Solution probing of metal ion binding by helix 27 from Escherichia coli 16S rRNA.

Helix (H)27 from Escherichia coli 16S ribosomal (r)RNA is centrally located within the small (30S) ribosomal subunit, immediately adjacent to the decoding center. Bacterial 30S subunit crystal structures depicting Mg(2+) binding sites resolve two magnesium ions within the vicinity of H27: one in the major groove of the G886-U911 wobble pair, and one within the GCAA tetraloop. Binding of such metal cations is generally thought to be crucial for RNA folding and function. To ask how metal ion-RNA interactions in crystals compare with those in solution, we have characterized, using solution NMR spectroscopy, Tb(3+) footprinting and time-resolved fluorescence resonance energy transfer (tr-FRET), location, and modes of metal ion binding in an isolated H27. NMR and Tb(3+) footprinting data indicate that solution secondary structure and Mg(2+) binding are generally consistent with the ribosomal crystal structures. However, our analyses also suggest that H27 is dynamic in solution and that metal ions localize within the narrow major groove formed by the juxtaposition of the loop E motif with the tandem G894-U905 and G895-U904 wobble pairs. In addition, tr-FRET studies provide evidence that Mg(2+) uptake by the H27 construct results in a global lengthening of the helix. We propose that only a subset of H27-metal ion interactions has been captured in the crystal structures of the 30S ribosomal subunit, and that small-scale structural dynamics afforded by solution conditions may contribute to these differences. Our studies thus highlight an example for differences between RNA-metal ion interactions observed in solution and in crystals.

Dynamics inherent in helix 27 from Escherichia coli 16S ribosomal RNA.

The original interpretation of a series of genetic studies suggested that the highly conserved Escherichia coli 16S ribosomal RNA helix 27 (H27) adopts two alternative secondary structure motifs, the 885 and 888 conformations, during each cycle of amino acid incorporation. Recent crystallographic and genetic evidence has called this hypothesis into question. To ask whether a slippery sequence such as that of H27 may harbor inherent conformational dynamics, we have designed a series of model RNAs based on E. coli H27 for in vitro physicochemical studies. One-dimensional (1)H NMR spectroscopy demonstrates that both the 885 and 888 conformations are occupied to approximately the same extent (f(888) = 0.427 +/- 0.04) in the native H27 sequence at low pH (6.4) and low ionic strength (50 mM NaCl). UV irradiation assays conducted under conditions analogous to those used for assays of ribosomal function (pH 7.5 and 20 mM MgCl(2)) suggest that nucleotides 892 and 905, which are too far apart in the known 885 crystal structures, can approach each other closely enough to form an efficient cross-link. The use of a fluorescence resonance energy transfer (FRET)-labeled RNA together with a partially complementary DNA oligonucleotide that induces a shift to the 888 conformation shows that H27 interchanges between the 885 and 888 conformations on the millisecond time scale, with an equilibrium constant of 0.33 +/-0.12. FRET assays also show that tetracycline interferes with the induced shift to the 888 conformation, a finding that is consistent with crystallographic localization of tetracycline bound to the 885 conformation of H27 in the 30S ribosomal subunit. Taken together, our data demonstrate the innate tendency of an isolated H27 to exist in a dynamic equilibrium between the 885 and 888 conformations. This begs the question of how these inherent structural dynamics are suppressed within the context of the ribosome.