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The first step of gene expression in all organisms requires opening the DNA duplex to expose one strand for templated RNA synthesis. In Escherichia coli, promoter DNA sequence fundamentally determines how fast the RNA polymerase (RNAP) forms “open” complexes (RPo), whether RPo persists for seconds or hours, and how quickly RNAP transitions from initiation to elongation. These rates control promoter strength in vivo but their structural origins remain largely unknown. Here we use cryo-electron microscopy to determine structures of RPo formed de novo at three promoters with widely differing lifetimes at 37°C: λPR (t1/2 ∼ 10 hours), T7A1 (t1/2 ∼ 4 minutes), and a point mutant in λPR (λPR-5C) (t1/2 ∼ 2 hours). Two distinct RPo conformers are populated at λPR, likely representing productive and unproductive forms of RPo observed in solution studies. We find that changes in the sequence and length of DNA in the transcription bubble just upstream of the start site (+1) globally alter the network of DNA-RNAP interactions, base stacking, and strand order in the single-stranded DNA of the transcription bubble; these differences propagate beyond the bubble to upstream and downstream DNA. After expanding the transcription bubble by one base (T7A1), the nontemplate-strand “scrunches” inside the active site cleft; the template-strand bulges outside the cleft at the upstream edge of the bubble. The structures illustrate how limited sequence changes trigger global alterations in the transcription bubble that modulate RPo lifetime and affect the subsequent steps of the transcription cycle.

Recent biophysical studies of mycobacterial transcription have shed new light on this fundamental process in a group of bacteria that includes deadly pathogens such as Mycobacterium tuberculosis (Mtb), Mycobacterium abscessus (Mab), Mycobacterium leprae (Mlp), as well as the nonpathogenic Mycobacterium smegmatis (Msm). Most of the research has focused on Mtb, the causative agent of tuberculosis (TB), which remains one of the top ten causes of death globally. The enzyme RNA polymerase (RNAP) is responsible for all bacterial transcription and is a target for one of the crucial antibiotics used for TB treatment, rifampicin (Rif). Here, we summarize recent biophysical studies of mycobacterial RNAP that have advanced our understanding of the basic process of transcription, have revealed novel paradigms for regulation, and thus have provided critical information required for developing new antibiotics against this deadly disease.

The first step in gene expression in all organisms requires opening the DNA duplex to expose one strand for templated RNA synthesis. In Escherichia coli, promoter DNA sequence fundamentally determines how fast the RNA polymerase (RNAP) forms “open” complexes (RPo), whether RPo persists for seconds or hours, and how quickly RNAP transitions from initiation to elongation. These rates control promoter strength in vivo, but their structural origins remain largely unknown. Here, we use cryoelectron microscopy to determine the structures of RPo formed de novo at three promoters with widely differing lifetimes at 37 °C: λP(R) (t(1/2) ∼10 h), T7A1 (t(1/2) ∼4 min), and a point mutant in λP(R) (λP(R-5C)) (t(1/2) ∼2 h). Two distinct RPo conformers are populated at λP(R), likely representing productive and unproductive forms of RPo observed in solution studies. We find that changes in the sequence and length of DNA in the transcription bubble just upstream of the start site (+1) globally alter the network of DNA–RNAP interactions, base stacking, and strand order in the single-stranded DNA of the transcription bubble; these differences propagate beyond the bubble to upstream and downstream DNA. After expanding the transcription bubble by one base (T7A1), the nontemplate strand “scrunches” inside the active site cleft; the template strand bulges outside the cleft at the upstream edge of the bubble. The structures illustrate how limited sequence changes trigger global alterations in the transcription bubble that modulate the RPo lifetime and affect the subsequent steps of the transcription cycle.

Recent advances in single particle cryogenic electron microscopy (cryo-EM) have enabled the structural determination of numerous protein assemblies at high resolution, yielding unprecedented insights into their function. However, despite its extraordinary capabilities, cryo-EM remains time-consuming and resource-intensive. It is therefore beneficial to have a means for rapidly assessing and optimizing the quality of samples prior to lengthy cryo-EM analyses. To do this, we have developed a native mass spectrometry (nMS) platform that provides rapid feedback on sample quality and highly streamlined biochemical screening. Because nMS enables accurate mass analysis of protein complexes, it is well-suited for routine evaluation of the composition, integrity, and homogeneity of samples prior to their plunge-freezing on EM grids. We demonstrate the utility of our nMS-based platform for facilitating cryo-EM studies using structural characterizations of exemplar bacterial transcription complexes as well as the replication-transcription assembly from the SARS-CoV-2 virus that is responsible for the COVID-19 pandemic.

We present an approach for preparing cryoEM grids to study short-lived molecular states. Using piezo electric dispensing, two independent streams of ~50 pL sample drops are deposited within 10 ms of each other onto a nanowire EM grid surface, and the mixing reaction stops when the grid is vitrified in liquid ethane, on the order of ~100 ms later. We demonstrate the utility of this approach for four biological systems where short-lived states are of high interest.

We present an approach for preparing cryo-electron microscopy (cryo-EM) grids to study short-lived molecular states. Using piezoelectric dispensing, two independent streams of ~50-pl droplets of sample are deposited within 10 ms of each other onto the surface of a nanowire EM grid, and the mixing reaction stops when the grid is vitrified in liquid ethane ~100 ms later. We demonstrate this approach for four biological systems where short-lived states are of high interest. A spraying-mixing approach for preparing cryo-EM grids using the Spotiton robot allows time-resolved observations of short-lived biomolecular states.

Transcription initiation requires formation of the open promoter complex, RPo. To generate RPo, RNA polymerase (RNAP) unwinds the DNA duplex to form the transcription bubble and loads the DNA into the RNAP active site. RPo formation is a multi-step process with transient intermediates of unknown structure. We used single particle cryo-electron microscopy to visualize seven intermediates containing Escherichia coli RNAP with the transcription factor TraR en route to forming RPo. The structures span the RPo formation pathway from initial recognition of the duplex promoter in a closed complex to the final RPo. The structures and supporting biochemical data define RNAP and promoter DNA conformational changes that delineate steps on the pathway, including previously undetected transient promoter-RNAP interactions that contribute to populating the intermediates but do not occur in RPo. Our work provides a structural basis for understanding RPo formation and its regulation, a major checkpoint in gene expression throughout evolution.

Recent advances in single particle cryogenic electron microscopy (cryo-EM) have enabled the structural determination of numerous protein assemblies at high resolution, yielding unprecedented insights into their function. However, despite its extraordinary capabilities, cryo-EM remains time-consuming and resource-intensive. It is therefore beneficial to have a means for rapidly assessing and optimizing the quality of samples prior to lengthy cryo-EM analyses. To do this, we have developed a native mass spectrometry (nMS) platform that provides rapid feedback on sample quality and highly streamlined biochemical screening. Because nMS enables accurate mass analysis of protein complexes, it is well-suited for routine evaluation of the composition, integrity, and homogeneity of samples prior to their plunge-freezing on EM grids. We demonstrate the utility of our nMS-based platform for facilitating cryo-EM studies using structural characterizations of exemplar bacterial transcription complexes as well as the replication-transcription assembly from the SARS-CoV-2 virus that is responsible for the COVID-19 pandemic. Funding: This work is supported by the Pels Foundation to The Rockefeller University, NIH grants P41 GM109824 and P41 GM103314 to BTC, R35 GM118130 to SAD, and R01 GM114450 to EAC. Access to the cryo-EM microscopes and support was through The Rockefeller University Evelyn Gruss Lipper Cryo-EM Resource Center and at The Simons Electron Microscopy Center (SEMC), National Resource for Automated Molecular Microscopy (NRAMM), and National Center for CryoEM Access and Training (NCCAT) at the NYSBC, supported by NIH NIGMS (P41 GM103310), NYSTAR, the Simons Foundation (SF349247), the NIH Common Fund Transformative High Resolution CryoElectron Microscopy program (U24 GM129539) and NY State Assembly Majority. Conflict of Interest: The authors declare there are no competing interests.

RbpA and CarD are essential transcription regulators in mycobacteria. Mechanistic analyses of promoter open complex (RPo) formation establish that RbpA and CarD cooperatively stimulate formation of an intermediate (RP2) leading to RPo; formation of RP2 is likely a bottleneck step at the majority of mycobacterial promoters. Once RPo forms, CarD also disfavors its isomerization back to RP2. We determined a 2.76 Å-resolution crystal structure of a mycobacterial transcription initiation complex (TIC) with RbpA as well as a CarD/RbpA/TIC model. Both CarD and RbpA bind near the upstream edge of the −10 element where they likely facilitate DNA bending and impede transcription bubble collapse. In vivo studies demonstrate the essential role of RbpA, show the effects of RbpA truncations on transcription and cell physiology, and indicate additional functions for RbpA not evident in vitro. This work provides a framework to understand the control of mycobacterial transcription by RbpA and CarD. DOI: http://dx.doi.org/10.7554/eLife.22520.001

Previous isothermal titration calorimetry (ITC) and Forster resonance energy transfer studies demonstrated that Escherichia coli HU(αβ) binds nonspecifically to duplex DNA in three different binding modes: a tighter-binding 34-bp mode that interacts with DNA in large (>34 bp) gaps between bound proteins, reversibly bending it by 140(o) and thereby increasing its flexibility, and two weaker, modestly cooperative small site-size modes (10 bp and 6 bp) that are useful for filling gaps between bound proteins shorter than 34 bp. Here we use ITC to determine the thermodynamics of these binding modes as a function of salt concentration, and we deduce that DNA in the 34-bp mode is bent around-but not wrapped on-the body of HU, in contrast to specific binding of integration host factor. Analyses of binding isotherms (8-bp, 15-bp, and 34-bp DNA) and initial binding heats (34-bp, 38-bp, and 160-bp DNA) reveal that all three modes have similar log-log salt concentration derivatives of the binding constants (Sk(i)) even though their binding site sizes differ greatly; the most probable values of Sk(i) on 34-bp DNA or larger DNA are -7.5±0.5. From the similarity of Sk(i) values, we conclude that the binding interfaces of all three modes involve the same region of the arms and saddle of HU. All modes are entropy-driven, as expected for nonspecific binding driven by the polyelectrolyte effect. The bent DNA 34-bp mode is most endothermic, presumably because of the cost of HU-induced DNA bending, while the 6-bp mode is modestly exothermic at all salt concentrations examined. Structural models consistent with the observed Sk(i) values are proposed.

Noncovalent self-assembly of biopolymers is driven by molecular interactions between functional groups on complementary biopolymer surfaces, replacing interactions with water. Since individually these interactions are comparable in strength to interactions with water, they have been difficult to quantify. Solutes (osmolytes, denaturants) exert often large effects on these self-assembly interactions, determined in sign and magnitude by how well the solute competes with water to interact with the relevant biopolymer surfaces. Here, an osmometric method and a water-accessible surface area (ASA) analysis are developed to quantify and interpret the interactions of the remarkable osmolyte glycine betaine (GB) with molecular surfaces in water. We find that GB, lacking hydrogen bond donors, is unable to compete with water to interact with anionic and amide oxygens; this explains its effectiveness as an osmolyte in the Escherichia coli cytoplasm. GB competes effectively with water to interact with amide and cationic nitrogens (hydrogen bonding) and especially with aromatic hydrocarbon (cation-pi). The large stabilizing effect of GB on lac repressor-lac operator binding is predicted quantitatively from ASA information and shown to result largely from dehydration of anionic DNA phosphate oxygens in the protein-DNA interface. The incorporation of these results into theoretical and computational analyses will likely improve the ability to accurately model intra- and interprotein interactions. Additionally, these results pave the way for development of solutes as kinetic/mechanistic and thermodynamic probes of conformational changes and formation/disruption of molecular interfaces that occur in the steps of biomolecular self-assembly processes.

Escherichia coli HU(alphabeta), a major nucleoid-associated protein, organizes chromosomal DNA and facilitates numerous DNA transactions. Using isothermal titration calorimetry, fluorescence resonance energy transfer and a series of DNA lengths (8 bp, 15 bp, 34 bp, 38 bp and 160 bp) we established that HU(alphabeta) interacts with duplex DNA using three different nonspecific binding modes. Both the HU to DNA molar ratio ([HU]/[DNA]) and DNA length dictate the dominant HU binding mode. On sufficiently long DNA (or =34 bp), at low [HU]/[DNA], HU populates a noncooperative 34 bp binding mode with a binding constant of 2.1+/-0.4x10(6) M(-1), and a binding enthalpy of +7.7+/-0.6 kcal/mol at 15 degrees C and 0.15 M Na(+). With increasing [HU]/[DNA], HU bound in the noncooperative 34 bp mode progressively converts to two cooperative (omega approximately 20) modes with site sizes of 10 bp and 6 bp. These latter modes exhibit smaller binding constants (1.1+/-0.2x10(5) M(-1) for the 10 bp mode, 3.5+/-1.4x10(4) M(-1) for the 6 bp mode) and binding enthalpies (4.2+/-0.3 kcal/mol for the 10 bp mode, -1.6+/-0.3 kcal/mol for the 6 bp mode). As DNA length increases to 34 bp or more at low [HU]/[DNA], the small modes are replaced by the 34 bp binding mode. Fluorescence resonance energy transfer data demonstrate that the 34 bp mode bends DNA by 143+/-6 degrees whereas the 6 bp and 10 bp modes do not. The model proposed in this study provides a novel quantitative and comprehensive framework for reconciling previous structural and solution studies of HU, including single molecule (force extension measurement), fluorescence, and electrophoretic gel mobility-shift assays. In particular, it explains how HU condenses or extends DNA depending on the relative concentrations of HU and DNA.

The architecture of cellular RNA polymerases (RNAPs) dictates that transcription can begin only after promoter DNA bends into a deep channel and the start site nucleotide (+1) binds in the active site located on the channel floor. Formation of this transcriptionally competent “open” complex (RP o ) by Escherichia coli RNAP at the λP R promoter is greatly accelerated by DNA upstream of base pair −47 (with respect to +1). Here we report real-time hydroxyl radical (·OH) and potassium permanganate (KMnO 4 ) footprints obtained under conditions selected for optimal characterization of the first kinetically significant intermediate (I 1 ) in RP o formation. ·OH footprints reveal that the DNA backbone from −71 to −81 is engulfed by RNAP in I 1 but not in RP o ; downstream protection extends to approximately +20 in both complexes. KMnO 4 footprinting detects solvent-accessible thymine bases in RP o , but not in I 1 . We conclude that upstream DNA wraps more extensively on RNAP in I 1 than in RP o and that downstream DNA (−11 to +20) occupies the active-site channel in I 1 but is not yet melted. Mapping of the footprinting data onto available x-ray structures provides a detailed model of a kinetic intermediate in bacterial transcription initiation and suggests how transient contacts with upstream DNA in I 1 might rearrange the channel to favor entry of downstream duplex DNA.

Transcription initiation is a multistep process involving a series of requisite conformational changes in RNA polymerase (R) and promoter DNA (P) that create the open complex (RP(o)). Here, we use the small solutes urea and glycine betaine (GB) to probe the extent and type of surface area changes in the formation of RP(o) between Esigma(70) RNA polymerase and lambdaP(R) promoter DNA. Effects of urea quantitatively reflect changes in amide surface and are particularly well-suited to detect coupled protein folding events. GB provides a qualitative probe for the exposure or burial of anionic surface. Kinetics of formation and dissociation of RP(o) reveal strikingly large effects of the solutes on the final steps of RP(o) formation: urea dramatically increases the dissociation rate constant k(d), whereas GB decreases the rate of dissociation. Formation of the first kinetically significant intermediate I(1) is disfavored in urea, and moderately favored by GB. GB slows the rate-determining step that converts I(1) to the second kinetically significant intermediate I(2); urea has no effect on this step. The most direct interpretation of these data is that recognition of promoter DNA in I(1) involves only limited conformational changes. Notably, the data support the following hypotheses: (1) the negatively charged N-terminal domain of sigma(70) remains bound in the "jaws" of polymerase in I(1); (2) the subsequent rate-determining isomerization step involves ejecting this domain from the jaws, thereby unmasking the active site; and (3) final conversion to RP(o) involves coupled folding of the mobile downstream clamp of polymerase.

Binding of activators to upstream DNA sequences regulates transcription initiation by affecting the stability of the initial RNA polymerase (RNAP)–promoter complex and/or the rate of subsequent conformational changes required to form the open complex (RP O ). Here we observe that the presence of nonspecific upstream DNA profoundly affects an early step in formation of the transcription bubble. Kinetic studies with the λP R promoter and Escherichia coli RNAP reveal that the presence of DNA upstream of base pair -47 greatly increases the rate of forming RP O , without significantly affecting its rate of dissociation. We find that this increase is largely due to an acceleration of the rate-limiting step (isomerization) in RP O formation, a step that occurs after polymerase binds. Footprinting experiments reveal striking structural differences downstream of the transcription start site (+1) in the first kinetically significant intermediate when upstream DNA is present. On the template strand, the DNase I downstream boundary of this early intermediate is +20 when upstream DNA is present but is shortened by approximately two helical turns when upstream DNA beyond -47 is removed. KMnO 4 footprinting reveals an identical initiation bubble (-11 to +2), but unusual reactivity of template strand upstream cytosines (-12, -14, and -15) on the truncated promoter. Based on this work, we propose that early wrapping interactions between upstream DNA and the polymerase exterior strongly affect the events that control entry and subsequent unwinding of the DNA start site in the jaws of polymerase.

Interactions of the solutes glycine betaine (GB) and urea with mononucleosomal calf thymus DNA in aqueous salt solutions are characterized by vapor pressure osmometry (VPO). Analysis of osmolality as a function of solute and DNA concentration yields the effect of the solute on the chemical potential, mu(2), of the DNA. Although both GB and urea generally are nucleic acid denaturants and therefore must interact favorably with the nucleic acid surface exposed upon melting, VPO demonstrates that neither interacts favorably with duplex DNA. Addition of GB greatly increases mu(2) of DNA, indicating that the average local concentration of GB in the vicinity of the double helix is much less than its bulk concentration. By contrast, addition of urea has almost no effect on mu(2) of duplex DNA, indicating that the average local concentration of urea in the vicinity of duplex DNA is almost the same as in bulk solution. Qualitatively, we conclude that the nonuniform distribution of GB occurs primarily because duplex DNA and GB prefer to interact with water rather than with each other. Comparison with thermodynamic data for the interaction of GB with various protein surfaces (Felitsky et al., Biochemistry, 43, 14732-14743) shows that GB is excluded primarily from anionic DNA surface and that the hydration of anionic DNA phosphate oxygen surface (>or approximately 17 H(2)O per nucleotide or >or approximately 0.22 H(2)O A(-)(2)) involves at least two layers of water. From analysis of literature data for effects of urea and of GB on DNA melting, we propose that urea is an effective nonspecific nucleic acid denaturant because of its favorable interactions with the polar amide-like surface of G, C, and especially T or U bases exposed in denaturation, whereas GB is a specific GC denaturant because of its favorable interaction with G and/or C surface in the single-stranded state.

A denaturant m-value is the magnitude of the slope of a typically linear plot of the unfolding free energy change DeltaG degrees (obs) vs. molar concentration (C(3)) of denaturant. For a given protein, the guanidinium chloride (GuHCl) m-value is approximately twice as large as the urea m-value. Myers et al. (Protein Sci 1995;4:2138-2148) found that experimental m-values for protein unfolding in both urea and GuHCl are proportional to DeltaASA(corr)(max), the calculated maximum amount of protein surface exposed to water in unfolding, corrected empirically for the effects of disulfide crosslinks: (urea m-value/DeltaASA(corr)(max)) = 0.14+/-0.01 cal M(-1) A(-2) and (GuHCl m-value/DeltaASA(corr)(max)) = 0.28+/-0.03 cal M(-1) A(-2). The observed linearity of plots of DeltaG degrees (obs) vs. C(3) indicates that the difference in preferential interaction coefficients DeltaGamma(3) characterizing the interactions of these solutes with denatured and native protein surface is approximately proportional to denaturant concentration. The proportionality of m-values to DeltaASA(corr)(max) indicates that the corresponding DeltaGamma(3) are proportional to DeltaASA(corr)(max) at any specified solute concentration. Here we use the local-bulk domain model of solute partitioning in the protein solution (Courtenay et al., Biochemistry 2000;39:4455-4471) to obtain a novel quantitative interpretation of denaturant m-values. We deduce that the proportionality of m-value to DeltaASA(corr)(max) results from the proportionality of B(1)(0) (the amount of water in the local domain surrounding the protein surface exposed upon unfolding) to DeltaASA(corr)(max). We show that both the approximate proportionality of DeltaGamma(3) to denaturant concentration and the residual dependence of DeltaGamma(3)/m(3) (where m(3) is molal concentration) on denaturant concentration are quantitatively predicted by the local-bulk domain model if the molal-scale solute partition coefficient K(P) and water-solute exchange stoichiometry S(1,3) are independent of solute concentration. We obtain K(P,urea) = 1.12+/-0.01 and K(P,GuHCl) = 1.16+/-0.02 (or K(P,GuH+) congruent with 1.48), values which will be useful to characterize the effect of accumulation of those solutes on all processes in which the water-accessible area of unfolded protein surface changes. We demonstrate that the local-bulk domain analysis of an m-value plot justifies the use of linear extrapolation to estimate ( less, similar 5% error) the stability of the native protein in the absence of denaturant (DeltaG(o)(o)), with respect to a particular unfolded state. Our surface area calculations indicate that published m-values/DeltaASA ratios for unfolding of alanine-based alpha-helical oligopeptides by urea and GuHCl exceed the corresponding m-value/DeltaASA ratios for protein unfolding by approximately fourfold. We propose that this difference originates from the approximately fourfold difference (48% vs. 13%) in the contribution of polar backbone residues to DeltaASA of unfolding, a novel finding which supports the long-standing but not universally accepted hypothesis that urea and guanidinium cation interact primarily with backbone amide groups. We propose that proteins which exhibit significant deviations from the average m-value/DeltaASA ratio will be found to exhibit significant deviations from the expected amount and/or average composition of the surface exposed on unfolding.

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 ( K obs ) and their salt concentration dependences for the formation of 1:1 (TO) and especially 1:2 (TO 2 ) complexes. To explore the origin of this striking behavior we report and analyze binding data on 1:1 (TO) and 1:2 (TO 2 ) complexes between repressor and a single O sym 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 ( K obs TO , K obs TO 2 ) 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.

Formation of many site-specific protein-nucleic acid complexes involves sequential conformational changes subsequent to initial binding which create functionally active assemblies. Characterization of population distributions and structural characteristics of intermediate and product conformations is necessary to understand both the mechanisms and the thermodynamics of these processes. For these purposes, here we develop the quantitative method of multiple hit footprinting (MHF), where chemical or enzymatic probing is performed as a function of either concentrations of the footprinting agent and/or time of exposure to it, in the multiple hit regime where many of the population or subpopulation of reactive DNA molecules are modified at more than one site. Properly controlled MHF experiments yield both the population distribution of different conformers and reactivity rate constants of the footprinting agent at all reactive positions in each conformer, which may be interpreted in terms of the accessibility of the site or the local concentration of the reagent. MHF experiments are particularly well-suited for dissecting effects at sites where unbound DNA is non-reactive and bound DNA is reactive with base-specific probes (e.g. KMnO4, DMS). We suggest that this method will also be applicable to analysis of enhancements in reactivity of other footprinting agents (e.g. DNase I, HO.). To demonstrate the utility of the MHF analysis, we quantify fragment distributions and individual site reactivities from multiple-hit KMnO4 footprinting of the non-template strand of Esigma70 RNA polymerase-lambdaPR promoter DNA complexes populated at binding equilibrium at 37 degreesC and transiently populated at a fixed time after a temperature downshift from 37 degreesC to 0 degreesC. For this system, a MHF analysis directly addresses the following questions: (i) what fraction of the population of promoter DNA molecules is open in the vicinity of the transcription start site (RPo) both at 37 degreesC and (transiently) after a downshift to 0 degreesC; (ii) does opening of the start site region in RPo occur entirely in one mechanistic step at the lambdaPR promoter and (iii) does the structure of RPo vary with temperature? In addition, we use the MHF-determined population distribution of KMnO4-reactive (RPo) and non-reactive promoter DNA to normalize the biphasic kinetics of decay of RPo to free promoter DNA after a 37 degrees to 0 degreesC temperature downshift, and thereby characterize the kinetics of the conformational changes involved in forming RPo.

Kinetic studies of formation and dissociation of open-promoter complexes (RPo) involving Eσ70 RNA polymerase (R) and the λPR promoter (P) demonstrate the existence of two kinetically significant intermediates, designated I1 and I2, and facilitate the choice of conditions under which each accumulates. For such conditions, we report the results of equilibrium and transient DNase I and KMnO4 footprinting studies which characterize I1 and I2. At 0°C, where extrapolation of equilibrium data indicates I1 is the dominant complex, DNA bases in the vicinity of the transcription start site (+1) do not react with KMnO4, indicating that this region is closed in I1. However, the DNA backbone in I1 is extensively protected from DNase I cleavage; the DNase I footprint extends ∼30 bases downstream and at least ∼40 bases upstream from the start site. I1 has a short lifetime (⩽15 seconds), based on its sensitivity to competition with heparin. Shortly after a temperature downshift from 37°C to 0°C, in the time-range where we conclude that the dominant, transiently accumulated complex is I2, DNase I and KMnO4 footprinting reveal a complex with a closed-start site and an extended DNase I footprint like that of I1. However, unlike I1, I2 is insensitive to heparin competition and has a much longer dissociation lifetime at 0°C. Based on footprinting, kinetic and thermodynamic studies, we conclude that in the short-lived intermediate I1 the promoter start site and downstream region are bound in a cleft defined by the open clamp-like jaws of Eσ70. We propose that binding of the start site and downstream DNA in this cleft triggers massive, relatively slow conformational changes which likely include RNA polymerase jaw closing with coupled folding. These proposed conformational changes occur prior to opening of the promoter start site region, and are responsible for the much longer lifetime of I2. Closing of the jaws of polymerase around the downstream region of promoter DNA appears to trigger opening of the start site region. From a quantitative analysis of the biphasic decay of KMnO4 reactivity of RPo at 0°C, we obtain the equilibrium constant K3 for the conversion of I2 to RPo and the rate constant k−2 for the conversion of I2 to I1 (i.e. jaw opening). These quantitative results were previously unavailable at any temperature, and are necessary for the dissection of dissociation kinetic data at higher temperatures.

In this issue of Cell, Hsu et al. (2006) report on the binding activity of a variant of the bacterial transcriptional specificity factor sigma (sigma) to promoter DNA. This study demonstrates that the sigma variant induces a large distortion in the transcriptional start site in the absence of core RNA polymerase, raising intriguing new questions about the roles of sigma and core RNA polymerase in transcription initiation.

The interaction of lac operator DNA with lac repressor (LacI) is a classic example of a genetic regulatory switch. To dissect the role of stoichiometry, subunit association, and effects of DNA length in positioning this switch, we have determined binding isotherms for the interaction of LacI with a high affinity (Osym) operator on linearized plasmid (2500 bp) DNA over a wide range of macromolecular concentrations (10(-14) to 10(-8) M). Binding data were analyzed using a thermodynamic model involving four equilibria: dissociation of tetramers (T) into dimers (D), and binding of operator-containing plasmid DNA (O) to dimers and tetramers to form three distinct complexes, DO, TO, and TO2. Over the range of concentrations of repressor, operator, and salt (0.075 M K+ to 0.40 M K+) investigated, we find no evidence for any significant thermodynamic effect of LacI dimers. Instead, all isotherms can be interpreted in terms of just two equilibria, involving only T and the TO and TO2 complexes. As a reference binding equilibrium, which we propose must approximate the DO binding interaction, we compare the plasmid Osym results with our extensive studies of the binding of a 40 bp Osym DNA fragment to LacI. On this basis, we obtain a lower bound on the LacI dimer-tetramer equilibrium constant and values of the equilibrium constants for formation of TO and TO2 complexes. At a salt concentration of 0.40 M, the Osym plasmid binding data are consistent with a model with two independent and identical binding sites for operator per LacI tetramer, in which the binding to a site on the tetramer is only slightly more favorable than the reference binding interaction. Increasingly large deviations from the independent-site model are observed as the salt concentration is reduced; binding of a second operator to from TO2 becomes strongly disfavored relative to formation of TO at low salt concentrations (0.075 to 0.125 M). In addition, binding of both the first and second plasmid operator DNA molecules to the tetramer becomes increasingly more favorable than the reference binding interaction as [K+] is reduced from 0.40 M to 0.125 M. At 0.075 M K+, however, the strength of binding of the second plasmid operator DNA to the LacI tetramer is dramatically reduced; this interaction is much less favorable than binding the first plasmid operator DNA, and becomes much less favorable than the reference binding interaction. We propose that these differences arise from changes in the nature of the TO and TO2 complexes with decreasing salt concentration. At low salt concentration, we suggest the hypothesis that flanking non-operator sequences bind non-specifically (coulombically) by local wrapping, and that distant regions of non-operator DNA occupy the second operator-binding site by looping. We propose that wrapping stabilizes both 1:1 and 2:1 complexes at low salt concentration, and that looping stabilizes the 1:1 complex but competitively destabilizes the 2:1 TO2 complex at low salt concentration. These effects must play a role in adjusting the stability and structure of the LacI-lac operator repression complex as the cytoplasmic [K+] varies in response to changes in extracellular osmolarity.

Ion concentrations (K+, Glu-) in the cytoplasm of growing Escherichia coli cells increase strongly with increases in the osmolarity of a defined growth medium. While in vitro experiments demonstrate that the extent of protein-nucleic acid interactions (PNAI) depends critically on salt concentration, in vivo measurements indicate that cells maintain a relatively constant extent of PNAI independent of the osmolarity of growth. How do cells buffer PNAI against changes in the cytoplasmic environment? At high osmolarity, the increase in macromolecular crowding which accompanies the reduction in amount of cytoplasmic water in growing cells appears quantitatively sufficient to compensate for the increase in [K+]. At low osmolarity, however, changes in crowding appear to be insufficient to compensate for changes in [K+], and additional mechanisms must be involved. Here we report quantitative determinations of in vivo total concentrations of polyamines (putrescine(2+), spermidine(3+)) as a function of osmolarity (OsM) of growth, and in vitro binding data on the effects of putrescine concentration on a specific PNAI (lac repressor-lac operator) as a function of [K+]. The total concentration of putrescine in cytoplasmic water decreases at least eightfold from low osmolarity (approximately 64 mmol (l H2O)-1 at 0.03 OsM) to high osmolarity (approximately 8 mmol (l H2O)-1 at 1.02 OsM). Over this osmotic range the total [K+] increases from approximately 0.2 mol (l H2O)-1 to approximately 0.8 mol (lH2O)-1. We find that the effect of putrescine concentration on the repressor-operator interaction in vitro is purely competitive and is quantitatively described by a simple competition formalism in which lac repressor behaves a a specific-binding oligocation (ZR = 8+/-3). We demonstrate that this thermodynamic result is consistent with a structural analysis of the number of positively charged side-chains on two DNA binding domains of repressor which interact with the phosphodiester backbone of the operator site. Since this oligocation character of the binding surface of DNA-binding proteins appears to be general, we propose the competitive effects of putrescine and K+ concentrations on the strength of specific binding are general. At low osmolarity, compensating changes in putrescine and K+ concentration in response to changes in external osmolarity provide a general mechanism for E. coli to vary cytoplasmic osmolarity while maintaining a constant extent of PNAI.

Initiation of RNA synthesis from DNA templates by RNA polymerase (RNAP) is a multi-step process, in which initial recognition of promoter DNA by RNAP triggers a series of conformational changes in both RNAP and promoter DNA. The bacterial RNAP functions as a molecular isomerization machine, using binding free energy to remodel the initial recognition complex, placing downstream duplex DNA in the active site cleft and then separating the nontemplate and template strands in the region surrounding the start site of RNA synthesis. In this initial unstable "open" complex the template strand appears correctly positioned in the active site. Subsequently, the nontemplate strand is repositioned and a clamp is assembled on duplex DNA downstream of the open region to form the highly stable open complex, RP(o). The transcription initiation factor, σ(70), plays critical roles in promoter recognition and RP(o) formation as well as in early steps of RNA synthesis.

Transcription by all RNA polymerases (RNAPs) requires a series of large-scale conformational changes to form the transcriptionally competent open complex RP(o). At the lambdaP(R) promoter, Escherichia coli sigma(70) RNAP first forms a wrapped, closed 100 bp complex I(1). The subsequent step opens the entire DNA bubble, creating the relatively unstable (open) complex I(2). Additional conformational changes convert I(2) to the stable RP(o). Here we probe these events by dissecting the effects of Na(+) salts of Glu(-), F(-), and Cl(-) on each step in this critical process. Rapid mixing and nitrocellulose filter binding reveal that the binding constant for I(1) at 25 degrees C is approximately 30-fold larger in Glu(-) than in Cl(-) at the same Na(+) concentration, with the same log-log salt concentration dependence for both anions. In contrast, both the rate constant and equilibrium constant for DNA opening (I(1) to I(2)) are only weakly dependent on salt concentration, and the opening rate constant is insensitive to replacement of Cl(-) with Glu(-). These very small effects of salt concentration on a process (DNA opening) that is strongly dependent on salt concentration in solution may indicate that the backbones of both DNA strands interact with polymerase throughout the process and/or that compensation is present between ion uptake and release. Replacement of Cl(-) with Glu(-) or F(-) at 25 degrees C greatly increases the lifetime of RP(o) and greatly reduces its salt concentration dependence. By analogy to Hofmeister salt effects on protein folding, we propose that the excluded anions Glu(-) and F(-) drive the folding and assembly of the RNAP clamp/jaw domains in the conversion of I(2) to RP(o), while Cl(-) does not. Because the Hofmeister effect of Glu(-) or F(-) largely compensates for the destabilizing Coulombic effect of any salt on the binding of this assembly to downstream promoter DNA, RP(o) remains long-lived even at 0.5 M Na(+) in Glu(-) or F(-) salts. The observation that Esigma(70) RP(o) complexes are exceedingly long-lived at moderate to high Glu(-) concentrations argues that Esigma(70) RNAP does not dissociate from strong promoters in vivo when the cytoplasmic glutamate concentration increases during osmotic stress.

Though opening of the start site (+1) region of promoter DNA is required for transcription by RNA polymerase (RNAP), surprisingly little is known about how and when this occurs in the mechanism. Early events at the λ P R promoter load this region of duplex DNA into the active site cleft of Escherichia coli RNAP, forming the closed, permanganate-unreactive intermediate I 1 . Conversion to the subsequent intermediate I 2 overcomes a large enthalpic barrier. Is I 2 open? Here we create a burst of I 2 by rapidly destabilizing open complexes (RP o ) with 1.1 M NaCl. Fast footprinting reveals that thymines at positions from -11 to +2 in I 2 are permanganate-reactive, demonstrating that RNAP opens the entire initiation bubble in the cleft in a single step. Rates of decay of all observed thymine reactivities are the same as the I 2 to I 1 conversion rate determined by filter binding. In I 2 , permanganate reactivity of the +1 thymine on the template (t) strand is the same as the RP o control, whereas nontemplate (nt) thymines are significantly less reactive than in RP o . We propose that: ( i ) the +1(t) thymine is in the active site in I 2 ; ( ii ) conversion of I 2 to RP o repositions the nt strand in the cleft; and ( iii ) movements of the nt strand are coupled to the assembly and DNA binding of the downstream clamp and jaw that occurs after DNA opening and stabilizes RP o . We hypothesize that unstable open intermediates at the λ P R promoter resemble the unstable, transcriptionally competent open complexes formed at ribosomal promoters.

Bacterial RNA polymerase and a “sigma” transcription factor form an initiation-competent “open” complex at a promoter by disruption of about 14 base pairs. Strand separation is likely initiated at the highly conserved − 11 A–T base pair. Amino acids in conserved region 2.3 of the main Escherichia coli sigma factor, σ 70 , are involved in this process, but their roles are unclear. To monitor the fates of particular bases upon addition of RNA polymerase, promoters bearing single substitutions of the fluorescent A-analog 2-aminopurine (2-AP) at − 11 and two other positions in promoter DNA were examined. Evidence was obtained for an open intermediate on the pathway to open complex formation, in which these 2-APs are no longer stacked onto their neighboring bases. The tyrosine at residue 430 in region 2.3 of σ 70 was shown to be involved in quenching the fluorescence of a 2-AP substituted at − 11, presumably through a stacking interaction. These data refine the structural model for open complex formation and reveal a novel interaction involved in DNA melting by RNA polymerase.

To characterize driving forces and driven processes in formation of a large-interface, wrapped protein-DNA complex analogous to the nucleosome, we have investigated the thermodynamics of binding the 34-base pair (bp) H' DNA sequence to the Escherichia coli DNA-remodeling protein integration host factor (IHF). Isothermal titration calorimetry and fluorescence resonance energy transfer are applied to determine effects of salt concentration [KCl, KF, K glutamate (KGlu)] and of the excluded solute glycine betaine (GB) on the binding thermodynamics at 20 degrees C. Both the binding constant K(obs) and enthalpy Delta H degrees (obs) depend strongly on [salt] and anion identity. Formation of the wrapped complex is enthalpy driven, especially at low [salt] (e.g., Delta H(o)(obs)=-20.2 kcal x mol(-1) in 0.04 M KCl). Delta H degrees (obs) increases linearly with [salt] with a slope (d Delta H degrees (obs)/d[salt]), which is much larger in KCl (38+/-3 kcal x mol(-1) M(-1)) than in KF or KGlu (11+/-2 kcal x mol(-1) M(-1)). At 0.33 M [salt], K(obs) is approximately 30-fold larger in KGlu or KF than in KCl, and the [salt] derivative SK(obs)=dlnK(obs)/dln[salt] is almost twice as large in magnitude in KCl (-8.8+/-0.7) as in KF or KGlu (-4.7+/-0.6). A novel analysis of the large effects of anion identity on K(obs), SK(obs) and on Delta H degrees (obs) dissects coulombic, Hofmeister, and osmotic contributions to these quantities. This analysis attributes anion-specific differences in K(obs), SK(obs), and Delta H degrees (obs) to (i) displacement of a large number of water molecules of hydration [estimated to be 1.0(+/-0.2)x10(3)] from the 5340 A(2) of IHF and H' DNA surface buried in complex formation, and (ii) significant local exclusion of F(-) and Glu(-) from this hydration water, relative to the situation with Cl(-), which we propose is randomly distributed. To quantify net water release from anionic surface (22% of the surface buried in complexation, mostly from DNA phosphates), we determined the stabilizing effect of GB on K(obs): dlnK(obs)/d[GB]=2.7+/-0.4 at constant KCl activity, indicating the net release of ca. 150 H(2)O molecules from anionic surface.

Nonspecific protein–DNA complexes form largely independently of deoxyribonucleic acid (DNA) sequence or structure. Typically, the thermodynamic driving force for forming these complexes is electrostatic due to the polyelectrolyte (polyanionic) nature of the DNA. Keywords: nonspecific binding; cooperativity; protein–nucleic interactions; polyelectrolyte effect

The stability of noncovalent protein–DNA complexes is typically sensitive to the ionic composition of the solution, in a manner that is dependent on the specific ion concentrations and is not a simple ionic strength effect. One important origin of this sensitivity to solution conditions is the polyelectrolyte effect. Keywords: Protein–nucleic acid interactions; thermodynamics; polyelectrolytes; binding

The formation of the transcriptionally-competent open complex (RPo) by E. coli RNA polymerase at the λPR promoter involves at least three steps and two kinetically-significant intermediates (I1 and I2). Understanding the sequence of conformational changes (rearrangements in the jaws of RNAP, DNA opening) that occur in the conversion of I1 to RPo requires: 1) dissecting the rate constant kd for the dissociation of RPo into contributions from individual steps and 2) isolating and characterizing I2. To deconvolute kd, we develop experiments involving rapid upshifts to elevated concentrations of RPo-destabilizing solutes (“perturbants”: urea and KCl) to create a burst in the population of I2. At high concentrations of either perturbant, kd approaches the same [perturbant]-independent value at both 10 °C and 37 °C, interpreted as the rate constant k−2 for I2 → I1. The large effects of [urea] and [salt] on K3 (the equilibrium constant for I2 ⇄ RPo) indicate that a large-scale folding transition in polymerase forms a new interface with the DNA late in the mechanism. We deduce that I2 at the λPR promoter is always unstable relative to RPo, even at 0 °C, explaining previous difficulties in detecting it by using temperature downshifts. Evidence for an additional unstable intermediate (I3) in the mechanism between I2 and RPo is presented. The large positive enthalpy change associated with open complex formation is divided between the steps converting I1 to RPo, consistent with a mechanism in which DNA opening occurs in several stages.

Noncoding small RNAs regulate gene expression in all organisms, in some cases through direct association with RNA polymerase (RNAP). Here we report that the mechanism of 6 S RNA inhibition of transcription is through specific, stable interactions with the active site of Escherichia coli RNAP that exclude promoter DNA binding. In fact, the DNA-dependent RNAP uses bound 6 S RNA as a template for RNA synthesis, producing 14-to 20-nucleotide RNA products (pRNA). These results demonstrate that 6 S RNA is functionally engaged in the active site of RNAP. Synthesis of pRNA destabilizes 6 S RNA–RNAP complexes leading to release of the pRNA-6 S RNA hybrid. In vivo, 6 S RNA–directed RNA synthesis occurs during outgrowth from the stationary phase and likely is responsible for liberating RNAP from 6 S RNA in response to nutrient availability.

Transcription initiation is a multistep process involving a series of requisite conformational changes in RNA polymerase (R) and promoter DNA (P) that create the open complex (RP(o)). Here, we use the small solutes urea and glycine betaine (GB) to probe the extent and type of surface area changes in the formation of RP(o) between Esigma(70) RNA polymerase and lambdaP(R) promoter DNA. Effects of urea quantitatively reflect changes in amide surface and are particularly well-suited to detect coupled protein folding events. GB provides a qualitative probe for the exposure or burial of anionic surface. Kinetics of formation and dissociation of RP(o) reveal strikingly large effects of the solutes on the final steps of RP(o) formation: urea dramatically increases the dissociation rate constant k(d), whereas GB decreases the rate of dissociation. Formation of the first kinetically significant intermediate I(1) is disfavored in urea, and moderately favored by GB. GB slows the rate-determining step that converts I(1) to the second kinetically significant intermediate I(2); urea has no effect on this step. The most direct interpretation of these data is that recognition of promoter DNA in I(1) involves only limited conformational changes. Notably, the data support the following hypotheses: (1) the negatively charged N-terminal domain of sigma(70) remains bound in the "jaws" of polymerase in I(1); (2) the subsequent rate-determining isomerization step involves ejecting this domain from the jaws, thereby unmasking the active site; and (3) final conversion to RP(o) involves coupled folding of the mobile downstream clamp of polymerase.

The organization of large regions of DNA on the surface of proteins is critical to many DNA 'transactions', including replication, transcription, recombination and repair, as well as the packaging of chromosomal DNA. Recent thermodynamic and structural studies of DNA binding by integration host factor indicate that the disruption of protein surface salt bridges (dehydrated ion pairs) dominates the observed thermodynamics of integration host factor binding and, more generally, allows the wrapping of DNA on protein surfaces. The proposed thermodynamic signature of wrapping with coupled salt bridge disruption includes large negative salt-concentration-dependent enthalpy, entropy and heat capacity changes and smaller than expected magnitudes of the observed binding constant and its power dependence on salt concentration. Examination of the free structures of proteins recently shown to wrap DNA leads us to hypothesize that a pattern of surface salt bridges interspersed with cationic sidechains provides a structural signature for wrapping and that the number and organization of salt bridges and cationic groups dictate the thermodynamics and topology of DNA wrapping, which in turn are critical to function.

The kinetics of interaction of Esigma(70) RNA polymerase (R) with the lambdaP(R) promoter (P) were investigated by filter binding over a broad range of temperatures (7.3-42 degrees C) and concentrations of RNA polymerase (1-123 nM) in large excess over promoter DNA. Under all conditions examined, the kinetics of formation of competitor-resistant complexes (I(2), RP(o)) are single-exponential with first order rate constant beta(CR). Interpretation of the polymerase concentration dependence of beta(CR) in terms of the three step mechanism of open complex formation yields the equilibrium constant K(1) for formation of the first kinetically significant intermediate (I(1)) and the forward rate constant (k(2)) for the conformational change converting I(1) to the second kinetically significant intermediate I(2): R + P--(K(1))--I(1)(k(2))--I(2). Use of rapid quench mixing allows K(1) and k(2) to be individually determined over the entire temperature range investigated, previously not possible at this promoter using manual mixing. Given the large (60 bp) interface formed in I(1), its relatively small binding constant K(1) at 37 degrees C at this [salt] (approximately 6 x 10(6) M(-1)) strongly argues that binding free energy is used to drive large-scale structural changes in polymerase and/or promoter DNA or other coupled processes. Evidence for coupling of protein folding is provided by the large and negative activation heat capacity of k(a)[DeltaC(o,++)(a)= -1.5(+/-0.2)kcal K(-1)], now shown to originate directly from formation of I(1) [DeltaC(o)(1)= -1.4(+/-0.3)kcal K(-1)] rather than from the formation of I(2) as previously proposed. The isomerization I(1)--I(2) exhibits relatively slow kinetics and has a very large temperature-independent Arrhenius activation energy [E(act)(2)= 34(+/-2)kcal]. This kinetic signature suggests that formation of the transition state (I(1)-I(2)++ involves large conformational changes dominated by changes in the exposure of polar and/or charged surface to water. Structural and biochemical data lead to the following hypotheses to interpret these results. We propose that formation of I(1) involves coupled folding of unstructured regions of polymerase (beta, beta' and sigma(70)) and bending of promoter DNA (in the -10 region). We propose that interactions with region 2 of sigma(70) and possibly domain 1 of beta induce a kink at the -11/-12 base pairs of the lambdaP(R) promoter which places the downstream DNA (-5 to +20) in the jaws of the beta and beta' subunits of polymerase in I(1). These early interactions of beta and beta' with the DNA downstream of position -5 trigger jaw closing (with coupled folding) and subsequent steps of DNA opening.

The thermodynamics of self-assembly of a 14 base pair DNA double helix from complementary strands have been investigated by titration (ITC) and differential scanning (DSC) calorimetry, in conjunction with van't Hoff analysis of UV thermal scans of individual strands. These studies demonstrate that thermodynamic characterization of the temperature-dependent contributions of coupled conformational equilibria in the individual "denatured" strands and in the duplex is essential to understand the origins of duplex stability and to derive stability prediction schemes of general applicability. ITC studies of strand association at 293 K and 120 mM Na+ yield an enthalpy change of -73 +/- 2 kcal (mol of duplex)-1. ITC studies between 282 and 312 K at 20, 50, and 120 mM Na+ show that the enthalpy of duplex formation is only weakly salt concentration-dependent but is very strongly temperature-dependent, decreasing approximately linearly with increasing temperature with a heat capacity change (282-312 K) of -1.3 +/- 0.1 kcal K-1 (mol of duplex)-1. From DSC denaturation studies in 120 mM Na+, we obtain an enthalpy of duplex formation of -120 +/- 5 kcal (mol of duplex)-1 and an estimate of the corresponding heat capacity change of -0.8 +/- 0.4 kcal K-1 (mol of duplex)-1 at the Tm of 339 K. van't Hoff analysis of UV thermal scans on the individual strands indicates that single helix formation is noncooperative with a temperature-independent enthalpy change of -5.5 +/- 0.5 kcal at 120 mM Na+. From these observed enthalpy and heat capacity changes, we obtain the corresponding thermodynamic quantities for two fundamental processes: (i) formation of single helices from disordered strands, involving only intrastrand (vertical) interactions between neighboring bases; and (ii) formation of double helices by association (docking) of single helical strands, involving interstrand (horizontal and vertical) interactions. At 293 K and 120 mM Na+, we calculate that the enthalpy change for association of single helical strands is approximately -64 kcal (mol of duplex)-1 as compared to -210 kcal (mol of duplex)-1 calculated for duplex formation from completely unstructured single strands and to the experimental ITC value of -73 kcal (mol of duplex)-1. The intrinsic heat capacity change for association of single helical strands to form the duplex is found to be small and positive [ approximately 0.1 kcal K-1 (mol of duplex)-1], in agreement with the result of a surface area analysis, which also predicts an undetectably small heat capacity change for single helix formation.

What are the thermodynamic consequences of the stepwise conversion of a highly specific (consensus) protein-DNA interface to one that is nonspecific? How do the magnitudes of key favorable contributions to complex stability (burial of hydrophobic surfaces and reduction of DNA phosphate charge density) change as the DNA sequence of the specific site is detuned? To address these questions we investigated the binding of lac repressor (LacI) to a series of 40 bp fragments carrying symmetric (consensus) and variant operator sequences over a range of temperatures and salt concentrations. Variant DNA sites contained symmetrical single and double base-pair substitutions at positions 4 and/or 5 [sequence: see text] in each 10 bp half site of the symmetric lac operator (Osym). Non-specific interactions were examined using a 40 bp non-operator DNA fragment. Disruption of the consensus interface by a single symmetrical substitution reduces the observed equilibrium association constant (K(obs)) for Osym by three to four orders of magnitude; double symmetrical substitutions approach the six orders in magnitude difference between specific and non-specific binding to a 40 bp fragment. At these adjacent positions in the consensus site, the free energy effects of multiple substitutions are non-additive: the first reduces /deltaG(obs)o/ by 3 to 5 kcal mol(-1), approximately halfway to the non-specific level, whereas the second is less deleterious, reducing /deltaG(obs)o/ by less than 3 kcal mol(-1). Variant-specific dependences of K(obs) on temperature and salt concentration characterize these LacI-operator interactions. In general, binding constants and standard free energies of binding both exhibit characteristic extrema near 290 K. As a consequence, both the enthalpic and entropic contributions to stability of Osym and variant complexes change from positive (i.e. entropy driven) at lower temperatures to negative (i.e. enthalpy driven) at higher temperatures, indicating that the heat capacity change upon binding, deltaC(obs)o, is large and negative. In general, /deltaC(obs)o/ decreases as the specificity and stability of the variant complex decreases. Stabilities of complexes of LacI with Osym and all variant operators are strongly [salt]-dependent. Binding constants for the variant complexes exhibit a power-dependence on [salt] that is larger in magnitude (i.e. more negative) than for Osym, but no obvious trend relates changes in contributions from the polyelectrolyte effect and the observed reductions in stability (delta deltaG(obs)o). These variant-specific thermodynamic signatures provide novel insights into the consequences of converting a consensus interface to a less specific one; such insights are not obtained from comparisons at the level of delta deltaG(obs)o. We propose that this variant-specific behavior arises from a strong effect of operator sequence on the extent of induced conformational changes in the protein (and possibly also in the DNA site) which accompany binding.

RNA polymerase (RNAP) is a complex molecular motor responsible for catalyzing the synthesis of RNA from DNA in a promoter sequence-dependent manner. Knowledge of the mechanism of transcription initiation is crucial to understanding the regulation of gene expression. However, the RNAP-DNA intermediates on the pathway to open complex formation during transcription initiation are extremely short-lived and thus have been very difficult to characterize using traditional structural methods. Here, we present work focused on developing rapid, solution-based methods that allow us to characterize RNAP-DNA structures in the millisecond time regime. These include: fast DNA footprinting (using hydroxyl radical and permanganate probes) to characterize the interaction of RNAP with the DNA backbone and the extent of thymine base unstacking; stopped-flow FRET experiments to monitor DNA bending in real time; and 2-aminopurine fluorescence experiments to characterize the kinetics of DNA opening. In a related project, we utilize thin layer chromatography and fluorescence spectroscopy to characterize the short (2, 3 and 4-mer) RNA products made by RNAP during repeated rounds of abortive cycling before the enzyme progresses to forming full-length RNA transcripts. These combinatorial approaches have allowed us to determine the timing of loading of duplex DNA into the RNAP active site cleft and the kinetic mechanism of large-scale RNAP conformation changes leading to initial RNA synthesis. These research activities have successfully developed new methods to characterize transient intermediates in solution and to begin to develop a detailed structural-mechanistic picture of transcription initiation.

Using “burst” kinetic methods to obtain near-homogeneous populations of transient intermediates for fast footprinting, together with solute probing experiments, we have characterized the series of large-scale conformational changes in E. coli RNA Polymerase (RNAP) and λPR promoter DNA that occur in “isomerization” of the initial recognition complex to form the stable open complex (RPo). We find that RNAP is a molecular isomerization machine that uses wrapping of upstream DNA to place the start-site region of the downstream duplex in the cleft (shown by HO protection and FRET in the closed intermediate I1).1 Then, in the rate determining step, RNAP opens the entire 13 bp initiation bubble (as judged by permanganate reactive thymines) and places the start site base of the template strand in the active site to form a transient open intermediate (I2).2 After this opening/ untwisting step, RNAP stabilizes the open DNA conformation by step-wise assembly of an encircling downstream jaw/ clamp, together with repositioning of the nontemplate strand in the cleft to form the more stable open intermediate I3 and convert it to the stable open complex RPo at λPR.2,3To test these conclusions, we are investigating deletions of the downstream “jaw” of RNAP [B’1149-1190], upstream and/ or downstream DNA, and/ or region 1.1 of σ70 subunit of RNAP [1-98] on the kinetics of formation and lifetime of open complexes. Remarkably, many of these deletions have large effects on the rate-determining, DNA-opening step, suggesting a synergy between upstream, downstream and in-cleft interactions in this sophisticated molecular machine.1. Davis et al. ’07; Drennan, Saecker et al., in preparation2. Gries et al. ‘103. Kontur, Gries et al.’06, ’08, ‘10Supported by NIH GM23467

The structural homologs HUαβ and IHF are major nucleoid associated proteins (NAPs) of Escherichia coli, which organize chromosomal DNA and facilitate numerous DNA transactions. Using isothermal titration calorimetry (ITC), fluorescence resonance energy transfer (FRET) and a series of DNA duplex lengths (8, 15, 34, 38 and 160 base pairs) we establish three different nonspecific binding modes for both HUαβ (Koh et al., 2008) and IHF. Both the NAP:DNA mole ratio ([NAP]/[DNA]) and DNA length dictate the dominant NAP binding mode. On sufficiently long DNA, at low [NAP]/[DNA], both HU and IHF populate a noncooperative 34 bp binding mode with a binding constant of ∼ 107 M−1 at 0.082 M Na+. With increasing [NAP]/[DNA], both HU and IHF bound in the noncooperative 34 bp mode progressively convert to two moderately cooperative modes with site sizes of 10 bp and 6 bp and smaller binding constants. As DNA length increases at low [NAP]/[DNA], fractional population of the 34 bp mode increases. The 34 bp mode of IHF exhibits a large negative ΔCp,obs° and an exothermic ΔHobs° (15 - 25°C), similar to previous observations for the specific complex of IHF and wrapped H'-DNA, whereas a small positive ΔCp,obs° and an endothermic ΔHobs° were observed for the 34 bp mode of HU. From these and parallel studies at various salt concentrations we propose that DNA is wrapped on the body of IHF in the nonspecific 34 bp mode like the specific complex of IHF and H'-DNA, whereas DNA is bent but not wrapped in the 34 bp nonspecific HU-DNA complex. Other structural features of the binding modes of HU and IHF deduced from these studies are also discussed.This work was supported by NIH grant GM 23467.

The precise mechanism by which multi-subunit, DNA-dependent RNA polymerases (RNAP) recognize promoter DNA and form stable, transcriptionally-competent open complexes (RPo) remains elusive. Chemical and enzymatic footprints of early intermediates and RPo provide detailed pictures of the DNA in these initial and final complexes in transcription initiation. We have recently discovered that the start site for transcription (+1) remains double-stranded when it is first loaded into the active site channel of E. coli RNAP at the λ phage PR promoter (Davis et al. PNAS, 2007). These experiments reveal unambiguously that opening of the transcription bubble occurs subsequently in the “jaws” of RNAP as RNAP actively destabilizes the duplex. To probe whether opening of ∼14 bp of DNA occurs in stages or is “all or none” we are using the perturbants urea and KCl to destabilize RPo and populate late transcription initiation intermediates. Analysis of the dissociation kinetics over a range of urea and KCl concentrations provides evidence for two transient intermediates in the DNA opening process. Using KMnO4 footprinting we are probing the extent of DNA opening in these intermediates under these conditions. Results from these novel rapid (millisecond) footprinting experiments and the implications for the mechanism of promoter opening will be presented.

Interactions between RNA polymerase and specific promoter DNA sequences trigger a precise progression of conformational changes in both biomolecules. These steps constitute the mechanism of DNA opening and the start of transcription; each step provides a critical checkpoint for regulatory input. Studies of E. coli RNA polymerase demonstrate that binding free energy alone opens the initiation bubble (−11 to +2), placing the +1 template base in the active site of the enzyme. Subsequent conformational changes are required to form the stable open complex RPo. Here we present recent fast footprinting experiments (hydroxyl radical, permanganate) that characterize the protection of the DNA backbone protection and the degree of thymine base unstacking in the three kinetically significant intermediates (I1, I2, I3) on the time scale of their formation. Experiments performed after mixing RNA polymerase and the λPR promoter DNA demonstrate that the DNA duplex containing the start site first loads in the RNA polymerase active site channel in duplex form to form I1, and that the subsequent step cooperatively opens the entire transcription bubble. In the back direction, [salt] upshift experiments demonstrate the existence of two unstable open intermediates, I2 and I3. Comparison of the degree of protection of the backbone in I2, I3 and RPo reveals differences between the nontemplate (NT) strand in these complexes but not the template (T) strand. We propose that the T strand is loaded first, followed by steps that reposition the NT strand, assemble the downstream clamp/jaw and thereby stabilize RPo. Experiments designed to test the role of the downstream RNA polymerase “jaw” and downstream DNA in the late steps will also be presented. This work was funded by NIH grant GM23467.