Abstract

The hairpin loop GUAAUA occurs frequently in ribosomal RNA. Optical melting studies show that r(GGCGUAAUAGCC) folds into a hairpin containing this loop. The structural features of the r(GGCGUAAUAGCC) hairpin have been determined by NMR and molecular modeling. NOEs from G4-H1' to A9-H2 and from A9-H2 to G10-H1' show that G4 and A9 form a sheared base pair with two hydrogen bonds: A-N7 to G-NH2 and A-NH6 to G-N3. One-dimensional NOE data show no NOEs between the imino protons of U5 and U8, but NOEs are observed between the U5-H1' and the U8-H6 and U8-H5, thus orienting the U8 imino proton away from U5. Thus U5 and U8 do not form an imino hydrogen-bonded U.U pair. The U5-H2' exhibits NOEs to both the A6-H8 and A7-H8, and the 3' phosphorus resonances of U5 and A6 are shifted downfield. This suggests that the helix turn is between the U5 and A6 nucleotides. The JH1'-H2 and JH3'-H4' coupling constants indicate that the loop is dynamic, particularly at 35 degrees C, well below the melting temperature of 63 degrees C. Structures were generated using 75 distance and 46 dihedral angle restraints. In these structures, the U5 base is stacked on the sheared base pair formed by G4 and A9 and can initiate a uridine turn similar to that observed in the anticodon loop of tRNA. The A6, A7, and U8 bases can stack on one another with their hydrogen-bonding surfaces exposed to the solvent, suggesting that they are available for tertiary interactions or protein recognition in rRNA. A range of loop structures are consistent with the data, however. The lack of formation of a U.U mismatch is consistent with a recent model that predicts the stability of hairpin loops of six nucleotides on the basis of the closing base pair and first mismatch in the loop [Serra, M. J., Axenson, T. J., & Turner, D. H. (1994) Biochemistry 33, 14289-14296].

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