Imino proton exchange in the 5S RNA of Escherichia coli and its complex with protein L25 at 490 MHz

Imino proton exchange has been examined by NMR in the 5S RNA of Escherichia coli, its principal RNase A resistant fragment, fragment 1 (bases 1-11, 69-120), and complexes between that fragment and ribosomal protein L25 by using both real-time and relaxation techniques. Fragment 1 RNA imino protons exchange at rates between 0.5 and 15 s-1 at 303 K in 5 mM cacodylate buffer, pH 7.4. In contrast with many tRNAs, intact 5S RNA contains no imino protons with exchange lifetimes as great as 1 min. Consistent with the results of Gueron and his colleagues [Leroy, J. L., Bolo, N., Figueroa, N., Plateau, P., & Gueron, M. (1985) J. Biomol. Struct. Dyn. 2,915-939; Leroy, J. L., Broseta, D., & Gueron, M. (1985) J. Mol. Biol. 184, 165-178] with tRNA, exchange in 5S RNA is catalyst-limited under conditions generally used for imino proton spectroscopy, such as those given above. Using Gueron's catalyst saturation technique, base pair opening rates have been measured for several AU and GU base pairs in fragment 1. They range from 50 to 300 s-1 at 303 K and depend on base pair type and also to some degree on context. Similar studies have been done on complexes of L25 and fragment 1. The binding of L25 to fragment 1 reduces the exchange rate of many imino protons within the region to which it binds, consistent with the hypothesis that its binding stabilizes the secondary structure of 5S RNA.     

NMR analysis of helix I from the 5S RNA of Escherichia coli.

The structure of helix I of the 5S rRNA from Escherichia coli has been determined using a nucleolytic digest fragment of the intact molecule. The fragment analyzed, which corresponds to bases (-1)-11 and 108-120 of intact 5S rRNA, contains a G-U pair and has unpaired bases at its termini. Its proton resonances were assigned by two-dimensional NMR methods, and both NOE distance and coupling constant information have been used to calculate structural models for it using the full relaxation matrix algorithm of the molecular dynamics program XPLOR. Helix I has A-type helical geometry, as expected. Its most striking departure from regular helical geometry occurs at its G-U, which stacks on the base pair to the 5' side of its G but not on the base pair to its 3' side. This stacking pattern maximizes interstrand guanine-guanine interactions and explains why the G-U in question fails to give imino proton NOE's to the base pair to 5' side of its G. These results are consistent with the crystal structures that have been obtained for wobble base pairs in tRNAPhe [Mizuno, H., & Sundaralingam, M. (1978) Nucleic Acids Res. 5, 4451-4461] and A-form DNA [Rabbinovich, D., Haran, T., Eisenstein, M., & Shakked, Z. (1988) J. Mol. Biol. 200, 151-161]. The conformations of the terminal residues of helix I, which corresponds to bases (-1)-11 and 108-120 of native 5S RNA, are less well-determined, and their sugar puckers are intermediate between C2' and C3'-endo, on average.     

Identification and assignment of base pairs in three helical stems of Torulopsis utilis ribosomal 5S RNA and its RNase T1 and RNase T2 cleaved fragments via 500-MHz proton homonuclear overhauser enhancements

Imino proton resonances in the downfield region (10-14 ppm) of the 500-MHz 1H NMR spectrum of Torulopsis utilis 5S RNA are identified (A X U, G X C, or G X U) and assigned to base pairs in helices I, IV, and V via analysis of homonuclear Overhauser enhancements (NOE) from intact T. utilis 5S RNA, its RNase T1 and RNase T2 digested fragments, and a second yeast (Saccharomyces cerevisiae) 5S RNA whose nucleotide sequence differs at only six residues from that of T. utilis 5S RNA. The near-identical chemical shifts and NOE behavior of most of the common peaks from these four RNAs strongly suggest that helices I, IV, and V retain the same conformation after RNase digestion and that both T. utilis and S. cerevisiae 5S RNAs share a common secondary and tertiary structure. Of the four G X U base pairs identified in the intact 5S RNA, two are assigned to the terminal stem (helix I) and the other two to helices IV and V. Seven of the nine base pairs of the terminal stem have been assigned. Our experimental demonstration of a G X U base pair in helix V supports the 5S RNA secondary structural model of Luehrsen and Fox [Luehrsen, K. R., & Fox, G.E. (1981) Proc. Natl. Acad. Sci. U.S.A. 78, 2150-2154]. Finally, the base-pair proton peak assigned to the terminal G X U in helix V of the RNase T2 cleaved fragment is shifted downfield from that in the intact 5S RNA, suggesting that helices I and V may be coaxial in intact T. utilis 5S RNA.     

A small angle x-ray scattering study of a fragment derived from E. coli 5S RNA.

The structure of a 62 base nuclease resistant fragment of E. coli 5S RNA (bases 1-11, 69-87, 89-120) has been examined by small angle x-ray scattering. The results obtained are indistinguishable from those expected if this oligonucleotide complex were a perfect RNA double helix of about 30 base pairs. These results indicate that this portion of 5S RNA is in a configuration which is approximately double helical, even though proper base pairing is possible over only half its length.     

Nuclear Overhauser experiments at 500 MHz on the downfield proton spectrum of a ribonuclease-resistant fragment of 5S ribonucleic acid

The downfield (9-15 ppm) proton NMR spectrum of a RNase A resistant fragment of E. coli 5S RNA has been studied by nuclear Overhauser methods. The fragment comprises bases 1-11 and 69-120 of the parent molecule [Douthwaite, S., Garrett, R.A., Wagner, R., & Feunteun, J. (1979) Nucleic Acids Res. 6, 2453-2470]. The nuclear Overhauser data identify two double helical structures in the fragment whose sequences are (GC)3(AU)(GC)3 and (GC)2(AU)(GU). These structures correspond exactly to the central portions of the terminal stem and procaryotic loop helices which should exist in the fragment sequences according to the Fox-Woese model [Fox, G.E., & Woese, C. R. (1975) Nature (London) 256, 505-506] of 5S RNA secondary structure. The significance of these and other nuclear Overhauser effects detected for the structure of 5S RNA and its fragment is discussed.     

An NMR study of the helix V-loop E region of the 5S RNA from Escherichia coli

Experiments are described that complete the assignment of the imino proton NMR spectrum of the fragment 1 domain from the 5S RNA of Escherichia coli. Most of the new assignments fall in the helix V-loop E portion of the molecule (bases 70-78 and 98-106), the region most sensitive to the binding of ribosomal protein L25. The spectroscopic data are incompatible with the standard, phylogenetically derived model for 5S RNA, which makes all the base pairs possible in loop E with the sequences aligned in parallel (C70-G106, C71-G105, etc.) [see Delihas et al. (1984) Prog. Nucleic Acid Res. Mol. Biol. 31, 161-190]. Furthermore, the alternative loop E model proposed for spinach chloroplast 5S RNA by Romby et al. [(1988) Biochemistry 27, 4721-4730] does not apply to the closely homologous 5S RNA from E. coli. The 5S RNAs from E. coli and spinach chloroplasts do not have the same secondary structures in solution despite their strong sequence homologies, and neither appears to conform to the standard model for 5S RNA in the loop E region.     

An approach to the structure determination of nucleic acid analogues hybridized to RNA. NMR studies of a duplex between 2'-OMe RNA and an oligonucleotide containing a single amide backbone modification.

The backbone modification amide-3, in which -CH2-NH-CO-CH2- replaces -C5'H2-O5'-PO2-O3'-, is studied in the duplex d(G1-C2-G3-T4.T5-G6-C7-G8)*mr(C9-G10-C11-A12-A13-C14-G15+ ++-C16) where . indicates the backbone modification and mr indicates the 2'-OMe RNA strand. The majority of the exchangeable and non-exchangeable resonances have been assigned. The assignment procedure differs from standard methods. The methyl substituent of the 2'-OMe position of the RNA strand can be used as a tool in the interpretation. The duplex structure is a right-handed double helix. The sugar conformations of the 2'-OMe RNA strand are predominantly N-type and the 2'-OMe is positioned at the surface of the minor groove. In the complementary strand, only the sugar of residue T4 is found exclusively in N-type conformation. The incorporation of the amide modification does not effect very strongly the duplex structure. All bases are involved in Watson-Crick base pairs.     

5S RNA structure and interaction with transcription factor A. 1. Ribonuclease probe of the structure of 5S RNA from Xenopus laevis oocytes

The structure of Xenopus laevis oocyte (Xlo) 5S ribosomal RNA has been probed with single-strand-specific ribonucleases T1, T2, and A with double-strand-specific ribonuclease V1 from cobra venom. The digestion of 5'- or 3'-labeled renatured 5S RNA samples followed by gel purification of the digested samples allowed the determination of primary cleavage sites. Results of these ribonuclease digestions provide support for the generalized 5S RNA secondary structural model derived from comparative sequence analysis. However, three putative single-stranded regions of the molecule exhibited unexpected V1 cuts, found at C36, U73, U76, and U102. These V1 cuts reflect additional secondary structural features of the RNA including A.G base pairs and support the extended base pairing in the stem containing helices IV and V which was proposed by Stahl et al. [Stahl, D. A., Luehrsen, K. R., Woese, C. R., & Pace, N. R. (1981) Nucleic Acids Res. 9, 6129-6137]. A conserved structure for helix V having a common unpaired uracil residue at Xlo position 84 is proposed for all eukaryotic 5S RNAs. Our results are compared with nuclease probes of other 5S RNAs.     

Identification and assignment of base pairs in four helical segments of Bacillus megaterium ribosomal 5S RNA and its ribonuclease T1 cleavage fragments by means of 500-MHz proton homonuclear Overhauser enhancements.

Three different fragments of Bacillus megaterium ribosomal 5S RNA have been produced by enzymatic cleavage with ribonuclease T1. Fragment A consists of helices II and III, fragment B contains helix IV, and fragment C contains helix I of the universal 5S rRNA secondary structure. All (eight) imino proton resonances in the downfield region (9-15 ppm) of the 500-MHz proton FT NMR spectrum of fragment B have been identified and assigned as G80.C92-G81.C91-G82.C90-A83.++ +U89-C84.G88 and three unpaired U's (U85, U86, and U87) in helix IV by proton homonuclear Overhauser enhancement connectivities. The secondary structure in helix IV of the prokaryotic loop is completely demonstrated spectroscopically for the first time in any native or enzyme-cleaved 5S rRNA. In addition, G21.C58-A20.U59-G19.C60-A18.U61 in helix II, U32.A46-G31.C47-C30.G48-C29.G49 in helix III, and G4.C112-G5.C111-U6.G110 in the terminal stem (helix I) have been assigned by means of NOE experiments on intact 5S rRNA and its fragments A and C. Base pairs in helices I-IV of the universal secondary structure of B. megaterium 5S RNA are described.     

Nuclear Overhauser experiments at 500 MHz on the downfield proton spectra of 5S ribonucleic acid and its complex with ribosomal protein L25

The downfield (9-15 ppm) proton spectrum of Escherichia coli 5S RNA has been examined at 500 MHz by using nuclear Overhauser methods. The data confirm the existence of the terminal and procaryotic loop helices within the molecule [Fox, G. E., & Woese, C. R. (1975) Nature (London) 256, 505-506]. Very little stable, double-helical structure is detectable in the third loop of the molecule, the one comprising bases 12-68. The downfield spectrum of 5S RNA is perturbed in a highly specific manner upon addition of protein L25 to the system. The changes seen strongly suggest that the binding site for L25 on 5S RNA includes the procaryotic loop helix, but not the terminal stem helix. Similar complexes formed between L25 and the 5S RNA fragment consisting of bases 1-11, 69-87, and 89-120 show exactly the same spectral alterations. A number of downfield resonances appear in the spectra of these complexes which have no counterparts in the free RNA, suggesting the stabilization of new RNA structures by the protein. There are some indications of protein-nucleic acid nuclear Overhauser effects.     

High-resolution nuclear magnetic resonance determination of transfer RNA tertiary base pairs in solution. 2. Species containing a large variable loop.

The number of base pairs in the solution structure of several class III D3VN tRNA species from E. coli has been determined by analyzing the number of low-field (-15 to -11 ppm) proton resonances in their nuclear magnetic resonance spectra at 360 MHz. Contrary to previous reports indicating the absence of tertiary resonances, all the spectra exhibit the expected number of secondary base pair resonances plus approximately ten extra resonances derived from tertiary base pairs in the three-dimensional folding of these molecules. The possible origins of some of these tertiary resonances are discussed; none of the spectra exhibits the characteristic resonance of the 8-14 tertiary base pair seen in class I D4V5 tRNA spectra.     

Hydration of transfer RNA molecules: a crystallographic study

Four crystal structures of transfer RNA molecules were refined at 3 A resolution with the inclusion of the solvent molecules found in the difference maps: yeast tRNA-phe in the orthorhombic form, yeast tRNA-phe in the monoclinic form and yeast tRNA-asp in the A and B forms. Over 100 solvent molecules were located in each tRNA crystal. Several hydration schemes are found repeatedly in the 4 crystals. The tertiary interactions in the corner of the L-shaped molecule attract numerous solvent molecules which bridge the ribose hydroxyl O(2') atoms, base exocyclic atoms and phosphate anionic oxygen atoms. Conservation of bases leads to conservative localized hydration patterns. Several solvent molecules are found stabilizing unusual base pairs like the G-U pairs and those involving the pseudouridine base. Water bridges between the O(2') and the exocyclic atom O2 of pyrimidines or the N3 atom of purines are common. Water bridges occur frequently between successive anionic oxygen atoms of each strand as well as between N7 or other exocyclic atoms of successive bases in the major groove. Magnesium ions or spermine molecules are found to bind in the major groove of tRNA helices without specific interactions.     

Identification of three G.U base pairs in Bacillus subtilis ribosomal 5S RNA via 500-MHz proton homonuclear Overhauser enhancements

Three distinct G.U base pairs in Bacillus subtilis 5S RNA have been identified via homonuclear Overhauser enhancements (NOE) of their low-field (9-15 ppm) proton Fourier transform nuclear magnetic resonances at 11.75 T. With these G.U resonances as starting points, short segments of NOE connectivity can be established. One G.U-G.C-G.C segment (most probably G4.C112-G5.C111-U6.G110) can definitely be assigned to the terminal helix. The existence of at least part of the terminal helical stem of the secondary structure of a Gram-positive bacterial 5S RNA has thus been established for the first time by direct experimental observation. Addition of Mg2+ produces almost no conformational changes in the terminal stem but results in major conformational changes elsewhere in the structure, as reflected by changes in the 1H 500-MHz low-field NMR spectrum. Assignment of the two remaining G.U base pairs will require further experiments (e.g., enzymatic-cleavage fragments). Finally, the implications of these results for analysis of RNA secondary structure are discussed.     

The 5S rRNA loop E: chemical probing and phylogenetic data versus crystal structure.

A significant fraction of the bases in a folded, structured RNA molecule participate in noncanonical base pairing interactions, often in the context of internal loops or multi-helix junction loops. The appearance of each new high-resolution RNA structure provides welcome data to guide efforts to understand and predict RNA 3D structure, especially when the RNA in question is a functionally conserved molecule. The recent publication of the crystal structure of the "Loop E" region of bacterial 5S ribosomal RNA is such an event [Correll CC, Freeborn B, Moore PB, Steitz TA, 1997, Cell 91:705-712]. In addition to providing more examples of already established noncanonical base pairs, such as purine-purine sheared pairings, trans-Hoogsteen UA, and GU wobble pairs, the structure provides the first high-resolution views of two new purine-purine pairings and a new GU pairing. The goal of the present analysis is to expand the capabilities of both chemical probing and phylogenetic analysis to predict with greater accuracy the structures of RNA molecules. First, in light of existing chemical probing data, we investigate what lessons could be learned regarding the interpretation of this widely used method of RNA structure probing. Then we analyze the 3D structure with reference to molecular phylogeny data (assuming conservation of function) to discover what alternative base pairings are geometrically compatible with the structure. The comparisons between previous modeling efforts and crystal structures show that the intricate involvements of ions and water molecules in the maintenance of non-Watson-Crick pairs render the process of correctly identifying the interacting sites in such pairs treacherous, except in cases of trans-Hoogsteen A/U or sheared A/G pairs for the adenine N1 site. The phylogenetic analysis identifies A/A, A/C, A/U and C/A, C/C, and C/U pairings isosteric with sheared A/G, as well as A/A and A/C pairings isosteric with both G/U and G/G bifurcated pairings. Thus, each non-Watson-Crick pair could be characterized by a phylogenetic signature of variations between isosteric-like pairings. In addition to the conservative changes, which form a dictionary of pairings isosterically compatible with those observed in the crystal structure, concerted changes involving several base pairs also occur. The latter covariations may indicate transitions between related but distinctive motifs within the loop E of 5S ribosomal RNA.     

NMR evidence for dynamic secondary structure in helices II and III of the RNA of Escherichia coli

A new ribonuclease A (RNase A) resistant fragment of the 5S ribonucleic acid (RNA) from Escherichia coli has been isolated and characterized. This fragment comprises helix III and most of helix II of the parent molecule, a part of the 5S RNA molecule for which several energetically equivalent secondary structures have been proposed [De Wachter, R., Chen, M.-W., & Vandenberghe, A. (1984) Eur. J. Biochem. 143, 175-182]. The imino proton spectrum of this fragment has been studied by nuclear magnetic resonance methods at 500 MHz. The data obtained are readily rationalized in terms of one of the structures proposed for this region of 5S RNA. They also suggest that upon heating, this structure is replaced by a second, different one, consistent with the view that the helix II-helix III region of 5S RNA is able to switch between alternative structures. Among the products of the nucleolytic digestion of 5S RNA is a species whose sequence indicates that RNase A can ligate RNA as well as hydrolyze it.     

Structure of SL4 RNA from the HIV-1 packaging signal.

The NMR-based structure is described for an RNA model of stem-loop 4 (SL4) from the HIV-1 major packaging domain. The GAGA tetraloop adopts a conformation similar to the classic GNRA form, although there are differences in the details. The type II tandem G.U pairs have a combination of wobble and bifurcated hydrogen bonds where the uracil 2-carbonyl oxygen is hydrogen-bonded to both G,H1 and G,H2. There is the likelihood of a Na(+) ion coordinated to the four carbonyl oxygens in the major groove for these G.U pairs and perhaps to the N7 lone pairs of the G bases as well. A continuous stack of five bases extends over nearly the whole length of the stem to the base of the loop in the RNA 16mer: C15/U14/G13/G5/C6. There is no evidence for a terminal G.A pair; instead, G1 appears quite unrestrained, and A16 stacks on both C15 and G2. Residues G2 through G5 exhibit broadened resonances, especially G3 and U4, suggesting enhanced mobility for the 5'-side of the stem. The structure shows G2/G3/U4 stacking along the same strand, nearly isolated from interaction with the other bases. This is probably an important factor in the signal broadening and apparent mobility of these residues and the low stability of the 16mer hairpin against thermal denaturation.     

RNA structure and dynamics: A base pairing perspective

RNA is now known to possess various structural, regulatory and enzymatic functions for survival of cellular organisms. Functional RNA structures are generally created by three-dimensional organization of small structural motifs, formed by base pairing between self-complementary sequences from different parts of the RNA chain. In addition to the canonical Watson–Crick or wobble base pairs, several non-canonical base pairs are found to be crucial to the structural organization of RNA molecules. They appear within different structural motifs and are found to stabilize the molecule through long-range intra-molecular interactions between basic structural motifs like double helices and loops. These base pairs also impart functional variation to the minor groove of A-form RNA helices, thus forming anchoring site for metabolites and ligands. Non-canonical base pairs are formed by edge-to-edge hydrogen bonding interactions between the bases. A large number of theoretical studies have been done to detect and analyze these non-canonical base pairs within crystal or NMR derived structures of different functional RNA. Theoretical studies of these isolated base pairs using ab initio quantum chemical methods as well as molecular dynamics simulations of larger fragments have also established that many of these non-canonical base pairs are as stable as the canonical Watson–Crick base pairs. This review focuses on the various structural aspects of non-canonical base pairs in the organization of RNA molecules and the possible applications of these base pairs in predicting RNA structures with more accuracy.     

Sequence dependence of the stability of RNA hairpin molecules with six nucleotide loops

Thermodynamic parameters are reported for hairpin formation in 1 M NaCl by RNA sequence of the types GCGXUAAUYCGC and GGUXUAAUYACC with Watson-Crick loop closure, where XY is the set of 10 possible mismatch base pairs. A nearest-neighbor analysis of the data indicates the free energy of loop formation at 37 degrees C varies from 3.1 to 5.1 kcal/mol. These results agree with the model previously developed [Vecenie, C. J., and Serra, M. J. (2004) Biochemistry 43, 11813] to predict the stability of RNA hairpin loops: DeltaG degrees (37L(n) = DeltaG degrees (37i(n) + DeltaG degrees (37MM) - 0.8 (if first mismatch is GA or UU) - 0.8 (if first mismatch is GG and loop is closed on the 5' side by a purine). Here, DeltaG degrees (37i(n) is the free energy for initiating a loop of n nucleotides, and DeltaG degrees (37MM) is the free energy for the interaction of the first mismatch with the closing base pair. Thermodynamic parameters are also reported for hairpin formation in 1 M NaCl by RNA sequence of the types GACGXUAAUYUGUC and GGUXUAAUYGCC with GU base pair closure, where XY is the set of 10 possible mismatch base pairs. A nearest-neighbor analysis of the data indicates the free energy of loop formation at 37 degrees C varies from 3.6 to 5.3 kcal/mol. These results allow the development of a model for predicting the stability of hairpin loops closed by GU base pairs. DeltaG degrees (37L(n) (kcal/mol) = DeltaG degrees (37i(n) - 0.8 (if the first mismatch is GA) - 0.8 (if the first mismatch is GG and the loop is closed on the 5' side by a purine). Note that for these hairpins, the stability of the loops does not depend on DeltaG degrees (37MM). For hairpin loops closed by GU base pairs, the DeltaG degrees (37i(n) values, when n = 4, 5, 6, 7, and 8, are 4.9, 5.0, 4.6, 5.0, and 4.8 kcal/mol, respectively. The model gives good agreement when tested against six naturally occurring hairpin sequences. Thermodynamic values for terminal mismatches adjacent to GC, GU, and UG base pairs are also reported.