Search of a model for melting temperature and cohesive energy of nanomaterials

Three different models viz. Nanda model, Jiang model and BK model with different physical origin have been used to study the size dependence of melting temperature and cohesive energy of nanomaterials. A critical analysis demonstrates that the suitability of Jiang model or Nanda model depends on the material considered. Moreover, BK model works well for different nanomaterials considered in the present work. This demonstrates the suitability of the models proposed earlier. We therefore, extend the BK model for the size dependence of cohesive energy and Debye temperature. Nanda model has been found to give the reverse trends for the size dependence of cohesive energy as observed experimentally. However, Jiang model and BK model give similar trends of variation as observed experimentally. A comparison of the computed results with the experimental data demonstrates the superiority of the BK model. We also extend the BK model for the study of size dependence of Debye temperature. A good agreement between theory and experiment demonstrates the validity of the model proposed

Mechanism of transcription initiation and promoter escape by E. coli RNA polymerase

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 What drives promoter escape? Escape involves disrupting all the favorable interactions involved in forming and stabilizing the binary OC as well as σ-core interactions. Escape from these interactions is fundamentally driven by the favorable chemical (free) energy change of RNA synthesis, but this energy must be stored in the ITC in each step before escape. Proposed means of energy storage as the length of the RNA-DNA hybrid increases include the stresses introduced by scrunching distortions of the discriminator regions of the open strands in the cleft (2, 5, 6) and by unfavorable interactions of the RNA-DNA hybrid with the hairpin loop of σ 3.2 (7-10). Scrunching of the discriminator region of the template strand is proposed to be most significant for Significance The enzyme RNA polymerase (RNAP) transcribes DNA genetic information into RNA. Regulation of transcription occurs largely in initiation; these regulatory mechanisms must be understood. Lifetimes of transcription-capable RNAP-promoter open complexes (OCs) vary greatly, dictated largely by the DNA discriminator region, but the significance of OC lifetime for regulation was unknown. We observe that a significantly longer RNA:DNA hybrid is synthesized before RNAP escapes from long-lived λP R -promoter OCs as compared with shorter-lived T7A1 promoter OCs. We quantify the free energy needed to overcome OC stability and allow escape from the promoter and elongation of the nascent RNA, and thereby predict escape points for ribosomal (rrnB P1) and lacUV5 promoters. Longer-lived OCs produce longer abortive RNAs, which likely have specific regulatory roles

Mechanism of transcription initiation and promoter escape by E. coli RNA polymerase

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 What drives promoter escape? Escape involves disrupting all the favorable interactions involved in forming and stabilizing the binary OC as well as σ-core interactions. Escape from these interactions is fundamentally driven by the favorable chemical (free) energy change of RNA synthesis, but this energy must be stored in the ITC in each step before escape. Proposed means of energy storage as the length of the RNA-DNA hybrid increases include the stresses introduced by scrunching distortions of the discriminator regions of the open strands in the cleft (2, 5, 6) and by unfavorable interactions of the RNA-DNA hybrid with the hairpin loop of σ 3.2 (7-10). Scrunching of the discriminator region of the template strand is proposed to be most significant for Significance The enzyme RNA polymerase (RNAP) transcribes DNA genetic information into RNA. Regulation of transcription occurs largely in initiation; these regulatory mechanisms must be understood. Lifetimes of transcription-capable RNAP-promoter open complexes (OCs) vary greatly, dictated largely by the DNA discriminator region, but the significance of OC lifetime for regulation was unknown. We observe that a significantly longer RNA:DNA hybrid is synthesized before RNAP escapes from long-lived λP R -promoter OCs as compared with shorter-lived T7A1 promoter OCs. We quantify the free energy needed to overcome OC stability and allow escape from the promoter and elongation of the nascent RNA, and thereby predict escape points for ribosomal (rrnB P1) and lacUV5 promoters. Longer-lived OCs produce longer abortive RNAs, which likely have specific regulatory roles

Search of a model for melting temperature and cohesive energy of nanomaterials

361-368Three different models viz. Nanda model, Jiang model and BK model with different physical origin have been used to study the size dependence of melting temperature and cohesive energy of nanomaterials. A critical analysis demonstrates that the suitability of Jiang model or Nanda model depends on the material considered. Moreover, BK model works well for different nanomaterials considered in the present work. This demonstrates the suitability of the models proposed earlier. We therefore, extend the BK model for the size dependence of cohesive energy and Debye temperature. Nanda model has been found to give the reverse trends for the size dependence of cohesive energy as observed experimentally. However, Jiang model and BK model give similar trends of variation as observed experimentally. A comparison of the computed results with the experimental data demonstrates the superiority of the BK model. We also extend the BK model for the study of size dependence of Debye temperature. A good agreement between theory and experiment demonstrates the validity of the model proposed

Fluorescence Resonance Energy Transfer Characterization of DNA Wrapping in Closed and Open <i>Escherichia coli</i> RNA Polymerase−λP_R Promoter Complexes

Initial recognition of promoter DNA by RNA polymerase (RNAP) is proposed to trigger a series of conformational changes beginning with bending and wrapping of the 40–50 bp of DNA immediately upstream of the −35 region. Kinetic studies demonstrated that the presence of upstream DNA facilitates bending and entry of the downstream duplex (to +20) into the active site cleft to form an advanced closed complex (CC), prior to melting of ∼13 bp (−11 to +2), including the transcription start site (+1). Atomic force microscopy and footprinting revealed that the stable open complex (OC) is also highly wrapped (−60 to +20). To test the proposed bent-wrapped model of duplex DNA in an advanced RNAP−λP_R CC and compare wrapping in the CC and OC, we use fluorescence resonance energy transfer (FRET) between cyanine dyes at far-upstream (−100) and downstream (+14) positions of promoter DNA. Similarly large intrinsic FRET efficiencies are observed for the CC (0.30 ± 0.07) and the OC (0.32 ± 0.11) for both probe orientations. Fluorescence enhancements at +14 are observed in the single-dye-labeled CC and OC. These results demonstrate that upstream DNA is extensively wrapped and the start site region is bent into the cleft in the advanced CC, reducing the distance between positions −100 and +14 on promoter DNA from >300 to <100 Å. The proximity of upstream DNA to the downstream cleft in the advanced CC is consistent with the proposed mechanism for facilitation of OC formation by upstream DNA