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. 2004 Sep 30;32(17):5126–5133. doi: 10.1093/nar/gkh841

Table 1. The thermodynamic parameters for the four hairpin pairs forming a kissing complex are shown. The Tm is shown for a total RNA concentration of 10−5 M.

Complementary loop sequence Na+ conc. (mM) Tm(°C) (for 10−5 M RNA conc.) ΔTm (°C) −ΔHapp (kcal/mol) −ΔSapp (cal/mol) −ΔG37app (kcal/mol) −ΔΔG37a (kcal/mol) −ΔΔG37b (kcal/mol)
CCUGCCGGACGG 1000 67.3 ± 0.4 19.0 75.7 ± 1.2 196.6 ± 0.5 14.72 −4.62 −1.12
CCGACCGGCUGG 1000 64.7 ± 0.4 19.8 68.0 ± 2.2 175.8 ± 0.9 13.48 −3.98 −0.48
GAGAGGCUCUCC 1000 57.0 ± 0.3 19.5 71.7 ± 1.6 191.6 ± 0.6 12.28 −4.08 −0.58
CUAAACGAUUUG 1000 32.0 ± 0.3 30.9 35.3 ± 2.2 89.8 ± 1.8 7.45 −4.15 −0.65
            mean: −4.21 −0.71

The ΔTm shows the differences between the measured melting temperatures and the predicted Tm for regular RNA duplexes with identical sequence and without dangling adenines. The two columns on the right show the differences in free energy compared to duplexes without dangling adenines (a) and with dangling adenines (b). In both cases, the free energy of the kissing complex is lower than for the corresponding RNA duplexes, indicating that at 1 M Na+, the kissing complex is more stable.