Abstract
The cyclic AMP-dependent transcriptional regulator GlxR from Corynebacterium glutamicum is a member of the super-family of CRP/FNR (cyclic AMP receptor protein/fumarate and nitrate reduction regulator) transcriptional regulators that play central roles in bacterial metabolic regulatory networks. In C. glutamicum, which is widely used for the industrial production of amino acids and serves as a non-pathogenic model organism for members of the Corynebacteriales including Mycobacterium tuberculosis, the GlxR homodimer controls the transcription of a large number of genes involved in carbon metabolism. GlxR therefore represents a key target for understanding the regulation and coordination of C. glutamicum metabolism. Here we investigate cylic AMP and DNA binding of GlxR from C. glutamicum and describe the crystal structures of apo GlxR determined at a resolution of 2.5 Å, and two crystal forms of holo GlxR at resolutions of 2.38 and 1.82 Å, respectively. The detailed structural analysis and comparison of GlxR with CRP reveals that the protein undergoes a distinctive conformational change upon cyclic AMP binding leading to a dimer structure more compatible to DNA-binding. As the two binding sites in the GlxR homodimer are structurally identical dynamic changes upon binding of the first ligand are responsible for the allosteric behavior. The results presented here show how dynamic and structural changes in GlxR lead to optimization of orientation and distance of its two DNA-binding helices for optimal DNA recognition.
Introduction
The Gram-positive soil bacterium Corynebacterium glutamicum is widely used for the industrial production of amino-acids with an annual production of more than 4 Mt of L-glutamate and L-lysine combined [1]. Due to the rapidly increasing knowledge of C. glutamicum metabolism and regulation, numerous efforts are currently underway to use this bacterium for the production of an increasing range of small organic compounds including amino acids [2], [3], several organic acids such as succinate and lactate [4]–[6], but also the biofuels ethanol and isobutanol [7]–[9]. Many of these compounds are derived from intermediates of the tricarboxylic acid (TCA) cycle which is tightly regulated [10] on a transcriptional level by a range of DNA-binding proteins including the TetR-type AcnR [11], the LuxR-type RamA [12], the AraC-type RipA [13], as well as orthologues of the iron-dependent DtxR family [14] and most notably the CRP orthologue GlxR [15]. GlxR from C. glutamicum (Cg-GlxR) has been identified as one of the central regulators of the Corynebacterium metabolism and more than 200 genes under GlxR control have so far been identified [16]–[18]. Cg-GlxR, which shares a sequence identity of approximately 29% with CRP from E. coli (Ec-CRP), is a protein of 227 amino acids (compared to 210 for Ec-CRP) comprising an N-terminal dimerisation and ligand binding domain, and a C-terminal DNA-binding domain. The protein forms a homodimer with two structurally identical binding sites for cAMP. Once activated by cAMP, the regulator interacts with its target pseudo-palindromic DNA sites with the consensus sequence 5-TGTGANNTANNTCACA-3′ located in the regulatory region of Cg-GlxR controlled genes [16], [19]. In most cases Cg-GlxR functions as an activator where RNA polymerase is recruited by protein-protein-interactions thus enabling transcription of the downstream genes. In E. coli the intracellular level of cAMP has been shown to increase in response to glucose starvation via adenylate cyclase activation which in turn is linked to the bacterial phosphotransferase system (PTS) for sugar uptake [20]. In contrast, cAMP levels in C. glutamicum have been found to be decreased on acetate growth and increased during growth on glucose [15]. Cg-GlxR presents a central control point in the bacterial response to different nutrient sources and increasing our understanding of the molecular basis of activation and allostery may help to improve the regulation of metabolic processes.
Ec-CRP has for many years been the standard model to investigate allosteric cAMP binding and the molecular mechanism of DNA recognition. Although CRP was the first transcriptional regulator whose three-dimensional structure was determined by crystallography [21], and a number of structures of the regulator bound to cAMP and DNA have been determined by crystallography [22]–[24], the mechanism for how ligand binding causes activation of DNA binding remains controversial. The NMR structure suggested that cAMP binding resulted in a large movement of the DNA-binding domain coupled with a coil-to-helix transition extending into the coiled-coil region of the dimerisation interface [25]. In contrast, the medium resolution structure of apo Ec-CRP revealed a large albeit different hinge motion of the DNA-binding domains with respect to the dimerisation domain [26]. More recently, the crystal structure of apo CRP of Mycobacterium tuberculosis (Mt-CRP), which shares approximately 79% sequence identity with Cg-GlxR, showed an astonishing asymmetry between the protein monomers in one crystal structure, which was interpreted as a significant contributor to the activation mechanism [27]. However, no significant asymmetry was detected in solution for E. coli CRP by NMR [28] and it thus remains unclear if this is a general feature of activation in the CRP/FNR family. Whereas the first binding event of cAMP to CRP appears to involve structural changes in all cases investigated, the binding of the second cAMP in the structurally identical site of the second monomer is not accompanied by significant structural changes. Therefore, the remarkable negative allostery has been explained by changes in the dynamic behavior of the protein rather than defined conformational changes. The proposed dynamic changes have been supported by a number of elegant NMR experiments [25], [29], [30] as well as coarse-grain modeling studies [31]–[33]. In order to shed further light on the activation mechanism and the structural and dynamic basis of allosteric regulation in the CRP/FNR family we determined the crystal structures of apo Cg-GlxR at a resolution of 2.5 Å. In addition, the regulator bound to cyclic AMP was solved in two crystal forms diffracting to 2.38 and 1.82 Å resolution. The comparison of apo and cAMP-bound Cg-GlxR structures reveals the conformational changes responsible for activating DNA-binding. Furthermore, one crystal form of the cAMP-bound structure crystallized with two independent dimers in the asymmetric unit, whereas the second form contains six monomers in the asymmetric unit allowing for a detailed analysis of the conformational flexibility. In addition, we investigated cAMP and DNA binding of the protein by Isothermal Titration Calorimetry (ITC) and Fluorescence Anisotropy (FA) measurements. Our results suggest that in contrast to apo Ec-CRP, apo Cg-GlxR adopts a well-defined conformation and undergoes a small but significant hinge motion of the DNA-binding domain upon cAMP binding. Once activated Cg-GlxR adopts a conformation suitable for DNA binding. Subtle structural differences between Ec-CRP and Cg-GlxR explain the observed differences in allosteric behavior. Similarly, seemingly small changes in sequence may lead to different dynamic behavior contributing to allosteric regulation.
Materials and Methods
Protein Expression and Purification
Cloning, expression and purification were performed as described previously. Briefly, Cg-GlxR was produced using E. coli BL21 (λDE3) transformed with the expression plasmid pET16b-glxr [34], [35]. Pre-cultures in 150 mL LB media supplemented with kanamycin (50 µg/L) were cultivated for 8 h at 37°C and then inoculated 1∶100 in 6 L of autoinducing media for overnight growth at 37°C [36]. Bacteria were harvested by centrifugation at 4,500 g for 15 minutes at 4°C, re-suspended in 50 mL wash buffer (20 mM TrisHCl pH 8, 2 mM EDTA), pelleted at 5,500 g for 30 minutes and stored at −80°C. Pellets were then thawed and re-suspended in lysis buffer (50 mM KH2PO4 pH 7.8, 200 mM KCl, 20% (v/v) glycerol, 2 mM 1-thioglylcerol, 1 tablet of Roche protease inhibitor cocktail). Cells were lysed by sonication and debris was removed by centrifugation at 50,000 g for 1 h at 4°C. The His6-tagged protein was isolated using Ni-NTA-agarose (Invitrogen) where the protein was eluted with 10 mL of lysis buffer containing 150 mM imidazole. The protein was further purified using an Akta Explorer with a Superdex75 size exclusion column using 50 mM KH2PO4 pH 7.8, 200 mM KCl, 5% glycerol and 2 mM 1-thioglycerol. Peak fractions were pooled and analysed by SDS PAGE and mass spectrometric analysis (data not shown). GlxR in complex with cAMP was purified from IPTG (1 mM) induced E. coli JM109 (λDE3) cells containing the pETCRP plasmid [37]. Cells were grown at 37°C in LB medium supplemented with 50 µg/L kanamycin. The protein was purified from cell-lysate using Ni-NTA agarose (Invitrogen) according to published protocols [37]. Further purification was accomplished with a gel filtration column (GE Healthcare). The sample was finally incubated with cAMP in 10 times molar excess prior to crystallisation.
Isothermal Titration Calorimetry
Apo Cg-GlxR was first dialyzed overnight against 100 mM KH2PO4 pH 7.8, 200 mM KCl, 2 mM 1-thioglycerol at 4°C. Protein sample and buffer for the cAMP solution were degassed under vacuum. cAMP concentrations were calculated using the Lambert-Beer Law and a molar extinction coefficient of 14,650 M−1 cm−1 at 259 nm. Data was generated using an iTC200 (MicroCal) by one 0.3 µL injection, followed by 10 sequential 0.5 µL and 24 1 µl injections of 20 mM cAMP into 202 µL 165 µM protein. Data for the first injection was routinely discarded as this is affected by diffusion between the syringe and the protein solution during equilibration prior to data collection. Ligand binding was described with a two-site binding model.
Fluorescence Anisotropy Measurements
Anisotropy was measured on a Carey Eclipse Fluorescence Spectrophotometer (Agilent Technologies) fitted with polarizing filters (λem = 520 nm, λex = 495 nm, bandwidth = 5 nm, averaging time 20 s). Anisotropy was determined in the presence of 5′-FITC end-labeled oligonucleotide (FITC-5′-ATTAATGTGAGTTAGCTCACTCATTA-3′) and unlabeled oligonucleotide (5′-TAATGAGTGAGCTAACTCACATTAAT-3′). Oligonucleotides were annealed by heating to 90°C for 5 minutes in ultra pure water before cooling slowly to room temperature. Experiments were performed by titrating 2 µL aliquots of 200 µM Cg-GlxR into 5 nM labelled oligonucleotide in 1 mL buffer (100 mM KH2PO4 pH 7.8, 200 mM KCl, 1 mM 1-thioglycerol), in the presence of 0 or 1.5 mM cAMP. Anisotropy was calculated using WinFLR software (Agilent Technologies).
Crystallisation and Data Collection
Initial screens of apo cg-GlxR were set up with an Innovadyne Screenmaker using 100 nL and 200 nL protein solution at approximately 10 mg/mL in sitting drops using commercially available crystallisation screens. Follow-up experiments were performed using standard hanging-drop setup. The best crystals were obtained with 100 mM Na/K phosphate, 25% (v/v) propandiol, 10% (v/v) glycerol. Crystals were cryoprotected using a 1∶1 mixture of the reservoir solution and 50% glycerol solution and frozen in liquid [38]. All diffraction data were collected at the Diamond beam line I04 and processed using XDS [39]. Holo Cg-GlxR was crystallised using hanging drop vapor diffusion methods with the following buffer composition: 0.1M Morpheus buffer 3 (Tris/Bicine) at pH 8.5; 30% Morpheus GOL_P4K (glycerol, PEG4000), Morpheus Alcohols Mix at 0.12M (Molecular Dimensions). Diffraction data were collected at the Swiss Light Source beam line X06D and processed with XDS [39].
Structure solution, refinement and analysis
Crystal form II of cAMP-bound Cg-GlxR was first solved by molecular replacement with PHASER [40] using the structure of CRP from M. tuberculosis [41] as a search model. Crystal form I was obtained later and solved with the structure from crystal form II. The apo form of the protein was solved with PHASER using the holo Cg-GlxR structure as a search model. Both structure were completed by iterative cycles of model building using COOT [42] and crystallographic refinement with REFMAC [43], and validated using the various tools in COOT and Procheck [44]. For the apo Cg-GlxR structure 92.9% of all residues are in the preferred region, 5.5% in the allowed regions. Holo Cg-GlxR present 95% in preferred and a further 3.9% in allowed region Those residues that lie in outlier regions are located in flexible and/or poorly defined loop regions. Further crystallographic data are summarized in Table 1. Atomic coordinates and structure factors have been deposited at the Protein Data Bank, Research Collaboratory for Structural Bioinformatics, Rutgers University, New Brunswick, NK with pdb codes 3R6S and 4CYD for holo Cg-GlxR and 4BYY for apo Cg-GlxR.
Table 1. Data collection and refinement statistics.
Molecule: | Apo Cg-GlxR | Holo Cg-GlxR - I | Holo Cg-GlxR - II |
Beamline | DLS I04 | DLS I04 | SLS X06DA |
Wavelength [Å] | 0.9795 | 0.9163 | 1.0 |
Space group | C2 | P21 | P3121 |
a [Å] | 95.64 | 63.93 | 111.25 |
b [Å] | 59.95 | 102.66 | 111.25 |
c [Å] | 90.88 | 82.22 | 186.95 |
α,β, χ [°] | 90, 110.0, 90 | 90, 108.5, 90 | 90, 90, 120 |
resolution range [Å] | 85-2.48 | 29.41 - 1.82 | 67-2.38 |
Wilson B [Å2] | 50.0 | 37.9 | 42.6 |
Rmerge [%]* | 0.042 (0.724) | 0.045 (0.52) | 0.088 (0.705) |
Completeness [%] | 99.6 | 98.4 | 99.4 |
R [%] | 0.207 | 0.192 | 0.210 |
Rfree [%]** | 0.285 | 0.246 | 0.288 |
No. of residues chain A | 1–226 | 3–15,17 169,171–227 | 3–227 |
No. of residues chain B | 3–164, 178–217 | 3–227 | 3–227 |
No. of residues chain C | 3–227 | 3–226 | |
No. of residues chain D | 3–227 | 3–226 | |
No. of residues chain E | 3–227 | ||
No. of residues chain F | 3–64, 68–227 | ||
Average B-factors per chains [Å2]*** | A: 47.6; B: 52.1 H2O: 76.8 | A: 41.1; B: 46.3;C: 43.9; D: 47.8; E; 35.7 F: 41.7; H2O:39.2; cAMP: 32.4 | |
No. of cAMP | 0 | 2 | 6 |
No. of water | 72 | 2 | 161 |
rmsd bond length [Å] | 0.012 | 0.019 | 0.016 |
rmsd bond angles[°] | 1.67 | 1.90 | 1.72 |
PDB code | 4BYY | 4CYD | 3R6S |
*number in brackets reveal to the last resolution shell.
**Rfree is based over a subset of 5% of reflection that have not been used through the refinement [59].
***Average B-factors without TLS contributions.
Results and Discussion
Overall structure of Cg-GlxR
The crystal structures of apo and holo Cg-GlxR were determined independently at resolutions ranging from 2.5 to 1.82 Å (Table 1). Apo Cg-GlxR crystallises in the monoclinic space group C2 with one homo-dimer in the asymmetric unit (Figure 1a). Chain A shown on the left-hand side in blue is well defined with residues 1–226 (out of 227) present in the model, chain B (green) shows a larger degree of flexibility, and hence the model contains residues 3–164 and 178–217. The loop region of residues 165–177 that forms part of an anti-parallel β-sheet shows no density and was consequently not included. In addition, the model contains two phosphate ions with an occupancy of 0.5 in the cAMP binding site, two glycerol molecules at the protein surface and 72 water molecules. Crystal form I of cAMP bound Cg-GlxR crystallizes with two independent dimers in the asymmetric unit. Each monomer contains one cAMP in the binding pocket (Figure 1b). In addition, each dimer contains a portion of the tag used for purification (20 residues, shown in cyan in Figure 1b) providing crystal contacts. Crystal form II of holo Cg-GlxR in contrast, crystallizes with six independent protein chains, two complete dimers and two monomers on crystallographic 2-fold axes in the asymmetric unit. Each homodimer contains two cAMP molecules bound in the ligand-binding pocket of the monomer (Figure 1c). The overall structures of apo and holo Cg-GlxR exhibit the familiar domain structure seen in CRP from E. coli and M. tuberculosis [21], [41], [45]. Each monomer is composed of an N-terminal ligand-binding domain, followed by the central long helix, which provides the dimer interface and contributes to cAMP binding, and the C-terminal DNA-binding domain with its characteristic DNA-binding helix-turn-helix motif. The two independent protein chains in the apo Cg-GlxR structure adopt a similar conformation with an rmsd of 1.36 Å for 200 equivalent Cα-atoms (all least-squares superpositions were calculated using the RAPIDO server [46], Table 2). It is noteworthy that the DNA binding domains show a higher degree of flexibility as indicated by higher B-factors and a partial disorder of two external β-strands (Figure 1a). In contrast, all DNA binding domains are well defined in all ten independent molecules of the two holo Cg-GlxR crystal forms, adopting a similar conformation with rmsd's for all equivalent Cα-atoms ranging from 0.5 to 1.5 Å. The main differences between the crystallographically independent molecules occur through a rearrangement of the protein monomers in each dimer with respect to each other. This mobility becomes apparent when only the ligand-binding domain of one chain (residues 3–119) is used to calculate the superposition matrix of all holo GlxR dimers (Figure 2a, 2b). The monomers that are used to calculate the superposition (left-hand side) fit very well with rmsds of less than 1 Å, however, two distinct dimer arrangements shown in red and pale red can clearly be seen. The conformational differences are due to the dissimilar environments in the crystals representative of the conformational flexibility of the active regulator in solution.
Table 2. Comparison of holo and cAMP bound Cg-GlxR in crystal form I and II.
apo A | apo B | holo I A | holo I B | holo I C | holo I D | holo II A | holo II B | holo II C | holo II D | holo II E | holo II F | |
apo A* | 1.36 200 | 1.96 222 | 1.66 224 | 2.13 224 | 2.02 214 | 2.05 224 | 1.86 224 | 1.75 224 | 2.17 224 | 1.98 221 | 2.06 220 | |
apo B | 1.36 (1) ** | 2.40 199 | 2.14 201 | 2.66 201 | 2.42 196 | 2.39 200 | 2.13 200 | 2.09 187 | 2.50 200 | 2.40 199 | 2.37 196 | |
holo I A | 1.02 (2) | 0.76 (3) | 0.69 223 | 1.01 222 | 0.65 214 | 0.65 222 | 0.77 223 | 0.84 222 | 0.71 222 | 1.25 222 | 1.17 218 | |
holo I B | 1.02 (3) | 1.25 (3) | 0.66 (1) | 0.88 225 | 0.94 212 | 0.76 225 | 0.69 225 | 0.46 224 | 0.91 224 | 1.19 223 | 1.25 220 | |
holo I C | 1.09 (3) | 0.86 (3) | 0.82 (1) | 0.71 (1) | 1.27 211 | 1.16 225 | 1.26 225 | 0.98 224 | 1.24 224 | 1.46 224 | 1.60 221 | |
holo I D | 1.24 (2) | 0.98 (2) | 0.62 (1) | 0.83 (1) | 0.95 (1) | 0.73 213 | 0.84 214 | 1.03 214 | 0.78 212 | 1.44 211 | 1.19 206 | |
holo II A | 1.08 (3) | 0.90 (3) | 0.63 (1) | 0.71 (2) | 0.75 (1) | 0.63 (1) | 0.63 225 | 0.86 224 | 0.57 224 | 1.42 224 | 1.10 219 | |
holo II B | 1.23 (2) | 0.82 (3) | 0.74 (1) | 0.69 (1) | 0.83 (2) | 0.78 (1) | 0.63 (1) | 0.71 223 | 0.75 224 | 1.25 225 | 1.10 221 | |
holo II C | 1.06 (3) | 0.95 (3) | 0.74 (1) | 0.46 (1) | 0.72 (1) | 0.89 (1) | 0.86 (1) | 0.71 (1) | 1.00 223 | 1.06 222 | 1.27 221 | |
holo II D | 1.17 (3) | 0.83 (3) | 0.61 (1) | 0.80 (1) | 0.87 (1) | 0.70 (1) | 0.57 (1) | 0.75 (1) | 1.0 (1) | 1.46 222 | 1.13 218 | |
holo II E | 1.20 (3) | 0.86 (3) | 0.80 (1) | 0.85 (1) | 0.83 (2) | 0.96 (1) | 1.42 (1) | 1.25 (1) | 1.06 (1) | 1.46 (1) | 0.85 222 | |
holo II F | 1.48 (3) | 0.81 (3) | 0.86 (1) | 0.81 (1) | 0.84 (2) | 0.84 (1) | 1.23 (1) | 1.10 (1) | 1.27 (1) | 1.13 (1) | 0.85 (1) |
Root-mean-squares deviations after least-squares superpositioning of individual protein chains.
*In the right upper half of the table, the upper number denotes the rmsd in Å assuming rigid molecules. The number of equivalent Cα-atoms used for the least-squares superposition is given in italics.
**The left lower half of the table gives the rmsd in Å for a flexible superposition where the number of domains is given in brackets. These rmsds are generally slightly lower even if only one rigid domain has been used compared to the full alignment because the single rigid domain identified is generally slightly smaller.
Comparison of apo and holo Cg-GlxR
Comparing the apo and holo GlxR structures shows that the rmsds for all equivalent Cα-atoms in each chain treated as rigid-body are significantly higher ranging from 1.8 to 2.2 Å for chain A and 2.0 to 2.5 Å for chain B, respectively (Table 2). In order to identify the conformational changes induced, the ligand-binding domain (residues 3–119) of one monomer was again used to calculate the least-squares superposition transformation matrix, which was then applied to the protein dimers. Whereas the ligand binding domains of apo and holo GlxR superimpose very well with no significant changes within the domain as indicated of rmsds ranging from 0.8–1.5 Å for flexible superpositions (Table 2), the position of the DNA-binding domain with respect to the ligand binding domain in the same monomer changes significantly. This motion becomes particularly apparent when ligand-binding domain of one monomer is used to calculate the superposition matrix (Figure 2c and 2d). The two DNA-recognition helices in apo Cg-GlxR (blue) and holo Cg-GlxR (red) have moved significantly with respect to each other. Equivalent Cα-positions at the tip of this helix move by up to 10 Å upon ligand binding. These differences maybe sufficient to explain the difference of apo and holo Cg-GlxR in DNA-binding capability.
Ligand and DNA binding
The Cg-GlxR homo-dimer contains two binding sites for its activator cAMP (Figure 3a). As reported previously, Cg-GlxR shows pronounced negative allosteric behavior where binding of the first ligand reduces the affinity of the second - structurally identical - site in the homo-dimer (KD1 = 1.7·10−5 mol/l; KD2 = 1.3·10−4 mol/L) [32]. Allostery in Ec-CRP arises from the fact that the first binding event is enthalpically and entropically favored (ΔH1 = −2.0 kcal/mol, −TΔS1 = −4.9 kcal/mol) presumably due to the large motion of the DNA-binding domains whereas the second binding event is enthalpically disfavored (ΔH1 = +8.2 kcal/mol) but entropically favored (−TΔS1 = −14.8 kcal/mol). The two binding events are thus highly correlated leading to large changes in dynamic behavior supporting the notion of a largely dynamically driven process of allostery [47]. The structural details presented here support the thermodynamic data where the two binding events of cAMP to Cg-GlxR show similar enthalpic and entropic contributions [32]. Both binding events show a positive enthalpic contribution but are entropically favored. Negative allostery arises from the fact that ΔH1 is smaller (2.9 kcal/mol) than ΔH2, (4.0 kcal/mol) and −TΔS1 (−10.1 kcal/mol) slightly more negative than −TΔS2 (−9.5 kcal/mol). The small differences in enthalpic and entropic contributions to the free enthalpies are consistent with the relatively small structural changes observed in the Cg-GlxR structures presented here. The dynamic contributions to allostery may arise from a tightening upon binding of the first cAMP molecule leading to a smaller entropic gain for the second binding event. The crucial difference in the cAMP-binding site between Cg-GlxR and Ec-CRP is the fact the Ser-128 (numbering according to the E. coli CRP sequence) is substituted by Asn-138 (Figure 3b). Both residues bind to cAMP in the other binding site (chain A to cAMP bound in monomer B and vice versa) however, only serine is able to form an additional H-bond back to the backbone carbonyl oxygen of Leu124 thus providing an additional route of linking the two separate binding events of cAMP (Figure 3c). This notion is supported by results from Mt-CRP, which shares the asparagine at this position and previous work on Ec-CRP where the Ser128 to Ala mutation abolished allosteric behavior [48], [49]. In addition, the side chain of asparagine can form two H-bonds to N6 and N7 of cAMP, respectively, thus providing a gain of enthalpic contribution as indicated by a significantly smaller value of ΔH2 in Cg-GlxR compared to Ec-CRP where the first binding event is not accompanied by a large conformational change. ITC experiments using a higher cAMP concentration were performed to investigate a possible low-affinity third binding site as reported for Ec-CRP. Unlike Ec-CRP [50], Cg-GlxR does not appear to possess a low-affinity second binding site per protein monomer (Figure 4a). Once activated, cAMP-bound GlxR's central role is to bind its target DNA sequences. DNA-binding was therefore further investigated by Fluorescence Anisotropy measurement (Figure 4b). These experiments showed an increase of affinity to DNA by more than 100-fold from a dissociation constant of 8.3 µM to 87 nM upon cAMP binding. These values compare well with binding affinities reported for Ec-CRP [51].
Comparison of Cg-GlxR with Mt-CRP
Although the apo- and holo-structures of a number of members of the CRP/FNR family have been structurally characterized, our understanding of the structural and dynamics changes caused by ligand-binding is still limited [52]. We therefore compared the structures of Cg-GlxR presented here with the structures of the closest orthologue, Mt-CRP (sequence identity of 79%) as well as with Ec-CRP. The cAMP-free CRP dimer from M. tuberculosis has been found to exhibit significant asymmetry between the monomers which has been suggested to be responsible for inactivation [27], however, this profound asymmetry was not observed in an independently determined different crystal form and may therefor be an artifact of crystallisation [53]. The apo Cg-GlxR structure presented here shows some degree of asymmetry as indicated by missing loop regions in one of the two monomers, however, the two monomers superimpose very well with an rmsd of 1.36 Å for all equivalent Cα-atoms. Consequently, the superposition of apo Cg-GlxR with apo Mt-CRP results in relatively large rmsd's ranging from 2.0–3.3 Å (Table 3). As expected these larger differences are due to subunit and domain motions of the C-terminal DNA-binding with respect to the N-terminal ligand-binding domain as illustrated in Figure 5a where only one ligand-binding domain was used to calculate the superposition for the entire dimer. Remarkably, the holo structures of Cg-GlxR and Mt-CRP superimpose with significantly lower rmsds ranging from 0.9 to 1.5 Å (Table 4) as illustrated in Figure 5b. Clearly, the activated cAMP-bound forms of Cg-GlxR and Mt-CRP adopt a more defined conformation better suited for DNA recognition. Apo Cg-GlxR and Mt-CRP in contrast show larger conformational flexibility as illustrated by a larger degree of disorder in the DNA-binding domains and the difference in structures depending on crystallization conditions and crystal packing environments. These finding underline the notion that changes in dynamics play an important role in the activation of DNA binding activity.
Table 3. Comparison of apo Cg-GlxR with apo Mt-CRP.
Apo Mt-CRP (A) | Apo Mt-CRP (B) | |
Apo Cg-GlxR (A) | 2.27* (221) | 3.27 (215) |
Apo Cg-GlxR (B) | 2.71 (197) | 3.31(201) |
Root-mean-squares deviations after least-squares superpositioning of protein chains.
*The first number denotes the rmsd in Å for a rigid superpositioning of protein chains. The number of brackets gives the number of Cα-atoms used.
Table 4. Comparison of holo nCg-GlxR with cAMP-bound forms of Mt-CRP (PDB code 3I54), Ec-CRP (PDB code: 1G6N) and Ec-CRP bound to DNA (PDBP code: 1J59).
holo Mt-CRP (A)* | holo Mt-CRP (B) | holo Ec-CRP (A) | holo Ec-CRP (B) | DNA holo Ec-CRP A | DNA holo Ec-CRP B | |
holo Cg-GlxR (A) | 0.92 (216) | 0.89 (206) | 2.02 (183) | 3.79 (181) | 1.81 (183) | 1.97 (180) |
holo Cg-GlxR (B) | 0.95 (219) | 1.12 (206) | 1.99 (194) | 3.80 (186) | 1.85 (191) | 1.91 (188) |
holo Cg-GlxR (C) | 1.11 (218) | 1.34 (210) | 2.31 (190) | 4.10 (188) | 2.20 (194) | 2.34 (193) |
holo Cg-GlxR (D) | 1.15 (207) | 1.05 (201) | 2.14 (181) | 3.77 (183) | 1.97 (182) | 2.14 (187) |
holo Cg-GlxR (A) | 1.08 (218) | 1.09 (207) | 2.02 (192) | 3.69 (186) | 1.84 (187) | 1.95 (188) |
holo Cg-GlxR (B) | 0.97 (218) | 1.07 (207) | 2.18 (194) | 3.87 (182) | 1.98 (189) | 2.11 (189) |
holo Cg-GlxR (C) | 0.99 (218) | 1.21 (207) | 2.28 (194) | 3.95 (188) | 2.01 (190) | 2.10 (189) |
holo Cg-GlxR (D) | 1.10 (218) | 0.97 (207) | 2.01 (189) | 3.69 (183) | 1.87 (189) | 2.02 (188) |
holo Cg-GlxR (E) | 1.16 (217) | 1.45 (206) | 2.48 (193) | 4.22 (183) | 2.32 (190) | 2.40 (188) |
Holo Cg-GlxR (F) | 1.31 (213) | 1.54 (208) | 2.32 (189) | 3.96 (182) | 2.15 (187) | 2.27 (186) |
The four independent monomers of crystal form I are in the first four rows and, the six independent monomers of crystal form II in the remaining six rows.
*The first number denotes the rmsd in Å for a rigid superpositioning of protein chains using RAPIDO. The number of brackets gives the number of Cα-atoms used.
Comparison of Cg-GlxR with Ec-CRP
In order to assess if the findings presented here based on the structures can be generalized for the diverse CRP/FNR family, we compared the structures of holo-GlxR with Ec-CRP in its cAMP-bound state [50] and in complex with DNA [23]. It should be noted that the apo-form of Ec-CRP has only been solved at medium resolution and shows a significant degree of disorder [26] and was therefore not included in this comparison. Instead we used on representative structure from the NMR ensemble of apo Ec-CRP (pdb code 2WC2 [25]) for least-squares superpositioning (Figure 6a). As expected the overall structures are similar but the NMR structures shows significant motion of the individual domains with respect to each other which could be due to the fact that the NMR structures are not constrained by the crystal lattice. The same argument could account for the observation that the C-terminal loop of the long dimerization helix appears to be more flexible in apo Ec-CRP compared to apo Cg-GlxR despite a high level of sequence conservation in this area. A more detailed comparison can be performed using the multiple crystal structures of holo Cg-GlxR with holo Ec-CRP. As expected given the low sequence identity the overall structures are similar but differ far more on a detailed level. The rmsds for each of the six Cg-GlxR chains with Ec-CRP range from 2.0 to 4.2 Å indicating large conformational changes (see Table 4). As the two separate domains superimpose very well with rmsd of 1.0–1.2 Å when motions of 2 (or in some cases 3) domains are taken into account, we used the same least-squares superposition of one N-terminal ligand binding domain to superimpose equivalent dimers of Cg-GlxR and Ec-CRP. The results shown in Figure 6b indicate that there is a small re-orientation of the monomer-to-monomer position combined with a larger re-arrangement of the DNA-binding domain with respect to the ligand-binding domain. Remarkably, this re-arrangement is not symmetric with a much larger difference seen in the second monomer (depicted on the right-hand side of protein dimer in Figure 6b). However, it is important to note that the differences in orientation of domains in two identical protein chains may be due to crystal packing effects. This notion is supported by the fact that the cAMP-bound Cg-GlxR structure superimposes significantly better with the activated Ec-CRP conformation found in its active DNA-bound form (Figure 6c). The rmsds in this case range only from 1.8–2.4 Å. It is therefore highly likely that the ligand-bound form of Cg-GlxR structure represents the active state capable of DNA-recognition.
Conclusions
The structures of apo and cAMP-bound GlxR from C. glutamicum presented here provide a detailed picture of the structural changes required for DNA-binding. As seen in a number of homo-dimeric bacterial regulator proteins, the re-arrangement of the DNA-binding domains with respect to the ligand-binding and dimerisation domain(s) is at least partially responsible for activation [54]–[56]. In this case cAMP-binding re-orientates the position of the DNA-binding domains in the Cg-GlxR dimer to optimize DNA recognition. The fact that the cAMP-bound form of Cg-GlxR crystallises in two crystal forms with six different dimers allows us to assess the still considerable conformational flexibility of holo-GlxR. The crystal structure provides an ensemble of energetically almost identical conformations where the positions of the DNA-binding domains differ by up to 3 Å for equivalent Cα-positions. Binding to its target DNA sequence will presumably lock the conformation in the most favorable position for forming the ternary cAMP-Cg-GlxR-DNA complex. The structural changes shown here for Cg-GlxR upon cAMP binding, however, are quite distinct from those observed previously for Ec-CRP. Based on the structure determination by NMR a rotation of about 60° of the DNA-binding domain coupled with a coil-to-helix transition has been reported for Ec-CRP [25]. Likewise, the asymmetric homo-dimer observed in one crystal structure of apo Mt-CRP cannot be reproduced here. All Cg-GlxR structures form symmetric homo-dimers. While apo Cg-GlxR is clearly more flexible compared to cAMP-bound form as indicated by partially disordered loops in one of the two independent DNA-binding domains the structural change caused by cAMP binding depicted in Figure 2 is smaller than observed for other members of the CRP/FNR family. Nevertheless, there is a significant movement changing the position of the DNA-binding helix in monomer A with respect to monomer B by up to 10 Å (measured by comparing equivalent Cα-positions of the DNA-binding helix in monomer B). This motion is more than enough to render the apo Cg-GlxR less suited for DNA-binding. It is important to note that, whereas the cAMP-bound form of Ec-CRP does not adopt the optimal conformation for DNA binding, the activated Cg-GlxR structure presented here superimposed better with the DNA-bound form of holo Ec-CRP than with the DNA-free form of holo Ec-CRP (Figure 6c). The biophysical and structural studies determined in this work underline the notion that the mechanisms of allosteric binding and activation of DNA binding differ considerably in the CRP/FNR family without dramatic structural changes. The same 3-dimensional fold is finely tuned using seemingly small structural changes couple with changes in dynamic behavior to achieve the optimal combination of allostery and DNA recognition.
Acknowledgments
We would like to thank Ian Edwards for his technical support in protein purification and crystallisation, and Andrew Foster and Professor Nigel Robinson for support and access to the Fluorescence spectrophotometer. Finally, we gratefully acknowledge excellent support by the beam line staff at Diamond and the Swiss Light Source.
Data Availability
The authors confirm that all data underlying the findings are fully available without restriction. All relevant data are within the paper.
Funding Statement
Funding provided by Engineering and Physical Sciences Research Council (www.epsrc.ac.uk), EP/H051759/1 to MJC and EP and Swiss National Science Foundation (www.snf.ch), 31003A_140778 to STC. The funders had no role in study design, data collection and analysis, decision to publish, or preparation of the manuscript.
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Associated Data
This section collects any data citations, data availability statements, or supplementary materials included in this article.
Data Availability Statement
The authors confirm that all data underlying the findings are fully available without restriction. All relevant data are within the paper.