Monovalent ions modulate the flux through multiple folding pathways of an RNA pseudoknot.

The functions of RNA pseudoknots (PKs), which are minimal tertiary structural motifs and an integral part of several ribozymes and ribonucleoprotein complexes, are determined by their structure, stability, and dynamics. Therefore, it is important to elucidate the general principles governing their thermodynamics/folding mechanisms. Here, we combine laser temperature-jump experiments and coarse-grained simulations to determine the folding/unfolding pathways of VPK, a variant of the mouse mammary tumor virus (MMTV) PK involved in ribosomal frameshifting. Fluorescent nucleotide analogs (2-aminopurine and pyrrolocytidine) placed at different stem/loop positions in the PK serve as local probes allowing us to monitor the order of assembly of VPK that has two constituent hairpins with different intrinsic stabilities. We show that at 50 mM KCl, the dominant folding pathway populates only the more stable hairpin intermediate; as the salt concentration is increased, a parallel folding pathway emerges involving the less stable hairpin as an alternate intermediate. Notably, the flux between the pathways is modulated by the ionic strength. Our findings support the principle that the order of PK structure formation is determined by the relative stabilities of the hairpins, which can be altered by sequence variations or salt concentrations. The experimental results of salt effects on the partitioning between the two folding pathways are in remarkable agreement with simulations that were performed with no adjustable parameters. Our study not only unambiguously demonstrates that VPK folds by parallel pathways but also showcases the power of combining experiments and simulations for a more enriched description of RNA self-assembly.

Exploring the energy landscape of nucleic acid hairpins using laser temperature-jump and microfluidic mixing.

We have investigated the multidimensionality of the free energy landscape accessible to a nucleic acid hairpin by measuring the relaxation kinetics in response to two very different perturbations of the folding/unfolding equilibrium, either a laser temperature-jump or ion-jump (from rapid mixing with counterions). The two sets of measurements carried out on DNA hairpins (4 or 5 base pairs in the stem and 21-nucleotide polythymine loop), using FRET between end labels or fluorescence of 2-aminopurine in the stem as conformational probes, yield distinctly different relaxation kinetics in the temperature range 10-30 °C and salt range 100-500 mM NaCl, with rapid mixing exhibiting slower relaxation kinetics after an initial collapse of the chain within 8 µs of the counterion mixing time. The discrepancy in the relaxation times increases with increasing temperatures, with rapid mixing times nearly 10-fold slower than T-jump times at 30 °C. These results rule out a simple two-state scenario with the folded and unfolded ensemble separated by a significant free energy barrier, even at temperatures close to the thermal melting temperature T(m). Instead, our results point to the scenario in which the conformational ensemble accessed after counterion condensation and collapse of the chain is distinctly different from the unfolded ensemble accessed with T-jump perturbation. Our data suggest that, even at temperatures in the vicinity of T(m) or higher, the relaxation kinetics obtained from the ion-jump measurements are dominated by the escape from the collapsed state accessed after counterion condensation.

Fast folding of RNA pseudoknots initiated by laser temperature-jump.

RNA pseudoknots are examples of minimal structural motifs in RNA with tertiary interactions that stabilize the structures of many ribozymes. They also play an essential role in a variety of biological functions that are modulated by their structure, stability, and dynamics. Therefore, understanding the global principles that determine the thermodynamics and folding pathways of RNA pseudoknots is an important problem in biology, both for elucidating the folding mechanisms of larger ribozymes as well as addressing issues of possible kinetic control of the biological functions of pseudoknots. We report on the folding/unfolding kinetics of a hairpin-type pseudoknot obtained with microsecond time-resolution in response to a laser temperature-jump perturbation. The kinetics are monitored using UV absorbance as well as fluorescence of extrinsically attached labels as spectroscopic probes of the transiently populated RNA conformations. We measure folding times of 1-6 ms at 37 °C, which are at least 100-fold faster than previous observations of very slow folding pseudoknots that were trapped in misfolded conformations. The measured relaxation times are remarkably similar to predictions of a computational study by Thirumalai and co-workers (Cho, S. S.; Pincus, D.L.; Thirumalai, D. Proc. Natl. Acad. Sci. U. S. A. 2009, 106, 17349-17354). Thus, these studies provide the first observation of a fast-folding pseudoknot and present a benchmark against which computational models can be refined.

Solvent friction changes the folding pathway of the tryptophan zipper TZ2.

Because the rate of a diffusional process such as protein folding is controlled by friction encountered along the reaction pathway, the speed of folding is readily tunable through adjustment of solvent viscosity. The precise relationship between solvent viscosity and the rate of diffusion is complex and even conformation-dependent, however, because both solvent friction and protein internal friction contribute to the total reaction friction. The heterogeneity of the reaction friction along the folding pathway may have subtle consequences. For proteins that fold on a multidimensional free-energy surface, an increase in solvent friction may drive a qualitative change in folding trajectory. Our time-resolved experiments on the rapidly and heterogeneously folding beta-hairpin TZ2 show a shift in the folding pathway as viscosity increases, even though the energetics of folding is unaltered. We also observe a nonlinear or saturating behavior of the folding relaxation time with rising solvent viscosity, potentially an experimental signature of the shifting pathway for unfolding. Our results show that manipulations of solvent viscosity in folding experiments and simulations may have subtle and unexpected consequences on the folding dynamics being studied.

Kinetics of folding and binding of an intrinsically disordered protein: the inhibitor of yeast aspartic proteinase YPrA.

The 68 residue peptide IA 3 is an intrinsically unstructured protein that serves as an endogenous inhibitor of the yeast aspartic proteinase A (YPrA). Although unstructured in free solution, IA 3 forms an N-terminal alpha helix as it binds to YPrA, leading to subnanomolar inhibition of the protease. Equilibrium structural and inhibition studies provide little insight into the mechanism and kinetics of the coupled folding and binding interaction. We have used laser temperature jump spectroscopy to study the kinetics of folding of free IA 3 and of the interaction between IA 3 and YPrA. Inducing folding with trifluoroethanol cosolvent allows us to determine the folding rate (kf approximately 0.3 (micros)(-1)) and the unfolding rate (ku approximately 3 (micros)(-1)) for free IA 3 in water at 25 degrees C. A substantially faster relaxation process is observed in the presence of the proteinase; this process appears to be the kinetic signature of an intermediate binding step in the coupled folding and binding interaction of IA 3 and YPrA.