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. 2015 May 4;43(11):5572–5585. doi: 10.1093/nar/gkv414

Table 1. Fit results of the individual base-pair stabilities in hsp17.

hsp17 ΔHdiss ΔΔHdiss ΔSdiss ΔΔSdiss ΔGdiss (T = 20°C) ΔΔGdiss (T = 20°C)
[kJ/mol] [kJ/mol] [J/(mol K)] [J/(mol K)] [kJ/mol] [kJ/mol]
G3/U40 n.d. n.d. n.d. n.d. n.d. n.d.
U4 64.3 8.5 182.6 30.9 10.8 0.6
U38 71.2 10.8 200.9 39.3 12.3 0.7
U37 65.9 12.8 190.2 46.9 10.1 1.0
U7 n.d. n.d. n.d. n.d. n.d. n.d.
U32 n.d. n.d. n.d. n.d. n.d. n.d.
U31 / / / / / /
U11 38.8 3.7 82.9 13.1 14.5 0.2
G30 46.1 3.7 100.7 12.9 16.6 0.2
U12 / / / / / /
G28 193.5 23.7 561.9 77.5 28.8 1.0
G27 148.4 20.4 416.1 67.1 26.2 0.8
U15 n.d. n.d. n.d. n.d. n.d. n.d.

n.d., not determinable due to low base-pair stability and resultant exchange broadening of the imino resonance. U31 and U12 could not be analysed due to spectral overlap. ΔΔHdiss, ΔΔSdiss and ΔΔGdiss (T = 20°C) represent the Monte Carlo error.