BLS has been successfully used as a structural scaffold for vaccine design displaying a multiple variety of epitopes,28–31 ranging from linear peptides to protein domains and to entire proteins.32–34
Two strategies have been previously applied to link two different functions into the same BLS particle. One of them consists of the chemical dissociation of two different homodecameric chimeras of BLS into monomers using a chaotropic agent (for example guanidinium chloride), followed by a mixture and re-association of the monomers by dialysis.28 The second strategy is based on the genetic fusion of a set of leucine zipper peptide adaptors (leu1 and leu2), one to the BLS N-termini and the other to the proteins of interest.34 Then, by mixing leu1-BLS with the two target proteins each fused to leu2, the leucine zippers link both target proteins to BLS. In both cases, the target proteins are stochastically distributed within the scaffold, obtaining a heterogeneous population of heterodecamers.
The next step in tailoring functions of PNPs consists of organizing two or more functional moieties in exact spatial configurations within the same particle. Here, we demonstrate a redesign of the BLS into a Janus-like nanoparticle35 by generating a decameric structure built from two different pentamers. Based on structural analyses and rational design, we engineered the BLS pentamer–pentamer interface in order to (i) disrupt major interactions between homopentamers and (ii) enable the interaction between heteropentamers. Finally, we performed proof-of-concept functional assays in which we show that this novel protein scaffold presents potential uses in nanobiotechnology such as vaccine design, antigen production and imaging tool development.
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| Fig. 1 Type-II LS comparative analysis. (A) B. abortus and M. loti Type-II LS structures; PDB entries 1XN1 and 2OBX, respectively. Left panels: side view of the decameric particles. Each pentamer is differently shown in cartoon and surface representations. Right panels: top view of pentamer homodimeric interfaces. Pentamer–pentamer interacting residues are colored by type: positive (blue), negative (red), hydrophobic (green) and polar (violet). Interface interacting residues from one protomer are labeled. (B) Structural alignments of BLS (UniProt Q2YKV1, blue) and MLS (UniProt Q986N2, pink). Arrows and cylinders represent α-helices and β-sheets, respectively; interacting residues from the pentamer–pentamer interfaces (see Table 1) are highlighted. | ||
| Pair of residues | Type of interaction | Distance (Å) |
|---|---|---|
| BLS | ||
| D81-H120 | Electrostatic | 3.9 ± 0.3 |
| D81-H117 | Electrostatic | 3.5 ± 0.7 |
| I84-H118 | Hydrophobic | 3.2 ± 0.2 |
| H117-H118 | π–π stacking | 3.3 ± 0.2 |
| H120-H120 | π–π stacking | 3.2 ± 0.2 |
| E124-H132 | Electrostatic | 3.4 ± 0.6 |
| F128-F128 | Hydrophobic | 3.9 ± 0.3 |
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||
| MLS | ||
| I85-H126 | Hydrophobic | 3.6 ± 0.3 |
| Y120-H121 | Electrostatic | 3.8 ± 0.2 |
| H121-H121 | π–π stacking | 3.1 ± 0.2 |
| E125-K137 | Electrostatic | 3.1 ± 0.5 |
| R128-E132 | Electrostatic | 3.2 ± 0.4 |
In order to evaluate the significance of the role of each interface interaction, we decided to further characterize the BLS interface. For that aim, we performed thermodynamic calculations in silico by an alanine scanning strategy on all residues identified above as part of the interactions between the two pentamers, called A and B. We used the software FoldX36 to calculate Gibbs free energy between pentamers (ΔGpp) by finding local minima using a library of rotamers for each mutant (Table S2†). The ΔGpp relative changes of the alanine mutants, taking the wild-type protein (BLSWT) as the reference, are shown in Fig. 2A. Interestingly, two important sets of interactions between pentamers A and B were identified, exhibiting ΔGpp reductions of 42% and 90%, which were designated “velcro 1” (H117A and H118A) and “velcro 2” (E124A and F128A/H132A), respectively (Fig. 2A). These patches of interactions are highlighted in the BLS structure shown in Fig. 2B in more detail as two insets.
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| Fig. 2 In silico analysis of the pentamer–pentamer interface contacts in BLS. (A) Relative pentamer–pentamer interaction energy calculations between BLSWT and BLS alanine interface mutants using FoldX and PDB 1XN1 as templates. Residues from “velcro 1” and “velcro 2” are indicated as V1 and V2, respectively. Values are expressed as mean ± SD. Statistical analysis was performed by non-parametric analysis of variance (Kruskal–Wallis) followed by paired comparisons (Mann–Whitney) (*P < 0.05, **P < 0.01, ***P < 0.001). Data derive from five independent calculations. (B) The identified interactions from velcros 1 and 2 are shown in the structure of BLS. A side view of the BLS superimposing surface and the cartoon representation highlights two monomers from different pentamers with different colors. Velcros side chains are represented as sticks within the dashed box; insets show in detail the velcro 1 and velcro 2 from opposing pentamers. Residues are indicated and color coded by type: positive (blue), negative (red), hydrophobic (green) and polar (violet). | ||
| Mutant | Interface mutations | |||
|---|---|---|---|---|
| BLSDR | H117D | H118D | D127R | A131R |
| BLSKE | H117K | H118K | D127E | A131E |
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| Fig. 3 BLSDRKE pentameric interface structural model. Top view of the pentameric interfaces of BLS proteins. The wild-type residues to be substituted from BLSWT are shown in the structure (PDB 1XN1). The mutant residues from BLSDR and BLSKE were modeled using FoldX. The proteins are depicted in surface representation and the wild-type and mutant residues are represented as surfaces and sticks. Alanine, histidine, positive and negative residues are colored in cyan, violet, blue and red, respectively. Residues from one protomer are indicated. | ||
aterials and methods for details). The quaternary structure of these new proteins was first characterized by performing size exclusion chromatography (SEC) coupled to static light scattering (SLS) measurements for each mutant separately and mixed together, from which their molecular weight (MW) was determined. Fig. 4A shows the SEC elution profiles, indicating the mean MW calculated for each sample. Both BLSDR and BLSKE present higher elution volumes (smaller particles) than BLSWT, and the calculated MWs correspond to pentameric species. In accordance with our design, pre-incubation of an equimolar mix of BLSDR and BLSKE produces a new species in the SEC-SLS experiment that matches the elution volume of BLSWT with a MW of 176 ± 2 kDa, which is in agreement with a decameric structure (Fig. 4A). The BLSDRKE decameric peak was assayed again by SEC-SLS immediately after mixing (0 h) and after 24 h. In both cases, a single decameric peak was detected of approximately the same MW (Fig. 4B). This rules out the existence of a pentamer–decamer dynamic equilibrium, and allows us to conclude that the BLSDRKE heterodimer assembly is stable under these experimental conditions. Due to the electrostatic nature of the novel pentamer–pentamer interactions introduced in BLSDRKE, we wondered whether ionic strength could alter the heteropentamer dimer stability. Therefore, we pre-incubated BLSDRKE in buffers with different NaCl concentrations ranging from 0 to 2 M, and performed SEC-SLS measurements of the samples using the same buffers. All NaCl concentrations assayed yielded decameric species (Fig. 4C) similar to BLSWT, indicating a comparably high stability in both decamers under elevated ionic strength conditions.
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Fig. 4 BLSDRKE heteropentamer dimer assembly and stability. (A) The MWs of BLSWT, BLSDR, BLSKE or a 30 min co-incubation of both species (BLSDRKE) were calculated from SEC-SLS measurement elution profiles. (B) The BLSDRKE peak from (A) was collected and re-injected immediately (0 h) or after 24 h. (C) SEC-SLS BLSDRKE in 50 mM or 2 M NaCl. (A–C) Calculated MWs are indicated. (D) BLSWT and BLSDRKE decamer dissociation at pH values 4–7. The data presented correspond to the decamer : pentamer ratio calculated from SEC-SLS measurements at each pH value (see Fig. S3†). (E) FRET efficiency calculated from 520 and 570 nm signals obtained from A488BLSDR fluorescence spectra (λexc: 470 nm) incubated with increasing A555BLSKE concentrations (Fig. S4†) using eqn (1), see Materials and methods. Values are expressed as mean ± SD (n = 3). A fitting curve using eqn (2) is shown. (F) Apparent melting temperature of BLS proteins. Temperature dependence of circular dichroism molar ellipticity signal at 222 nm of BLS variants relative to 25 °C values. The graph corresponds to a representative experiment of three independent experiments. Values in the inset table are expressed as mean ± SD (n = 3). | ||
BLSWT presents a pH-dependent pentamer–pentamer dimer dissociation, with a 50% dissociation at a pH of ∼5.7 (Fig. 4D and S3†). Histidine residues are natural candidates for explaining this phenomenon. Due to the elevated amount of histidine residues participating in pentamer–pentamer contacts (25 from a total of 55 residues involved per decamer) and considering that BLSDRKE has 10 histidine residues replaced, we next evaluated whether the pH dependent stability remained unchanged. The results show that, BLSDRKE exhibits a nearly identical pH dissociation curve compared to BLSWT, with a 50% dissociation at a pH value of ∼5.7 (Fig. 4D). Thus, the replaced histidine residues H117 and H118 do not play a significant role in pentamer–decamer equilibrium driven by pH.
To further verify the interpentameric interaction, we performed a Förster resonance energy transfer (FRET) assay by conjugating donor and acceptor fluorophores on each pentamer. A point mutation was introduced at position 123 to replace a lysine residue by a cysteine residue, which was subsequently used to chemically link dyes containing maleimide groups in positions near the interface. According to the structure of BLS, the expected separation distance between donor and acceptor fluorophores ranges from 19 to 23 Å, being suitable for efficient FRET. The new cysteine mutant variants for BLSDR and BLSKE were expressed, purified and derivatized with Alexa Fluor 488 and Alexa Fluor 555, named A488BLSDR and A555BLSKE, respectively. The fluorescence spectrum of A488BLSDR incubated at increasing A555BLSKE amounts was determined under excitation at 470 nm (Fig. S4†). At higher A555BLSKE concentrations, the emission peak corresponding to the acceptor (570 nm) increases while the emission peak corresponding to the donor (520 nm) decreases. A FRET efficiency plot was derived from these values (Fig. 4E). The presence of a clear FRET effect indicates the close spatial proximity of both pentamers in the BLSDRKE particles.
Additionally, the structure and stability of BLSDR, BLSKE and BLSDRKE were assessed by temperature curves measured by circular dichroism (CD). First, we compared the CD spectra of BLS pentameric and decameric variants at room temperature, presenting similar curves with two main negative peaks at 208 and 222 nm, and a positive peak at 190–195 nm (Fig. S5A†), evidencing a combination of α/β structures with a major α-helical component. These results indicate that the mutations do not introduce significant changes in the secondary structures of BLSDR, BLSKE or BLSDRKE. Next, in order to interrogate the thermal stability of the BLS variants, their molar ellipticity signal at 222 nm was recorded as a function of temperature. The results show similar unfolding curves for BLSDRKE and BLSWT with melting temperatures (Tm) of 86.7 and 85.4 °C, respectively (Fig. 4F). BLSDR displays a thermal unfolding curve shifted towards lower temperatures and a lower Tm (75.6 °C). This result is in concordance with previous work where it was shown that the pentameric form of BLS has lower thermal stability.20 Surprisingly, BLSKE appeared to be as stable as the decameric structures. The mutational effects in BLSDR in the decameric context of the heteropentamer dimer BLSDRKE are counteracted by the interaction with BLSKE even showing a slightly enhanced Tm of ca. 2 °C compared to BLSWT (Fig. 4F).
:
200 serum dilution. The response curves from BLSDRKE and BLSKE recapitulate the BLSWT curve, while BLSDR does not induce a significant humoral response. Noteworthy, these results are reminiscent of the thermal stabilities obtained in Fig. 4F, where the heteropentamer decamer and the BLSKE pentamer both share comparable Tm values and humoral responses to BLSWT; while on the other hand, BLSDR presents both significantly lower Tm and capacity to elicit antibodies in mice.
Then, we performed two different labelling assays to demonstrate the potential, versatility and specificity of this platform. The first assay consisted of incubating a monolayer of adhered HeLa cells with VP8-BLSKE and A488BLSDR, followed by several washing steps and then visualization by confocal microscopy (Fig. 7A). Cells treated in this way display a clear fluorescent signal. Control treatment using BLSKE and A488BLSDR showed no substantial signal, indicating that the labeling is specific due to the presence of VP8 (Fig. 7A). The second labeling assay was accomplished by incubating NS0 cells in suspension with a VP8-BLSKE and A488BLSDR equimolar mixture. The cells were then washed and analyzed by flow cytometry. NS0 cells exhibited an ∼10-fold higher fluorescence signal compared to control cells treated with an A488BLSDR and BLSKE mixture (Fig. S6†). Altogether, these results indicate that the presence of the VP8 domain in the fluorescent decamer confers binding specificity to molecules of sialic acid present on the cell surface. We then assayed how the heterodecamer concentration affects the labeling. For that purpose, cell suspensions were incubated with increasing amounts of VP8-BLSKE and A488BLSDR. This experiment showed that there is a clear dependency of the signal distribution on the amount of VP8-BLSKE and A488BLSDR used in each treatment, also indicating that the system did not reach its saturation limit in the range tested (Fig. 7B).
We began to explore the use of the bifunctional BLS PNPs as a synthetic model to study multichromophoric FRET at the single molecule level (smFRET). We labeled positions 123 of the monomers of BLSDR and BLSKE with the Cy3 and Cy5 fluorescent dyes, respectively, as suitable donor and acceptor dyes for smFRET. Individual Cy3BLSDR and Cy5BLSKE pentamers were readily detected on a two-color wide-field epifluorescence microscope in total internal reflection illumination mode (TIRF), upon excitation with laser light of 532 and 642 nm, respectively (Fig. S7†). Although 10–12% of cross-talk was found in the Cy5 channel when Cy3BLSDR was excited at 532 nm, this is clearly differentiated from direct signals (Fig. S8†). The isolated Cy3BLSDR and Cy5BLSKE particles display multiple discrete fluorescence intensity steps. Approximately 10% of the PNPs showed 5 intensity steps (Fig. 8A and B), while the rest of the PNPs displayed 2, 3 or 4 fluorescence steps, indicating that the protein complexes were labeled with varying amounts of fluorophores.
The next step was to assemble the heterodecamer, positioning multiple fluorophores in the equatorial part of the molecules (Fig. 8C). For that aim, equimolar mixtures of labeled pentamers or pentamers alone were pre-incubated at room temperature prior to their deposition onto microscope coverslips. Co-incubation of Cy3BLSDR and Cy5BLSKE produced fluorescent particles with signals corresponding to Cy5BLSKE that could be detected in the Cy5 emission channel when excited with both 532 and 642 nm. These fluorescent spots also overlapped with fluorescent signals from the Cy3 emission channel under excitation at 532 nm (Fig. S8†). These results indicate that FRET indeed occurs within those doubly labeled fluorescent PNPs. The two-color emission time traces of the multichromophoric particles present complex anticorrelated signals (Fig. 8D), revealing a variety of smFRET events probably due to the different number and orientation of active fluorophores (e.g. caused by chemical bond rotations and protein backbone movements) at each given time within individual particles.
It is important to note that these new pentameric proteins conserve many of the structural properties of BLSWT and bring new characteristics that may be interesting for nanotechnological developments. When BLSKE and BLSDR are assembled into a decameric particle, it shows high temperature stability, and quaternary structure stability in a wide range of ionic strengths and at pH values over 5.5. Decameric BLSDRKE also conserves the intrinsic immunogenicity of BLSWT, which makes this system useful for vaccine engineering. In this sense, the BLS scaffold has been demonstrated to be successful for displaying foreign antigens, which has led to the patenting of this technology.43,44 In this work, we have expanded its capabilities, bringing the possibility to display two types of antigens (i.e. for multivalent vaccines) or an antigen and an immunomodulator (i.e. for immunomodulatory antigen delivery systems) within the same particle. On the other hand, the cellular labeling assays performed in this work indicate that the engineered versions of BLS could eventually be used as diagnostic or therapeutic tools.
DNA origami technology has recently become a powerful nanofabrication tool. However, achieving 3D or rigid structures using DNA is challenging due to the intrinsic flexibility of DNA. Proteins, on the other hand, can present naturally rigid and thermally stable tertiary and quaternary structures. Here, we have demonstrated that BLS and its variants can be used as versatile nanometric scaffolds to organize various molecular entities in space. In addition to the multivalent fluorescent labeling, we have used bifunctional PNPs to construct a multichromophoric energy transfer system, a highly challenging task as it requires the organization of multiple molecules at separation distances of 1–3 nm. Model systems in which the location and distances between chromophores are well controlled at this scale are powerful tools to understand in deeper detail photosynthetic processes and/or to engineer artificial photosynthetic structures.
In summary we have presented a new method for devising asymmetric, bifunctional PNPs with clear potential applications in (bio)nanotechnology. As we gain detailed knowledge of protein structures and interactions, new nanofabrication avenues through biomolecular self-assembly analogous to the one here presented will be opened.
In silico thermodynamic stability studies and complex formation were carried out using the FoldX program (http://foldxsuite.crg.eu/). The PDB 1XN1 model was used as a template for all BLS in silico mutations. An alanine scanning was performed in all residues identified in the pentamer dimer interface using CoCoMaps. For each residue, mutations were made in all monomers at the same time. Each mutation was performed 5 times and the contribution to the total interaction energy between pentamers was calculated as the average. The set of selected mutations to simultaneously disrupt the self-interactions between mutant pentamers and to favor heteropentamer interactions are shown in Table 2. BLSDR, BLSKE and BLSDRKE mutant decamers were analyzed using FoldX Stability and AnalyzeComplex functions.
The VP8-BLS fusion construct was achieved first by PCR amplification of the 18 kDa sialic acid binding domain product from the C486 bovine rotavirus (BRV) VP8 core protein (VP8d), including the pentapeptide linker GSGSG, using Pfx DNA polymerase (Invitrogen), specific primers with homologous ends to the target plasmid and the pVP8-BLS plasmid as templates. The pVP8-BLS plasmid was kindly provided by Dr Patricio Craig.29 Then, the 0.5 kbp VP8d amplicon was used as the primer in a whole plasmid amplification PCR using the Q5 High-Fidelity DNA Polymerase and the pBLSKE plasmid as templates. Similarly as explained above, the reaction was treated with DpnI and transformed into E. coli DH5α cells. Clones carrying the 1.0 kbp fragment from the VP8d-linker fused to the BLSKE N-terminus at residue number 7 were screened using PCR and confirmed by Sanger sequencing, resulting in the pVP8-BLSKE plasmid (Table S1†).
For full details on the protein sequences used in this work see section “BLS protein sequences” in the ESI.†
000 g for 30 min. The soluble fraction was purified using a Q-Sepharose column (GE Healthcare Life Sciences) in a fast performance liquid chromatography apparatus (Gilson) with a 0–1 M NaCl linear gradient in 50 mM Tris pH 8.0. The samples enriched in BLS proteins were further purified on a Superdex-200 column (GE Healthcare Life Sciences) in 50 mM Tris–HCl pH 8.0, 0.25 M NaCl buffer. Each step was monitored by 15% SDS-PAGE. BLS proteins were concentrated up to 1–10 mg ml−1, flash-frozen in liquid N2, and stored at −80 °C for future use.
![]() | (1) |
A fitting to FRET efficiency was performed assuming a simplified model of one-to-one interaction between A488BLSDR and A555BLSKE using the following equation:45
![]() | (2) |
smFRET was carried out using a microscope home-built around an Olympus IX-73 body, operating in wide-field epifluorescence mode. Two color images were acquired with an oil immersion objective Olympus PlanApo 60x NA 1.42. Total internal reflection illumination mode (TIRF) was enabled by moving a linear stage (Thorlabs) so that the focus of the lasers translated laterally within the back focal plane of the objective. Fluorescence emission from Cy3 and Cy5 was separated with a dichroic mirror (Chroma ZT647rdc), filtered with bandpass emission filters (Semrock 582/75 BrightLine HC and Chroma ET700/75m) and imaged onto adjacent areas of the EMCCD camera operated at −50 °C (Andor iXon3 897). The camera and the lasers were controlled with custom software previously described.46 A 642 nm 1.5 W laser (MPB Communications, 2RU/VFL/P/1500/642) and a 532 nm 1.5 W laser (Laser Quantum, ventus 532) were used for fluorescence excitation of Cy5 and Cy3, respectively. The lasers were combined with dichroic mirrors (Semrock LM01-427, LM01-552 and Di03-R405/488/532/635-t1) and then focused to the back focal plane of the objective. Further blocking of the illumination lasers was performed with a multi-edge notch filter (Semrock NF03-05/488/532/635E). Laser power densities used during acquisition were 555 W cm−2 and 610 W cm−2 for 532 and 642 nm, respectively. A Pre-Amp Gain of 5.1 and an EM Gain of 50 were used in the CCD camera. Different regions of 128 × 128 pixels (∼290 μm2) were observed using 100 ms exposure times. Single molecule time traces were achieved after background subtraction, using a region of interest of 5 × 5 pixels (∼0.44 μm2). Cross-talk was characterized in samples containing either Cy3 or Cy5, and was then used to correct Cy3 and Cy5 traces. Differences between the two channels were corrected by imaging isolated fluorescent markers visible on both channels (Life Technologies Tetraspeck 0.1 μm) and then finding the affine transformation that minimizes the distance between the same markers as detected in each detection channel as previously described.46
Footnotes |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c8na00375k |
| ‡ Current address: Centre de Biochimie Structurale, CNRS UMR5048, INSERM U1054, Université de Montpellier, 29 rue de Navacelles (34090), Montpellier, France. |
| This journal is © The Royal Society of Chemistry 2019 |