A characterization of the conformation and stability of model peptide systems that form β-sheets in aqueous solutions is considerably important in gaining insights into the mechanism of β-sheet formation in proteins. We have characterized the conformation and equilibrium folding and unfolding of two 20-residue peptides whose NMR spectra suggest a three-stranded β-sheet topology in aqueous solution: Betanova [Kortemme, T., Ramirez-Alvarado, M., and Serrano, L. (1998) Science 281, 253−256] and DPDP with d-Pro-Gly segments at the turns [Schenck, H. L., and Gellman, S. H. (1998) J. Am. Chem. Soc. 120, 4869−4870]. Both circular dichroism (CD) and infrared measurements indicate only 20−26% β-sheet-like structure at 5 °C for Betanova and 42−59% β-sheet for DPDP. For both peptides, the CD and infrared spectra change nearly linearly with increasing temperatures (or urea concentrations) and lack a sigmoidal signature characteristic of cooperative unfolding. Fluorescence resonance energy transfer (FRET) measurements between donor and acceptor molecules attached to the two ends confirm that Betanova is largely unstructured even at 10 °C; the average end-to-end distance estimated from FRET is closer to that of a random coil than a structured β-sheet. In DPDP, the FRET results indicate a more compact structure that remains compact even at high temperatures (∼80 °C) or high urea concentrations (∼8 M). These results indicate that both these peptides access an ensemble of conformations at all temperatures or denaturant concentrations, with no significant free energy barrier separating the "folded" and "unfolded" conformations.
The dynamics and mechanism of how site-specific DNA-bending proteins initially interrogate potential binding sites prior to recognition have remained elusive for most systems. Here we present these dynamics for Integration Host factor (IHF), a nucleoid-associated architectural protein, using a μs-resolved T-jump approach. Our studies show two distinct DNA-bending steps during site recognition by IHF. While the faster (∼100 μs) step is unaffected by changes in DNA or protein sequence that alter affinity by >100-fold, the slower (1-10 ms) step is accelerated ∼5-fold when mismatches are introduced at DNA sites that are sharply kinked in the specific complex. The amplitudes of the fast phase increase when the specific complex is destabilized and decrease with increasing [salt], which increases specificity. Taken together, these results indicate that the fast phase is non-specific DNA bending while the slow phase, which responds only to changes in DNA flexibility at the kink sites, is specific DNA kinking during site recognition. Notably, the timescales for the fast phase overlap with one-dimensional diffusion times measured for several proteins on DNA, suggesting that these dynamics reflect partial DNA bending during interrogation of potential binding sites by IHF as it scans DNA.
An intriguing puzzle in biopolymer science is the observation that single-stranded DNA and RNA oligomers form hairpin structures on time scales of tens of microseconds, considerably slower than the estimated time for loop formation for a semiflexible polymer of similar length. To address the origin of the slow kinetics and to determine whether hairpin dynamics are diffusion-controlled, the effect of solvent viscosity (eta) on hairpin kinetics was investigated using laser temperature-jump techniques. The viscosity was varied by addition of glycerol, which significantly destabilizes hairpins. A previous study on the viscosity dependence of hairpin dynamics, in which all the changes in the measured rates were attributed to a change in solvent viscosity, reported an apparent scaling of relaxation times (tau(r)) on eta as tau(r) approximately eta(0.8). In this study, we demonstrate that if the effect of viscosity on the measured rates is not deconvoluted from the inevitable effect of change in stability, then separation of tau(r) into opening (tau(o)) and closing (tau(c)) times yields erroneous behavior, with different values (and opposite signs) of the apparent scaling exponents, tau(o) approximately eta(-0.4) and tau(c) approximately eta(1.5). Under isostability conditions, obtained by varying the temperature to compensate for the destabilizing effect of glycerol, both tau(o) and tau(c) scale as approximately eta(1.1+/-0.1). Thus, hairpin dynamics are strongly coupled to solvent viscosity, indicating that diffusion of the polynucleotide chain through the solvent is involved in the rate-determining step.
Elucidating the mechanism of folding of polynucleotides depends on accurate estimates of free energy surfaces and a quantitative description of the kinetics of structure formation. Here, the kinetics of hairpin formation in single-stranded DNA are measured after a laser temperature jump. The kinetics are modeled as configurational diffusion on a free energy surface obtained from a statistical mechanical description of equilibrium melting profiles. The effective diffusion coefficient is found to be strongly temperature-dependent in the nucleation step as a result of formation of misfolded loops that do not lead to subsequent zipping. This simple system exhibits many of the features predicted from theoretical studies of protein folding, including a funnel-like energy surface with many folding pathways, trapping in misfolded conformations, and non-Arrhenius folding rates.
The effects on the structure dynamics of the Escherichia coli wild‐type formamidopyrimidine‐DNA glycosylase (Fpg) protein of the single mutations Lys57←Gly (FpgK57G), Pro2←Gly (FpgP2G) and Pro2←Glu (FpgP2E) were studied by fluorescence techniques, namely : lifetime measurements and acrylamide quenching of the fluorescence of Trp residues. The fluorescence decays of Fpg and its mutant forms were analysed by the maximum‐entropy method and lifetime distributions in the range 200 ps to 9 ns were obtained. The lifetime distribution profiles of FpgK57G, FpgP2G and FpgP2E are different from that of wild‐type Fpg. Both dynamic and static quenching by acrylamide were observed for all the proteins. At 20 +C, the bimolecular collisional quenching rate constant of the FpgP2E fluorescence by acrylamide was only 0.8 M −1 s −1 as compared to about 1.4 M −1 s −1 for the three other proteins. At 6 +C, all the spectroscopic properties of these four proteins are about the same. The analysis of experimental data demonstrates that all three mutations induce a structural reorganization of the Fpg protein. However, only the P2E mutation lead to a reduced accessibility of some Trp residues to acrylamide quenching. It is concluded that the single P2E replacement induces a conformational change leading to a more rigid globular structure as opposed to the wild type and K57G and P2G mutations. The influence of the single mutations on the enzyme activities of the Fpg protein is discussed.
