Host factor titration by chromosomal R-loops as a mechanism for runaway plasmid replication in transcription termination-defective mutants of Escherichia coli

Two Escherichia coli genes, rnhA and recG, encode products that disrupt R-loops by hydrolysis and unwinding, respectively. It is known that the propensity for R-loop formation in vivo is increased during growth at 21 °C. We have identified several links between rnhA, recG, and R-loop-dependent plasmid replication on the one hand, and genes rho and nusG involved in factor-dependent transcription termination on the other. A novel nusG-G146D mutation phenocopied a rho-A243E mutation in conferring global deficiency in transcription termination, and both mutants were killed at 21 °C following overexpression of rnhA+. Mutant combinations rnhA-nusG or recG-rho were synthetically lethal at 21 °C, with the former being suppressed by recG+ overexpression. rho and nusG mutants were killed following transformation with plasmids such as pACYC184 or pUC19 (which have R-loop replication intermediates) even at 30 °C or 37 °C, and the lethality was correlated with greatly increased content of supercoiled monomer species of these and other co-resident R-loop-dependent plasmids. Plasmid-mediated lethality in the mutants was suppressed by overexpression of rnhA+ or recG+. Two additional categories of trans-acting suppressors of the plasmid-mediated lethality were identified whose primary effects were, respectively, a reduction in plasmid copy number even in the wild-type strain, and a restoration of the proficiency of in vivo transcription termination in the nusG and rho mutant strains. The former category of suppressors included rom+, and mutations in rpoB(Q513L), pcnB, and polA, whereas the latter included a mutation in rho (R221C) and several non-null mutations (E74K, L26P, and Δ64-137) in the gene encoding the nucleoid protein H-NS. We propose that an increased occurrence of chromosomal R-loops in the rho and nusG mutants leads to titration of a cyloplasmic host factor(s) that negatively modulates the stability of plasmid R-loop replication intermediates and consequently to runaway plasmid replication

A dnaC mutation in Escherichia coli that affects copy number of ColE1-like plasmids and the PriA-PriB (but Not Rep-PriC) pathway of chromosomal replication restart

Escherichia coli nusG and rho mutants, which are defective in transcription termination, are killed following transformation with several ColE1-like plasmids that lack the plasmid-encoded copy-number regulator gene rom because of uncontrolled plasmid replication within the cells. In this study, a mutation [dnaC1331(A84T)] in the dnaC gene encoding the replicative helicase-loading protein was characterized as a suppressor of this plasmid-mediated lethality phenotype. The mutation also reduced the copy number of the plasmids in otherwise wild-type strains. In comparison with the isogenic dnaC+ strain, the dnaC mutant was largely unaffected for (i) growth on rich or minimal medium, (ii) tolerance to UV irradiation, or (iii) survival in the absence of the PriA, RecA, or RecB proteins. However, it was moderately SOS-induced and was absolutely dependent on both the Rep helicase and the PriC protein for its viability. A dnaC1331(A84T) dam mutant, but not its mutH derivative, exhibited sensitivity to growth on rich medium, suggestive of a reduced capacity in the dnaC1331(A84T) strains to survive chromosomal double-strand breaks. We propose that DnaC-A84T is proficient in the assembly of replication forks for both initiation of chromosome replication (at oriC) and replication restart via the Rep-PriC pathway, but that it is specifically defective for replication restart via the PriA-PriB pathway (and consequently also for replication of the Rom- ColE1-like plasmids)

Why is transcription coupled to translation in bacteria?

Active mechanisms exist to prevent transcription that is uncoupled from translation in the protein-coding genes of bacteria, as exemplified by the phenomenon of nonsense polarity. Bacterial transcription-translation coupling may be viewed as one among several co-transcriptional processes, including those for mRNA processing and export in the eukaryotes, that operate in the various life forms to render the nascent transcript unavailable for formation of otherwise deleterious R-loops in the genome

Basic Features of a Cell Electroporation Model: Illustrative Behavior for Two Very Different Pulses

Science increasingly involves complex modeling. Here we describe a model for cell electroporation in which membrane properties are dynamically modified by poration. Spatial scales range from cell membrane thickness (5 nm) to a typical mammalian cell radius (10 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}\upmu\end{document}m), and can be used with idealized and experimental pulse waveforms. The model consists of traditional passive components and additional active components representing nonequilibrium processes. Model responses include measurable quantities: transmembrane voltage, membrane electrical conductance, and solute transport rates and amounts for the representative “long” and “short” pulses. The long pulse—1.5 kV/cm, 100 \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}\upmu\end{document}s—evolves two pore subpopulations with a valley at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\sim}$$\end{document}5 nm, which separates the subpopulations that have peaks at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\sim}$$\end{document}1.5 and \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$${\sim}$$\end{document}12 nm radius. Such pulses are widely used in biological research, biotechnology, and medicine, including cancer therapy by drug delivery and nonthermal physical tumor ablation by causing necrosis. The short pulse—40 kV/cm, 10 ns—creates 80-fold more pores, all small (\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$<$$\end{document}3 nm; \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\sim$$\end{document}1 nm peak). These nanosecond pulses ablate tumors by apoptosis. We demonstrate the model’s responses by illustrative electrical and poration behavior, and transport of calcein and propidium. We then identify extensions for expanding modeling capability. Structure-function results from MD can allow extrapolations that bring response specificity to cell membranes based on their lipid composition. After a pulse, changes in pore energy landscape can be included over seconds to minutes, by mechanisms such as cell swelling and pulse-induced chemical reactions that slowly alter pore behavior. Electronic supplementary material The online version of this article (doi:10.1007/s00232-014-9699-z) contains supplementary material, which is available to authorized users