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Vol. 20, Issue 21, 4620-4628, November 1, 2009
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*Institut für Biochemie und Molekularbiologie, ZBMZ,
Fakultät für Biologie, Albert-Ludwigs-Universität, 79104 Freiburg, Germany;
Groningen Biomolecular Sciences and Biotechnology Institute, University of Groningen, 9747 AG Groningen, The Netherlands; and
Fakultät für Biologie, Universität Bielefeld, D-33501 Bielefeld, Germany
Submitted April 20, 2009;
Revised September 10, 2009;
Accepted September 15, 2009
Monitoring Editor: Reid Gilmore
| ABSTRACT |
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1.6–2.2 MDa. Six different types of rings were found with an unusual 12–17-fold symmetrical conformation. The simultaneous existence of multiple types of rings is very unusual and suggests a special function of Vipp1. Involvement of diverse ring structures in vesicle formation is suggested. | INTRODUCTION |
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For biogenesis of thylakoid membranes many cellular processes, like lipid biosynthesis, membrane formation, protein synthesis in the cytoplasm and/or at a membrane, protein transport, protein translocation, and protein folding have to be organized, chronologically aligned, and controlled. Although for many years genes and proteins specifically involved in formation and biogenesis of thylakoid membranes remained unidentified, in 2001 a protein was described that could be involved in thylakoid membrane biogenesis in plant chloroplasts and cyanobacteria (Kroll et al., 2001
; Westphal et al., 2001
). The observation that deletion of the open reading frame hcf155 in Arabidopsis thaliana resulted in a complete absence of thylakoid membranes indicated that the encoded protein is involved in thylakoid membrane biogenesis. Further analysis has suggested that the protein might be involved in vesicle trafficking between the inner envelope and thylakoid membranes of chloroplasts (Kroll et al., 2001
). Consequently, the protein was named vesicle-inducing protein in plastids 1 (Vipp1). Depletion of Vipp1 in the cyanobacterium Synechocystis PCC 6803 strongly affected the ability of cyanobacterial cells to form thylakoid membranes (Westphal et al., 2001
) and consequently, also in cyanobacteria Vipp1 appears to be involved in thylakoid membrane formation. A Vipp1 depletion strain of A. thaliana is deficient in photosynthesis, and the defects appeared to be caused by dysfunction of the entire photosynthetic electron transfer chain (Aseeva et al., 2007
). On depletion of Vipp1 in cells of the cyanobacterium Synechocystis sp. PCC 6803 a decrease in paired thylakoid membranes has been observed together with a significant reduction of active trimeric photosystem 1 centers (Fuhrmann et al., 2009
). Although chloroplast Vipp1 was found to be localized in both the thylakoid and inner envelope membrane (Li et al., 1994
; Kroll et al., 2001
), the cyanobacterial protein has been suggested to be exclusively bound to the cytoplasmic membrane (Westphal et al., 2001
).
Vipp1 shows a high degree of sequence similarity to the phage shock protein A (PspA) from Escherichia coli and other eubacteria, and—in line with this—Vipp1 can functionally replace PspA in E. coli (DeLisa et al., 2004
). The low-resolution structure of the E. coli PspA has been resolved by electron microscopy (EM) and single-particle analysis (Hankamer et al., 2004
). The homooligomeric PspA organizes into a ring structure with ninefold rotational symmetry and a molecular mass of
1 MDa. Formation of ring structures has also been suggested for Vipp1 from A. thaliana (Aseeva et al., 2004
). However, the oligomeric organization and structure of both PspA and Vipp1 has been challenged recently. Vipp1 from the green alga Chlamydomonas reinhardtii forms very long rod-like structures in vitro, and a function of these structures in vivo has been suggested (Liu et al., 2007
). Furthermore, it has been suggested that PspA from E. coli forms cage-like structures that mimic eukaryotic clathrin coats (Standar et al., 2008
), rather than ring structures. These contradicting structural data make further studies relevant.
Here we present a detailed analysis of the oligomeric organization of Vipp1 from the cyanobacterium Synechocystis PCC 6803. Vipp1 forms stable dimers and higher-ordered oligomers that are localized in the cytoplasm and at the internal membranes. The higher-ordered oligomeric Vipp1 species have a molecular mass of
1.9 ± 0.3 MDa and are organized in ring structures with a remarkably variable number of monomer copies. They might be involved in vesicle formation by a yet unknown mechanism.
| MATERIALS AND METHODS |
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0.6, and protein expression was induced by addition of 0.5 mM isopropyl-beta-D-thiogalactopyranoside. After 3 h cells were harvested and resuspended in 20 ml 50 mM Na phosphate, pH 7.6, and 5 mM EDTA buffer. Cells were subsequently broken by sonication, and afterward cell debris and inclusion bodies were removed by centrifugation at 10, 000 x g for 10 min. The remaining supernatant was directly used to purify Vipp1. The supernatant was loaded onto a Ni-NTA agarose column (Qiagen, Hilden, Germany). The column was washed five times with buffer (50 mM Na phosphate, 300 mM NaCl, and 40 mM imidazole), and proteins were finally eluted in buffer + 500 mM imidazole. The eluted protein was subsequently dialyzed against 50 mM Na phosphate, pH 7.6. For determination of the subcellular protein localization in E. coli, the supernatant retained after removal of debris and inclusion bodies was centrifuged for 1 h at 100,000 x g, and sedimented membranes were redissolved in buffer and brought to the same volume as the soluble protein fraction. Equal volumes of the fractions were loaded per lane for the SDS-PAGE analysis.
Synechocystis Cell Culture
A glucose tolerant Synechocystis sp. PCC 6803 wild-type strain (kind gift of M. Rögner, Bochum, Germany) was grown photoautotrophically in liquid BG11 medium (Rippka et al., 1979
) at 34°C under 33 µE/m2 of fluorescent cold white light or under light-activated heterotrophic growth conditions (Anderson and McIntosh, 1991
).
Preparation of Cyanobacterial Membranes
Synechocystis cells were harvested in the midlog growth phase and pelleted by centrifugation (5000 x g, 10 min, 4°C). Cells were resuspended in buffer (20 mM HEPES/KOH, pH 7.5, 150 mM NaCl, 5 mM MgCl2, and 5 mM CaCl2) and disrupted in a bead beater homogenizer (BioSpec, Bartlesville, OK) using 0.5-mm glass beads. Glass beads, unbroken cells, and cell debris were removed by centrifugation at 5000 x g for 5 min at 4°C. After subsequent centrifugation at 100,000 x g for 40 min at 4°C the membrane pellet was resuspended in a buffer at a chlorophyll concentration of
1 mg chlorophyll/ml, and thylakoid membranes were extracted with 1.5% n-dodecyl-β-D-maltoside (DDM) for 1 h at room temperature. Proteins and protein complexes of the soluble fraction as well as extracted membrane proteins were separated on a Biosept S4000 SEC column (Phenomenex, Aschaffenburg, Germany) in buffer (20 mM HEPES/KOH, pH 7.5, 150 mM NaCl, 5 mM MgCl2, 5 mM CaCl2, and 0.04% DDM). Individual fractions were analyzed by immunoblot analysis using an anti-Vipp1 antibody (Fuhrmann et al., 2009
) to identify Vipp1-containing fractions.
For blue native (BN) PAGE analysis freshly prepared Synechocystis membranes in buffer (50 mM HEPES/KOH, pH 7.0, 5 mM MgCl2, 25 mM CaCl2, and 10% glycerol) were extracted with 1.5% DDM, and membrane-attached proteins were separated exactly as described in detail in Dühring et al. (2006)
. Individual lanes were separated in a second dimension on a 12% SDS-gel (Laemmli, 1970
), and Vipp1 was identified by immunoblot analysis using an anti-Vipp1 antibody.
Electron Microscopy
Synechocystis PCC 6803 cells were grown and harvested as described above. A cell pellet obtained from a 10-ml cell suspension was washed three times with EM buffer (50 mM KH2PO4/Na2HPO4, pH 7.0). The ultrastructural and immunocytochemical (immunogold) investigations were performed as described previously (Gathmann et al., 2008
).
On purification Vipp1 was dialyzed against 20 mM Tris/HCl, pH 7.5, 75 mM NaSCN, and 50 mM NaCl. Samples of purified Vipp1 were negatively stained with 2% uranyl acetate (UA) or 4% methylamine tungstate (MT) on glow-discharged carbon-coated copper grids. Images were recorded with a Gatan 4K slow-scan charge-coupled device camera (Pleasanton, CA) on a Philips CM12 electron microscope (FEI, Eindhoven, The Netherlands) equipped with a LaB6 tip operated at 120 kV, using Grace software for semiautomated specimen selection and data acquisition (Oostergetel et al., 1998
). The final magnification was x80,000, with a pixel size (after binning the images) of 3.75 Å at the specimen level.
About 1400 electron micrographs were recorded from a specimen stained with MT. In total 13,943 single-particle projections representing top views were selected and extracted from 1402 electron micrographs, recorded from an MT-stained specimen, by a reference-based automated particle selection procedure incorporated in GRIP (Groningen Image Processing) from these micrographs. From the UA-stained specimen, 600 electron micrographs were recorded, and 625 single particles of side views were selected and extracted by hand.
Single-particle analysis was performed with the GRIP software package on a PC cluster. The single-particle projections (144 x 144-pixel frame for the top views and 160 x 160-pixel frame for the double-ring side views) were subjected to multireference alignment and reference-free alignment procedure, multivariate statistical analysis, and hierarchical ascendant classification (van Heel et al., 2000
). Finally, two-dimensional projection maps of Vipp1 top views were calculated from the best resolved classes, which represented
15% of the whole data. For the final two-dimensional projection maps of the Vipp1 side views, all (80% of the) selected single particles were used to calculate averages from the best resolved classes.
To validate the imposed symmetry, cross-correlation factors (CCFs) between a nonrotated projection map and rotated views of the same projection map were calculated. The rotation angles were such chosen that they correspond to certain symmetry (a rotation of 180° corresponds to twofold symmetry, 120° rotation to threefold symmetry, etc.). Symmetry was identified based on the highest CCF score and the smallest rotation angle because structures with, for example, 12-fold symmetry also show two-, three-, four-, and sixfold symmetry.
Circular Dichroism Measurements
The secondary structure of Vipp1 was determined by circular dichroism (CD) spectroscopy. CD spectra were measured with an Jasco J-810 CD spectrometer (Jasco, Tokyo, Japan) in the 190–350-nm range every 1 nm at a scan speed of 200 nm min–1 in a cuvette with a 1-mm path length at a protein concentration of 0.125 mg/ml in 10 mM Na phosphate buffer (pH 7.5). The bandwidth was set to 1 nm.
GALLEX Analyses of the In Vivo Oligomerization in E. coli
The GALLEX system was used to determine homotypic interactions of Vipp1 in E. coli. Therefore, the vipp1 gene was amplified by PCR from genomic Synechocystis DNA using the following primers: vipp3'-GALLEX: 5'-tatgcgagctcgatgggattatttgaccgtttagand-3' and vipp5': 5'-tatgccatatgggattatttgaccgtttagg-3', and the resulting vipp1 fragment was subsequently ligated to the plasmid pLexA (Schneider and Engelman, 2003
) after restriction digestion of the PCR fragment and the plasmid with SacI and BamHI.
E. coli SU101 cells (Dmitrova et al., 1998
) were transformed with the resulting plasmid pLexA-SynVipp1 as well as with the control plasmids. Growth of the cells and GALLEX measurements were done exactly as described in detail in Schneider and Engelman (2003)
.
| RESULTS |
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Oligomerization of Vipp1 in Synechocystis
To analyze the oligomeric organization of Vipp1 from Synechocystis in more detail, we have separated soluble as well as membrane-bound and/or associated protein complexes and subsequently performed BN-PAGE and Western blot analyses. As can be seen in Figure 2, after separation of membrane-associated proteins and protein complexes a Vipp1 species with an apparent molecular mass of
66 kDa was detected as well as a higher-ordered Vipp1 oligomer, which hardly entered the BN gel. These apparent molecular masses correspond to a Vipp1 dimer and a large Vipp1 oligomer with a high molecular mass (>1 MDa), although the exact mass cannot be resolved by BN-PAGE analysis. Interestingly, when soluble proteins from Synechocystis were analyzed by BN-PAGE, only the dimeric Vipp1 population was detected. Because this might indicate that the large Vipp1 oligomers form exclusively at membranes, we further analyzed the oligomeric state of Vipp1 by size exclusion chromatography (SEC). This milder technique more likely preserves oligomeric structures. In line with the BN-PAGE analysis a Vipp1 population with a molecular mass of
66 kDa (dimer) as well as a large Vipp1 oligomer with masses ranging from 1.6 MDa to
2 MDa were identified (Figure 3). In contrast to the BN-PAGE analysis, the higher-ordered Vipp1 oligomers were found in both the soluble as well as in the membrane protein fraction. These data indicate that Vipp1 forms higher-ordered oligomers in Synechocystis, and there may exist a dynamic equilibrium between monomers, dimers, and higher-ordered oligomers.
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The results of the GALLEX measurements are shown in Figure 4. Based on these results, Vipp1 forms stable oligomers in a living cell, and compared with GpA, which forms a stable helix dimer, Vipp1 has a rather strong oligomerization propensity. For all expressed chimeric proteins we found similar expression levels when tested with an anti-LexA antibody. It has to be noted at this stage, however, that although the GALLEX assay allows a meaningful description of a proteins general oligomerization propensity the measurement does not allow drawing any conclusion about the exact oligomeric state of the protein.
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2 MDa that exist in vivo as nonbound and membrane-bound complexes.
Heterologous Expression of Vipp1
The above described measurements of Vipp1 oligomerization in E. coli cells have indicated that Vipp1 can be expressed as a stable oligomer in E. coli. Thus, to purify large amounts of the protein for further structural studies, we heterologously expressed the Synechocystis Vipp1 in E. coli cells. As can be seen in Figure 5, after expression of Vipp1 the protein was found to be mainly associated with membranes. Furthermore, as in Synechocystis a small pool of soluble Vipp1 was identified. To subsequently analyze these oligomeric structures in more detail, we have purified the protein from E. coli cell extracts (membranes and supernatant) without using any detergent or denaturant, because it has been suggested that the use of detergents can modify the Vipp1 structure, resulting in nonnative structural alterations (Standar et al., 2008
). On purification we have analyzed the secondary structure of Vipp1 by CD spectroscopy. Computational analysis of the Vipp1 amino acid sequence with the program Jpred3 (Cole et al., 2008
) predicts that
80% of the protein is
-helical, and many regions are predicted to have a high propensity to form coiled-coil structures (Figure 6A). The CD spectra of the purified Synechocystis Vipp1 is shown in Figure 6B and deconvolution of the spectra with the program CDSSTR (Compton and Johnson, 1986
; Manavalan and Johnson, 1987
; Sreerama and Woody, 2000
; Whitmore and Wallace, 2004
, 2008
) predicts that 83% of Vipp1 is
-helical, which is in very good agreement with the computational prediction.
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25,000 nm3, compatible with a mass of 1.5–2.5 MDa. A mass of
2 MDa was also actually measured. Because the smallest building block of each ring is the Vipp1 monomer with a molecular mass of
32 kDa and because the ring structures most likely consist of Vipp1 tetramers, rings with 12–17 tetrameric units would result in predicted masses of
1500–2200 kDa. To further assess the nature of the Vipp1 building units shaping the various Vipp1 rings, we have analyzed Vipp1 oligomers by BN-PAGE after mild SDS denaturation of the Vipp1 rings. Addition of gradually increasing concentrations of SDS to Vipp1 dissolved in 5 mM DDM resulted in the formation of mixed DDM/SDS micelles and gradual disassembly of the Vipp1 oligomers.
At SDS concentrations above 4 mM the large oligomer disappears, whereas dimeric and tetrameric Vipp1 species appear, as well as a small fraction of octameric Vipp1 (Figure 10). At increasing SDS concentrations the higher-ordered oligomers disassemble completely, and only the dimeric Vipp1 remains stable. Thus, in line with the above presented observations Vipp1 forms stable dimers in solution. Therefore, we propose that the repeating unit for a Vipp1 ring is a dimer of Vipp1 dimers. This implies, e.g., for the ring with N = 12 spikes that 24 Vipp1 dimers are involved in formation of the oligomer, with each spike representing a dimer. However, because the spikes facing inside the protein have an electron density different that of the spikes facing to the outside, we suggest that the Vipp1 oligomer is built up by an alternating interaction of Vipp1 dimers, potentially in an antiparallel manner. The side views of the Vipp1 rings indicate that there is no clear separation within distinct domains in the vertical direction (Figure 9, D–H). Because the rings have a height of
22 nm, this means that more than half of the Vipp1 monomer must exist in an extended
-helical conformation, spanning the entire height of the complex, which is 22 nm.
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Taken together, the presented results show that Vipp1 from Synechocystis can form ring structures with different diameters but constant heights, and dimeric Vipp1 is the minimal building block involved in formation of the observed higher-ordered oligomeric structures.
| DISCUSSION |
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Structural Organization of Vipp1
Analysis of soluble as well as membrane-bound proteins from Synechocystis by BN-PAGE indicates that in Synechocystis Vipp1 exists as a stable dimer as well as oligomers with a molecular mass of >>1 MDa. Thus, the protein appears to form larger oligomers than its homologue PspA from E. coli. Interestingly, our BN-PAGE analyses indicated that the oligomers were present only in the membrane protein fraction and not in the soluble protein fraction, which indicates that the membrane-bound oligomer is more stable than the soluble one. To further characterize the oligomeric organization of the Synechocystis Vipp1, we have subsequently analyzed the protein organization by SEC, and dimeric Vipp1 as well as a Vipp1 population with a significantly higher molecular mass was identified in the soluble as well as in the membrane-bound protein fractions from Synechocystis. The molecular mass of the larger oligomer was estimated to be
2 MDa. Formation of rod-like structures with molecular masses >>2 MDa, as described in Liu et al., (2007)
, was not observed, and, thus, the described results strongly suggest that—at least the Synechocystis—Vipp1 does not form larger oligomeric assemblies.
After expression of the Synechocystis Vipp1 in E. coli the monomeric protein strongly interacts and forms higher-ordered oligomers (Figures 5 and 7). Analysis of the purified protein by SEC demonstrated that also the isolated protein forms large oligomeric structures with a molecular mass of
2 MDa, as observed in Synechocystis before. Because an impact of detergent on the structural organization of PspA from E. coli has been emphasized (Standar et al., 2008
), it has to be mentioned that the protein was purified without any detergent. Because the protein can be well purified and, thus, effectively washed off the membranes by this method, this observation may indicate that Vipp1 is not very tightly bound to the internal membranes, at least not in E. coli. This might be caused by the different lipid composition of the E. coli membranes compared with the Synechocystis membranes. However, as also the homologous protein PspA from E. coli was purified by a similar method after homologous expression this protein appears also not to bind tightly to membranes (Standar et al., 2008
). Weak membrane attachment could thus be a common feature of PspA/Vipp1 proteins.
EM shows that Vipp1 monomers can form various higher-ordered structures, and the BN-PAGE analysis shown in Figure 10 suggests that the these structures are build up by accumulation of multiple dimeric Vipp1 species. Numerous Vipp1 proteins laterally associate to form small strings (Figure 9, A–C), which eventually close to form Vipp1 rings. The strings shown in Figure 9, A–C, could either represent assembly intermediates or an early step during Vipp1 ring degradation. In either case the strings clearly indicate an organization of Vipp1 by lateral accumulation of multiple monomers. Occasionally, two Vipp1 rings can further interact to form a double-ring structure (Figure 9, D–H). It is appealing to speculate that both Vipp1 rings interact with a rather hydrophobic surface, which is otherwise involved in membrane binding. Single-particle EM analysis of purified Vipp1 showed formation of various homooligomeric Vipp1 ring structures with different diameters. Actually, Vipp1 is to our knowledge rather special to make such a variety of rings, which means that there must be a special function linked to it, as will be discussed below. A similar diversity of ring structure with different compositions of the building units has—to our knowledge—only been described so far for the IsiA complex from Synechocystis (Boekema et al., 2001
; Kouril et al., 2003
, 2005
; Yeremenko et al., 2004
).
It is also interesting to compare the Vipp1 rings with those of the structural and functional homologous PspA protein. The Vipp1 rings have a 12–17-fold symmetry and a diameter of 25–33 nm, whereas the PspA rings are uniform with a ninefold symmetrical configuration (Hankamer et al., 2004
). If we extrapolate to a hypothetical Vipp1 ring with ninefold symmetry, this ring would have a diameter of 22 nm. This is close to the actual PspA ring diameter of 20 nm, if we take into account that the latter ring has a rather smooth surface because it lacks spikes like Vipp1 has. The PspA rings were considered to be composed of tetrameric building blocks to form uniform rings with a molecular mass of
1 MDa (Hankamer et al., 2004
). This equals the size of half of the Vipp1 rings, which can be explained by the fact that the ring height is only 8.5 nm. This difference in the height of the PspA rings versus the Vipp1 rings indicates that packing of the PspA and Vipp1 monomers in the two rings must be different. Although Vipp1 is C-terminally prolonged when compared with PspA, oligomerization of the Vipp1 monomers depends only on the PspA-like N-terminal domains (Aseeva et al., 2004
). Thus, the C-terminal extension of Vipp1 is most likely not directly involved in formation of the ring structures. Because of this, the N-terminal core domain of PspA and Vipp1 must pack differently. Although only
25% of the PspA amino acid residues must form an extended
-helix to span the height of the PspA ring (8 nm),
50% of Vipp1 has to form an extended
-helix to span 22 nm. For both proteins a domain of
140 amino acids of the N-terminal region is predicted to form an
-helix with a high propensity for coiled-coil formation. For Vipp1 this predicted
-helical domain of 140 amino acids would have the right length to account for the determined height of the rings of 22 nm, if present as one giant extended
-helix. In the case of PspA this helix is most likely folded as a hairpin and may form an
-helix bundle that would result in an increase of the PspA ring width. Different structural organization of PspA and Vipp1 might also indicate small differences in the respective protein functions, which would, e.g., explain why Synechocystis contains PspA as well as Vipp1.
It has to be noted that we did not observe cage-like structures as described before for the PspA from E. coli. Because for the preparation of the Synechocystis Vipp1 no detergent was used the suggested major impact of detergent on the PspA structure (ring vs. cage structures) should be revisited.
The observed diverse ring structures of Vipp1 could be involved in vesicle formation in cyanobacteria and chloroplasts. It is intriguing to speculate that Vipp1 assembled into a ring around the neck of a forming budding vesicle, similar to dynamin in eukaryotic cells.
Stepwise release of individual Vipp1 units results in formation of rings with smaller diameters, which would bring the membranes into a close contact, resulting in membrane fusion and pitching off of a vesicle. If Vipp1 performs such a dynamin-like function, the protein will most likely recruit other proteins that are, for example, involved in initial membrane bending and vesicle fission. Proteins involved in regulating the controlled Vipp1 (dis)assembly could involve Hsp70 chaperones and cochaperones, as discussed recently (Liu et al., 2007
).
Taken together, we show here that Synechocystis Vipp1 forms various oligomeric rings with different monomer stoichiometries. Although some of these rings exist in the cytoplasm of Synechocystis in a soluble form, most Vipp1 oligomers are tightly attached to both the thylakoid and the cytoplasmic membrane of the cyanobacterium Synechocystis sp. PCC 6803. Formation of promiscuous Vipp1 ring structures could play a critical role in vesicle formation in cyanobacteria and chloroplasts.
| ACKNOWLEDGMENTS |
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| Footnotes |
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Address correspondence to: Dirk Schneider (Dirk.Schneider{at}biochemie.uni-freiburg.de).
Abbreviations used: BN, blue-native; DDM, n-dodecyl-β-D-maltoside; EM, electron microscopy; SEC, size exclusion chromatography; Vipp1, vesicle-inducing protein in plastids 1.
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