Tetrameric Repressor Research Articles

Roadblocks by Protein-Mediated DNA Loops

RNA polymerase elongation during transcription may be hindered by the many proteins bound to DNA (roadblocks). Conversely, RNA polymerase might displace a roadblocking transcription factor (TF) and compromise regulation. The mechanism by which an RNA polymerase might elongate past DNA-bound proteins without disturbing with their regulatory functions is poorly understood. Many TFs from organisms spanning all kingdoms recognize specific sites on DNA to shape the genome and regulate transcription and, unlike nucleosomes, are not targets for combinatorial chemical modifications that impact complex pathways. Instead, their regulatory effects stem from the presence of multiple operators to which they bind with different affinities and/or cooperatively. Such interactions often modify DNA topology, such as DNA looping, but little is known about how topology affects transcriptional roadblocks either in vivo or in vitro. Recently we used scanning force microscopy (SFM), to assay how the presence of a DNA loop affects elongation by RNAP through a lac repressor tetramer (LacI) roadblock. LacI oligomerizes to form a tetramer with two DNA binding domains and is a strong roadblock to transcription elongation even when bound to just one binding site (operator). However, it can also mediate DNA looping between two separate operator sites. We found that the strength of a roadblock depends on the strength of the first operator encountered by RNAP and whether or that operator forms one end of a LacI-mediated DNA loop. To assess how higher order TF oligomerization and operator multiplicity might affect the strength of a roadblock, we compare LacI roadblocks with those of λ bacteriophage CI. The results provide insight into how transcription factors generate complex responses in genomic contexts.

LacI-DNA-IPTG Loops: Equilibria among Conformations by Single-Molecule FRET

The E. coli Lac repressor (LacI) tetramer binds simultaneously to a promoter-proximal DNA binding site (operator) and an auxiliary operator, resulting in a DNA loop, which increases repression efficiency. Induction of the lac operon by allolactose reduces the affinity of LacI for DNA, but induction does not completely prevent looping in vivo. Our previous work on the conformations of LacI loops used a hyperstable model DNA construct, 9C14, that contains a sequence directed bend flanked by operators. Single-molecule fluorescence resonance energy transfer (SM-FRET) on a dual fluorophore-labeled LacI-9C14 loop showed that it adopts a single, stable, high-FRET V-shaped LacI conformation. Ligand-induced changes in loop geometry can affect loop stability, and the current work assesses loop population distributions for LacI-9C14 complexes containing the synthetic inducer IPTG. SM-FRET confirms that the high-FRET LacI-9C14 loop is only partially destabilized by saturating IPTG. LacI titration experiments and FRET fluctuation analysis suggest that the addition of IPTG induces loop conformational dynamics and re-equilibration between loop population distributions that include a mixture of looped states that do not exhibit high-efficiency FRET. The results show that repression by looping even at saturating IPTG should be considered in models for regulation of the operon. We propose that persistent DNA loops near the operator function biologically to accelerate rerepression upon exhaustion of inducer.

Intramolecular signal transmission in a tetrameric repressor of the IclR family

Members of the IclR family control bacterial genes involved in a number of physiological processes. The IclR-family member TtgV crystallizes as a tetramer, with each TtgV monomer consisting of two domains--a DNA binding domain and an effector recognition domain, which are interconnected by an extended α-helix. When bound to DNA, a kink is introduced so that the extended helix is split in two α-helices (helix-4 and -5). Differential scanning calorimetry studies revealed that TtgV unfolds in a single event, suggesting that the two domains unfold cooperatively. When mutations are introduced in helix-5 that disrupt interactions between Arg98 and Glu102, the thermal unfolding of the TtgV domains becomes uncoupled without compromising effector binding. Two of these mutants (TtgVE102R and TtgVE102A) showed impaired release from target DNA, suggesting that these mutations alter signal transmission. By combining various mutants, we found that the mutations in the connecting α-helix exhibited a dominant effect over mutations in DNA binding and effector binding domains. We propose a model in which the loss of cooperativity of unfolding of TtgV reflects perturbed interdomain communication, and that the transition from the continuous to discontinuous helix may mediate interdomain communication necessary for the proper functioning of TtgV.

Structure and Organisation of SinR, the Master Regulator of Biofilm Formation in Bacillus subtilis

sinR encodes a tetrameric repressor of genes required for biofilm formation in Bacillus subtilis. sinI, which is transcribed under Spo0A control, encodes a dimeric protein that binds to SinR to form a SinR–SinI heterodimer in which the DNA-binding functions of SinR are abrogated and repression of biofilm genes is relieved. The heterodimer-forming surface comprises residues conserved between SinR and SinI. Each forms a pair of α-helices that hook together to form an intermolecular four-helix bundle. Here, we are interested in the assembly of the SinR tetramer and its binding to DNA. Size-exclusion chromatography with multi-angle laser light scattering and crystallographic analysis reveal that a DNA-binding fragment of SinR (residues 1–69) is a monomer, while a SinI-binding fragment (residues 74–111) is a tetramer arranged as a dimer of dimers. The SinR(74–111) chain forms two α-helices with the organisation of the dimer similar to that observed in the SinR–SinI complex. The tetramer is formed through interactions of residues at the C-termini of the four chains. A model of the intact SinR tetramer in which the DNA binding domains surround the tetramerisation core was built. Fluorescence anisotropy and surface plasmon resonance experiments showed that SinR binds to an oligonucleotide duplex, 5′-TTTGTTCTCTAAAGAGAACTTA-3′, containing a pair of SinR consensus sequences in inverted orientation with a Kd of 300 nM. The implications of these data for promoter binding and the curious quaternary structural transitions of SinR upon binding to (i) SinI and (ii) the SinR-like protein SlrR, which “repurposes” SinR as a repressor of autolysin and motility genes, are discussed.

The lysis-lysogeny decision of bacteriophage 933W: a 933W repressor-mediated long-distance loop has no role in regulating 933W P(RM) activity.

Our data show that unlike bacteriophage λ, repressor bound at O(L) of bacteriophage 933W has no role in regulation of 933W repressor occupancy of 933W O(R)3 or the transcriptional activity of 933W P(RM). This finding suggests that a cooperative long-range loop between repressor tetramers bound at O(R) and O(L) does not form in bacteriophage 933W. Nonetheless, 933W forms lysogens, and 933W prophage display a threshold response to UV induction similar to related lambdoid phages. Hence, the long-range loop thought to be important for constructing a threshold response in lambdoid bacteriophages is dispensable. The lack of a loop requires bacteriophage 933W to use a novel strategy in regulating its lysis-lysogeny decisions. As part of this strategy, the difference between the repressor concentrations needed to bind O(R)2 and activate 933W P(RM) transcription or bind O(R)3 and repress transcription from P(RM) is <2-fold. Consequently, P(RM) is never fully activated, reaching only ∼25% of the maximum possible level of repressor-dependent activation before repressor-mediated repression occurs. The 933W repressor also apparently does not bind cooperatively to the individual sites in O(R) and O(L). This scenario explains how, in the absence of DNA looping, bacteriophage 933W displays a threshold effect in response to DNA damage and suggests how 933W lysogens behave as "hair triggers" with spontaneous induction occurring to a greater extent in this phage than in other lambdoid phages.

Comparing native and irradiated E. coli lactose repressor-operator complex by molecular dynamics simulation

The function of the E. coli lactose operon requires the binding of the tetrameric repressor protein to the operator DNA. We have previously shown that gamma-irradiation destabilises the repressor-operator complex because the repressor gradually loses its DNA-binding ability (Radiat Res 170:604-612, 2008). It was suggested that the observed oxidation of tyrosine residues and the concomitant structural changes of irradiated headpieces (DNA-binding domains of repressor monomers) could be responsible for the inactivation. To unravel the mechanisms that lead to repressor-operator complex destabilisation when tyrosine oxidation occurs, we have compared by molecular dynamic simulations two complexes: (1) the native complex formed by two headpieces and the operator DNA, and (2) the damaged complex, in which all tyrosines are replaced by their oxidation product 3,4-dihydroxyphenylalanine (DOPA). On a 20 ns time scale, MD results show effects consistent with complex destabilisation: increased flexibility, increased DNA bending, modification of the hydrogen bond network, and decrease of the positive electrostatic potential at the protein surface and of the global energy of DNA-protein interactions.

First-principles Calculation Of DNA Looping In Tethered Particle Experiments

We show how to calculate the probability of DNA loop formation mediated by regulatory proteins such as Lac repressor, using a mathematical model of DNA elasticity. Our approach has new features enabling us to compute quantities directly observable in Tethered Particle Motion (TPM) experiments; e.g. it accounts for all the entropic forces present in such experiments. Our model has no free parameters; it characterizes DNA elasticity using information obtained in other kinds of experiments. It can compute both the “looping J factor” (or equivalently, looping free energy) for various DNA construct geometries and repressor concentrations, as well as the detailed probability density function of bead excursions. We also show how to extract the same quantities from recent experimental data on tethered particle motion, and compare to our model's predictions. In particular, we present a new method to correct observed data for finite camera shutter time. The model successfully reproduces the detailed distributions of bead excursion, including their surprising three-peak structure, without any fit parameters and without invoking any alternative conformation of the repressor tetramer. However, for short DNA loops (around 95 bp) the experiments show more looping than is predicted by the linear-elasticity model, echoing other recent experimental results. Because the experiments we study are done in vitro, this anomalously high looping cannot be rationalized as resulting from the presence of DNA-bending proteins or other cellular machinery. We also show that it is unlikely to be the result of a hypothetical “open” conformation of the repressor. Ref: KB Towles et al, accepted for publication in Physical Biology.

Structural Basis for the Differential Regulation of DNA by the Methionine Repressor MetJ

The Met regulon in Escherichia coli encodes several proteins responsible for the biosynthesis of methionine. Regulation of the expression of most of these proteins is governed by the methionine repressor protein MetJ and its co-repressor, the methionine derivative S-adenosylmethionine. Genes controlled by MetJ contain from two to five sequential copies of a homologous 8-bp sequence called the metbox. A crystal structure for one of the complexes, the repressor tetramer bound to two metboxes, has been reported (Somers, W. S., and S. E. Phillips (1992) Nature 359, 387-393), but little structural work on the larger assemblies has been done presumably because of the difficulties in crystallization and the variability in the number and sequences of metboxes for the various genes. Small angle neutron scattering was used to study complexes of MetJ and S-adenosylmethionine with double-stranded DNA containing two, three, and five metboxes. Our results demonstrate that the crystal structure of the two-metbox complex is not the native solution conformation of the complex. Instead, the system adopts a less compact conformation in which there is decreased interaction between the adjacent MetJ dimers. Models built of the higher order complexes from the scattering data show that the three-metbox complex is organized much like the two-metbox complex. However, the five-metbox complex differs significantly from the smaller complexes, providing much closer packing of the adjacent MetJ dimers and allowing additional contacts not available in the crystal structure. The results suggest that there is a structural basis for the differences observed in the regulatory effectiveness of MetJ for the various genes of the Met regulon.

FLEXIBILITY AND CONTROL OF PROTEIN–DNA LOOPS

Protein–DNA loops are essential for efficient transcriptional repression and activation. The geometry and stability of the archetypal Lac repressor tetramer (LacI)–DNA loop were investigated using designed hyperstable loops containing lac operators bracketing a sequence-directed bend. Electrophoretic mobility shift assays, DNA cyclization, and bulk and single-molecule fluorescence resonance energy transfer (FRET) demonstrate that the DNA sequence controls whether the LacI–DNA loop forms a compact loop with positive writhe or an open loop with little writhe. Monte Carlo methods for simulation of DNA ring closure were extended to DNA loops, including treatment of variable protein hinge angles. The observed distribution of topoisomer products upon cyclization provides a strong constraint on possible models. The experiments and modeling imply that LacI–DNA can adopt a wide range of geometries but has a strong intrinsic preference for an open form. The flexibility of LacI helps explain in vivo observations that DNA looping is less sensitive to DNA length and shape than that expected from the physical properties of DNA. While DNA cyclization suggests two pools of precursor loops for the 9C14 construct, single-molecule FRET demonstrates a single population. This discrepancy suggests that the LacI–DNA structure is strongly influenced by flanking DNA.

A comparative three-dimensional model of the carboxy-terminal domain of the lambda repressor and its use to build intact repressor tetramer models bound to adjacent operator sites

A model for residues 93–236 of the λ repressor (1gfx) was predicted, based on the UmuD ′ crystal structure, as part of four intact repressor molecules bound to two adjacent operator sites. The structure of region 136–230 in 1gfx was found to be nearly identical to the independently determined crystal structure of the 132–236 fragment, 1f39, released later by the PDB. Later, two more tetrameric models of the λ repressor tetramer bound to two adjacent operator sites were constructed by us; in one of these, 1j5g, the N-domain and C-domain coordinates and hence monomer-monomer and dimer-dimer interactions are almost the same as in 1gfx, but the structure of the linker region is partly based on the linker region of the LexA dimer in 1jhe; in the other, 1lwq, the crystalline tetramer for region 140–236 has been coopted from the crystal structure deposited in 1kca, the operator DNA and N-domain coordinates of which are same as those in 1gfx and 1j5g, but the linker region is partly based on the LexA dimer structures 1jhe and 1jhh. Monomer-monomer interactions at the same operator site are stabilized by exposed hydrophobic side chains in β-strands while cooperative interactions are mostly confined to β 6 and some adjacent residues in both 1gfx and 1j5g. Mutational data, existence of a twofold axis relating two C-domains within a dimer, and minimization of DNA distortion between adjacent operator sites allow us to roughly position the C-domain with respect to the N-domain for both 1gfx and 1j5g. The study correlates these models with functional, biochemical, biophysical, and immunological data on the repressor in the literature. The oligomerization mode observed in the crystal structure of 132–236 may not exist in the intact repressor bound to the operator since it is shown to contradict several published biochemical data on the intact repressor.

Structure of a variant of lac repressor with increased thermostability and decreased affinity for operator

A single amino acid substitution, K84L, in the Escherichia coli lac repressor produces a protein that has substantially increased stability compared to wild-type. However, despite the increased stability, this altered tetrameric repressor has a tenfold reduced affinity for operator and greatly decreased rate-constants of inducer binding as well as a reduced phenotypic response to inducer in vivo. To understand the dramatic increase in stability and altered functional properties, we have determined the X-ray crystal structures of a dimeric repressor with and without the K84L substitution at resolutions of 1.7 and 3.0 Å, respectively. In the wild-type dimer, K84-11, Lys84 forms electrostatic interactions at the monomer-monomer interface and is partially exposed to solvent. In the K84L-11 substituted protein there is reorientation of the N-subdomains, which allows the leucine to become deeply buried at the monomer-monomer interface. This reorientation of the N-subdomains, in turn, results in an alteration of hydrogen bonding, ion pairing, and van der Waals interactions at the monomer-monomer interface. The lysine residue at position 84 appears to exert its key effects by destabilizing the “optimal” conformation of the repressor, effectively loosening the dimer interface and allowing the repressor to adopt the conformations necessary to function as a molecular switch.

In Vitro Interaction of theEscherichia coli Cyclic AMP Receptor Protein with the Lactose Repressor

Sedimentation equilibrium studies show that the Escherichia coli cyclic AMP receptor protein (CAP) and lactose repressor associate to form a 2:1 complex in vitro. This is, to our knowledge, the first demonstration of a direct interaction of these proteins in the absence of DNA. No 1:1 complex was detected over a wide range of CAP concentrations, suggesting that binding is highly cooperative. Complex formation is stimulated by cAMP, with a net uptake of 1 equivalent of cAMP per molecule of CAP bound. Substitution of the dimeric lacI-18 mutant repressor for tetrameric wild-type repressor completely eliminates detectable binding. We therefore propose that CAP binds the cleft between dimeric units in the repressor tetramer. CAP-lac repressor interactions may play important roles in regulatory events that take place at overlapping CAP and repressor binding sites in the lactose promoter.

Cooperativity: action at a distance in a classic system.

A new high resolution crystal structure of the phage lambda repressor reveals the basis for repressor dimer formation and, together with biochemical data, provides insights into the mechanism of repressor tetramer formation, a process essential to the cooperative binding and gene regulatory activities of this protein.

Dimerisation mutants of lac repressor. II. A single amino acid substitution, D278L, changes the specificity of dimerisation

Assembly of the lactose repressor tetramer involves two subunit interfaces, the C-terminal heptad repeats, and the monomer-monomer interface. Dimerisation between two monomers of Lac repressor of Escherichia coli lacking the two C-terminal heptad repeats occurs through the interactions between three α-helices of each monomer, which form a highly hydrophobic interface. Residues possibly involved in specific dimer formation are known from X-ray studies and from the phenotypes of more than 4000 single amino acid substitutions. During the examination of numerous mutants within the dimerisation interface of Lac repressor, we found that substitution of one amino acid, D278 to leucine, is sufficient to change the specificity of dimerisation. Analysis of this single substitution indicates that D278L mutant Lac repressor represses like wild-type. However, it no longer forms heterodimers with wild-type Lac repressor.

Structure and Dynamics of the Tetrameric Mnt Repressor and a Model for its DNA Complex

The tetrameric Mnt repressor of bacteriophage P22 consists of two dimeric DNA-binding domains and a tetramerization domain. The NOE and chemical shift data demonstrate that the structures of the domains in the wild-type repressor protein are similar to those of the separate domains, the three-dimensional structures of which have been determined previously. 15N relaxation measurements show that the linker that connects the anti-parallel four-helix bundle with the two β-sheet DNA-binding dimers is highly flexible. No evidence was found for interactions between the distinct modules. The 15N relaxation properties of the two domains differ substantially, confirming their structural independence. A model in which one two-stranded coiled coil of the four-helix bundle is attached to one N-terminal dimer is most consistent with the biochemical data and 15N relaxation data. For the Mnt-DNA complex this geometry fits with a model in which the two β-sheet DNA-binding domains are bound at two successive major grooves of the Mnt operator and the tetramerization domain is packed between these two DNA-bound dimers. In such a model the two-fold symmetry axis of the four-helix bundle coincides with that of the operator sequence and the two bound dimers. Bending of the Mnt operator of approximately 30° upon binding of the tetramer, as measured by gel-shift assays, is in agreement with this model of the Mnt-DNA complex.

Wrapping of flanking non-operator DNA in lac repressor-operator complexes: implications for DNA looping

In our studies of lac repressor tetramer (T)-lac operator (O) interactions, we observed that the presence of extended regions of non-operator DNA flanking a single lac operator sequence embedded in plasmid DNA produced large and unusual cooperative and anticooperative effects on binding constants (Kobs) and their salt concentration dependences for the formation of 1:1 (TO) and especially 1:2 (TO2) complexes. To explore the origin of this striking behavior we report and analyze binding data on 1:1 (TO) and 1:2 (TO2) complexes between repressor and a single Osym operator embedded in 40 bp, 101 bp, and 2514 bp DNA, over very wide ranges of [salt]. We find large interrelated effects of flanking DNA length and [salt] on binding constants (KobsTO, KobsTO2) and on their [salt]-derivatives, and quantify these effects in terms of the free energy contributions of two wrapping modes, designated local and global. Both local and global wrapping of flanking DNA occur to an increasing extent as [salt] decreases. Global wrapping of plasmid-length DNA is extraordinarily dependent on [salt]. We propose that global wrapping is driven at low salt concentration by the polyelectrolyte effect, and involves a very large number (≳20) of coulombic interactions between DNA phosphates and positively charged groups on lac repressor. Coulombic interactions in the global wrap must involve both the core and the second DNA-binding domain of lac repressor, and result in a complex which is looped by DNA wrapping. The non-coulombic contribution to the free energy of global wrapping is highly unfavorable (∼+30-50 kcal mol−1), which presumably results from a significant extent of DNA distortion and/or entropic constraints. We propose a structural model for global wrapping, and consider its implications for looping of intervening non-operator DNA in forming a complex between a tetrameric repressor (LacI) and one multi-operator DNA molecule in vivo and in vitro. The existence of DNA wrapping in LacI-DNA interactions motivates the proposal that most if not all DNA binding proteins may have evolved the capability to wrap and thereby organize flanking regions of DNA.

Hinge-helix formation and DNA bending in various lac repressor-operator complexes.

The hinge-region of the lac repressor plays an important role in the models for induction and DNA looping in the lac operon. When lac repressor is bound to a tight-binding symmetric operator, this region forms an alpha-helix that induces bending of the operator. The presence of the hinge-helices is questioned by previous data that suggest that the repressor does not bend the wild-type operator. We show that in the wild-type complex the hinge-helices are formed and the DNA is bent, similar to the symmetric complex. Furthermore, our data show differences in the binding of the DNA binding domains to the half-sites of the wild-type operator and reveal the role of the central base-pair of the wild-type operator in the repressor-operator interaction. The differences in binding to the operator half-sites are incorporated into a model that explains the relative affinities of the repressor for various lac operator sequences that contain left and right half-sites with different spacer lengths.

The tetramerization domain of the Mnt repressor consists of two right-handed coiled coils.

The tetrameric Mnt repressor is involved in the genetic switch between the lysogenic and lytic growth of Salmonella bacteriophage P22. The solution structure of its C-terminal tetramerization domain, which holds together the two dimeric DNA-binding domains, has been determined by NMR spectroscopy. This structure reveals an assembly of four alpha-helical subunits, consisting of a dimer of two antiparallel coiled coils with a unique right-handed twist. The superhelical winding is considerably stronger and the interhelical separation closer than those found in the well-known left-handed coiled coils in fibrous proteins and leucine zippers. An unusual asymmetry arises between the two monomers that comprise one right-handed coiled coil. A difference in the packing to the adjacent monomer of the other coiled coil occurs with an offset of two helical turns. The two asymmetric monomers within each coiled coil interconvert on a time scale of seconds. Both with respect to symmetry and handedness of helical packing, the C2 symmetric four-helix bundle of Mnt differs from other oligomerization domains that assemble DNA-binding modules, such as that in the tumor suppressor p53 and the E. coli lac repressor.

An evolutionary link between sporulation and prophage induction in the structure of a repressor:anti-repressor complex

Spore formation is an extreme response of some bacteria to adversity. In Bacillus subtilis the proteins of the sin, s porulation in hibition, region form a component of an elaborate molecular circuitry that regulates the commitment to sporulation. SinR is a tetrameric repressor protein that binds to the promoters of genes essential for entry into sporulation and prevents their transcription. This repression is overcome through the activity of SinI, which disrupts the SinR tetramer through the formation of a SinI-SinR heterodimer. The interactions governing this curious quaternary transition are revealed in the crystal structure of the SinI-SinR complex. The most striking, and unexpected, finding is that the tertiary structure of the DNA-binding domain of SinR is identical with that of the corresponding domains of the repressor proteins, CI and Cro, of bacteriophage 434 that regulate lysis/lysogeny. This structural similarity greatly exceeds that between SinR and any bacterial protein or between the 434 repressor proteins and their homologues in the closely related bacteriophage λ. The close evolutionary relationship implied by the structures of SinR and the 434 repressors provokes both comparison of their functions and a speculative consideration of the intriguing possibility of an evolutionary link between the two adaptive responses, sporulation and prophage induction.

Comparison of the DNA Association Kinetics of the Lac Repressor Tetramer, Its Dimeric Mutant LacI adi, and the Native Dimeric Gal Repressor

The rates of association of the tetrameric Lac repressor (LacI), dimeric LacIadi (a deletion mutant of LacI), and the native dimeric Gal repressor (GalR) to DNA restriction fragments containing a single specific site were investigated using a quench-flow DNase I "footprinting" technique. The dimeric proteins, LacIadi and GalR, and tetrameric LacI possess one and two DNA binding sites, respectively. The nanomolar protein concentrations used in these studies ensured that the state of oligomerization of each protein was predominantly either dimeric or tetrameric, respectively. The bimolecular association rate constants (ka) determined for the LacI tetramer exceed those of the dimeric proteins. The values of ka obtained for LacI, LacIadi, and GalR display different dependences on [KCl]. For LacIadi and GalR, they diminish as [KCl] increases from 25 mM to 200 mM, approaching rates predicted for three-dimensional diffusion. In contrast, the ka values determined for the tetrameric LacI remain constant up to 300 mM [KCl], the highest salt concentration that could be investigated by quench-flow footprinting. The enhanced rate of association of the tetramer relative to the dimeric proteins can be modeled by enhanced "sliding" (Berg, O. G., Winter, R. B., and von Hippel, P. H. (1981) Biochemistry 20, 6929-6948) of the LacI tetramer relative to the LacIadi dimer or a combination of enhanced sliding and the superimposition of "direct transfer" mediated by the bidentate DNA interactions of the tetramer.