Idealized atomic coordinates of yeast phenylalanine transfer RNA

A brief history of macromolecular crystallography, illustrated by a family tree and its Nobel fruits

As a contribution to the celebration of the year 2014, declared by the United Nations to be 'The International Year of Crystallography', the FEBS Journal is dedicating this issue to papers showcasing the intimate union between macromolecular crystallography and structural biology, both in historical perspective and in current research. Instead of a formal editorial piece, by way of introduction, this review discusses the most important, often iconic, achievements of crystallographers that led to major advances in our understanding of the structure and function of biological macromolecules. We identified at least 42 scientists who received Nobel Prizes in Physics, Chemistry or Medicine for their contributions that included the use of X-rays or neutrons and crystallography, including 24 who made seminal discoveries in macromolecular sciences. Our spotlight is mostly, but not only, on the recipients of this most prestigious scientific honor, presented in approximately chronological order. As a summary of the review, we attempt to construct a genealogy tree of the principal lineages of protein crystallography, leading from the founding members to the present generation.

Direct visualization of A-, P-, and E-site transfer RNAs in the Escherichia coli ribosome

Transfer RNA (tRNA) molecules play a crucial role in protein biosynthesis in all organisms. Their interactions with ribosomes mediate the translation of genetic messages into polypeptides. Three tRNAs bound to the Escherichia coli 70S ribosome were visualized directly with cryoelectron microscopy and three-dimensional reconstruction. The detailed arrangement of A- and P-site tRNAs inferred from this study allows localization of the sites for anticodon interaction and peptide bond formation on the ribosome.

UV photoelectron spectroscopy and ab initio characterization of valence orbital structures and conformations of neutral phosphate esters

The HeI UV photoelectron spectrum of trimethyl phosphate (TMP) has been measured and interpreted with the aid of SCF molecular orbital calculations carried out with STO-3G, STO-3G* and 4-31G basis functions. The photoelectron spectrum of TMP is more accurately reproduced by results from 4-31G calculations than by results from STO-3G or STO-3G* calculations. However, all three basis sets yield results which predict the same assignment of the photoelectron spectrum. Results at the 4-31G level indicate that whether calculations are based on crystallographic bond angles and bond lengths or on STO-3G optimized geometries has little effect on the energetic ordering of the upper occupied orbitals. The energetic ordering of orbitals is also found to be only weakly dependent upon the torsional angle phi, describing rotation of ester groups about P-O bonds and upon the torsional angle psi, describing rotation of methyl groups about C-O bonds. For trimethyl phosphate, with C3 symmetry, the vertical ionization potentials of the upper occupied orbitals are 10.81 eV (8e), 11.4 eV (9a), 11.93 eV (7e), 12.6-12.9 eV (8a and 6e), 14.4 eV (7a) and 15.0-16.0 eV (5e and 6a). Calculations at the 4-31G level indicate that many of the highest occupied orbitals in neutral dimethyl phosphate and methyl phosphate have energies and electron distributions similar to orbitals in TMP. For TMP, a search for optimized values of phi and psi has been carried out at the STO-3G*level. In agreement with previous NMR studies and with classical potential calculations, the STO-3G* results indicate that both the gauche (phi = 53.1 degrees) and anticlinal (phi = 141.9 degrees) conformations are thermally accessible. Also in agreement with the classical potential calculations, the STO-3G* results predict that in the all gauche conformation energy is minimized when the methyl groups assume a staggered geometry (psi = 60 degrees to 80 degrees) and that an energy maximum occurs for an eclipsed geometry (phi = 0 degrees to 20 degrees). A study of the dependence of optimized values of O-P-O ester bond angles on the torsional angles, phi, was carried out at the STO-3G, STO-3G* and 4-31G levels. The results demonstrate that for C3 symmetry, the coupling of O-P-O angles to phi is influence by repulsive steric 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.

Structural studies of DNA fragments: the G.T wobble base pair in A, B and Z DNA; the G.A base pair in B-DNA

The crystal structures of five double helical DNA fragments containing non-Watson-Crick complementary base pairs are reviewed. They comprise four fragments containing G.T base pairs: two deoxyoctamers d(GGGGCTCC) and d(GGGGTCCC) which crystallise as A type helices; a deoxydodecamer d(CGCGAATTTGCG) which crystallises in the B-DNA conformation; and the deoxyhexamer d(TGCGCG), which crystallises as a Z-DNA helix. In all four duplexes the G and T bases form wobble base pairs, with bases in the major tautomer forms and hydrogen bonds linking N1 of G with O2 of T and O6 of G with N3 of T. The X-ray analyses establish that the G.T wobble base pair can be accommodated in the A, B or Z double helix with minimal distortion of the global conformation. There are, however, changes in base stacking in the neighbourhood of the mismatched bases. The fifth structure, d(CGCGAATTAGCG), contains the purine purine mismatch G.A where G is in the anti and A in the syn conformation. The results represent the first direct structure determinations of base pair mismatches in DNA fragments and are discussed in relation to the fidelity of replication and mismatch recognition.

High-resolution structure of a DNA helix containing mismatched base pairs

The concept of complementary base pairing, integral to the double-helical structure of DNA, provides an effective and elegant mechanism for the faithful transmission of genetic information. Implicit in this model, however, is the potential for incorporating non-complementary base pairs (mismatches) during replication or subsequently, for example, during genetic recombination. As such errors are usually damaging to the organism, they are generally detected and repaired. Occasionally, however, the propagation of erroneous copies of the genome confers a selective advantage, leading to genetic variation and evolutionary change. An understanding of the nature of base-pair mismatches at a molecular level, and the effect of incorporation of such errors on the secondary structure of DNA is thus of fundamental importance. We now report the first single-crystal X-ray analysis of a DNA fragment, d(GGGGCTCC), which contains two non-complementary G X T base pairs, and discuss the implications of the results for the in vivo recognition of base-pair mismatches.

Crystal structure of yeast tRNAAsp: atomic coordinates

The atomic coordinates of yeast aspartic acid transfer RNA, as determined from a crystallographic investigation to 3 A resolution, are presented. In the ribose phosphate backbone sugars are in the C(3')-endo pucker, except for residues A7, A9, D16, G17, G18, D19, C20, U48, A58, and U60 which are in the C(2')-endo pucker. A least-squares superposition of the phosphorus atoms of yeast tRNAAsp and yeast tRNAPhe enlightens both an overall structural similarity and significant conformational differences. The largest deviations occur in the D-loop and the anticodon region.

A-form to A'-form conformational switch of double helices in rat liver 5S and 5.8S rRNA. Solution X-ray scattering evidence and circular dichroic measurements

The wide-angle X-ray scattering of rat liver 5S rRNA and 5.8S rRNA molecules showed significant differences in the positions of the scattering maxima when dissolved in Mg2+-containing Tris/HCl buffer or in Mg2+-depleted buffer. A comparison of the experimental curves with theoretical curves calculated from atomic coordinates of double-helical models proved a switch from A form to A' form of the double-helical regions within the molecules by changing the buffer conditions. This result was supported by circular dichroic measurements. The A to A' transition may have important consequences for RNA-protein interactions.

Crosslinking of tRNAs by the carcinostatic agent dirhodium tetraacetate

A crystalline complex of yeast tRNA(phe) and dirhodium tetraacetate (DRTA) was prepared and its X-ray structure determined. The bifunctional DRTA forms an intermolecular cross-link between the N(1) position of adenine A36 in the anticodon triplet and possibly a ribose hydroxyl group of residue A76 at the 3' terminus of a symmetry related tRNA molecule. The rhodium complex apparently shows a preference for binding to the N(1) position of adenine in a single strand region of the tRNA molecule.

An unexpected major groove binding of netropsin and distamycin A to tRNA(phe)

Crystalline complexes of yeast tRNA(phe) and the oligopeptide antibiotics netropsin and distamycin A were prepared by diffusing drugs into crystals of tRNA. X-ray structure analyses of these complexes reveal a single common binding site for both drugs which is located in the major or deep groove of the tRNA T-stem. The netropsin-tRNA complex is stabilized by specific hydrogen bonds between the amide groups of the drug and the tRNA bases G51 O(6), U52 O(4) and G53 N(7) on one strand, and is further stabilized by electrostatic interactions between the positively charges guanidino side chain of the drug and the tRNA phosphate P53 on the same strand and the positively charged amidino propyl side chain and the phosphates P61, P62 and P63 on the opposite strand of the double helix. These results are in contrast to the implicated minor groove binding of these drugs to non-guanine sequences in DNA. The binding to the GUG sequence in tRNA implies that major groove binding to certain DNA sequences is possible.

Lead ion binding and RNA chain hydrolysis in phenylalanine tRNA

Crystalline complexes of yeast phenylalanine tRNA and Lead (II) ion were prepared by soaking pregrown orthorhombic crystals of tRNA in saturated lead chloride solutions. The locations of tightly bound lead ions on the tRNA were determined by difference Fourier methods. There are three major lead binding sites; two of these replace tightly bound magnesium ions in the native tRNA structure. Site I is located in the dihydrouridine loop of the molecule adjacent to phosphate P18 which is specifically cleaved by lead. This is evident from changes observed in the Pb-native difference electron density maps. A possible mechanism for lead ion hydrolysis of the polynucleotide chain is proposed.

Molecular dynamics of phenylalanine transfer RNA

The atomic motions of yeast phenylalanine transfer RNA have been simulated using the molecular dynamics algorithm. Two simulations were carried out for a period of 12 picoseconds, one with a normal Van der Waals potential and the other with a modified Van der Waals potential intended to mimic the effect of solvent. An analysis of large scale motions, surface exposure, root mean square displacements, helical oscillations and relaxation mechanisms reveals the maintenance of stability in the simulated structures and the general similarity of the various dynamic features of the two simulations. The regions of conformational flexibility and rigidity for tRNA(Phe) have been shown in a quantitative measure through this approach.

Similar binding of the carcinostatic drugs cis-[Pt(NH3)2Cl2] and [Ru(NH3)5Cl] Cl2 to tRNAphe and a comparison with the binding of the inactive trans-[Pt(NH3)2Cl2] complex - reluctance in binding to Watson-Crick base pairs within double helix

A comparative study of the binding of square planar cis- and trans-[Pt(NH3)2Cl2] complexes and the octahedral [Ru(NH3)5(H2O)]3+ complex to tRNAphe from yeast was carried out by X-ray crystallography. Both of the carcinostatic compounds, cis-[Pt(NH3)2Cl2] and [Ru(NH3)5(H2O)]3+ show similarities in their mode of binding to tRNA. These complexes bind specifically to the N(7) positions of guanines G15 and G18 in the dihydrouridine loop. [Ru(NH3)5(H2O)]3+ has an additional binding site at N(7) of residue G1 after extensive soaking times (58 days). A noncovalent binding site for ruthenium is also observed in the deep groove of the acceptor stem helix with shorter (25 days) soaking time. The major binding site for the inactive trans-[Pt(NH3)Cl2] complex is at the N(1) position of residue A73, with minor trans-Pt binding sites at the N(7) positions of residues Gm34, G18 and G43. The similarities in the binding modes of cis-[Pt(NH3)2Cl2] and [Ru(NH3)5(H2O)]3+ are expected to be related to their carcinostatic properties.

A novel guanine-guanine base pairing: crystal structure of a complex between 7-methylguanosine and its iodide

7-Methylguanosine, one of the biologically important minor nucleosides, could be crystallized as a complex of its zwitterionic form and its iodide, and the crystal structure was determined by the X-ray diffraction method. The crystals belong to the triclinic space group P1 with the unit cell dimensions: a = 7.678(1), b = 18.094(3), and c = 5.711(1) A, alpha = 79.32(1), beta = 80.14(1) and gamma = 76.90(1) degrees. The structure was solved by the heavy atom method and refined by the least-squares method to give a final R index of 0.075. The novel reverse Watson-Crick type base pairing observed between a positively charged molecule and a deprotonated one indicates that the deprotonation at the N(1) position promoted by the alkylation at the N(7) position may interrupt the formation of the normal Watson-Crick type GC base pair. The conformations about the glycosidic bond and the sugar puckering are quite different between the two molecules: the former has anti and C(4')-exo,C(3')-endo and the latter syn and C(1')-exo-C(2')-endo.

Conformational characteristics of the dinucleoside triphosphate pCpGp from energy-minimization studies

The influence of the 3'- and 5'- terminal phosphates on the conformational characteristics of the dinucleoside monophosphate CpG is described in this paper. The computed potential energy of the system is minimized with respect to the relevant 10 dihedral angles permitting the two sugar rings to adopt the alternative puckering states, 2E and 3E. Of the 84 conformations considered, 22 become energetically accessible. The familiar A-, B-, Z- and Watson-Crick-type backbone states of DNA subunits become low-energy forms for this RNA unit pCpGp also. The Watson-Crick-type backbone is invariably preferred in all the four sugar pucker sequences, indicating its importance in the dynamics of sugar pucker fluctuations and in the DNA-RNA association. The interphosphate geometries and the possible hydrogen-bonded states are discussed in relation to the varied folded/extended polynucleotide structures.

Conformational flexibility in single-stranded oligonucleotides: crystal structure of a hydrated calcium salt of adenylyl-(3'--5')-adenosine

The crystal and molecular structure of a hydrated calcium salt of adenylyl-(3'--5')-adenosine(ApA) was determined from X-ray diffraction data collected on an automated diffractometer. Crystals of the salt are orthorhombic, space group P21212, with a = 30.614 (3), b = 17.894 (2), and c = 5.373 (1) A. The structure was solved by a combination of Patterson and direct methods and refined by least squares. The final value of the R index is 0.08. The 5'-terminal adenosine residue has a C(2')-endo ribose and assumes a syn conformation, which is stabilized by an O(5')-H...N(3) hydrogen bond within the nucleoside. The 3'-terminal nucleoside has a C(3')-endo ribose and is in the anti conformation. Both omega and omega', the torsion angles within the phosphodiester group, are approximately 60 degrees. Adenine bases from adjacent anions are joined by pairs of N(6)-H...N(1) hydrogen bonds and are stacked with symmetry-related bases. The calcium ion is bound to the dinucleoside phosphate by a direct interaction with the phosphate group and by outer-sphere, ligand-mediated interactions with O(2') of the 5'-terminal nucleoside and N(7) of the 3'-terminal nucleoside. This tridentate interaction of the ApA anion with the calcium coordination sphere probably enhances the stability of the observed ApA conformation. When combined with other crystallographic studies of ApA conformations, the crystal structure of this calcium salt provides additional evidence that dinucleoside phosphates have considerable conformational flexibility.

Conformational characteristics of dimeric subunits of RNA from energy minimization studies. Mixed sugar-puckered ApG, ApU, CpG, and CpU

Following the procedure described in the preceding article, the low energy conformations located for the four dimeric subunits of RNA, ApG, ApU, CpG, and CpU are presented. The A-RNA type and Watson-Crick type helical conformations and a number of different kinds of loop promoting ones were identified as low energy in all the units. The 3E-3E and 3E-2E pucker sequences are found to be more or less equally preferred; the 2E-2E sequence is occasionally preferred, while the 2E-3E is highly prohibited in all the units. A conformation similar to the one observed in the drug-dinucleoside monophosphate complex crystals becomes a low energy case only for the CpG unit. The low energy conformations obtained for the four model units were used to assess the stability of the conformational states of the dinucleotide segments in the four crystal models of the tRNAPhe molecule. Information on the occurrence of the less preferred sugar-pucker sequences in the various loop regions in the tRNAPhe molecule has been obtained. A detailed comparison of the conformational characteristics of DNA and RNA subunits at the dimeric level is presented on the basis of the results.

A 1:2 crystalline complex of ApA:proflavine: a model for binding to single-stranded regions in RNA

The structure of a 1"2 complex of adenylyl-(3',5')-adenosine phosphate and proflavine hemisulfate has been determined using the methods of x-ray crystallography. Since the ApA does not form a mini double helix, it may serve as a model for the interaction of planar molecules with single stranded nucleic acids. The dinucleotide adopts an extended conformation with the adenines in adjacent molecules forming base pairs. A most unusual feature of the molecule is that it does not obey the "rigid nucleotide" concept although none of the torsion angles occur in energetically unfavourable regions. This is most probably due to the strong interactions between the proflavine and the oligonucleotide.

Stacking of Crick Wobble pair and Watson-Crick pair: stability rules of G-U pairs at ends of helical stems in tRNAs and the relation to codon-anticodon Wobble interaction

The occurrence of the noncomplementary G-U base pair at the end of a helix is found to be governed by stacking interactions. As a rule, a G-U pair with G on the 5'-side of a Watson-Crick base pair exhibits strikingly greater stacking overlap with the Watson-Crick base pair than a G-U pair on the 3'-side of a Watson-Crick base pair. The former arrangement is expected to be more stable and indeed is observed 29 times out of 32 in the known transfer RNA molecules. In accordance with this rule, the major wobble base pairs G-U or I-U in codon-anticodon interactions have G or I on the 5'-side of the anticodon. Similarly, in initiator tRNAs, this rule is obeyed where now the G is the first letter of the codon (5'-side). In the situation where U is in the wobble position of the anticodon, it is usually substituted at C(5) andmay also have a 2-thio group and it can read one to four codons depending on its modifications. A G at the wobble position of the anticodon can recognize the two codons ending with U or C and modification of G (unless it is I) does not change its reading properties.

Base pairing structure in the poly d(G-T) double helix: wobble base pairs

High resolution nuclear magnetic resonance (NMR) and ethidium bromide binding studies are used to demonstrate that poly d(G-T) forms an ordered double helical structure at low temperatures (below 24 degrees C in 0.3 M NaCl) in which G and T are hydrogen bonded together in a wobble base pair hydrogen bonding scheme as proposed earlier by Lezius and Domin. Alternative hydrogen bonding schemes involving the tautomeric form of either T or G, such as have been proposed to account for mutation rates in DNA synthesis, are eliminated.

Modified bases in tRNA: the structures of 5-carbamoylmethyl- and 5-carboxymethyl uridine

The crystal structures of two nucleosides, 5-carbamoylmethyluridine (1) and 5-carboxymethyluridine (2), were determined from three-dimensional x-ray diffraction data, and refined to R = 0.036 and R = 0.047, respectively. Compound 1 is in the C3'-endo conformation with chi +5.2 degrees (anti), psiinfinity = +63.4 degrees and psialpha = +180.0 degrees (tt); 2 is in the C2'endo conformation with chi +49.4 degrees (anti), psiinfinity -60.5 degrees and psialpha +60.0 degrees (gg). For each derivative, the plane of the side chain substituent is skewed with respect to the plane of the nucleobase; for 1, the carboxamide group is on the same side of the uracil plane vis a vis the ribose ring; for 2, the carboxyl group is on the opposite side of this plane. No base pairing is observed for either structure. Incorporation of structure 1 into a 3'-stacked tRNA anticodon appears to place 08 within hydrogen bonding distance of the 02' hydroxyl of ribose 33, which may limit the ability of such a molecule of tRNA to "wobble".

A molecular orbital investigation of the conformation of transfer RNA

The PCILO method has been used for a theoretical exploration of the conformational properties of tRNAPhe with respect to the phosphodiester torsion angles. The computations were based on the utilisation of the dinucleoside triphosphate model and took into account the different combinations of sugar puckers and different conformations about the C4'-C5' bond. The dependence of the (omega'-omega) conformational energy maps upon these factors was specified. A detailed comparison is carried out between the theoretical results and experimental data on the crystal structure of tRNAPhe produced by four different groups of investigators.

Manganese(II) as a paramagnetic probe of the tertiary structure of transfer RNA

The effect of manganese on both the low field (10--15 ppm) and the high field (o--3 ppm) NMR spectra of unfractionated tRNA and yeast tRNAPhe has been investigated. Trace amounts of Mn2+ cause selective broadening of resonances which are assigned to specific tertiary interactions. The order in which resonances broaden is the same as the order in which they are stabilized by the addition of magnesium, namely s4U8 - A14, U33 and A58 - T54. From this we conclude that three of the strong binding sites probably are the same for both Mn2+ and Mg2+, and that these sites are located close to the tertiary interactions which are stabilized by the strongly bound metals. The broadening data, taken in conjunction with published X-ray data on yeast tRNAPhe, permit us to suggest some plausible locations for the strong binding sites.

Effect of magnesium and polyamines on the structure of yeast tRNAPhe

The effect of magnesium and polyamines (spermine, spermidine, putrescine and cadaverine) on the structure of yeast tRNAPhe has been investigated. It is found that magnesium induces structural changes and stabilizes hydrogen bonds in the temperature range 22--44 degrees C in 0.17 M sodium. The number of Mg2+ which affect tRNA structure increases from 1 +/- 1 at 22 degrees C to 4 +/- 1 at 44 degrees C and the number of additional base pairs formed in the presence of magnesium increases from 1 +/- 1 at 22 degrees C to 4 +/- 1 at 44 degrees C. The spectral changes are more-or-less sequential. The polyamine spermine stabilizes some, but not all, of the structural features stabilized by magnesium at 44 degrees C, and the combination of magnesium and spermine, at low levels, is more effective than either cation alone in stabilizing tRNA structure. Comparison of the effects of spermine, spermidine, putrescine and cadaverine indicates that it is the asymmetric triamine unit which is important in the stabilization. Some spectral changes induced by magnesium can be assigned to stabilization of specific tertiary structure interactions and to alteration of stacking adjacent to U8-A14.

1H NMR studies of transfer RNA III: the observed and the computed spectra of the hydrogen-bonded NH resonances of baker's yeast transfer-RNA Phe

The hydrogen-bonded NH resonances of Baker's yeast tRNAphe in H2O solution with Mg++ have been measured by a 360 MHz spectrometer at 23 degrees C. Totally, fifteen peaks and one shoulder can be resolved which represent 25 +/- 1 protons. Based on the refined atomic coordinates of the tRNAphe in the orthorhombic crystal, on the recent advances in the distance dependence of the ring-current magnetic field effects and on the adopted values for the isolated hydrogen-bonded NH resonances, a computed spectrum consisting of 23 protons was constructed. A quantitative comparison by computer was made between the computed spectrum and the spectrum simulated from the observed spectrum. These two spectra are closely similar but not identical. We suggest that the conformation of yeast tRNAphe in aqueous solution is closely similar but not identical to that found in the crystal, especially in the T psi C region and D region. Also the NH resonances in 3-4 proposed hydrogen bonds (most likely for tertiary structure) may exchange very rapidly in aqueous solution.

RNA structure

This review is concerned primarily with the physical structure and changes in the structure of RNA molecules. It will be evident that we have not attempted comprehensive coverage of what amounts to a vast literature. We have tried to stay away from particular areas that have been recently reviewed elsewhere. Citations to and information from them are included, however, so that access to the literature is available. Much of what we treat in depth deals with the crystal structures and solution behaviour of model RNA compounds, including synthetic polymers and molecular fragments such as dinucleoside phosphates. Sequence data on natural RNA are cited, but not in detail. Similarly, apart from tRNA, natural RNAs the structural determinations of which are presently not so far advanced, are not dwelt upon. We have tried to present in detail the available structural data with scaled drawings that permit facile comparisons of molecular geometries.

An NMR approach to tRNA tertiary structure in solution

Atomic coordinates of E. Coli tRNA1Val have been generated from the X-ray crystal structure of Yeast tRNAPhe by base substitution followed by idealization...

Structural domains of transfer RNA molecules

In this article, we have described various detailed features of the conformation of yeast tRNA(Phe) revealed by recent refinement analysis of x-ray diffraction data at 2.5 A resolution. The gross features of the molecule observed in the unrefined version have been largely confirmed and a number of new features found. The unique role of the ribose 2' hydroxyl groups in maintaining a series of nonhelical conformations in this RNA molecule has become apparent. Many of these features are a direct consequence of the geometry of the ribose phosphate backbone of RNA molecules, and these may also be found in structured regions of other RNA species as well. Special attention has been directed toward two conformational motifs revealed by this analysis. These include the striking similarity between the TpsiC and anticodon hairpin turns in the polynucleotide chain, which are stabilized by the participation of uridine in the U turn. In addition, there is frequent occurrence of an arch conformation in the polynucleotide chian which is stabilized by hydrogen bonds from 2' hydroxyl residues to phosphate groups across the base of the arch. The importance of the 2' hydroxyl interactions in defining tertiary structure is illustrated by the fact that, in the nonhelical regions, almost half of the ribose residues are involved in O2' hydrogen-bonding interactions which stabilize the conformation of the molecule.