To investigate roles of the discriminator and open complex (OC) lifetime in transcription initiation by Escherichia coli RNA polymerase (RNAP; α 2 ββ'ωσ 70 ), we compare productive and abortive initiation rates, short RNA distributions, and OC lifetime for the λP R and T7A1 promoters and variants with exchanged discriminators, all with the same transcribed region. The discriminator determines the OC lifetime of these promoters. Permanganate reactivity of thymines reveals that strand backbones in open regions of longlived λP R -discriminator OCs are much more tightly held than for shorter-lived T7A1-discriminator OCs. Initiation from these OCs exhibits two kinetic phases and at least two subpopulations of ternary complexes. Long RNA synthesis (constrained to be single round) occurs only in the initial phase (<10 s), at similar rates for all promoters. Less than half of OCs synthesize a full-length RNA; the majority stall after synthesizing a short RNA. Most abortive cycling occurs in the slower phase (>10 s), when stalled complexes release their short RNA and make another without escaping. In both kinetic phases, significant amounts of 8-nt and 10-nt transcripts are produced by longer-lived, λP R -discriminator OCs, whereas no RNA longer than 7 nt is produced by shorter-lived T7A1-discriminator OCs. These observations and the lack of abortive RNA in initiation from short-lived ribosomal promoter OCs are well described by a quantitative model in which ∼1.0 kcal/mol of scrunching free energy is generated per translocation step of RNA synthesis to overcome OC stability and drive escape. The different length-distributions of abortive RNAs released from OCs with different lifetimes likely play regulatory roles.RNA polymerase | open complex lifetime | transcription initiation | abortive RNA | hybrid length M any facets of transcription initiation by E. coli RNA polymerase (RNAP; α 2 ββ′ωσ 70 ) have been elucidated, but significant questions remain about the mechanism or mechanisms by which initial transcribing complexes (ITC) with a short RNA-DNA hybrid decide to advance and escape from the promoter to enter elongation mode, or, alternately, to stall, release their short RNA, and reinitiate (abortive cycling). For RNAP to escape, its sequencespecific interactions with promoter DNA in the binary open complex (OC) must be overcome.The open regions of promoter DNA in the binary OC are the −10 region (six residues, with specific interactions between σ 2.2 and the nontemplate strand), the discriminator region (typically six to eight residues with no consensus sequence, the upstream end of which interacts with σ 1.2 ), and the transcription start site (TSS, +1) and adjacent residue (+2), which are in the active site of RNAP (Table 1). The interactions involving and directed by the six-residue λP R discriminator make its OC longlived and highly stable (1). A six-residue discriminator allows the OC to form without deforming (prescrunching) either open discriminator strand (2). Less extensive interactions involving and directed...

Quantitative information about amide interactions in water is needed to understand their contributions to protein folding and amide effects on aqueous processes, and to compare with computer simulations. Here we quantify interactions of urea, alkylated ureas and other amides by osmometry and amide-aromatic hydrocarbon interactions by solubility. Analysis of these data yields strengths of interaction of ureas and naphthalene with amide sp2O, amide sp2N, aliphatic sp3C, and amide and aromatic sp2C unified atoms in water. Interactions of amide sp2O with urea and naphthalene are favorable, while amide sp2O-alkyl urea interactions are unfavorable, becoming more unfavorable with increasing alkylation. Hence amide sp2O-amide sp2N interactions (proposed n–σ* hydrogen bond) and amide sp2O-aromatic sp2C (proposed n – π*) interactions are favorable in water, while amide sp2O-sp3C interactions are unfavorable. Interactions of all ureas with sp3C and amide sp2N are favorable and increase in strength with increasing alkylation, indicating favorable sp3C-amide sp2N and sp3C-sp3C interactions. Naphthalene results show that aromatic sp2C-amide sp2N interactions in water are unfavorable while sp2C-sp3C interactions are favorable. These results allow interactions of amide and hydrocarbon moieties and effects of urea and alkyl ureas on aqueous processes to be predicted or interpreted in terms of structural information. We predict strengths of favorable urea-benzene and N-methylacetamide interactions from experimental information to compare with simulations, and indicate how amounts of hydrocarbon and amide surface buried in protein folding and other biopolymer processes and transition states can be determined from analysis of urea and diethyl urea effects on equilibrium and rate constants.

To determine the step-by-step kinetics and mechanism of transcription initiation and escape by E. coli RNA polymerase from the λPR promoter, we quantify the accumulation and decay of transient short RNA intermediates on the pathway to promoter escape and full-length (FL) RNA synthesis over a wide range of NTP concentrations by rapid-quench mixing and phosphorimager analysis of gel separations. Experiments are performed at 19 °C, where almost all short RNAs detected are intermediates in FL-RNA synthesis by productive complexes or end-products in nonproductive (stalled) initiation complexes, and not from abortive initiation. Analysis of productiveinitiation kinetic data yields composite second-order rate constants for all steps of NTP binding and hybrid extension up to the escape point (11-mer). The largest of these rate constants is for incorporation of UTP into the dinucleotide pppApU in a step which does not involve DNA opening or translocation. Subsequent steps, each of which begins with reversible translocation and DNA opening, are slower with rate constants that vary more than ten-fold, interpreted as effects of translocation stress on the translocation equilibrium constant. Rate constants for synthesis of 4-and 5-mer, 7-mer to 9-mer and 11-mer are particularly small, indicating that RNAP-promoter interactions are disrupted in these steps. These reductions in rate constants are consistent with the previously-determined 9 kcal cost of escape from λPR. Structural modeling and previous results indicate that the three groups of small rate constants correspond to sequential disruption of incleft, −10 and −35 interactions. Parallels to escape by T7 RNAP are discussed.

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