E. coli TraR allosterically regulates transcription initiation by altering RNA polymerase conformation
Transcription initiation is a major control point for gene expression . In bacteria , a single RNA polymerase ( RNAP ) performs all transcription . In Escherichia coli ( Eco ) , the essential primary σ factor , σ70 , binds to RNAP to form the σ70-holoenzyme ( Eσ70 ) that is capable of recognizing and initiating at promoters for most genes . Upon locating the promoter , Eσ70 melts a ~ 13 bp segment of DNA to form the open promoter complex ( RPo ) in which the DNA template strand ( t-strand ) is loaded into the RNAP active site , exposing the transcription start site ( Bae et al . , 2015b; Zuo and Steitz , 2015 ) . A key feature of the RPo formation pathway is that it is a multi-step process , with the RNAP-promoter complex passing through multiple intermediates before the final , transcription competent RPo is formed ( Hubin et al . , 2017a; Ruff et al . , 2015a; Saecker et al . , 2002 ) . A variety of transcription factors bind to the promoter DNA and/or to RNAP directly to regulate initiation ( Browning and Busby , 2016; Haugen et al . , 2008 ) . Bacterial RNAP-binding factors , encoded by the chromosome or by bacteriophage or extrachromosomal elements , interact with different regions of the enzyme to regulate its functions ( Haugen et al . , 2008 ) . One such factor is ppGpp , a modified nucleotide that functions together with the RNAP-binding protein DksA in Eco to reprogram bacterial metabolism in response to nutritional stresses during the so-called stringent response . Following amino acid starvation , ppGpp is synthesized by the RelA factor in response to uncharged tRNAs in the ribosomal A site ( Brown et al . , 2016; Cashel and Gallant , 1969; Ryals et al . , 1982 ) . Together , ppGpp and DksA alter the expression of as many as 750 genes within 5 min of ppGpp induction ( Paul et al . , 2004a; Paul et al . , 2005; Sanchez-Vazquez et al . , 2019 ) , inhibiting , for example , promoters responsible for ribosome biogenesis and activating promoters responsible for amino acid synthesis . The overall RNAP structure is reminiscent of a crab claw , with one pincer comprising primarily the β’ subunit , and the other primarily the β subunit ( Zhang et al . , 1999 ) . Between the two pincers is a large cleft that contains the active site . In Eσ70 without nucleic acids , this channel is occupied by the σ701 . 1 domain which is ejected upon entry of the downstream duplex DNA ( Bae et al . , 2013; Mekler et al . , 2002 ) . The Bridge Helix ( BH ) bridges the two pincers across the cleft , separating the cleft into the main channel , where σ701 . 1 or nucleic acids reside , and the secondary channel , where NTPs enter the RNAP active site . DksA binds in the RNAP secondary channel ( Lennon et al . , 2012; Molodtsov et al . , 2018; Perederina et al . , 2004 ) . ppGpp binds directly to RNAP at two binding sites: site 1 , located at the interface of the β′ and ω subunits ( Ross et al . , 2013; Zuo et al . , 2013 ) , and site 2 , located at the interface of β′ and DksA ( Molodtsov et al . , 2018; Ross et al . , 2016 ) . The ppGpp bound at site one inhibits transcription ~2 fold under conditions where the effects of ppGpp bound at both sites together with DksA are as much as 20-fold ( Paul et al . , 2004b; Ross et al . , 2016 ) . By contrast , ppGpp/DksA at site two has a larger effect on inhibition and is necessary and sufficient for activation ( Ross et al . , 2016 ) . TraR is a distant homolog of DksA . Although only half the length of DksA , TraR regulates Eco transcription by binding to the RNAP secondary channel and mimicking the combined effects of ppGpp and DksA ( Gopalkrishnan et al . , 2017 ) . TraR is encoded by the conjugative F plasmid and is expressed from the pY promoter as part of the major tra operon transcript ( Frost et al . , 1994; Maneewannakul and Ippen-Ihler , 1993 ) . Like DksA , TraR inhibits Eσ70-dependent transcription from ribosomal RNA promoters ( e . g . rrnB P1 ) and ribosomal protein promoters ( e . g . rpsT P2 , expressing S20 ) , and activates amino acid biosynthesis and transport promoters ( e . g . pthrABC , phisG , pargI , plivJ ) in vivo and in vitro ( Gopalkrishnan et al . , 2017 ) . The affinity of TraR for RNAP is only slightly higher than that of DksA , yet its effects on promoters negatively regulated by ppGpp/DksA in vitro are as large or larger than those of ppGpp/DksA ( Gopalkrishnan et al . , 2017 ) . The effects of TraR on promoters positively regulated by ppGpp/DksA are also independent of ppGpp ( Gopalkrishnan et al . , 2017 ) . Models for ppGpp/DksA and TraR binding to RNAP have been proposed based on biochemical and genetic approaches ( Gopalkrishnan et al . , 2017; Parshin et al . , 2015; Ross et al . , 2013; Ross et al . , 2016 ) . Crystal structures of ppGpp/DksA/RNAP and TraR/RNAP confirmed the general features of these models and provided additional detail about their interactions with RNAP ( Molodtsov et al . , 2018 ) , but did not reveal the mechanism of inhibition or activation , in large part because of crystal packing constraints on the movement of mobile regions of the complex . Thus , the structural basis for the effects of ppGpp/DksA or TraR on transcription has remained elusive . To help understand TraR regulation and principles of the regulation of transcription initiation in general , we used single particle cryo-electron microscopy ( cryo-EM ) to examine structures of Eσ70 alone , Eσ70 bound to TraR ( TraR-Eσ70 ) , and Eσ70 bound to a promoter inhibited by TraR [rpsT P2; Gopalkrishnan et al . , 2017] . Cryo-EM allows the visualization of multiple discrete conformational states populated in solution and in the absence of crystal packing constraints . Furthermore , new software tools allow for the analysis of continuous distributions of conformational heterogeneity in the cryo-EM data ( Nakane et al . , 2018 ) . The TraR-Eσ70 structures show TraR binding in the secondary channel of the RNAP , consistent with the TraR-Eσ70 model ( Gopalkrishnan et al . , 2017 ) and crystal structure ( Molodtsov et al . , 2018 ) . However , the cryo-EM structures reveal major TraR-induced changes to the RNAP conformation that were not evident in the crystal structure due to crystal packing constraints . Structural analyses generated mechanistic hypotheses for TraR function in both activation and inhibition of transcription that were then tested biochemically . Based on the combined structural and functional analyses , we propose a model in which TraR accelerates multiple steps along the RPo formation pathway and at the same time modulates the relative stability of intermediates in the pathway . Whether a promoter is activated or inhibited by TraR is determined by the intrinsic kinetic properties of the promoter ( Galburt , 2018; Haugen et al . , 2008; Paul et al . , 2005 ) .
We used single-particle cryo-EM to examine the structure of the Eco TraR-Eσ70 complex in the absence of crystal packing interactions that could restrict conformational states of the complex . We also determined cryo-EM structures of Eσ70 alone and the Eσ70-rpsT P2 promoter RPo for comparison . TraR function under cryo-EM solution conditions ( Chen et al . , 2019 ) was indistinguishable from function under standard in vitro transcription assay conditions ( Figure 1—figure supplement 1A–C ) . Analysis of the cryo-EM data for the TraR-Eσ70 complex gave rise to three distinct conformational classes ( Figure 1—figure supplement 1D ) . All three structures are essentially identical except for the disposition of Si3 [also called β’i6; Lane and Darst , 2010a] , a 188-residue lineage-specific insertion ( LSI ) in the trigger-loop ( TL ) of Eco RNAP ( Chlenov et al . , 2005 ) ( Figure 1A , B ) . The first class [TraR-Eσ70 ( I ) ] contained approximately 41% of the particles and resolved to a nominal resolution of 3 . 7 Å ( Figure 1A ) . The second class [TraR-Eσ70 ( II ) ] contained approximately 33% of the particles and resolved to a nominal resolution of 3 . 8 Å ( Figure 1B ) . The third class [TraR-Eσ70 ( III ) ] contained the remaining 26% of the particles and resolved to a nominal resolution of 3 . 9 Å ( Figure 1—figure supplement 1D , Figure 1—figure supplement 2; Supplementary file 1 ) . With Si3 ( β’ residues 948–1126 ) excluded , the structures superimpose with a root-mean-square deviation ( rmsd ) of 0 . 495 Å over 3 , 654 α-carbons . The overall binding mode of TraR in the cryo-EM structures ( Figure 1A–D ) is consistent with the effects of TraR or RNAP substitutions on TraR function ( Gopalkrishnan et al . , 2017 ) and is broadly consistent with the X-ray structure ( Molodtsov et al . , 2018 ) . TraR can be divided into three structural elements , an N-terminal helix ( TraRN , residues 2–27; Figure 1D , E ) , a globular domain ( TraRG , residues 28–57; Figure 1D , F ) , and a C-terminal helix ( TraRC , residues 58–73; Figure 1D , G ) . A 4-Cys Zn2+-binding motif spans TraRG and TraRC ( Figure 1F ) . TraRN extends from the RNAP active site out through the RNAP secondary channel to the β’rim-helices ( at the entrance to the RNAP secondary channel ) , interacting with key RNAP structural elements surrounding the active site , including the -NADFDGD- motif that chelates the active site Mg2+ ( Zhang et al . , 1999 ) , the F-loop ( Miropolskaya et al . , 2009 ) , and the bridge-helix ( Figure 1D ) . The N-terminal tip of TraRN ( TraR residue S2 ) is only 4 . 3 Å from the active site Mg2+ ( Figure 1E ) . TraRG interacts primarily with the β’rim-helices at the entrance of the secondary channel ( Figure 1D ) . The interactions of TraRC with RNAP differ substantially between the cryo-EM and X-ray structures due to conformational changes induced by TraR binding detected by the cryo-EM structure that were not observed in the X-ray structure ( see below ) . Indeed , the cryo-EM and X-ray structures superimpose with an rmsd of 4 . 26 Å over 3 , 471 α-carbons , indicating significant conformational differences . Cryo-EM data for Eσ70 resolved to a nominal resolution of 4 . 1 Å ( Figure 1—figure supplements 3 and 4; Supplementary file 1 ) . Analysis of the rpsT P2-RPo cryo-EM data ( Figure 2 ) gave rise to two conformational classes that differed only in the disposition of the upstream promoter DNA and αCTDs ( Figure 2—figure supplement 1 ) . We focus here on the highest resolution class at a nominal resolution of 3 . 4 Å ( Figure 2—figure supplement 1 , Figure 2—figure supplement 2; Supplementary file 1 ) . The closed-clamp RNAP in the rpsT P2-RPo cryo-EM structure interacts with the promoter DNA in the same way as in RPo structures determined by X-ray crystallography ( Bae et al . , 2015b; Bae et al . , 2015a; Hubin et al . , 2017b ) or cryo-EM ( Boyaci et al . , 2019 ) and is consistent with the DNase I footprint of the rpsT P2 RPo ( Gopalkrishnan et al . , 2017 ) . In the rpsT P2-RPo structure we observed an α-subunit C-terminal domain [αCTD; Ross et al . , 1993] bound to the promoter DNA minor groove ( Benoff et al . , 2002; Ross et al . , 2001 ) just upstream of the promoter −35 element [−38 to −43 , corresponding to the proximal UP element subsite; Estrem et al . , 1999] . This αCTD interacts with σ704 through an interface previously characterized through genetic analyses ( Ross et al . , 2003 ) ( Figure 2B , C ) . The αCTDs are linked to the α-N-terminal domains ( αNTDs ) by ~15 residue flexible linkers ( Blatter et al . , 1994; Jeon et al . , 1995 ) . Density for the residues connecting the αCTD and αNTD was not observed in the cryo-EM map . Comparing the RNAP conformations of the TraR-Eσ70 , Eσ70 , and rpsT P2-RPo cryo-EM structures revealed key differences that suggest how TraR activates and inhibits transcription . Below we outline these differences and test their implications for function . The three TraR-Eσ70 structures differ from each other only in the disposition of Si3 . Si3 comprises two tandem repeats of the sandwich-barrel hybrid motif ( SBHM ) fold ( Chlenov et al . , 2005; Iyer et al . , 2003 ) , SBHMa and SBHMb ( Figure 3A ) . Si3 is linked to the TL-helices by extended , flexible linkers . In TraR-Eσ70 ( I ) and TraR-Eσ70 ( II ) , Si3 is in two distinct positions with respect to the RNAP ( Figures 1A , B and 3A ) , while in TraR-Eσ70 ( III ) Si3 is disordered ( Figure 1—figure supplement 1D ) . Si3 in the TraR-Eσ70 ( I ) structure [Si3 ( I ) ] interacts primarily with the β’shelf ( SBHMa ) and the β’jaw ( SBHMb ) in a manner seen in many previous Eco RNAP X-ray ( Bae et al . , 2013 ) and cryo-EM structures ( Chen et al . , 2017; Kang et al . , 2017; Liu et al . , 2017 ) . Si3 in the TraR-Eσ70 ( II ) structure [Si3 ( II ) ] is rotated 121° such that SBHMa interacts with the β’jaw and SBHMb interacts with TraRG ( Figure 3A–C ) , a disposition of Si3 that , to our knowledge , has not been observed previously . To test if this alternative conformation [Si3 ( II ) ] is relevant to TraR function , we compared TraR-mediated function with wild-type ( WT ) and ΔSi3-RNAPs at promoters where TraR inhibits or activates transcription . Deletion of Si3 had little to no effect on TraR-mediated inhibition of rrnB P1 and rpsT P2 ( Figure 3D , Figure 3—figure supplement 1A ) but transcription by ΔSi3-RNAP was activated only ~50% compared with WT-RNAP on three different TraR-activated promoters ( pthrABC , Figure 3E; pargI , Figure 3—figure supplement 1B; phisG , Figure 3—figure supplement 1C ) . Three TraRG residues ( TraR-E46 , R49 , and K50 ) are central to the Si3-TraRG interface ( Figure 3B , C ) . Individual alanine substitutions of these TraR residues ( TraR-E46A , R49A , or K50A ) gave rise to similar results as deleting Si3 . Inhibition of rrnB P1 was similar to WT-TraR for TraR-K50A , and mildly impaired for TraR-E46A or R49A ( Figure 3F; legend for IC50 values ) . Maximal inhibition was achieved at higher E46A or R49A TraR concentrations . However , these same variants exhibited at least ~2 fold reduced activation at the thrABC promoter ( Figure 3G ) even at saturating TraR concentrations , indicating a role for the TraR-Si3 interaction in the mechanism of activation . Consistent with these results , these TraR variants were proficient in RNAP binding in a competition assay ( Figure 3—figure supplement 1F ) . By contrast , substitutions for nearby TraR variants P43A and P45A were defective for binding to RNAP , and their functional defects were overcome at higher TraR concentrations ( Figure 3—figure supplement 1D–F ) . The combination of the TraR-Si3 interface and the ΔSi3-RNAP mutants was epistatic; the same ~2 fold reduction in activation was observed as with the Si3-TraR interface mutants or the ΔSi3-RNAP mutant individually ( Figure 3—figure supplement 1G ) . These results indicate that the Si3 ( SBHMb ) -TraRG interaction enabled by the Si3 ( II ) conformation accounts for part of the TraR-mediated effect on activation . The large cleft between the two pincers in the structure of RNAP forms a channel that accommodates the downstream duplex DNA between the β’shelf and the clamp on one side , and the βlobe-Si1 domains on the other ( Figure 2B , C ) . In Eσ70 without nucleic acids , this channel is occupied by the σ701 . 1 domain , which is ejected upon entry of the downstream duplex DNA ( Figure 1D ) ( Bae et al . , 2013; Mekler et al . , 2002 ) . TraR binding induces a ~ 18° rotation of the RNAP βlobe-Si1 domains ( the two domains move together as a rigid body ) , shifting the βlobe-Si1 towards TraR , allowing the βlobe-Si1 to establish an interface with TraRG and TraRC ( 615 Å2 interface area; Figure 4A ) . Si1 [also called βi4; Lane and Darst , 2010a] is an LSI within the βlobe . Most of the TraR/βlobe-Si1 interface ( 77% ) is between TraR and Si1 . Deleting Si1 from RNAP nearly abolishes activation function [pargI , Figure 4C; thrABC , Gopalkrishnan et al . , 2017] , even at saturating concentrations of TraR to overcome weakened TraR binding ( Gopalkrishnan et al . , 2017 ) . These results suggest that the βlobe-Si1 rotation induced by TraR is essential to TraR-mediated activation . The rotation of the βlobe-Si1 widens the gap between the βprotrusion and the βlobe ( Figure 4A ) and changes the shape of the RNAP channel , altering RNAP contacts with σ701 . 1 in Eσ70 . We hypothesize that altering the RNAP contacts with σ701 . 1 in the channel facilitates σ701 . 1 ejection during RPo formation , contributing to activation of promoters that are limited at this step . To test this hypothesis , we investigated TraR function on an inhibited ( rrnB P1 ) and an activated ( thrABC ) promoter with holoenzyme lacking σ701 . 1 ( EΔ1 . 1σ70 ) . Eσ70 exhibited weak transcription from the thrABC promoter in the absence of TraR ( referred to here as basal transcription ) , and transcription from this promoter was stimulated about ~4 fold in the presence of TraR ( Figure 4D ) . EΔ1 . 1σ70 exhibited a striking increase in basal transcription activity from this promoter ( ~32 fold ) compared to WT-Eσ70 activity ( Figure 4D ) . Only a small further increase in transcription was observed upon the addition of TraR ( Figure 4D ) . These results suggest that σ701 . 1 is an obstacle to promoter DNA entering the RNAP channel and that TraR partially overcomes this barrier . In contrast to deletion of region σ701 . 1 , which almost entirely bypassed the requirement for TraR , rotation of the βlobe-Si1 did not weaken σ701 . 1-RNAP contacts sufficiently to release σ701 . 1 completely ( Figure 1D ) . Rather , we propose that βlobe-Si1 rotation facilitated the competition between promoter DNA and σ701 . 1 during RPo formation . Our results suggest that TraR-activated promoters are defined , in part , by being limited at the σ701 . 1 ejection step , but that the system has evolved to allow activation of WT-RNAP to a level appropriate for the biological need for the gene products , not the maximum level that could be achieved by full ejection of σ701 . 1 . βSi1 was also required for inhibition of rpsT P2 ( Figure 4B ) and rrnB P1 transcription by TraR ( Gopalkrishnan et al . , 2017 ) . However , in contrast to the effect of EΔ1 . 1σ70 on activated promoters , deletion of σ701 . 1 had little effect on basal transcription from the TraR-inhibited rrnB P1 promoter; inhibition of rrnB P1 by TraR with EΔ1 . 1σ70 was only slightly defective ( Figure 4—figure supplement 1A , B ) . Thus , in contrast to the effects of Si1 on activation by TraR , we suggest that the effect of TraR on inhibition of transcription involves the βlobe-Si1 domains but this is not mediated by σ701 . 1 ( see Discussion ) . We propose that TraR-mediated stimulation of σ701 . 1 release still occurs at inhibited promoters like rrnB P1 and rpsT P2 , but this has little effect on transcription because these promoters are limited by their unstable RPo ( Barker et al . , 2001 ) ( Figure 4—figure supplement 1 ) . In summary , deletion of σ701 . 1 has a major effect on basal transcription of an activated promoter ( Figure 4D ) but only a minor effect on an inhibited promoter ( Figure 4—figure supplement 1A , B ) . To qualitatively understand this striking result in terms of kinetic/energetic schemes for transcription initiation from a hypothetical inhibited and activated promoter , we adapted the flux calculator ( Galburt , 2018 ) to a four-step linear mechanism ( see Materials and methods ) that culminates in the irreversible generation of RPITC that has initiated RNA chain synthesis ( Buc and McClure , 1985; Roe et al . , 1985; Sclavi et al . , 2005; Rutherford et al . , 2009; Ruff et al . , 2015b; Hubin et al . , 2017a ) :R+P⇄RP1⇄RP2⇄RPo→RPITC Ejection of σ701 . 1 is thought to be a relatively late step on the pathway to RPo formation ( Ruff et al . , 2015a ) so we modeled the effect of deleting σ701 . 1 as lowering the kinetic barrier separating RP2 and RPo ( Figure 4—figure supplement 1C ) . The basal energy landscapes for a hypothetical inhibited and activated promoter were modeled after ( Galburt , 2018 ) [see Figure 6B of Galburt ( 2018 ) . The overall qualitative kinetic/thermodynamic features of inhibited vs . activated promoters are described later in the Discussion . The details of how we used the flux calculator ( Galburt , 2018 ) are described in Materials and methods and Supplementary file 2 . In this scheme , lowering the kinetic barrier separating RP2 and RPo has no effect on transcription output from the negatively regulated promoter but gives rise to a large increase in transcription output from the positively regulated promoter ( Figure 4—figure supplement 1C ) , reflecting the experimental results ( Figure 4D , Figure 4—figure supplement 1A , B ) . TraR binding induces a ~ 4 . 5° rotation of the β’shelf module ( Figure 5A , B ) . The BH leads directly into the shelf module , and a kink is introduced in the BH , a long α-helix that traverses the RNAP active site cleft from one pincer to the other , directly across from the active site Mg2+ ( Figure 5B , C ) . The BH plays critical roles in the RNAP nucleotide addition cycle ( Lane and Darst , 2010b ) , including interacting with the t-strand DNA at the active site ( Figure 5D ) . TraR causes the BH to kink towards the t-strand DNA ( Figure 5C ) , similar to BH kinks observed previously ( Tagami et al . , 2011; Tagami et al . , 2010; Weixlbaumer et al . , 2013; Zhang et al . , 1999 ) , resulting in a steric clash with the normal position of the t-strand nucleotide at +2 ( Figure 5E ) . Thus , the TraR-induced BH kink would sterically prevent the proper positioning of the t-strand DNA in RPo , likely contributing to inhibition of transcription . TraR induces conformational changes in the RNAP β'Si3 ( Figure 1A , B ) , βlobe-Si1 ( Figure 4A ) , β'shelf , and BH ( Figure 5 ) structural modules . We noted modest changes in clamp positions ( Supplementary file 3 ) , but we suspected that conformational heterogeneity of Eσ70 ( limiting the resolution of the single particle analysis; Figure 1—figure supplement 3 ) likely arose primarily from a continuous distribution of clamp positions that could not be easily classified into distinct conformational states . We also suspected that the range of clamp positions was dampened in the TraR-Eσ70 and rpsT P2-RPo structures . We therefore analysed and compared the heterogeneity of RNAP clamp positions between the Eσ70 , TraR-Eσ70 , and rpsT P2-RPo datasets using multibody refinement as implemented in RELION 3 ( Nakane et al . , 2018 ) . The maps used for multi-body refinement were carefully chosen to be equivalently processed . After initial classification to remove junk particles , particles were 3D auto-refined , then the refinement metadata and post-processing were used as inputs for RELION CTF refinement and Bayesian Polishing ( Zivanov et al . , 2018 ) . After a final round of 3D auto-refinement ( but no further classification ) , the rpsT P2-RPo dataset had the smallest number of particles ( 370 , 965 ) , so a random subset of particles from the other datasets ( TraR-Eσ70 and Eσ70 ) were processed so that each map for multi-body refinement was generated from the same number of particles ( 370 , 965 ) . The final maps used for multi-body refinement had nominal resolutions of 4 . 0 Å ( TraR-Eσ70; red dashed box in Figure 1—figure supplement 1 ) , 4 . 6 Å ( Eσ70; red dashed box in Figure 1—figure supplement 3 ) , and 3 . 5 Å ( rpsT P2-RPo; red dashed box in Figure 2—figure supplement 1 ) . We note that dynamic clamp behavior has been observed by single-molecule FRET in solution ( Duchi et al . , 2018 ) . For Eσ70 , three major components ( Eigenvectors ) of clamp changes were revealed ( Figure 6A–D ) . For each Eigenvector , the histogram of Eigenvalues closely approximated a Gaussian distribution ( Figure 6B–D ) . To quantitate the range of clamp conformations represented by the Eigenvalues , we divided the particles into three bins according to their Eigenvalues such that each bin contained an equal number of particles ( red , gray , and blue in Figure 6B–D ) . Three-dimensional alignments and reconstructions were then calculated for each bin . For component 1 , the red and blue particles gave rise to reconstructions that differed in clamp positions by a rotation angle of 2 . 7° in a direction we call opening/closing ( Figure 6E ) . The low Eigenvalue particles yielded a closed clamp ( red ) , while the high Eigenvalue particles ( blue ) gave an open clamp . In the middle , the particles having intermediate Eigenvalues ( gray ) gave a clamp position half-way in between the red and the blue , as expected ( not shown ) . Component two gave rise to clamp positions that differed by a 4 . 6° rotation about a rotation axis roughly perpendicular to the open/close rotation axis , a conformational change we call twisting ( Figure 6F ) . Finally , component three gave rise to clamp positions that differed by a 2 . 0° rotation about a third rotation axis parallel with the long axis of the clamp , a conformational change we call rolling ( Figure 6G ) . Using the parameters of the Gaussian fits to the Eigenvalue histograms ( Figure 6B–D ) , we could estimate the full range of clamp rotations for each component , which we defined as the rotation range that accounted for 98% of the particles ( excluding 1% of the particles at each tail; Figure 7 ) . These same conformational changes ( opening/closing , twisting , rolling ) were represented in major components of clamp changes for the TraR-Eσ70 and rpsT P2-RPo particles as well . The same analyses revealed that TraR binding significantly reduced the range of clamp positions for each of the three clamp motions ( Figure 7 ) . As expected , the clamp positions for RPo , with nucleic acids stably bound in the downstream duplex channel , were restricted even further for all three of the major clamp motions ( Figure 7 ) . See Discussion for potential mechanism ( s ) of effects of clamp conformational changes on transcription .
Together , several lines of structural , biochemical , genetic and kinetic evidence , presented here or published previously , lead to a model for the structural mechanism of activation by TraR . Previous data showed that TraR or its homolog DksA ( in conjunction with ppGpp ) enhance the transcription output from activated promoters relative to that with RNAP alone ( i . e . , in the absence of factor; Paul et al . , 2005; Gopalkrishnan et al . , 2017 ) . In addition , kinetic analyses demonstrated that the TraR homolog ppGpp/DksA enhances the rate and amount of RPo formation at an activated promoter ( Paul et al . , 2005 ) primarily by increasing the rates of step ( s ) subsequent to RNAP binding to the promoter . Here we show that in the absence of TraR , RNAP with a deletion of σ701 . 1 displayed greatly increased promoter activity on the thrABC promoter relative to the activity with WT RNAP ( 32-fold increase; Figure 4D ) , indicating that the presence of σ701 . 1 in the RNAP channel presents a major barrier to the formation of RPo on activated promoters . This large effect on promoter activity was not observed with rrnB P1 , an inhibited promoter ( Figure 4—figure supplement 1 ) . These results are consistent with previous reports that deletion of σ701 . 1 had different effects on different promoters , increasing RPo at some promoters but not at others ( Ruff et al . , 2015b; Hook-Barnard and Hinton , 2009; Vuthoori et al . , 2001 ) . We suggest that σ701 . 1 poses the most significant barrier to RPo formation at activated promoters , but not the only one , since addition of TraR to RNAP lacking σ701 . 1 resulted in a small TraR-dependent increase in transcription of the thrABC promoter ( Figure 4D ) . We suggest that this small increase could result from the restriction of clamp motion by TraR ( described in the Results section ) at a step prior to σ701 . 1 ejection , perhaps transcription bubble nucleation ( Feklistov et al . , 2017 ) . We propose that TraR binding allosterically alters and weakens σ701 . 1 interactions in the RNAP channel by causing a large ( ~18° ) rotation of the βlobe-Si1 module that forms one wall of the channel ( Figure 4A; see also Video 1 ) . In addition , the interaction of TraRG with the SBHMa motif of Si3 ( Figure 3 , Figure 3—figure supplement 1 ) may also contribute to weakening of σ701 . 1 interactions with the main channel , because Si3 is inserted within the trigger loop ( TL ) and its interactions with TraR could perturb interactions of the TL/BH/Switch one region with σ701 . 1 . Deletion of β’Si3 has been shown to reduce the lifetime of open complexes by 3–10 fold ( Ruff et al . , 2015b ) , suggesting the possibility that the reduced activation observed with the Si3 deletion RNAP could also result from effects on RPo stability . The TraR-induced conformational changes that alter and weaken σ701 . 1 interactions in the main channel are proposed to facilitate displacement of σ701 . 1 by promoter DNA ( Figures 1 and 4; see also Video 1 ) . However , effects of TraR on clamp conformation may also contribute to the increase in RPo by increasing bubble nucleation , as proposed by Feklistov et al . ( 2017 ) . Together , these effects could be sufficient to account for the TraR-dependent increase in the amount of RPo formed at an activated promoter . Since the structural data indicate that TraR bound to the RNAP complex would sterically block initial NTP access to the active site , along with t-strand positioning and catalysis ( Figure 5; see also Molodtsov et al . , 2018 ) , TraR must dissociate from the complex in order to allow initiation from the activated promoter . The proposal that TraR dissociates from the complex at an activated promoter prior to the dissociation of RNAP from the promoter is supported by previous data on the lifetimes of these complexes . The lifetime of RPo at activated promoters ( measured in hours; Barker et al . , 2001 ) is much longer than the lifetime of the transcription factors on RNAP ( GreB , DksA and by extension TraR; measured in seconds; Stumper et al . , 2019 ) . The kinetics of transcription initiation are illustrated by a schematic energy landscape in Figure 8 , where specific structural effects of TraR are correlated with changes in free energy at positively and negatively regulated promoters . The TraR-dependent changes in RNAP conformation and the resulting effects on σ701 . 1 would lower the kinetic barrier to RPo formation . At an activated promoter , the free energy of the transition state between RP2 and RPo is rate-limiting , and it is reduced by the TraR-induced weakening of σ701 . 1 interactions in the main channel , leading to an increase in transcription ( Figure 8 ) . TraR ( and ppGpp/DksA ) -inhibited promoters form RPo rapidly ( Rao et al . , 1994 ) but their intrinsically unstable RPo results in significant population of earlier intermediates ( Gopalkrishnan et al . , 2017; Rutherford et al . , 2009 ) . Although TraR likely accelerates bubble nucleation and σ701 . 1 ejection at inhibited promoters , these steps are already rapid and transcription output is not affected . In contrast to its effects on an activated promoter , deletion of σ701 . 1 had much smaller effects on basal transcription and inhibition by TraR on an inhibited promoter ( Figure 4—figure supplement 1 ) . However , TraR binding induces two distinct conformational changes in RNAP that we propose disfavor RPo formation , accounting for inhibition . Most prominent is a direct interaction of TraR with βSi1 that leads to the 18 Å displacement of the βlobe that alters the shape of the main channel and may stabilize DNA contacts in an intermediate prior to RPo ( such as RP2; Figure 8 ) . Stabilization of an intermediate compared to RPo at inhibited promoters would have a dramatic effect on transcription output by further shifting occupancy by RNAP to earlier intermediates in the RPo formation pathway . Consistent with these hypotheses , ΔSi1-RNAP has reduced TraR-mediated inhibition ( Figure 4B ) , and footprints with RNAP on negatively regulated promoters like rrnB P1 and rpsT P2 have a shortened downstream boundary of DNase I protection ( Gopalkrishnan et al . , 2017 ) . Inhibition by TraR is multipartite . In addition to causing rotation of the βlobe-Si1 , TraR binding also induces a kinked BH that sterically clashes with proper positioning of the t-strand DNA near the active site ( Figure 5 ) , as reported previously ( Molodtsov et al . , 2018 ) . Precise positioning of the t-strand DNA at the active site is critical for efficient catalysis of phosphodiester bond formation by RNAP in the SN2 mechanism ( Yee et al . , 1979 ) . Occupancy of the secondary channel by TraR would be expected to block catalysis by sterically blocking TL folding required for catalysis and preventing access of initiating NTPs to the active site , ensuring that any complexes containing TraR that proceeded to RPo could not initiate transcription . Why not attribute inhibition entirely to this ability of TraR to block iNTP access to the active site ? Recent single molecule fluorescence studies ( Stumper et al . , 2019 ) indicated that secondary channel binding factors ( GreB , DksA and by extension TraR ) formed an RNAP-factor complex prior to binding to promoter DNA , and dissociated together with RNAP from an inhibited promoter complex ( rrnB P1 ) because the lifetime of RNAP on rrnB P1 is shorter than the lifetime of the factors on RNAP ( Stumper et al . , 2019 ) . Since the affinity of TraR for RNAP is similar to that of DksA ( Gopalkrishnan et al . , 2017 ) , it is likely that TraR exhibits similar properties . Binding of the factors to preformed RPo was not observed ( Stumper et al . , 2019 ) , consistent with the ten-fold reduced affinity of DksA for RPo ( Lennon et al . , 2009 ) . These data are consistent with our model for inhibition , suggesting that TraR would bind together with RNAP to an inhibited promoter and severely reduce RPo formation by stabilizing an intermediate ( Figure 8 ) . TraR would remain associated with the complex until RNAP dissociated . TraR's presence in the complex for the entire time of RNAP occupancy of the promoter would leave little opportunity for RPo to form and would also prevent catalysis by any RPo that did form . The β and β' subunits of the bacterial RNAP are conserved throughout evolution , containing 16 and 11 sequence regions , respectively , common to all bacterial RNAPs ( Lane and Darst , 2010a ) . These shared sequence regions are separated by relatively nonconserved spacer regions in which large LSIs can occur ( Lane and Darst , 2010a ) . The LSIs are typically independently-folded , highly mobile domains , ranging in size from 50 to 500 amino acids on the RNAP surface . A key feature of the mechanism of TraR function is modulation of Eco RNAP transcription initiation through conformational changes brought about by interactions with two of the Eco RNAP LSIs , βSi1 ( Figure 4A ) and β'Si3 ( Figure 3A–C ) . Eco βSi1 was originally designated dispensible region 1 ( Severinov et al . , 1994 ) , but its deletion reduced growth at 30 °C and prevented growth at 42° , suggesting that it might serve as a binding determinant for regulatory factors ( Artsimovitch et al . , 2003 ) . Indeed , TraR interacts with βSi1 as well as with the nearby βlobe to distort the RNAP channel ( Figure 4A ) , effecting both inhibition ( Figure 4B ) and activation ( Figure 4C ) by TraR . Eco β'Si3 is an unusual LSI as it is inserted in the middle of the TL , a key structural element in the RNAP nucleotide addition cycle that is conserved in all multi-subunit RNAPs ( Lane and Darst , 2010a ) . As a consequence , Si3 plays a central role in Eco RNAP function , and cells deleted for Si3 are not viable ( Artsimovitch et al . , 2003; Zakharova et al . , 1998 ) . Si3 is highly mobile , rotating about 33° to accommodate folding and unfolding of the TL at each RNAP nucleotide addition cycle ( Malinen et al . , 2012; Zuo and Steitz , 2015 ) . Si3 was often disordered in Eco RNAP crystal structures [for example , see Molodtsov et al . , 2018] . In our cryo-EM analysis , TraR engages with Si3 , stabilizing a previously undetected conformation of Si3 affecting activation ( Figure 3 ) . Si3 has been implicated previously in RPo formation since the Δβ'Si3-RNAP forms an unstable RPo ( Artsimovitch et al . , 2003 ) . TraR-like proteins are widespread in proteobacteria , related bacteriophage , and plasmids ( Gopalkrishnan et al . , 2017; Gourse et al . , 2018 ) . While TraR function in vivo is incompletely understood , TraR engages with RNAP in much the same way as ppGpp/DksA and regulates transcription similarly . The structural and functional analyses described here identify the RNAP conformational changes responsible for the effects of TraR on transcription , deconvoluting the complicated , multifaceted mechanism that distinguishes activation from inhibition . The complex interplay between TraR binding and RNAP conformation and conformational heterogeneity allows TraR to modulate multiple features of the energy landscape of RPo formation ( Figure 8 ) , which is key to allowing TraR to effect differential regulation across promoter space without directly interacting with DNA . The very similar effects of ppGpp/DksA and TraR on RNAP function ( Gopalkrishnan et al . , 2017; Gourse et al . , 2018 ) suggests that DksA-ppGpp works via a similar structural mechanism .
Plasmids are listed in Supplementary file 4 and oligonucleotide and geneblock sequences are in Supplementary file 5 . Bacteria were grown in LB Lennox media or on LB agar plates . Media was supplemented with ampicillin ( 100 µg/ml ) or kanamycin ( 30 µg/ml ) if needed . TraR was made by cloning the traR gene in a pET28-based His10-SUMO vector which allowed removal of the cleavable N-terminal His10-SUMO tag with Ulp1 protease . ESI-Mass Spectrometry revealed that the molecular mass of purified TraR corresponded to that of a monomer lacking the N-terminal methionine [Figure S6 of Gopalkrishnan et al . , 2017] , hence traR without the initial M was cloned into the SUMO vector . This tag-less version of TraR exhibited the same level of activity as a previous TraR construct with four additional residues ( LVPR ) at the C-terminal end leftover after His6 tag cleavage in the TraR-thrombin site-His6 construct ( Gopalkrishnan et al . , 2017 ) . The His10-SUMO-TraR plasmid was transformed into competent Eco BL21 ( DE3 ) by heat shock . The cells were grown in the presence of 25 µg/mL kanamycin to an OD600 of 0 . 5 in a 37°C shaker . TraR expression was induced with a final concentration of 1 mM isopropyl ß-D-thiogalactopyranoside ( IPTG ) for 3 hr at 37°C . Cells were harvested by centrifugation and resuspended in 50 mM Tris-HCl , pH 8 . 0 , 250 mM NaCl , 5 mM imidazole , 10% glycerol ( v/v ) , 2 . 5 mM dithiothreitol ( DTT ) , 10 µM ZnCl2 , 1 mM phenylmethylsulfonyl fluoride ( PMSF , Sigma-Aldrich , St . Louis , MO ) , 1x protease inhibitor cocktail ( PIC , Sigma-Aldrich ) . Cells were homogenized using a continuous-flow French Press ( Avestin , Ottawa , ON , Canada ) at 4°C and the resulting lysate was centrifuged to isolate the soluble fraction . The supernatant was loaded onto two 5 mL HiTrap IMAC HP columns ( GE Healthcare , Pittsburgh , PA ) for a total column volume ( CV ) of 10 mL . His10-SUMO-TraR was eluted at 300 mM imidazole in Ni-column buffer [50 mM Tris-HCl , pH 8 . 0 , 500 mM NaCl , 10% glycerol ( v/v ) , 10 µM ZnCl2 , 2 . 5 mM DTT] . Peak fractions were combined , treated with ULP1 SUMO-protease overnight , and dialyzed against 20 mM Tris-HCl , pH 8 . 0 , 5% glycerol ( v/v ) , 0 . 1 mM ethylenediaminetetraacetic acid ( EDTA ) , 500 mM NaCl , 10 µM ZnCl2 , 2 . 5 mM DTT , resulting in a final imidazole concentration of 25 mM . The ULP1-cleaved sample was loaded onto one 5 mL HiTrap IMAC HP column to remove His10-SUMO-tag along with any remaining uncut TraR . Tagless TraR was collected in the flowthrough and concentrated by centrifugal filtration ( Amicon Ultra , EMD Millipore , Burlington , MA ) . The sample was purified in a final step on a HiLoad 16/60 Superdex 200 column ( GE Healthcare ) . Purified TraR was concentrated to 16 mg/mL by centrifugal filtration , flash-frozen in liquid N2 , and stored at −80°C . A pET-based plasmid overexpressing each subunit of RNAP ( full-length α , β , ω ) as well as β'-PPX-His10 ( PPX; PreScission protease site , LEVLFQGP , GE Healthcare ) was co-transformed with a pACYCDuet-1 plasmid containing Eco rpoZ into Eco BL21 ( DE3 ) . The cells were grown in the presence of 100 µg/mL ampicillin and 34 μg/mL chloramphenicol to an OD600 of 0 . 6 in a 37°C shaker . Protein expression was induced with 1 mM IPTG ( final concentration ) for 4 hr at 30°C . Cells were harvested by centrifugation and resuspended in 50 mM Tris-HCl , pH 8 . 0 , 5% glycerol ( v/v ) , 10 mM DTT , 1 mM PMSF , and 1x PIC . After French Press lysis at 4°C , the lysate was centrifuged twice for 30 min each . Polyethyleneimine [PEI , 10% ( w/v ) , pH 8 . 0 , Acros Organics - ThermFisher Scientific , Waltham , MA] was slowly added to the supernatant to a final concentration of ~0 . 6% PEI with continuous stirring . The mixture was stirred at 4°C for an addition 25 min , then centrifuged for 1 . 5 hr at 4°C . The pellets were washed three times with 50 mM Tris-HCl , pH 8 . 0 , 500 mM NaCl , 10 mM DTT , 5% glycerol ( v/v ) , 1 mM PMSF , 1x PIC . For each wash , the pellets were homogenized then centrifuged again . RNAP was eluted by washing the pellets three times with 50 mM Tris-HCl , pH 8 . 0 , 1 M NaCl , 10 mM DTT , 5% glycerol ( v/v ) , 1x PIC , 1 mM PMSF . The PEI elutions were combined and precipitated with ammonium sulfate overnight . The mixture was centrifuged and the pellets were resuspended in 20 mM Tris-HCl , pH 8 . 0 , 1 M NaCl , 5% glycerol ( v/v ) , 5 mM DTT . The mixture was loaded onto three 5 mL HiTrap IMAC HP columns for a total CV of 15 ml . RNAP ( β'-PPX-His10 ) was eluted at 250 mM imidazole in Ni-column buffer . The eluted RNAP fractions were combined and dialyzed against 20 mM Tris-HCl , pH 8 . 0 , 100 mM NaCl , 5% glycerol ( v/v ) , 5 mM DTT . The sample was then loaded onto a 35 mL Biorex-70 column ( Bio-Rad , Hercules , CA ) , washed with 10 mM Tris-HCl , pH 8 . 0 , 0 . 1 mM EDTA , 5% glycerol ( v/v ) , 5 mM DTT] in a gradient from 0 . 2 M to 0 . 7 M NaCl . The eluted fractions were combined , concentrated by centrifugal filtration , then loaded onto a 320 mL HiLoad 26/600 Superdex 200 column ( GE Healthcare ) equilibrated in gel filtration buffer [10 mM Tris-HCl , pH 8 . 0 , 0 . 1 mM EDTA , 0 . 5 M NaCl , 5% glycerol ( v/v ) , 5 mM DTT] . The eluted RNAP was supplemented with glycerol to 20% ( v/v ) , flash frozen in liquid N2 , and stored at −80°C . Plasmid encoding Eco His10-SUMO-σ70 was transformed into Eco BL21 ( DE3 ) by heat shock . The cells were grown in the presence of 50 µg/mL kanamycin to an OD600 of 0 . 6 at 37°C . Protein expression was induced with 1 mM IPTG for 1 hr at 30°C . Cells were harvested by centrifugation and resuspended in 20 mM Tris-HCl , pH 8 . 0 , 5% glycerol ( v/v ) , 500 mM NaCl , 0 . 1 mM EDTA , 5 mM imidazole , 0 . 5 mM 2-mercaptoethanol ( BME ) , 1 mM PMSF , 1x PIC . After French Press lysis at 4°C , cell debris was removed by centrifugation . The lysate was loaded onto two 5 mL HiTrap IMAC HP for a total CV of 10 ml . His10-SUMO-σ70 was eluted at 250 mM imidazole in 20 mM Tris-HCl , pH 8 . 0 , 500 mM NaCl , 0 . 1 mM EDTA , 5% glycerol ( v/v ) , 0 . 5 mM BME . Peak fractions were combined , cleaved with ULP1 , and dialyzed against 20 mM Tris-HCl pH 8 . 0 , 500 mM NaCl , 0 . 1 mM EDTA , 5% glycerol ( v/v ) , 0 . 5 mM BME , resulting in a final imidazole concentration of 25 mM . The cleaved sample was loaded onto one 5 mL HiTrap IMAC HP to remove His10-SUMO-tag along with any remaining uncut σ70 . Tagless σ70 was collected in the flowthrough and concentrated by centrifugal filtration . The sample was then loaded onto a HiLoad 16/60 Superdex 200 in gel filtration buffer . Peak fractions of σ70 were pooled , supplemented with glycerol to a final concentration of 20% ( v/v ) , flash-frozen in liquid N2 , and stored at −80°C . Eσ70 was formed by mixing purified RNAP and 2 . 5-fold molar excess of σ70 and incubating for 20 min at 37°C . Eσ70 was purified on a Superose 6 Increase 10/300 GL column ( GE Healthcare ) in gel filtration buffer ( 10 mM Tris-HCl , pH 8 . 0 , 200 mM KCl , 5 mM MgCl2 , 10 µM ZnCl2 , 2 . 5 mM DTT ) . The eluted Eσ70 was concentrated to ~10 mg/mL ( ~21 μM ) by centrifugal filtration ( Amicon Ultra ) . Eσ70 was formed by mixing purified RNAP and a 2-fold molar excess of σ70 and incubating for 15 min at room temperature . Eσ70 was purified over a Superose 6 Increase 10/300 GL column in gel filtration buffer . The eluted Eσ70 was concentrated to ~5 . 0 mg/mL ( ~10 μM ) by centrifugal filtration . Purified TraR was added ( 5-fold molar excess over RNAP ) and the sample was incubated for 15 min at room temperature . An rrnB P1 promoter fragment ( Integrated DNA Technologies , Coralville , IA ) was added ( 2-fold molar excess over RNAP ) and the sample was incubated for a further 15 min at room temperature . The rrnB P1 promoter fragment did not bind to TraR-Eσ70 under the cryo-EM grid preparation conditions - the subsequent structural analyses did not reveal any evidence of promoter binding . Eσ70 was prepared as described for TraR-Eσ70 , but after the size exclusion chromatography the complex was concentrated to ~10 mg/mL ( ~20 μM ) by centrifugal filtration . Duplex rpsT P2 promoter fragment ( −60 to +25 , Figure 2A , IDT ) was added to the concentrated Eσ70 to 3-fold molar excess . The sample was incubated for 20 mins at room temperature prior to cryo-EM grid preparation . CHAPSO {3- ( [3-cholamidopropyl]dimethylammonio ) −2-hydroxy-1-propanesulfonate} ( Anatrace , Maumee , OH ) was added to the samples to a final concentration of 8 mM ( Chen et al . , 2019 ) . The final buffer condition for all the cryo-EM samples was 10 mM Tris-HCl , pH 8 . 0 , 100 mM KCl , 5 mM MgCl2 , 10 μM ZnCl2 , 2 . 5 mM DTT , 8 mM CHAPSO . C-flat holey carbon grids ( CF-1 . 2/1 . 3-4Au ) were glow-discharged for 20 s prior to the application of 3 . 5 μL of the samples . Using a Vitrobot Mark IV ( FEI , Hillsboro , OR ) , grids were blotted and plunge-froze into liquid ethane with 100% chamber humidity at 22°C . Grids were imaged using a 300 keV Krios ( FEI ) equipped with a K2 Summit direct electron detector ( Gatan , Pleasanton , CA ) . Datasets were recorded with Serial EM ( Mastronarde , 2005 ) with a pixel size of 1 . 3 Å over a defocus range of 0 . 8 μm to 2 . 4 μm . Movies were recorded in counting mode at eight electrons/physical pixel/second in dose-fractionation mode with subframes of 0 . 3 s over a 15 s exposure ( 50 frames ) to give a total dose of 120 electrons/physical pixel . Dose-fractionated movies were gain-normalized , drifted-corrected , summed , and dose-weighted using MotionCor2 ( Grant and Grigorieff , 2015; Zheng et al . , 2017 ) . CTFFIND4 ( Rohou and Grigorieff , 2015 ) was used for contrast transfer function estimation . Particles were picked using Gautomatch ( http://www . mrc-lmb . cam . ac . uk/kzhang/ ) using a 2D template . Picked particles were extracted from the dose-weighted images with RELION ( Zivanov et al . , 2018 ) using a box size of 256 pixels . Two TraR-Eσ70 datasets were collected: dataset 1 consisted of 1546 motion-corrected images with 631 , 880 particles and dataset 2 consisted of 2132 motion-corrected images with 378 , 987 particles . The particles from each dataset were curated using RELION 3D classification ( N = 3 ) using a cryoSPARC ab-initio reconstruction ( Punjani et al . , 2017 ) generated from a subset of the particles . The highest resolution classes from each dataset were subjected to RELION 3D auto-refinement resulting in a 4 . 69 Å resolution map from dataset 1 and a 4 . 38 Å resolution map from dataset 2 . Refinement metadata and post-processing were used as inputs for RELION CTF refinement and Bayesian Polishing ( Zivanov et al . , 2018 ) . The polished particles from both datasets were combined , resulting in 372 , 670 particles . The particles were aligned using RELION 3D auto-refinement resulting in a consensus map with nominal resolution of 3 . 62 Å . Using the refinement parameters , subtractive 3D classification ( N = 3 ) was performed on the particles by subtracting density outside of β'Si3 and classifying in a mask around β'Si3 . Classification revealed three distinct β'Si3 dispositions ( Figure S1D ) . Local refinement metadata ( highlighted in red dotted box , Figure S1D ) for TraR-Eσ70 ( I ) and TraR-Eσ70 ( II ) were used for RELION multi-body refinements to examine clamp motions ( Nakane et al . , 2018 ) . Local resolution calculations were performed using blocres and blocfilt from the Bsoft package ( Cardone et al . , 2013 ) . The Eσ70 image acquisition and processing were the same as for TraR-Eσ70 except with the following differences . Grids were imaged using a 200 keV Talos Arctica ( FEI ) equipped with a K2 Summit direct electron detector . Datasets were recorded with a pixel size of 1 . 3 Å over a defocus range of −1 . 0 μm to −2 . 5 μm . Movies were recorded in counting mode at 8 . 4 electrons/physical pixel/second in dose-fractionation mode with subframes of 0 . 2 s over a 10 s exposure ( 50 frames ) to give a total dose of 84 electrons/physical pixel . Picked particles were extracted from the dose-weighted images in RELION ( Scheres , 2012 ) using a box size of 200 pixels . The Eσ70 dataset consisted of 3548 motion-corrected images with 1 , 387 , 166 particles . A subset of the particles was subjected to cryoSPARC ab-initio reconstruction ( Punjani et al . , 2017 ) to generate a 3D template for 3D classifications in cryoSPARC and 3D refinements in RELION ( Scheres 2012 ) . Particles were split into two groups ( 1st group: particles from images 1-2 , 000; 2nd group: particles from images 2001–3548 . Particles from each group were curated using cryoSPARC heterogeneous refinement ( N = 3 ) resulting in a subset of 479 , 601 particles for the first group and 329 , 293 particles for the second group . Curated particles were combined and a consensus refinement was performed in RELION using the cryoSPARC generated initial model resulting in a map with nominal resolution of 4 . 54 Å ( without post-processing ) . Particles from this refinement ( highlighted in red dotted box , Figure 1—figure supplement 3 ) were further analyzed using RELION multi-body refinement as described in the text ( Nakane et al . , 2018 ) . Additionally , particles were further curated using RELION 3D classification ( N = 3 ) without alignment . Classification revealed two lower resolution class and a higher resolution class . The higher resolution class containing 358 , 725 particles was RELION 3D auto-refined and subjected to RELION CTF refinement and RELION Bayesian Polishing ( Zivanov et al . , 2018 ) . After polishing , particles were refined to a nominal resolution of 4 . 05 Å after RELION post-processing . The rpsT P2-RPo cryo-EM image acquisition and processing were the same as for TraR-Eσ70 except with the following differences . The imaging defocus range was 0 . 5 μm to 2 . 5 μm . Movies were recorded in super-resolution mode at eight electrons/physical pixel/second in dose-fractionation mode with subframes of 0 . 2 s over a 10 s exposure ( 50 frames ) to give a total dose of 80 electrons/physical pixel . The rpsT P2-RPo dataset consisted of 6912 motion-corrected images with 973 , 481 particles . In RELION , a consensus refinement was performed using the extracted particles and a cryoSPARC generated initial model resulting in a 4 . 62 Å resolution map . Using the refinement parameters , 3D classification ( N = 2 ) was performed on the particles without alignment . Classification revealed a lower resolution class and a higher resolution class , the latter with 370 , 965 particles with nominal resolution of 4 . 38 Å after RELION 3D auto-refinement . Refinement metadata and post-processing were used as inputs for RELION CTF refinement and RELION Bayesian Polishing ( Zivanov et al . , 2018 ) . Subsequent 3D classification ( N = 3 ) was used to further classify the polished particles resulting in one junk class and two high-resolution classes ( Figure 2—figure supplement 1 ) . The highest resolution reconstruction ( 3 . 43 Å ) contained 289 , 679 particles . To build initial models of the protein components of the complexes , a crystal structure of Eco Eσ70 [PDB ID 4LJZ , with σ701 . 1 from 4LK1; ( Bae et al . , 2013 ) was manually fit into the cryo-EM density maps using Chimera ( Pettersen et al . , 2004 ) and manually adjusted using Coot ( Emsley and Cowtan , 2004 ) . For TraR-Eσ70 , σ701 . 1 from 4LK1 ( Bae et al . , 2013 ) and TraR from 5W1S ( Molodtsov et al . , 2018 ) were also added . For rpsT P2-RPo , the promoter DNA was manually added . Appropriate domains of each complex were rigid-body refined , then subsequently refined with secondary structure and nucleic acid restraints using PHENIX real-space refinement ( Adams et al . , 2010 ) . IPTG ( 1 mM final ) was used to induce expression of TraR ( WT or variant ) from Eco BL21 DE3 dksA::Tn10 ( RLG7075 ) host cells . TraR and variants were purified as described ( Gopalkrishnan et al . , 2017 ) , either from His6-TraR overexpression plasmids with removal of the His6-tag with thrombin , or from His10-SUMO-TraR constructs with removal of the His10-SUMO-tag with Ulp1 protease , resulting in a 72 amino acid TraR lacking the N-terminal Met . WT-TraR purified by the two methods gave comparable results . WT and variant RNAPs were purified as described previously ( Ross et al . , 2016 ) . The Δ1 . 1σ70 was expressed and purified as described previously ( Chen et al . , 2017 ) . EΔ1 . 1σ70 was reconstituted with a 4:1 molar ratio of Δ1 . 1σ70 to core RNAP . The purified core RNAP lacked detectable WT-σ70 activity . All of these procedures were carried out exactly as previously described ( Gopalkrishnan et al . , 2017 ) . We modeled the hypothesized effects of RNAP mutants ( Δ1 . 1σ70 ) or TraR on the energy diagram for transcription initiation using the flux calculator developed by Galburt ( 2018 ) . Since the relevant rate constants for promoters inhibited or activated by TraR are not known , the energy diagrams illustrating the kinetic/energetic schemes for transcription initiation from a hypothetical inhibited and activated promoter ( Figure 4—figure supplement 1C , Figure 8 ) are meant to only qualitatively illustrate features of the promoters and the effects of manipulations [either σ701 . 1 deletion ( Figure 4—figure supplement 1C ) or addition of TraR ( Figure 8 ) ] . We hypothesize that TraR influences multiple steps along the RPo formation pathway so we wanted to model RPo formation as a three-step linear mechanism ( Buc and McClure , 1985; Roe et al . , 1985; Sclavi et al . , 2005; Rutherford et al . , 2009; Ruff et al . , 2015a; Hubin et al . , 2017a ) rather than the two-step mechanism used in the flux calculator ( Galburt , 2018 ) . However , a kinetic analysis of ppGpp/DksA activation on the pargI promoter revealed only a very small ( <2 fold ) effect on KB ( the equilibrium constant for the initial step of RNAP binding to the free promoter ) and a large effect on subsequent isomerization rates ( ~16 fold; Paul et al . , 2005 ) . Similarly , activation by TraR at low and high ( saturating ) concentrations of RNAP gave the same fold activation on the pthrABC promoter , indicating TraR also does not affect the initial binding step . We make the assumption that deletion of σ701 . 1 also would not dramatically affect the initial binding step . Therefore , the initial binding step ( R + P ⇄ RP1 ) was included in the illustrations of the kinetic scheme but did not need to be accounted for in the calculations of fold-inhibition or fold-activation because deletion of σ701 . 1 or addition of TraR has no effect on this step . In this way , the rate constants for the first step of the flux calculator ( kon and koff; Galburt , 2018 ) could be used as the rate constants for the second step of our kinetic scheme ( k2 and k-2; Figure 4—figure supplement 1C; Figure 8 ) and so on . The precise values used in the calculations are tabulated in Supplementary file 2 . The illustrations ( Figure 4—figure supplement 1C; Figure 8 ) were not taken directly from the flux calculator ( Galburt , 2018 ) but have been skewed vertically to make the differences between the inhibited and activated promoter easier to visualize .
TraR and its homolog DksA are bacterial proteins that regulate transcription initiation by binding directly to RNA polymerase ( RNAP ) rather than to promoter DNA . Effects of TraR mimic the combined effects of DksA and its cofactor ppGpp , but the structural basis for regulation by these factors remains unclear . Here , we use cryo-electron microscopy to determine structures of Escherichia coli RNAP , with or without TraR , and of an RNAP-promoter complex . TraR binding induced RNAP conformational changes not seen in previous crystallographic analyses , and a quantitative analysis revealed TraR-induced changes in RNAP conformational heterogeneity . These changes involve mobile regions of RNAP affecting promoter DNA interactions , including the βlobe , the clamp , the bridge helix , and several lineage-specific insertions . Using mutational approaches , we show that these structural changes , as well as effects on σ70 region 1 . 1 , are critical for transcription activation or inhibition , depending on the kinetic features of regulated promoters .
Cells need to make proteins in order to survive . To make a protein , a cell first needs to take the information from a gene coded in its DNA and copy it into a template made of a different molecule called RNA via a process called transcription . Not all genes are transcribed or expressed at the same time or the same rate , because a cell needs different proteins depending on its environment . The molecules that regulate when each gene is transcribed are called transcription factors . When the bacterium Escherichia coli is starved for the building blocks it needs to make proteins , it changes the expression of almost one quarter of its genes within 5 minutes . This broad response requires two transcription factors , ppGpp and DksA . Unlike most transcription factors , these two molecules bind directly to the enzyme responsible for transcribing DNA into RNA , the RNA polymerase , but they do not bind to DNA . Another transcription factor called TraR can mimic the combined effects of ppGpp and DksA on transcription , changing the conformation of RNA polymerase in the same way . Now , Chen et al . have used a high-resolution imaging technique called cryo-electron microscopy to reveal the details of how the structure of RNA polymerase changes in response to TraR binding , and by analogy , in response to ppGpp and DksA . The experiments showed that TraR interacts with regions of RNA polymerase that move when the protein binds DNA . These interactions can either help or hinder the start of transcription depending on which DNA sequence the RNA polymerase binds . Using the structures obtained via cryo-electron microscopy as guides , Chen et al . mutated each of the mobile parts of RNA polymerase individually to determine which interactions with TraR were necessary to change gene expression . These results shed light on a fundamental process in all living cells , the initiation of transcription , and how it changes in response to the cell's nutritional environment . This may help explain how different cells regulate gene expression and may also lead to the development of new antibiotics .