research papers
Structural analysis of DNA binding by C.Csp231I, a member of a novel class of R-M controller proteins regulating gene expression
aBiophysics Laboratories, Institute of Biomedical and Biomolecular Sciences, School of Biological Sciences, University of Portsmouth, Portsmouth PO1 2DY, England
*Correspondence e-mail: geoff.kneale@port.ac.uk
In a wide variety of bacterial restriction–modification systems, a regulatory `controller' protein (or C-protein) is required for effective transcription of its own gene and for transcription of the endonuclease gene found on the same operon. We have recently turned our attention to a new class of controller proteins (exemplified by C.Csp231I) that have quite novel features, including a much larger DNA-binding site with an 18 bp (∼60 Å) spacer between the two palindromic DNA-binding sequences and a very different recognition sequence from the canonical GACT/AGTC. Using X-ray crystallography, the structure of the protein in complex with its 21 bp DNA-recognition sequence was solved to 1.8 Å resolution, and the molecular basis of sequence recognition in this class of proteins was elucidated. An unusual aspect of the promoter sequence is the extended spacer between the dimer binding sites, suggesting a novel interaction between the two C-protein dimers when bound to both recognition sites correctly spaced on the DNA. A U-bend model is proposed for this tetrameric complex, based on the results of gel-mobility assays, hydrodynamic analysis and the observation of key contacts at the interface between dimers in the crystal.
Keywords: DNA–protein interactions; helix–turn–helix; restriction–modification; controller protein; gene regulation; EMSA.
PDB references: C.Csp231I–DNA complexes, 4jcx; 4jcy; 4jqd
1. Introduction
Restriction–modification (R-M) systems protect bacteria from invasion by foreign DNA. They are involved in the horizontal transfer of genes in bacterial populations, and may play a role in the spread of antibiotic-resistant genes (Loenen et al., 2014; Lindsay, 2010; Waldron & Lindsay, 2006; Kobayashi, 2001; Akiba et al., 1960). R-M systems employ a variety of mechanisms to ensure the correct temporal regulation of the methyltransferase and restriction-endonuclease genes. This is frequently achieved by controller proteins (C-proteins) that regulate the transcription of the R-M genes (Tao et al., 1991; Ives et al., 1992; Rimšeliené et al., 1995; Vijesurier et al., 2000; Cesnaviciene et al., 2003; Knowle et al., 2005). Restriction-endonuclease activity must be delayed until the host DNA has been protected from cleavage by the cognate DNA methyltransferase, which methylates specific sites in the bacterial genome and prevents cleavage by the endonuclease. If this temporal control mechanism is impaired, this leads to degradation of the host genome and results in cell death (Mruk & Blumenthal, 2008; Enikeeva et al., 2010). Our goal is to understand the structure and mechanism of such control systems.
A bioinformatics study has identified many hundreds of potential C-protein genes in the DNA sequence database (Sorokin et al., 2009). However, only a fraction of these genes have been shown to encode functional proteins, and even fewer of these have been the subject of structural or biophysical analysis. C-proteins have been divided into several classes based on motifs in their predicted DNA-recognition sites and/or the amino-acid sequences of the proteins (Sorokin et al., 2009; Mruk et al., 2007). X-ray crystallographic and functional information now exists for the controller proteins of AhdI (McGeehan et al., 2004, 2005, 2006; Bogdanova et al., 2008), BclI (Sawaya et al., 2005) and Esp1396I (Ball et al., 2009; McGeehan et al., 2008, 2012; Bogdanova et al., 2009; Martin et al., 2013, 2014). Other systems such as PvuII, although extensively studied in vitro and in vivo (Rimšeliené et al., 1995; Vijesurier et al., 2000; Mruk et al., 2007), have not been studied at a detailed structural level. Together, these studies have revealed a highly cooperative, concentration-dependent genetic switch which ensures that expression of the endonuclease is delayed until the methyltransferase has been produced (Streeter et al., 2004; Mruk et al., 2007; McGeehan et al., 2008; Bogdanova et al., 2008, 2009).
Upstream of the C-gene, the majority of such R-M systems have two C-protein binding sites, usually quasi-palindromic, having the consensus sequence GACTTATAGTC but with variations on this motif (Ives et al., 1992; Ball et al., 2012). The two dimer-binding sites on the DNA are typically separated by ∼4 bp, such that the two C-protein dimers overlap on opposite sides of the DNA helix and interact across the major groove (McGeehan et al., 2008). To date, all structural studies have been confined to this class of C-protein.
However, bioinformatic analysis revealed additional classes of C-proteins based on a variety of distinct DNA-recognition sites (Sorokin et al., 2009), and 517 putative C-proteins have now been reported in ReBase (https://rebase.neb.com/cgi-bin/azlist?cp). The control regions of the R-M systems classified by Sorokin and coworkers as motif 8 [typified by EcoO1091I (Imasaki et al., 2004; Kita et al., 2002) and Csp231I (Streeter et al., 2009; McGeehan et al., 2011)] have very different sequence motifs to those previously studied. In C.Csp231I, this region consists of two sets of 5 bp palindromic sequences with a 5 bp spacer (Fig. 1a). C.Csp231I has the recognition sequence CTAAGN5CTTAG, in which the inverted repeat sequences are separated by A-rich pentanucleotides (GAAAA and AAAAT, respectively, for the distal and proximal operators OL and OR). The distance separating the two 15 bp recognition sites (18 bp) is much longer than the ∼4 bp sequence found in the systems that have previously been studied, in which the binding sites partially overlap. For the related system EcoO109I the spacer between the palindromic operators is even longer (25 bp). Thus, in neither case can the protein dimers interact on the DNA in the manner of other C-protein systems, and an alternative mode of interaction is required for this class of R-M controller proteins.
The C.Csp231I controller protein (Mr = 11 360) is ∼30% larger than those for which structures have been investigated to date (e.g. C.AhdI and C.Esp1396I). Comparison of the 98-amino-acid sequence of C.Csp231I with C.AhdI shows only 29% identity over 62 core residues, with C.Csp231I having a 32-amino-acid extension at the C-terminus to form two additional helices (McGeehan et al., 2011). In contrast, C.Csp231I and C.EcoO109I share almost 70% sequence identity over the first 80 amino-acid residues, consistent with their almost identical DNA-recognition sites (McGeehan et al., 2011).
In order to further our understanding of this group of transcriptional regulators, we embarked on structural and functional analysis of this member of a new class of C-proteins bound to various DNA sites corresponding to regions of the operator region upstream of its own gene. Here, we present the X-ray crystal structures of these DNA–protein complexes, together with analysis of the DNA-binding properties of C.Csp231I by electrophoretic mobility-shift assays (EMSAs) and analytical ultracentrifugation, leading to an understanding of the molecular interactions responsible for DNA-sequence recognition and a novel model for the tetrameric protein–DNA complex at the promoter site.
2. Materials and methods
2.1. Expression, purification and crystallization
The cloning and purification of the C.Csp231I protein from Citrobacter sp. RFL231 have been described previously (Streeter et al., 2009). For crystallization trials, the protein was dialysed against buffer consisting of 50 mM Tris–HCl pH 8.0, 0.1 M NaCl, 1 mM Na2EDTA. HPLC-purified DNA were purchased from ATDBio. DNA duplexes were prepared in 10 mM Tris–HCl pH 8.0, 0.1 M NaCl, 1 mM EDTA. The duplexes were annealed by heating to 95°C for 5 min and then slowly cooled to room temperature over a period of 12–15 h. The annealed duplexes were purified using a Superdex 200 10/300 GL (25 ml) size-exclusion column and concentrated using Vivaspin concentrator columns.
The protein–DNA complexes were prepared by mixing protein and DNA in various ratios, followed by incubation at room temperature for 30 min. Crystallization conditions were screened with the aid of a Honeybee X8 nanodrop robot (Digilabs) by sitting-drop vapour diffusion using the PACT screening kit (Molecular Dimensions). The prepared protein–DNA complex was mixed in a 1:1 ratio with the reservoir solutions (0.1 µl + 0.1 µl) and incubated at 289 K for several days. Further crystal-growth optimizations were performed manually employing the hanging-drop vapour-diffusion method. Several different oligonucleotide constructs with varying lengths were used in crystallization trials.
2.2. X-ray data collection, phasing and structure refinement
Prior to cryocooling in liquid nitrogen, the crystals were cryoprotected by transfer into a solution containing the same components as the well solution with an increase of 3–5% in the precipitant and the addition of 15–20%(v/v) glycerol. The crystals were cryocooled in liquid nitrogen following mounting on cryoloops. Diffraction data for two crystal forms of the OL 21-mer DNA–protein complex were collected on beamline ID14-4 at ESRF, France equipped with an ADSC Q315r X-ray detector. The crystals were maintained at 100 K and data were collected at a wavelength of 0.9393 Å with an oscillation width of 1.0° for monoclinic data or 0.5° otherwise. Data for one crystal form of the OR 21-mer DNA–protein complex were collected on beamline I02 at the Diamond Light Source, UK. The crystals were maintained at 100 K using an Oxford Instruments Cryojet XL and data were collected at a wavelength of 0.9795 Å with an oscillation width of 1.0° using an ADSC Q315 CCD detector.
All crystallographic data were processed with iMosflm (Leslie, 1992) and SCALA (Evans, 2006). Data-collection and processing statistics for all crystal forms are given in Table 1. The scaled data were phased by with Phaser (McCoy et al., 2005) using a dimer of C.Csp231I as a search model (PDB entry 3lis; McGeehan et al., 2011). From these initial phases, the DNA duplexes were fitted by iterative rounds of building and in Coot (Emsley & Cowtan, 2004) and REFMAC5.5 with TLS restraints enabled (Murshudov et al., 2011). The first crystal form of the OL 21-mer DNA–protein complex was found to be twinned (twinning fraction of 0.3). In this case, the amplitude-based option implemented in REFMAC was used. During the of the OR complex, we located two iodide ions in the structure (see Supplementary Fig. S1). Similar binding sites for iodide ions have been observed in a number of structures (Abendroth et al., 2011).
‡Rwork = , where Fobs is the observed structure-factor amplitude and Fcalc is the calculated structure-factor amplitude. Rfree is the same as Rwork but for the 5% of structure-factor amplitudes that were set aside during §Estimation based on the Rfree value (estimated by REFMAC). |
Stereochemical quality was analysed using PROCHECK (Laskowski et al., 1993), and coordinate and structure-factor files have been deposited in the Protein Data Bank with accession codes 4jcx, 4jcy and 4jqd. Biological interfaces were analysed using PISA (Krissinel & Henrick, 2007). Structural parameters of the bound DNA duplexes were analysed using CURVES (Lavery et al., 2009). All structural figures were produced using PyMOL (Schrödinger).
2.3. shift assays (EMSAs)
EMSAs were performed using nondenaturing gel M Tris–HCl pH 8.0, 0.1 M NaCl, 1 mM EDTA) at room temperature for 30 min. The samples were loaded onto a 1 h pre-run 6.5% native polyacrylamide gel and run at room temperature in 0.25× TBE at 100 V for 100 min. The gels were stained with ethidium bromide and were then scanned using a G-Box imaging system (SynGene).
Complementary DNA strands corresponding to the sequence upstream of the C.Csp231I gene were purchased (ATDBio) and were annealed to form a duplex. Different molar ratios of the protein and DNA duplexes were incubated in binding buffer (10 mSeveral different oligonucleotide constructs were used to test the DNA-binding properties of the protein, including the normal 54-mer sequence and modified 54 bp sequences in which the second DNA-binding site or the linker region was mutated or deleted (Fig. 1b). The concentration of the DNA duplex was kept constant at 2 µM while adding increasing amounts of protein to reach the required molar ratios.
2.4. Analytical ultracentrifugation
For analytical ultracentrifugation, samples were dialyzed against a buffer consisting of 10 mM Tris–HCl pH 8.0, 100 mM NaCl, 1 mM EDTA using Slide-A-Lyzer MINI dialysis units (Thermo Scientific). The 56-mer DNA duplex (Fig. 1) was used to study the interaction with the C.Csp231I protein. Sedimentation-velocity experiments were performed in a Beckman XL-A analytical ultracentrifuge equipped with an An50-Ti rotor. Double-sector Epon cells with path lengths of 1.2 cm were used with quartz window assemblies. The volume of loaded sample was 400 µl and the corresponding sample buffer volume was 420 µl. Samples were equilibrated at 20°C for 30 min and then accelerated to 20 000 rev min−1. Radial scans were performed at 10 min intervals at 260 nm. The DNA concentration was 0.76 µM and for the tetrameric complex the protein was at a 4:1 molar ratio (subunits per DNA duplex). The for C.Csp231I was calculated from the amino-acid composition using SEDNTERP (Laue et al., 1992) at 0.7448 ml g−1, with a buffer density of 1.00283 g ml−1 and a viscosity of 0.010137 P. Analysis of the scans was performed using SEDFIT (Schuck, 2000) to produce a distribution plot [c(S)] of the sedimentation-coefficient profile.
3. Results
3.1. Crystallization of protein–DNA complexes
Several different oligonucleotide constructs were used in crystallization trials. The best diffracting crystals were obtained using 21 bp duplexes corresponding to the core sequences of the OL and OR operator DNA (Fig. 1). Two crystal forms were obtained for the OL complex, depending on the crystallization conditions, with the best diffracting crystals obtained using the following conditions: (i) buffer 1 [0.2 M ammonium chloride, 0.1 M MES pH 6.0, 20%(w/v) PEG 6K; protein (subunit):DNA molar ratio 1:1; protein concentration 1.2 mg ml−1; PACT condition B8], which produced a hexagonal form (P61), and (ii) buffer 2 [0.2 M sodium nitrate, 0.1 M bis-tris propane pH 7.5, 24%(w/v) PEG 3350; protein (subunit):DNA molar ratio 2:1, protein concentration 1.5 mg ml−1], which produced a monoclinic form (C2). For the OR complex, the optimum crystallization conditions were 0.2 M sodium iodide, 0.1 M bis-tris propane pH 6.0, 15%(w/v) PEG 3350, 10 mM spermidine; protein (subunit):DNA molar ratio 2:1; protein concentration 4.6 mg ml−1, which produced a hexagonal form (P61).
3.2. Comparison of the three crystal forms
The C.Csp231I–21-mer DNA duplex complexes crystallized in three crystal forms. For the OL complexes (space groups P61 and C2), the resolutions obtained were 2.30 and 2.75 Å, respectively, while the OR (P61) crystal form diffracted to a resolution of 1.80 Å (see Table 1). Molecular-replacement methods were used to phase all crystal forms using PDB entry 3lis (McGeehan et al., 2011) as the search model. The structures of the two OL DNA–protein complexes that crystallized in C2 (two complexes per asymmetric unit) are very similar to the P61 OL structure. We note here that the intermolecular interactions observed between the two complexes in the of the C2 crystal form may be of biological significance (this is further elaborated in §4.4).
A comparison between the OL and OR structures reveals minor conformational differences, and these are principally in the flexible C-terminal region (residues 86–95); the latter are unlikely to be significant given the flexibility of this region of the protein. The overall r.m.s.d. between the two complex structures is 0.4 Å (or 0.3 Å if the flexible C-terminal region is excluded); subsequent analysis of the interactions of C.Csp231I with DNA is therefore based only on the OR complex, since this has the highest resolution (1.8 Å) and the lowest R factor (Rwork and Rfree of 13.5 and 14.8%, respectively).
3.3. Overall structure of the complex
The overall structure of the complex (Fig. 2) consists of a C-protein dimer bound to a DNA duplex. The structure of the free C.Csp231I protein dimer contains seven helices, as found in the free protein (McGeehan et al., 2011), but with subtle conformational differences in the DNA-bound form of the protein. In the complex, each subunit interacts with the DNA by inserting recognition helix 3 (residues 28–40) of the classical helix–turn–helix motif into the major groove of the DNA either side of the central GAAAA motif. Superposition of monomer-to-monomer main-chain atoms reveals only minor differences when comparing subunits within the dimer. The maximum displacement between the main-chain atoms of separate monomers is confined to the C-terminal region (residues 86–95) of the protein (1.1 Å). This difference reflects conformational flexibility in this region of the protein, which has elevated values of crystallographic temperature (B) factors (see Supplementary Fig. S2). The observed flexibility of the C-terminal domain is similar in magnitude to that of the free protein structure (McGeehan et al., 2011).
3.4. DNA-binding studies
EMSA analysis of C-protein binding to the left and right operators showed no differences in affinity between the two sites (data not shown). We thus investigated the interaction of C.Csp231I with longer DNA sequences corresponding to the 54 bp region encompassing the operator sites upstream of the C-gene (Fig. 1). EMSA experiments using the wild-type 54 bp fragment (Fig. 3a) revealed a single complex at ratios of up to 2:1 (protein subunits per DNA duplex). At ratios of 4:1 and above a larger complex becomes apparent. These species are most likely to correspond to one and two bound dimers, respectively: one dimer bound at each palindromic of the DNA. We also looked at binding to an equivalent 54 bp oligonucleotide in which the sequence of the right-hand operator had been randomized (see Fig. 1). It is clear that mutation of this binding site blocks formation of the second species, suggesting that now only a single dimer binds to the wild-type OL site (Fig. 3b).
We then mutated the central spacer that is located between the dimer binding sites (see Fig. 1) to observe the effect of the DNA sequence of the spacer on protein binding. We found that random mutation of a 12 bp section of the central spacer had little effect on DNA binding (Fig. 3c); however, a shorter (48 bp) oligonucleotide duplex in which the central 6 bp of the spacer had been removed allowed the binding of one protein dimer but prevented the binding of a second dimer (Fig. 3d). Thus, the length of spacer is critical for binding two protein dimers simultaneously on the DNA, while the precise sequence of the spacer DNA appears to be unimportant. This suggests that there may be a structural role for the central spacer, rather than any sequence-specific interaction of the protein with the DNA bases in the spacer.
4. Discussion
4.1. Conformation of bound DNA
The DNA duplex in both complexes is significantly distorted from canonical B-form DNA (Fig. 4), with a bend of 39 and 43° for the complexes with OL and OR, respectively, similar to the value (41°) observed in complexes of C.Esp231I with the OL operator (McGeehan et al., 2012). The bend angle induced in DNA when bound to the related C.EcoO109, as estimated from gel assays, was reported to be 54° (Kita et al., 2002), although the results are not strictly comparable as they were obtained using different techniques.
The bend is stabilized by amino-acid contacts to the DNA backbone: principally electrostatic interactions with the phosphate groups on either side of the
It can be seen from the of the DNA–protein complex that the charged and/or polar amino-acid side chains of Arg10, Gln17, Ser30, Arg34, Asn36, Tyr38, Lys40, Lys42 and His43 of each subunit interact electrostatically with the phosphodiester backbone at each half-site. These interactions are responsible in large part for contracting the minor groove of the DNA, which drives DNA bending of the DNA–protein complex.4.2. Comparison of bound and free protein structures
The C-protein recognition helix (residues 28–40) undergoes a conformational change upon DNA binding (Fig. 5). The maximum DNA-induced displacement of the main-chain atoms in this region is 2.8 Å. The conformation of the C-terminal region also changes in the protein–DNA complex, but this is most likely to be due to conformational flexibility rather than to any effect of DNA binding. A similar conformational change involving the recognition helix was also observed in C.Esp1396I protein–DNA complexes, but in this case the displacement upon DNA binding was ∼1.4 Å (McGeehan et al., 2012; Ball et al., 2012). The interface area between the DNA duplex and the protein dimer is 1424 Å2, which is comparable to the values found for C.Esp1396I complexes (1541–1517 Å2).
4.3. DNA recognition
There are clear contacts to the bases that form the ). All three amino-acid side chains are also involved in a network of water-mediated hydrogen bonds to additional bases and/or phosphate groups on the DNA, further stabilizing the complex. There are no base-specific contacts with A9/T13 in OR (or the equivalent G9/C13 in OL), which is the only site within the 15 bp core sequence that differs between the two binding sites (see Fig. 1). The same is true for the A2/T20 (C2/G20 in OL) and C19/G3 (T19/A3 in OL) base pairs that lie outside the This is consistent with the DNA-binding affinity at theses two sites being effectively identical. This is in stark contrast to the situation for C.Esp1396I, where the Kd value for the OL and OR operator sequences differ by many orders of magnitude, consistent with the variation in base sequences at the sites where base-specific contacts are made.
from the side chains of Ser32, Gln37 and His43 in the DNA–protein complex structure (Fig. 6We note that the Ser32, Gln37 and His43 amino-acid residues involved in DNA-sequence recognition are identical in the amino-acid sequence of C.EcoO109I. Furthermore, the nine charged and/or polar amino-acid residues that can be seen contacting the phosphate groups of the DNA backbone in the C.Csp231I DNA–protein complex are also identically located in C.EcoO109I. Thus, there can be little doubt that the latter protein will interact with the DNA-recognition site in the same manner as we see here.
4.4. Interactions between adjacent dimers at the OL and OR operator sites
In common with most other C-protein systems, there are two C-protein binding sites upstream of the C.Csp231I gene. In other systems that have been studied in detail, the left-hand operator (OL) distal to the gene is responsible for enhancing transcription of the C-gene by recruiting RNA polymerase; in contrast, the right-hand operator (OR) proximal to the gene represses transcription by sterically blocking RNA polymerase. The OR binding site is only occupied at elevated concentrations of C-protein, at which point it switches the gene off to avoid overproduction of the C-protein (and the co-transcribed endonuclease). For C.Csp231I, however, the DNA-binding affinities for the two sites are effectively identical and there is no obvious cooperativity between the two binding sites, and thus we conclude that a different mechanism must be in operation. Moreover, the binding sites are separated by 15 bp (∼60 Å of extended B-form DNA), a distance that is far too great to allow two protein dimers to contact in a side-by-side fashion as seen in other C-protein complexes. If they do contact each other, then the dimers must interact in a `back-to-back' fashion, which implies DNA looping.
Our EMSA experiments show that the length of the DNA spacer (but not its sequence) is critical for forming the tetrameric complex, and thus the two bound dimers most likely interact with each other by looping and folding back of the intervening spacer DNA between bound dimers, rather than adopting an extended conformation. [If there were no interactions between the two dimers bound to the OL and OR sites (i.e. if they bound independently), then changing the spacer length should not affect formation of the tetrameric complex.]
As an additional test of whether the tetrameric complex was in a compact or an extended linear structure, we performed sedimentation-velocity analysis by analytical ultracentrifugation (AUC). For comparison, we also performed an equivalent run on the free DNA. The results show that the tetrameric complex has the expected molecular mass of ∼84 kDa and a
of 6.14 S indicative of a compact structure (see Supplementary Fig. S3).One interesting possibility is that the two dimeric complexes found in the C2 crystal form of the complex (Figs. 7a and 7b) represent such an interaction but lacking a covalently linked DNA spacer. The two dimeric complexes in the of the C2 crystal (Figs. 7a and 7b) are held together by protein–protein interactions between adjacent dimers (Fig. 7c). Following the notation used in the PDB (entry 4jqd), the dimer at the first site is represented by protein subunits A and B and the two DNA strands in the complex are labelled G and H. Likewise, the subunits of the second complex are labelled E and F and the associated DNA strands C and D. There are clear contacts between adjacent protein dimers in this tetrameric assembly, including a number of ion-pair interactions, in which Asn90 and Glu83 of subunit B in one dimer contact Glu48 and Arg34 (respectively) of subunit F in the adjacent protein dimer. In addition, Lys40 of subunit A is in proximity to Glu83 of subunit F, and these two residues may also interact. There are also potential contacts between a protein subunit of one dimer and the DNA bound to the second dimer; for example, the interaction of Lys87 (subunit B) with a phosphate of the DNA (strand H). We note that three of these interacting residues (Glu83, Lys87 and Asn90) are located in helix 7 at the C-terminus of the protein. This C-terminal region of the amino-acid sequence is rich in basic amino acids (seven from 13 residues, including three arginines and four lysines). This helix is not found in typical C-proteins, suggesting that it has a unique function that may promote protein–protein and protein–DNA interactions to stabilize the tetrameric complex.
of theSuch interactions between the two complexes could stabilize a looped tetrameric complex. Fig. 7(d) shows a model of such a complex with a 54 bp sequence. It has been constructed by inserting a 12 bp highly curved segment of DNA to link the two 21 bp duplexes of the two complexes in the In this model, there would be no sequence-specific interactions from the C-protein to the spacer DNA, consistent with the EMSA results showing that mutating the spacer sequence had no observable effect on DNA binding. It would also explain why the length of the DNA spacer is important, as shorter sequences would be unable to span the gap between adjacent dimeric complexes.
Using the HYDROPRO computer program (Ortega et al., 2011), we can predict the of the tetrameric structure that we propose. The calculated value for the model (6.60 S) is close to the experimental value (6.14 S), adding further support for the looped-back model of the protein–DNA complex. It should be emphasized that the dimer–dimer interactions in our proposed model are stabilized only by the tethering of two dimers when bound to the native 56 bp DNA sequence with an appropriate distance between dimer binding sites, as indicated by our EMSA experiments. For the free unbound protein, we found no evidence of tetramer formation by AUC (McGeehan et al., 2011).
The proposed U-turn bend induced by the inserted 12 bp spacer is an unusual DNA conformation. However, similar DNA conformations have been observed for structures of Escherichia coli IHF (integration host factor) and HU (histone-like protein) proteins (Swinger & Rice, 2004), the eubacterial integration host Hbb factor from Borrelia burgdorferi (Mouw & Rice, 2007) and the human mitochondrial transcription and packaging factor Tfam (Rubio-Cosials et al., 2011; Ngo et al., 2011). The degree of DNA distortion is dramatic in the cases of the Hbb and Tfam protein–DNA complexes, causing an overall DNA bend of ∼180° and a reversal in the direction of the DNA helical axis.
Such a `folded-back' structure for the DNA complex when both left and right operators are bound is very different to the only experimentally determined tetrameric C-protein–DNA complex structure, that of the controller protein C.Esp136I bound to the 35 bp upstream DNA fragment containing both operator sites (McGeehan et al., 2008), which is essentially an extended linear structure (with some local bending at each dimer binding site). C.Csp231I (together with C.EcoO1019I) represents a unique family of C-proteins, and their amino-acid sequences and DNA-recognition sites are very different from those previously studied. Given the quite different DNA-recognition modes employed by these two C-proteins, as well as the much greater length of the spacer between the dimer binding sites, we expect that their mechanisms of gene activation and/or repression will be very different from other known systems, as exemplified by C.Esp136I.
Supporting information
PDB references: C.Csp231I–DNA complexes, 4jcx; 4jcy; 4jqd
Supporting Information. DOI: https://doi.org/10.1107/S139900471402690X/cb5069sup1.pdf
Footnotes
‡Current address: Laboratory of Structural Biology of GPCRs, Moscow Institute of Physics and Technology, Dolgoprudniy 141700, Russia.
Acknowledgements
We are grateful to the Biotechnology and Biological Sciences Research Council UK (BBSRC) for research grant BB/H00680X/1 to GGK and JEM and to the Diamond Light Source (UK), ESRF (France) and associated beamline staff for the provision of synchrotron-radiation facilities. We thank our colleagues Dr Richard Martin and Dr James Taylor for helpful discussions on crystallography and AUC, respectively.
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