 RNA hairpin

An RNA hairpin is a stem-loop formed when two regions of one RNA strand make base pairs, leaving an intervening unpaired loop. It is a local RNA secondary structure motif: covalent continuity runs through the loop while pairing brings separated parts of the sequence together. The motif does not require a second RNA molecule and need not describe the fold of the whole RNA.

For an original sequence illustration, consider 5'-GGCCUUCGGGCC-3'. Pair positions1–12,2–11,3–10 and4–9. The four pairs are G–C, G–C, C–G and C–G, leaving positions5–8, UUCG, as a four-nucleotide loop. Thus four pairs use eight nucleotides, and the loop supplies four more, giving twelve in total. The corresponding illustrative dot-bracket notation is ((((....)))). This proposed pairing is a structural example, not an experimental demonstration that an isolated sequence occupies only that conformation.

A four-residue loop is an RNA tetraloop. Both the paired stem and the loop sequence influence stability. In a 2010 experiment, researchers optically melted24 stem–loop sequences containing common tetraloops and determined their thermodynamic parameters. Measuring absorbance as temperature changes connects sequence differences to an experimental folding transition rather than inferring stability from the number of pairs alone.^[ref]

A two-state model makes RNA hairpin melting quantitative. If only folded F and unfolded U states are allowed, set $K=[F]/[U]=\exp [-\Delta G/(RT)]$, with $\Delta G=G_F-G_U$ and $R$ the molar gas constant. The folded fraction is $K/(1+K)$. A stipulated $\Delta G=-RT\ln 4$ gives $K=4$ and folded fraction $0.8$; equal free energies give $0.5$. These model fractions are not the paper's measurements. Alternative folds, non-two-state transitions and assay conditions can require a richer interpretation.