Specific and non-specific purine trap in the T-loop of normal and suppressor tRNAs

To elucidate the general constraints imposed on the structure of the D and T-loops in functional tRNAs, active suppressor tRNAs were selected in vivo from a combinatorial tRNA gene library in which several nucleotide positions in these loops were randomized. Analysis of the nucleotide sequences of the selected clones demonstrates that most of them contain combination U54-A58 allowing the formation of the standard reverse-Hoogsteen base-pair 54-58 in the T-loop. With only one exception, all these clones fall into two groups, each characterized by a distinct sequence pattern. Analysis of these two groups has allowed us to suggest two different types of nucleotide arrangement in the DT region. The first type, the so-called specific purine trap, is found in 12 individual tRNA clones and represents a generalized version of the standard D-T loop interaction. It consists of purine 18 sandwiched between the reverse-Hoogsteen base-pair U54-A58 and purine 57. The identity of purine 18 is restricted by the specific base-pairing with nucleotide 55. Depending on whether nucleotide 55 is U or G, purine 18 should be, respectively, G or A. The second structural type, the so-called non-specific purine trap, corresponds to the nucleotide sequence pattern found in 16 individual tRNA clones and is described here for the first time. It consists of purine 18 sandwiched between two reverse-Hoogsteen base-pairs U54-A58 and A55-C57 and, unlike the specific purine trap, requires the T-loop to contain an extra eighth nucleotide. Since purine 18 does not form a base-pair in the non-specific purine trap, both purines, G18 and A18, fit to the structure equally well. The important role of both the specific and non-specific purine traps in the formation of the tRNA L-shape is discussed.     

Key elements in maintenance of the tRNA L-shape

Based on in vivo selection of effective suppressor tRNAs from two different combinatorial gene libraries in which several nucleotides in the D and T-loops were randomized, we show that the position of the reverse-Hoogsteen base-pair in the T-loop, normally formed between nucleotides 54-58, co-varies with the length of the D-domain. When the D-domain has the normal length, the position of the reverse-Hoogsteen base-pair in the T-loop is always such that it allocates two unpaired nucleotides 59-60 for the bulge that fills the space between the D and T-domains. However, when the D-domain becomes shorter, the position of the reverse-Hoogsteen base-pair changes in the way that more nucleotides are now allocated to the T-loop bulge, so that the total length of the D-domain and of the bulge remains the same. Such compensation guarantees that in all tRNAs, the D and T-domains are always juxtaposed in the standard way. It also demonstrates the major role of the two T-loop elements, the bulge and the reverse-Hoogsteen base-pair, in the formation of the canonical tRNA L-shape.     

Nuclear magnetic resonance studies on transfer ribonucleic acid: assignment of AU tertiary resonances.

The hydrogen-bonded ring NH nuclear magnetic resonance (NMR) spectra of several transfer ribonucleic acid (RNA) species have been examined with particular emphasis on the extreme low-field portion. Betwen --13.8 and --15 ppm there are two extra resonances which are not derived from cloverleaf base pairs. A combined approach involving undermodified tRNAs, chemical modification, and hairpin fragment studies has assigned the T54--A58 resonance at --14.3 ppm in yeast tRNAPhe and Escherichia coli tRNA1 Val., the U8--A14 resonance has been assigned at --14.3 ppm, and the s4U8--A14 resonance in bacterial tRNAs has been assigned at --14.9 ppm. The T54--A58 resonance shifts between --14.3. and --13.8 ppm depending on the surrounding nucleotide sequence in the ribothymidine loop.     

Importance of the reverse Hoogsteen base pair 54-58 for tRNA function

To elucidate the general constraints imposed on the structure of the D- and T-loops in functional tRNAs, active suppressor tRNAs were selected in vivo from a combinatorial tRNA gene library in which several nucleotide positions of these loops were randomized. Analysis of the nucleotide sequences of the selected clones demonstrates that among the randomized nucleotides, the most conservative are nucleotides 54 and 58 in the T-loop. In most cases, they make the combination U54-A58, which allows the formation of the normal reverse Hoogsteen base pair. Surprisingly, other clones have either the combination G54-A58 or G54-G58. However, molecular modeling shows that these purine–purine base pairs can very closely mimic the reverse Hoogsteen base pair U-A and thus can replace it in the T-loop of a functional tRNA. This places the reverse Hoogsteen base pair 54-58 as one of the most important structural aspects of tRNA functionality. We suggest that the major role of this base pair is to preserve the conformation of dinucleotide 59–60 and, through this, to maintain the general architecture of the tRNA L-form.     

A computational and experimental study of the bending induced at a double-triple helix junction.

We have studied the conformation of a 17 base-pair homopyrimidine.homopurine triple helix formed on a fragment of duplex DNA derived from Simian Virus SV40. Gel retardation assays indicate that an 80 base-pair fragment has an altered conformation when the triple helix is formed, which is most likely to result from an induced bend in the DNA. Investigation of the detailed conformation of the double helix-triple helix junctions has been performed by means of molecular modelling. Bending on the 5' and 3' sides of the third strand oligonucleotide are not located at equivalent positions with respect to the junctions, which is explained in terms of base stacking. The junction effects on DNA structure, induced by the requirement for cytosine protonation in the Hoogsteen-bonded strand to form CGC+ base triplets, are also discussed.     

Studies of the complex between transfer RNAs with complementary anticodons: I. Origins of enhanced affinity between complementary triplets

We used the temperature-jump method to study the complex between yeast t RNA^Pheand Escherichia coli tRNA^Glu, which have the complementary anticodons GmAA and s²UUC, respectively. The binding constant (3.6 × 10⁵m^?1 at 25 °C) is about six orders of magnitude larger than expected for two complementary trinucleotides. The association rate constant (3 × 10⁶m^?1 at 25 °C) is similar to typical values observed for oligonucleotides, so the enhanced affinity in the tRNA · tRNA complex is due entirely to a much slower dissociation than expected for a three base-pair helix. We found an association enthalpy of ?25 kcal/mol, nearly twice as large as expected for two stacking interactions in a three base-pair helix. The association entropy (?58 cal/deg per mol) is close to the expected value. The reaction occurs with a single relaxation, and therefore does not involve any slow reorganization of the tRNA molecule.We studied structural variations to investigate the origin of affinity enhancement. The following general factors are important. (1) The “loop constraint”, or closure of the two anticodon sequences into hairpin loops, accounts for about a factor 50 in the affinity. (2) “Dangling ends”, or non-complementary nucleotides at the end of the double helix contribute strongly to the affinity. (3) Modified nucleotides, like the Y base, in the dangling ends can contribute a special stabilization of up to a factor seven. These observations can be understood in terms of a model in which the short three base-pair helix is sandwiched between stacked bases and hence stabilized. The potential importance of loop-loop interactions and stacking effects for codon-anticodon bonding is emphasized. The results suggest a possible simple physical basis for the evolutionary choice of a triplet coding system.     

Solution structure and backbone dynamics of the DNA-binding domain of mouse Sox-5

The fold of the murine Sox-5 (mSox-5) HMG box in free solution has been determined by multidimensional NMR using (15)N-labeled protein and has been found to adopt the characteristic twisted L-shape made up of two wings: the major wing comprising helix 1 (F10--F25) and helix 2 (N32--A43), the minor wing comprising helix 3 (P51--Y67) in weak antiparallel association with the N-terminal extended segment. (15)N relaxation measurements show considerable mobility (reduced order parameter, S(2)) in the minor wing that increases toward the amino and carboxy termini of the chain. The mobility of residues C-terminal to Q62 is significantly greater than the equivalent residues of non-sequence-specific boxes, and these residues show a weaker association with the extended N-terminal segment than in non-sequence boxes. Comparison with previously determined structures of HMG boxes both in free solution and complexed with DNA shows close similarity in the packing of the hydrophobic cores and the relative disposition of the three helices. Only in hSRY/DNA does the arrangement of aromatic sidechains differ significantly from that of mSox-5, and only in rHMG1 box 1 bound to cisplatinated DNA does helix 1 have no kink. Helix 3 in mSox-5 is terminated by P68, a conserved residue in DNA sequence-specific HMG boxes, which results in the chain turning through approximately 90 degrees.     

Functional compensation by particular nucleotide substitutions of a critical G*U wobble base-pair during aminoacylation of transfer RNA

Expression of the genetic code depends on precise tRNA aminoacylation by cognate aminoacyl-tRNA synthetase enzymes. The G.U wobble base-pair in the acceptor helix of Escherichia coli alanine tRNA is the primary aminoacylation determinant of this molecule. Previous work on the process of synthetase recognition of the G.U pair showed that replacing G.U by a G.C Watson-Crick base-pair inactivates alanine acceptance by the tRNA, but that C.A and G.A wobble pair replacements preserve acceptance. Work by another group reported that the effects of a G.C replacement were reversed by a distal wobble base-pair in the anticodon helix. This result is potentially interesting because it suggests that distant regions in alanine tRNA are functionally coupled during synthetase recognition and more generally because recognition determinants of many other tRNAs lie in both the acceptor helix and anticodon helix region. Here, we have conducted an extensive in vivo analysis of the distal wobble pair in alanine tRNA and report that it does not behave like a compensating mutation. Restoration of alanine acceptance was not detected even when the synthetase enzyme was overproduced. We discuss the previous experimental evidence and suggest how the distal wobble pair was incorrectly analyzed. The available data indicate that all principal recognition determinants of alanine tRNA lie in the molecule's acceptor helix.     

The lonepair triloop: a new motif in RNA structure

The lonepair triloop (LPTL) is an RNA structural motif that contains a single ("lone") base-pair capped by a hairpin loop containing three nucleotides. The two nucleotides immediately outside of this motif (5' and 3' to the lonepair) are not base-paired to one another, restricting the length of this helix to a single base-pair. Four examples of this motif, along with three tentative examples, were initially identified in the 16S and 23S rRNAs with covariation analysis. An evaluation of the recently determined crystal structures of the Thermus thermophilus 30S and Haloarcula marismortui 50S ribosomal subunits revealed the authenticity for all of these proposed interactions and identified 16 more LPTLs in the 5S, 16S and 23S rRNAs. This motif is found in the T loop in the tRNA crystal structures. The lonepairs are positioned, in nearly all examples, immediately 3' to a regular secondary structure helix and are stabilized by coaxial stacking onto this flanking helix. In all but two cases, the nucleotides in the triloop are involved in a tertiary interaction with another section of the rRNA, establishing an overall three-dimensional function for this motif. Of these 24 examples, 14 occur in multi-stem loops, seven in hairpin loops and three in internal loops. While the most common lonepair, U:A, occurs in ten of the 24 LPTLs, the remaining 14 LPTLs contain seven different base-pair types. Only a few of these lonepairs adopt the standard Watson-Crick base-pair conformations, while the majority of the base-pairs have non-standard conformations. While the general three-dimensional conformation is similar for all examples of this motif, characteristic differences lead to several subtypes present in different structural environments. At least one triloop nucleotide in 22 of the 24 LPTLs in the rRNAs and tRNAs forms a tertiary interaction with another part of the RNA. When a LPTL containing the GNR or UYR triloop sequence forms a tertiary interaction with the first (and second) triloop nucleotide, it recruits a fourth nucleotide to mediate stacking and mimic the tetraloop conformation. Approximately half of the LPTL motifs are in close association with proteins. The majority of these LPTLs are positioned at sites in rRNAs that are conserved in the three phylogenetic domains; a few of these occur in regions of the rRNA associated with ribosomal function, including the presumed site of peptidyl transferase activity in the 23S rRNA.     

A conserved base-pair between tRNA and 23 S rRNA in the peptidyl transferase center is important for peptide release

The 3' terminus of tRNAs has the universally conserved bases C74C75A76 that interact with the ribosomal large subunit. In the ribosomal P site, bases C74 and C75 of tRNA, form Watson-Crick base-pairs with G2252 and G2251, respectively, present in the conserved P-loop of 23 S rRNA. Previous studies have suggested that the G2252-C74 base-pair is important for peptide bond formation. Using a pure population of mutant ribosomes, we analyzed the precise role of this base-pair in peptide bond formation, elongation factor G-dependent translocation, and peptide release by release factor 1. Surprisingly, our results show that the G2252-C74 base-pair is not essential for peptide bond formation with intact aminoacyl tRNAs as substrates and for EF-G catalyzed translocation. Interestingly, however, peptide release was reduced substantially when base-pair formation between G2252 and C74 of P site tRNA was disrupted, indicating that this conserved base-pair plays an important role in ester bond hydrolysis during translation termination.     

Three-dimensional structures of bulge-containing DNA fragments.

The three-dimensional structure of a DNA tridecamer d(CGCAGAATTCGCG)2 containing bulged adenine bases was determined by single crystal X-ray diffraction methods, at 120 K, to 2.6 A resolution. The structure is a B-DNA type double helix with a single duplex in the asymmetric unit. One of the bulged adenine bases loops out from the double helix, while the other stacks in to it. This is in contrast to our preliminary finding, which indicated that both adenine bases were looped out. This revised model was confirmed by the use of a covalently bound heavy-atom derivative. The conformation of the looped-out bulge hardly disrupts base stacking interactions of the bases flanking it. This is achieved by the backbone making a "loop-the-loop" curve with the extra adenine flipping over with respect to the other nucleotides in the strand. The looped-out base intercalates into the stacked-in bulge site of a symmetrically related duplex. The looped-out and stacked-in bases form an A.A reversed Hoogsteen base-pair that stacks between the surrounding base-pairs, thus stabilizing both bulges. The double helix is frayed at one end with the two "melted" bases participating in intermolecular interactions. A related structure, of the same tridecamer, after soaking the crystals with proflavin, was determined to 3.2 A resolution. The main features of this B-DNA duplex are basically similar to the native tridecamer but differ in detail especially in the conformation of the bulged-out base. Accommodation of a large perturbation such as that described here with minimal disruption of the double helix shows both the flexibility and resiliency of the DNA molecule.     

G . T base-pairs in a DNA helix: the crystal structure of d(G-G-G-G-T-C-C-C)

The synthetic deoxyoctanucleotide d(G-G-G-G-T-C-C-C) crystallizes as an A-type DNA double helix containing two adjacent G . T base-pair mismatches. The structure has been refined to an R-factor of 14% at 2.1 A resolution with 104 solvent molecules located. The two G . T mismatches adopt the "wobble" form of base-pairing. The mismatched bases are linked by a network of water molecules interacting with the exposed functional groups in both the major and minor grooves. The presence of two mispaired bases in the octamer has surprisingly little effect on the global structure of the helix or the backbone and glycosidic torsional angles. Base stacking around the mismatch is perturbed, but the central G-T step shows particularly good base overlap, which may contribute to the relatively high stability of this oligomer.     

Structural features and hydration of a dodecamer duplex containing two C.A mispairs.

X-ray diffraction techniques have been used to characterise the crystal and molecular structure of the deoxyoligomer d(C-G-C-A-A-A-T-T-C-G-C-G) at 2.5A resolution. The final R factor is 0.19 with the location of 78 solvent molecules. The oligomer crystallises in a B-DNA type conformation with two strands coiled about each other to produce a duplex. This double helix consists of four A.T and six G.C Watson-Crick base pairs and two C.A mispairs. The mismatched base pairs adopt a "wobble" type structure with the cytosine displaced laterally into the major groove, the adenine into the minor groove. We have proposed that the two close contacts observed in the C.A pairing represent two hydrogen bonds one of which results from protonation of adenine. The mispairs are accommodated in the double helix with small adjustments in the conformation of the sugar-phosphate backbone. Details of the backbone conformation, base stacking interactions, thermal parameters and the hydration are now presented and compared with those of the native oligomer d(C-G-C-G-A-A-T-T-C-G-C-G) and with variations of this sequence containing G.T and G.A mispairs.     

A proposal for a specific double-helical structure in which the polynucleotide strands intercalate instead of forming base-pairs

Double helices, since the discovery of the DNA structure by Watson and Crick, represent the single most important secondary structural form of nucleic acids. The secondary structures of a variety of polynucleotide helices have now been well characterised with hydrogen-bonded base-pairs as building blocks. We wish to propose here the possibility, in a specific case, of a double stranded helical structure without any base-pair, but having a repeat unit of two nucleotides with their bases stacked through intercalation. The proposal comes from the initial models we have built for poly(dC) using the stacking patterns found in the crystal structures of 5'-dCMPNa2 which crystallises in two forms depending on the degree of hydration. These structures have pairs of nucleotides with the cytosine rings partially overlapping and separated by 3.3A. Using these as repeat units one could generate a model for poly(dC) with parallel strands, having a turn angle of 30 degrees and a base separation of 6.6A along each strand. Both right and left handed models with these parameters can be built in a smooth fashion without any obviously unreasonable stereochemical contacts. The helix diameter is about 13.5A, much smaller than that of normal helices with base-pair repeats. The changes in the sugar-phosphate backbone conformation in the present models compared to normal duplexes only reflect the torsional flexibility available for extension of polynucleotide chains as manifested by the crystal structures of drug-inserted oligonucleotide complexes. Intercalation proposed here could have some structural relevance elsewhere, for instance to the base-mismatched regions on the double helix and the packing of noncomplementary single strands as found in the filamentous bacteriophage Pf1.     

Identity elements required for enzymatic formation of N2,N2-dimethylguanosine from N2-monomethylated derivative and its possible role in avoiding alternative conformations in archaeal tRNA

Here, we have investigated the specificity of purified recombinant tRNA:m(2)(2)G10 methyltransferase of Pyrococcus abyssi ((Pab)Trm-m(2)(2)G10 enzyme). This archaeal enzyme catalyses mono- and dimethylation of the N(2)-exocyclic amino group of guanine at position 10 of several tRNA species. Our results indicate that only few identity elements are required for the efficient formation of m(2)(2)G10. They are composed of a G10.U25 wobble base-pair in the dihydrouridine arm (D-arm) and a four nucleotide variable loop (V-loop) within a canonical three-dimensional (3D) structure. The types of base-pairs in the D-arm or amino acid acceptor stem are also important for the enzymatic reaction, but appear to affect only the rate of tRNA methylation. However, in tRNA species harbouring a G10-C25 Watson-Crick base-pair and/or five nucleotide V-loop, only m(2)G10 is produced. To impair the monomethylation reaction, drastic amputation in the T-arm is required. Our observations contrast with those reported earlier for the identity elements required for a remotely related Pyrococcus furiosus Trm-m(2)(2)G26 enzyme (alias (Pfu)Trm1) that also catalyses the two step formation of m(2)(2)G but at position 26 in several tRNA species. In this case, a G10-C25 base-pair together with the five nucleotide V-loop were shown to be required for efficient formation of m(2)(2)G26. Thus, in the Pyrococcus genus, the major identity elements that preclude formation of m(2)(2)G at positions 10 or 26 in tRNA are mutually exclusive. Therefore, the Trm-m(2)(2)G10 and Trm-m(2)(2)G26 enzymes have evolved independently towards different specificities. In addition, identity elements for m(2)/m(2)(2)G10 formation in archaeal tRNA are different from the ones required for m(2)G10 formation in eukaryal tRNA. We propose that archaeal tRNA:m(2)(2)G10 methyltransferases, unlike the orthologous eukaryal tRNA:m(2)G10 methyltransferases, evolved towards m(2)(2)G10 specificity due to the possible requirement of preventing formation of alternative structures in G/C rich archaeal tRNA species.     

Inosine.adenine base pairs in a B-DNA duplex.

The structure of the synthetic deoxydodecamer d(C-G-C-I-A-A-T-T-A-G-C-G) has been determined by single crystal X-ray diffraction techniques at 2.5A resolution. The refinement converged with a crystallographic residual, R = 0.19 and the location of 64 solvent molecules. The sequence crystallises as a B-DNA helix with 10 Watson-Crick base-pairs (4 A.T. and 6 G.C) and 2 inosine.adenine (I.A) pairs. The present work shows that in the purine.purine base-pairs the adenine adopts syn orientation with respect to the furanose moiety while the inosine is in the trans (anti) orientation. Two hydrogen bonds link the I.A. base-pair, one between N-1(I) and N-7(A), the other between O-6(I) and N-6(A). This bulky purine.purine base-pair is incorporated in the double helix at two positions with little distortion of either local or global conformation. The pairing observed in this study is presented as a model for I.A base-pairs in RNA codon-anticodon interactions and may help explain the thermodynamic stability of inosine containing base-pairs. Conformational parameters and base stacking interactions are presented and where appropriate compared with those of the native compound, d(C-G-C-G-A-A-T-T-C-G-C-G) and with other studies of oligonucleotides containing purine.purine base-pairs.     

Structural compensation in an archaeal selenocysteine transfer RNA.

A new type of structural compensation between the lengths of two perpendicularly oriented RNA double helices was found in the archaeal selenocysteine tRNA from Methanococcus jannascii. This tRNA contains only four base-pairs in the T-stem, one base-pair less than in all other cytosolic tRNAs. Our analysis shows that such a T-stem in an otherwise normal tRNA cannot guarantee the formation of the normal interactions between the D and T-loops. The absence of these interactions would affect the juxtaposition of the two tRNA helical domains, potentially damaging the tRNA function. In addition to the short T-stem, this tRNA possesses another unprecedented feature, a very long D-stem consisting of seven base-pairs. Taken as such, a seven base-pair D-stem will also disrupt the normal interaction between the D and T-loops. On the other hand, the presence of the universal nucleotides in both the D and T-loops suggests that these loops probably interact with each other in the same way as in other tRNAs. Here, we demonstrate that the short T-stem and the long D-stem can naturally compensate each other, thus providing the normal D/T interactions. Molecular modeling has helped suggest a detailed scheme of mutual compensation between these two unique structural aspects of the archaeal selenocysteine tRNA. In the light of this analysis, other structural and functional characteristics of the selenocysteine tRNAs are discussed.