In minimal RNA kissing complexes formed between hairpins with cognate GACG tetraloops, the two tertiary GC pairs are likely stabilized by the stacking of 5’-unpaired adenines at each end of the short helix. To test this hypothesis, we mutated the flanking adenines to various nucleosides and examined their effects on the kissing interaction. Electrospray ionization mass spectrometry was used to detect kissing dimers in a multi-equilibria mixture, whereas optical tweezers were applied to monitor the (un)folding trajectories of single RNA molecules. The experimental findings were rationalized by molecular dynamics simulations. Together, the results showed that the stacked adenines are indispensable for the tertiary interaction. By shielding the tertiary base pairs from solvent and reducing their fraying, the stacked adenines made terminal pairs act more like interior base pairs. The purine double-ring of adenine was essential for effective stacking, whereas additional functional groups modulated the stabilizing effects through varying hydrophobic and electrostatic forces. Furthermore, formation of the kissing complex was dominated by base pairing, whereas its dissociation was significantly influenced by the flanking bases. Together, these findings indicate that unpaired flanking nucleotides play essential roles in the formation of otherwise unstable two-base-pair RNA tertiary interactions.

RNA folding in cells typically occurs at mesophilic temperatures. However, in vitro, RNA can be unfolded either by increasing temperature to values that are much higher than physiological, or by mechanically pulling structures apart at ambient temperature. To directly study RNA folding at physiological temperatures and to unify thermodynamics measured by melting and pulling, we developed temperature-controlled optical tweezers (thermal tweezers) that can be used to mechanically unfold single RNA molecules at mesophilic temperatures. Folding of a 20-base-pair tetraloop hairpin was studied under different ionic conditions and at temperatures ranging from 22 °C to 42 °C. At each temperature, single hairpin molecules were held at constant force, and their two-state folding equilibria were monitored. The change in free energy derived from these measurements was used to construct a phase diagram of RNA structure using force and temperature as variables. Furthermore, we derived ΔG(0pN,T), the folding free energy at zero force and temperature T, by subtracting the stretching energy of unfolded RNA from the reversible mechanical work done to unfold the hairpin. ΔG(0pN,T) and its salt dependence agree reasonably well with the predictions by the nearest neighbor model. Under each ionic condition, ΔG(0pN,T) depended linearly on temperature, yielding ΔH(exp) and ΔS(exp) that also matched the predictions. The combination of force and temperature to study RNA folding is a step toward unifying thermodynamics measured by thermal melting and mechanical unfolding, and opens a new path for directly monitoring temperature induced RNA structural changes, as it occurs often in biology.

No abstract

No abstract