Search

Proton NMR was used to study the secondary structure and melting behavior of six self-complementary oligoribonucleotide tetramers, each containing two guanosine and two cytidine residues (GGCC, CCGG, GCCG, CGGC, GCGC, and CGCG). GGCC and CCGG formed perfect duplexes containing four G.C base pairs with Tms of 54 and 47.8 degrees C, respectively; GCCG and CGGC formed staggered duplexes with two G.C base pairs and four 3' double-dangling bases, with Tms of 35.5 and 29.2 degrees C, respectively; GCGC formed a perfect duplex with a Tm of 49.9 degrees C, while CGCG formed a staggered duplex with a Tm of 36.9 degrees C. From these results, an order of stability of the cores containing two G.C base pairs was proposed: GC:GC is more stable than GG:CC which is more stable than CG:CG. The RY model for secondary structure stability prediction was applied to the above tetramers with reasonable success. Suggestions for refinements are discussed.

The stabilizing effects of dangling ends and terminal base pairs on the core helix GCGC are reported. Enthalpy and entropy changes of helix formation were measured spectrophotometrically for AGCGCU, UGCGCA, GGCGCCp, CGCGCGp, and the corresponding pentamers XGCGCp and GCGCYp containing the GCGC core plus a dangling end. Each 5' dangling end increases helix stability at 37 degrees C roughly 0.2 kcal/mol and each 3' end from 0.8 to 1.7 kcal/mol. The free energy increments for dangling ends on GCGC are similar to the corresponding increments reported for the GGCC core [Freier, S. M., Alkema, D., Sinclair, A., Neilson, T., & Turner, D. H. (1985) Biochemistry 24, 4533-4539], indicating a nearest-neighbor model is adequate for prediction of stabilization due to dangling ends. Nearest-neighbor parameters for prediction of the free energy effects of adding dangling ends and terminal base pairs next to G.C pairs are presented. Comparison of these free energy changes is used to partition the free energy of base pair formation into contributions of "stacking" and "pairing". If pairing contributions are due to hydrogen bonding, the results suggest stacking and hydrogen bonding make roughly comparable favorable contributions to the stability of a terminal base pair. The free energy increment associated with forming a hydrogen bond is estimated to be -1 kcal/mol of hydrogen bond.

The role of stacking in terminal base-pair formation was studied by comparison of the stability increments for dangling ends to those for fully formed base pairs. Thermodynamic parameters were measured spectrophotometrically for helix formation of the hexanucleotides AGGCCUp, UGGCCAp, CGGCCGp, GCCGGCp, and UCCGGAp and for the corresponding pentanucleotides containing a 5'-dangling end on the GGCCp or CCGGp core helix. In 1 M NaCl at 1 X 10(-4) M strands, a 5'-dangling nucleotide in this series increases the duplex melting temperature (Tm) only 0-4 degrees C, about the same as adding a 5'-phosphate. In contrast, a 3'-dangling nucleotide increases the Tm at 1 X 10(-4) M strands 7-23 degrees C, depending on the sequence [Freier, S. M., Burger, B. J., Alkema, D., Neilson, T., & Turner, D. H. (1983) Biochemistry 22, 6198-6206]. These results are consistent with stacking patterns observed in A-form RNA. The stability increments from terminal A.U, C.G, or U.A base pairs on GGCC or a terminal U.A pair on CCGG are nearly equal to the sums of the stability increments from the corresponding dangling ends. This suggests stacking plays a large role in nucleic acid stability. The stability increment from the terminal base pairs in GCCGGCp, however, is about 5 times the sum of the corresponding dangling ends, suggesting hydrogen bonding can also make important contributions.

A series of pentaribonucleotides, ApGpXpGpU (where X identical to A, G, C, or U), was synthesized to investigate the effects of flanking G . C pairs on internal Watson-Crick, G . U, and nonbonded base pairs. Sequences ApGpApCpU (Tm = 26 degrees C) and ApGpCpCpU (Tm = 25 degrees C) were each found to form a duplex with non-base-paired internal residues that stacked with the rest of the sequence but were not looped out. ApGpGpCpU also forms a duplex (Tm = 30 degrees C) but with dangling terminal nonbonded adenosines rather than internal nonbonded guanosines. ApGpUpCpU prefers a stacked single-strand conformation. In addition, contribution to duplex stability from an internal A . U or G . C base pair is enhanced by 6 degrees C when flanked by G . C base pairs as compared to A . U base pairs. G . C base pairs flanking an internal G . U base pair were found to be more tolerant to the altered conformation of a G . U pair and result in an increase to stability comparable with that found for an internal A . U base pair.