The structure of yeast tRNAAsp. A model for tRNA interacting with messenger RNA

Abstract

The anticodon of yeast tRNA^Asp, GUC, presents the peculiarity to be self-complementary, with a slight mismatch at the uridine position. In the orthorhombic crystal lattice, tRNA^Asp molecules are associated by anticodon-anticodon interactions through a two-fold symmetry axis. The anticodon triplets of symmetrically related molecules are base paired and stacked in a normal helical conformation. A stacking interaction between the anticodon loops of two two-fold related tRNA molecules also exists in the orthorhombic form of yeast tRNA^Phe. In that case however the GAA anticodon cannot be base paired. Two characteristic differences can be correlated with the anticodon-anticodon association: the distribution of temperature factors as determined from the X-ray crystallographic refinements and the interaction between T and D loops. In tRNA^Asp T and D loops present higher temperature factors than the anticodon loop, in marked contrast to the situation in tRNA^Phe. This variation is a consequence of the anticodon-anticodon base pairing which rigidities the anticodon loop and stem. A transfer of flexibility to the corner of the tRNA molecule disrupts the G19-C56 tertiary interactions. Chemical mapping of the N3 position of cytosine 56 and analysis of self-splitting patterns of tRNA^Asp substantiate such a correlation.     

Structural specificity of Rn nuclease I as probed on yeast tRNA(Phe) and tRNA(Asp).

A single-strand-specific nuclease from rye germ (Rn nuclease I) was characterized as a tool for secondary and tertiary structure investigation of RNAs. To test the procedure, yeast tRNA(Phe) and tRNA(Asp) for which the tertiary structures are known, as well as the 3'-half of tRNA(Asp) were used as substrates. In tRNA(Phe) the nuclease introduced main primary cuts at positions U33 and A35 of the anticodon loop and G18 and G19 of the D loop. No primary cuts were observed within the double stranded stems. In tRNA(Asp) the main cuts occurred at positions U33, G34, U35, C36 of the anticodon loop and G18 and C20:1 positions in the D loop. No cuts were observed in the T loop in intact tRNA(Asp) but strong primary cleavages occurred at positions psi 55, C56, A57 within that loop in the absence of the tertiary interactions between T and D loops (use of 3'-half tRNA(Asp)). These results show that Rn nuclease I is specific for exposed single-stranded regions.     

Minimal methylation of yeast messenger RNA

Most, if not all, yeast mRNAs are capped at their 5-terminus by m⁷G. Apart from m⁷G no other methylated nucleotides could be detected in poly (A)⁺ mRNA isolated from yeast polysomes.Abbreviations used poly (A)⁺ mRNA messenger RNA containing poly (A) - poly (A)^- RNA RNA lacking poly (A) - m⁷G N₇-methyl guanosine - N_m any 2-0 methylated nucleoside - mN any basemethylated nucleoside     

A model for messenger RNA sequences maximizing secondary structure due to code degeneracy.

The general occurrence of stable self-complementary mRNAs in the cells of higher organisms is assumed. As an example the amino acid sequence of human α-globin was “retranslated” into a hypothetical polynucleotide sequence, corrected as much as possible by mutant globins and completed by the chain termination variant “Constant Spring”. Under the idea of optimizing secondary structures due to code degeneracy models for α-globin mRNA with base paired regions were constructed on the basis of thermodynamic data. They were chosen by hand and by a Fortran program. Preservation of mRNA conformations is discussed as a possible function of code degeneracy during evolution.     

A model for the tertiary structure of tRNA

A model for tRNA is described which has as its basic structural mode a four stranded RNA helix, formed by pairing two stems respectively from the four ubiquitous arms of the clover-leaf secondary structure. The relation of the model to biochemical and crystallographic data on tRNA is considered.     

Calorimetric studies on melting of tRNA Phe (yeast).

The heat effects involved in thermal unfolding of tRNAPhe from yeast have been determined in various buffer systems by direct differential scanning calorimetry. Perfect reversibility of the melting process has been demonstrated for measurements in the absence of Mg2+ ions. The overall molar transition enthalpy, delta Ht = 298 +/- 15 kcal mol-1 (1247 +/- 63 kJ mol-1), has been shown to be independent of the NaCl concentration and the nature of the buffers used in this study. Delta Ht is identical in the presence and in the absence of Mg2+ ions within the margin of experimental error. This experimental result implies a vanishing or very small heat capacity change to be associated with melting. Decomposition of the calorimetrically determined complex transition curves, on the assumption that the experimental melting profile represents the sum of independent two-state transitions, results in five transitions which have been assigned to melting of different structural domains of the tRNA.     

Yeast aspartyl-tRNA synthetase residues interacting with tRNA(Asp) identity bases connectively contribute to tRNA(Asp) binding in the ground and transition-state complex and discriminate against non-cognate tRNAs.

Crystallographic studies of the aspartyl-tRNA synthetase-tRNA(Asp)complex from yeast identified on the enzyme a number of residues potentially able to interact with tRNA(Asp). Alanine replacement of these residues (thought to disrupt the interactions) was used in the present study to evaluate their importance in tRNA(Asp)recognition and acylation. The results showed that contacts with the acceptor A of tRNA(Asp)by amino acid residues interacting through their side-chain occur only in the acylation transition state, whereas those located near the G73 discriminator base occur also during initial binding of tRNA(Asp). Interactions with the anticodon bases provide the largest free energy contribution to stability of the enzyme-tRNA complex in its ground state. These contacts also favour catalysis, by acting connectively with each other and with those of G73, as shown by multiple mutant analysis. This implies structural communication transmitting the anticodon recognition signal to the distally located acylation site. This signal might be conveyed via tRNA(Asp)as suggested by the observed conformational change of this molecule upon interaction with AspRS. From binding free energy values corresponding to the different AspRS-tRNA(Asp)interaction domains, it might be concluded that upon complex formation, the anticodon interacts first. Finally, acylation efficiencies of AspRS mutants in the presence of pure tRNA(Asp)and non-fractionated tRNAs indicate that residues involved in the binding of identity bases also discriminate against non-cognate tRNAs.     

The primary structure of yeast mitochondrial tyrosine tRNA

The mitochondrial tyrosine tRNA from Saccharomyces cerevisiae has been sequenced. It has two interesting structural features: (i) it lacks two semi-invariant purine residues in the D-loop which are involved in tertiary interactions in the yeast cytoplasmic tRNAPhe; (ii) it has a large variable loop and therefore resembles procaryotic tRNAsTyr rather than eucaryotic cytoplasmic ones.     

An ultraviolet light-induced crosslink in yeast tRNA(Phe).

The irradiation of native or unmodified yeast tRNA(Phe) by short wavelength UV light (260 nM) results in an intramolecular crosslink that has been mapped to occur between C48 in the variable loop and U59 in the T loop. Photo-reversibility of the crosslink and the absence of fluorescent photo adducts suggest that the crosslink product is a cytidine-uridine cyclobutane dimer. This is consistent with the relative geometries of C48 and U59 in the crystal structure of yeast tRNA(Phe). Evaluation of the crosslinking efficiency of the mutants of tRNA(Phe) indicates that the reaction depends on the correct tertiary structure of the RNA.     

Yeast tRNA(Asp)-aspartyl-tRNA synthetase complex: low resolution crystal structure

Yeast aspartyl-tRNA synthetase, a dimer of molecular weight 125,000, and two molecules of its cognate tRNA (Mr = 24160) cocrystallize in the cubic space group I432 (a = 354 A). The crystal structure was solved to low resolution using neutron and X-ray diffraction data. Neutron single crystal diffraction data were collected in five solvents differing by their D2O content in order to use the contrast variation method to distinguish between the protein and tRNA. The synthetase was first located at 40 A resolution using the 65% D2O neutron data (tRNA matched) tRNA molecules were found at 20 A resolution using both neutron and X-ray data. The resulting model was refined against 10 A resolution X-ray data, using density modification and least-squares refinement of the tRNA positions. The crystal structure solved without a priori phase knowledge, was confirmed later by isomorphous replacement. The molecular model of the complex is in good agreement with results obtained in solution by probing the protected part of the tRNA by chemical reagents.     

Recognition of acceptor-stem structure of tRNA(Asp) by Escherichia coli aspartyl-tRNA synthetase

Protein-RNA recognition between aminoacyl-tRNA synthetases and tRNA is highly specific and essential for cell viability. We investigated the structure-function relationships involved in the interaction of the Escherichia coli tRNA(Asp) acceptor stem with aspartyl-tRNA synthetase. The goal was to isolate functionally active mutants and interpret them in terms of the crystal structure of the synthetase-tRNA(Asp) complex. Mutants were derived from Saccharomyces cerevisiae tRNA(Asp), which is inactive with E. coli aspartyl-tRNA synthetase, allowing a genetic selection of active tRNAs in a tRNA(Asp) knockout strain of E. coli. The mutants were obtained by directed mutagenesis or library selections that targeted the acceptor stem of the yeast tRNA(Asp) gene. The mutants provide a rich source of tRNA(Asp) sequences, which show that the sequence of the acceptor stem can be extensively altered while allowing the tRNA to retain substantial aminoacylation and cell-growth functions. The predominance of tRNA backbone-mediated interactions observed between the synthetase and the acceptor stem of the tRNA in the crystal and the mutability of the acceptor stem suggest that many of the corresponding wild-type bases are replaceable by alternative sequences, so long as they preserve the initial backbone structure of the tRNA. Backbone interactions emerge as an important functional component of the tRNA-synthetase interaction.     

The crystal structure of d(G-G-G-G-C-C-C-C). A model for poly(dG).poly(dC)

The structure of the DNA oligomer d(G-G-G-G-C-C-C-C) has been determined at a resolution of 2.5 A by single-crystal X-ray methods. There are two strands in the asymmetric unit, and these coil about each other to form a right-handed double-helix of the A-type with Watson-Crick hydrogen bonds between base-pairs. The helix has a shallow minor groove and a deep, water-filled major groove; almost all exposed functional groups on the DNA are hydrated, and 106 ordered solvent molecules have been found. The two d(G-G-G-G).d(C-C-C-C) segments in the octamer exhibit similar and uniform structures, but there is a slight discontinuity at the GpC step between them. A recurring feature of the structure is the overlap of adjacent guanine bases in each GpG step, with the five-membered ring of one guanine stacking on the six-membered ring of its neighbour. There is little or no overlap between adjacent cytosine rings. Conformational parameters for these GpG steps are compared with those from other single-crystal X-ray analyses. In general, GpG steps exhibit high slide, low roll and variable twist. Models for poly(dG).poly(dC) were generated by applying a simple rotation and translation to each of the unmodified d(G-G-G-G).d(C-C-C-C) units. Detailed features of these models are shown to be compatible with various assays of poly(dG).poly(dC) in solution, and are useful in understanding the polymorphic behaviour of this sequence under a variety of experimental conditions.     

The structure of pre-messenger RNA and messenger RNA from erythroid cells

Pre-mRNA fractions (greater than 45 S) were characterized by electron microscopy. High salt concentrations (0.2 M ammonium acetate, pH 8) yield linear molecules of different length (0.5--17 micrometer). In 10% of the molecules a compact-nonlinear contour (cn-contour) is detectable at one end. A significant enhancement of the number of cn-contour carrying molecules is observed after binding pre-mRNA to poly(U)-sepharose. The terminal cn-contour could be the depiction of a secondary and/or tertiary structure including the poly(A)-tail. 9 S globin mRNA appear in 80% with virtually the same cn-contour as detected in pre-mRNA molecules. After denaturing the mRNA in 80% formamide--4M urea in connection with heating to 90 degrees C from 10 min, a percentage of 77% of stretched, linear molecules results. This structural transformation is reversible when the denatured RNA is precipitated and redissolved in 0.2 M ammonium acetate. 73% of the stretched molecules are characterized by a mean length of 0.44 micrometer. This value is twice as high as commonly assumed for a globin mRNA chain.     

A nature of conformational changes of yeast tRNA(Phe). High hydrostatic pressure effects

We analysed conformational changes of yeast tRNA(Phe) induced by high hydrostatic pressure (HHP) measured by Fourier-transform infrared (FTIR) and fluorescence spectroscopies. High pressure influences RNA conformation without other cofactors, such as metal ions and salts. FTIR spectra of yeast tRNA(Phe) recorded at high hydrostatic pressure up to 13 kbar with and without magnesium ions showed a shift of the bands towards higher frequencies. That blue shift is due to an increase a higher energy of bonds as a result of shortening of hydrogen bonds followed by dehydration of tRNA. The fluorescence spectra of Y-base tRNA(Phe) at high pressure up to 3 kbar showed a decrease of the intensity band at 430 nm as a consequence of conformational rearrangement of the anticodon loop leading to exposure of Y-base side chain to the solution. We suggest that structural transition of nucleic acids is driven by the changes of water structure from tetrahedral to a cubic-like geometry induced by high pressure and, in consequence, due to economy of hydration.