Conformations et spectre Raman de l'acide ribonucléique de transfert, tRNA

The structure of yeast tRNA^Asp in aqueous solution has been studied in sight of Raman spectra recorded between 5 and 82°C. A conformational change is evidenced at 20°C and an endomelting is found around 70°C. This melting temperature, much higher than in tRNA-^Phe (near 50°C) is interpreted by the presence of a higher number of G-C bases in tRNA^Asp.At a same temperature, the Raman spectrum of a tRNA^Asp crystal is quasi-identical than that of an aqueous solution, indicating a high structural similarity except bands corresponding to G,C bases which show a more effective stacking of these bases in the solid.     

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.     

Crystallographic refinement of yeast aspartic acid transfer RNA

The structure of yeast transfer RNA aspartic acid has been refined in one crystal form to 3 Å resolution using the restrained least-squares method of Hendrickson and Konnert and real-space fitting using the FRODO program of Jones. The final Crystallographic discrepancy index R is 23.5% for 4585 reflections with magnitudes twice their standard deviations between 10 and 3 Å. With lower occupancies for some residues of the D-loop, the phosphate U1, and the base U33, the R-factor is 22.3%. The adaptation of the restrained least-squares program for nucleic acids and the progress of the refinement are described. The conformations are analysed with respect to stereochemistry and folding of the backbone. The contacts and hydrogen bonds of the secondary structure are compared with those of yeast tRNA^Phe. The presence of only four bases in the variable loop, instead of five as in yeast tRNA^Phe, leads to a rotation of residue 48 and a lateral movement of residue 46. These two rearrangements induce different environments for [U8 … A14] … A21 as well as for A9 and G45. Otherwise, all tertiary contacts observed in yeast tRNA^Phe are present in yeast tRNA^Asp, except for the absence of hydrogen-bonding between G18 of the D-loop and C56 of the T-loop. The presence of anticodon triplet pairing leads to a distribution of temperature factors different from that observed in yeast tRNA^Phe with a stabilization of the AC stem-and-loop and a destabilization of the T and D-loops. We are inclined to suggest that the labilization of the interactions between the T and D-loops is a consequence of the interaction of the anticodon triplets of symmetry-related molecules through hydrogen bonding, which mimics the interaction between the anticodon and its cognate codon on the messenger RNA.     

Calorimetric investigations of the helix-coil conversion of phenylalaninespecific transfer ribonucleic acid

The enthalpy of the helix-coil conversion of phenylalaninespecific transfer ribonucleic acid from brewer's yeast (tRNA^Phe_{brewer's yeast}) has been measured using both an LKB 10700-2 batch miciocalorimeter and an adiabatic differential scanning calorimeter. In the mixing calorimeter the conversion from coil to helix was induced by mixing a tRNA^Phe solution with a solution containing an excess of MgSO₄. We measured the enthalpy of this reaction stepwise in the temperature range from +9 to +60° C. For the enthalpy of folding of tRNA^Phe from coil to helix this method yielded the remarkably high value of ?310 $\text{kcal}\text{mole}$ of tRNA^Phe. With the differential scanning calorimeter in which the helix-coil conversion is simply induced by raising the temperature we found a value of +240 $\text{kcal}\text{mole}$ of tRNA^Phe at a Tm value of 76° C and a value of +200 $\text{kcal}\text{mole}$ of tRNA^Phe at a T_m value of 50° C. A comparison of the apparent van't Hoff enthalpies with the calorimetrically measured enthalpies shows, that the cooperativity of the system increases continually with rising melting temperatures - which are achieved by increasing Mg²⁺ concentrations - reaching a constant value at about 57° C. Above this temperature value the thermodynamic behaviour of the helix-coil conversion of tRNA^Phe may be approximately described by the model of an all-or-none process.     

Isolation and chromatographic behaviour of phenylalanine tRNA from barley embryos

Two fractions of phenylalanine tRNA (tRNA^Phe₁ and tRNA^Phe₂) were purified by BD-cellulose and RPC-5 chromatography of crude tRNA isolated from barley embryos. Successive RPC-5 rechromatography runs of tRNA^Phe₂ showed its conversion into more stable tRNA^Phe₁, suggesting that the two fractions have essentially the same primary structure. Both tRNA^Phe₁ and tRNA^Phe₂ had about the same acceptor activity, but tRNA^Phe₂ was aminoacylated much faster than tRNA^Phe₁. RPC-5 chromatography of crude aminoacylated tRNA showed higher contents of phe-tRNA^Phe₂ than of phe-tRNA^Phe₁ but the ratio of these two fractions estimated by relative fluorescence intensity was about 1. Fluorescence spectra of tRNA^Phe from barley embryos suggest that it contains Y base similar to Y_w from wheat tRNA^Phe.     

Study of the phosphorescent bases of yeast phenylalanine transfer RNA with the aid of optical detection of magnetic resonance

The phosphorescence of brewers' yeast phenylalanine transfer RNA has been investigated at 77 °K and at 1.2 °K in pumped liquid helium. Although the phosphorescence at 77 °K originates almost completely from the Y base in the anticodon loop, independent of excitation wavelength, the phosphorescence originates from normal bases with 270 nm excitation at temperatures in the helium range. The low-temperature phosphorescence is assigned to the triplet state of adenosine by optical detection of magnetic resonance measurements. The adenosine phosphorescence at 1.2 °K is quenched by the binding of the codon poly(U), as well as by the removal of Mg²⁺. The former result indicates that the adenosine phosphorescence originates from the anticodon, -Gm-A-A-, while the second shows that a conformational change introduced by removing Mg²⁺ (possibly involving unstacking of the anticodon) prevents energy trapping in the anticodon triplet state. The lack of triplet energy transfer from anticodon to Y indicates that Y cannot be stacked with the anticodon in the conformation that is stable at helium temperature. The adenosine phosphorescence of transfer RNA^Phe is nearly completely quenched at 77 °K, at least partially due to energy transfer to Y. We think that the thermally activated energy transfer is associated with some mobility of the Y base at 77 °K. Our observations are in contrast with previous results on bakers' yeast tRNA^Phe where there is apparently little, if any, energy transfer to Y from the normal nucleotides at 80 °K with 265 nm excitation. Optically detected magnetic resonance measurements on the triplet state of Y base in various environments indicate that removal of Mg²⁺ causes a shift of the Y base in tRNA^Phe to a more solvent-exposed position, whereas the binding of poly(U) has little effect on the environment of Y.     

Thermodynamics of transfer ribonucleic acids: the effect of sodium on the thermal unfolding of yeast tRNAPhe.

The thermal unfolding of yeast phenylalanine-specific tRNA (tRNA^Phe) has been calorimetrically investigated at several salt concentrations in the absence of magnesium. Application of the deconvolution theory of macromolecular conformational transitions allows calculation of the thermodynamic parameters of unfolding. It is demonstrated that the unfolding of tRNA^Phe occurs in a sequential fashion and that four separate transitions or five macromolecular thermodynamic states exist in the temperature range 8–72°C under the experimental conditions of these studies (0.067–0.52M Na⁺). The enthalpy and entropy changes between states and the relative population of each state as a function of temperature and salt concentration have been obtained. Sodium stabilizes the low-temperature conformations of tRNA^Phe. The increase in the melting temperatures of each transition is shown to be linearly dependent on the logarithm of sodium concentration. These results allow calculation of the “phase” diagram for the transitions as a function of salt concentration.     

Conformational Change of the L-Shaped tRNAPhe Molecule

Abstract

Fluorophore of proflavine was introduced onto the 3′-terminal ribose moiety of yeast tRNA^Phe. The distance between the fluorophore and the fluorescent Y base in the anticodon of yeast tRNA^Phe was measured by a singlet-singlet energy transfer. Conformational changes of tRNA^Phe with binding of tRNA^Glu ₂, which has the anticodon UUC complementary to the anticodon GAA of tRNA^Phe, were investigated. The distance obtained at the ionic strength of 100 mM K⁺ and 10 mM Mg²⁺ is very close to the distance from x-ray diffraction, while the distance obtained in the presence of tRNA^Glu ₂ is significantly smaller. Further, using a fluorescent probe of 4-bromomethl-7-methoxycoumarin introduced onto pseudouridine residue Ψ₅₅ in the TΨC loop of tRNA^Phe, Stern-Volmer quenching experiments for the probe with or without added tRNA^Glu ₂were carried out. The results showed greater access of the probe to the quencher with added tRNA^Glu ₂. These results suggest that both arms of the L-shaped tRNA structure tend to bend inside with binding of tRNA^Glu ₂ and some structural collapse occurs at the corner of the L-shaped structure.     

High resolution NMR study of the melting of yeast tRNA Phe

The 300 MHz NMR spectra of the hydrogen bonded NH ring protons of tRNA_Yeast^Phe have been measured as a function of temperature. In the presence of Mg⁺⁺ two resonances, one from the Aψ base pair and the other probably from the neighboring base pair, disappear between 56 and 58°C. In the absence of Mg⁺⁺ the DHU stem, the acceptor stem (in particular its AU base pair #6 and #7) and the Aψ base pair in the anticodon stem melt slightly earlier than the other parts of the molecule. Since the DHU stems in tRNA_Yeast^Phe and tRNA_Coli^fMet have the same base pairing scheme it is interesting that their melting behavior is entirely different in both molecules. This is discussed in terms of the tertiary structure.     

Nuclear and mitochondrial revertants of a yeast mitochondrial tRNA mutant

Summary We isolated revertants capable of respiration from the respiratory deficient yeast mutant, FF1210-6C/ 170, which displays greatly decreased mitochondrial protein synthesis due to a single base substitution at the penultimate base of the tRNA^Asp gene on mitochondrial (mt) DNA. Three classical types of revertant were identified: (1) same-site revertants; (2) intragenic revertants which restore the base pairing in the acceptor stem of the mitochondrial tRNA^Asp; and (3) extragenic suppressors located in nuclear DNA. In addition a fourth type of revertant was identified in which the mutant tRNA^Asp is amplified due to the maintenance of both the original mutant mtDNA and a modified form of the mutant mtDNA in which only a small region around the tRNA^Asp gene is retained and amplified. The latter form resembles the mtDNA in vegetative petite (rho ^-) strains which normally segregates rapidly from the wild-type mtDNA. Each revertant type was characterized genetically and by both DNA sequence analysis of the mitochondrial tRNA^Asp gene and analysis of the quantity and size of RNA containing the tRNA^Asp sequence. These results indicate that the mitochondrial tRNA^Asp of the mutant retains a low level of activity and that the presence of the terminal base pair in tRNA^Asp is a determinant of both tRNA^Asp function and the maintenance of wild-type levels of tRNA^Asp.     

An energy transfer equilibrium between two identical copies of a ribosome-bound fluorescent transfer RNA analogue: implications for the possible structure of codon-anticodon complexes.

When yeast tRNA_Pf^Phe, a derivative of tRNA^Phe in which proflavine replaces the Y base, is bound simultaneously to both the peptidyl and aminoacyl sites of a 70 S Escherichia coli ribosome, there is a rapid mutual energy transfer between the two bound tRNAs. Analysis of this energy transfer yields an upper limit for the proflavine-proflavine distance of 20 Å. It also allows an unequivocal measurement of the emission spectrum of tRNA_Pf^Phe bound at the aminoacyl site. In the presence of message this spectrum is very different from that seen in the peptidyl site, implying that in the two sites the hypermodified bases exist in significantly different environments. The rapid energy transfer leads to some loss of fluorescence anisotropy. This can be analyzed to obtain an estimate of the angle between the two proflavines: 28 ° ± 10 ° or 152 ° ± 10 °. Taken together all of these results place severe constraints on possible models of codon-anticodon complexes. The mutual energy transfer seen and analyzed on the ribosome is a convenient aspect of fluorescence spectroscopy, and it is one that should see broad application where multiple copies of a fluorescent ligand interact on a macromolecular substrate.     

Age-dependent changes in the specificity of tRNA methyltransferases in the cerebellum of the icteric and nonicteric Gunn rat

The activity of tRNA methyltransferases present in the cerebellum of 6- and 21-day-old nonicteric and icteric Gunn rats was compared using purifiedE. coli tRNAs as substrates. At 6 days the tRNA methyltransferases of the icteric animals were significantly more effective in methylating tRNA^Glu ₂ and tRNA^Phe than were those of their nonicteric counterparts. This relationship reversed itself at 21 days. The action of the tRNA methyltransferases from the 6-day-old icteric animals led to higher proportions of 1-methyladenine in tRNA^Glu ₂ and tRNA^Phe than were obtained using the corresponding enzymes of the nonicteric animals. The proportion ofN ²-methylguanine was also higher, yet only in tRNA^fMet and not in tRNA^Phe. The study reveals much more extensive fluctuations in the activity and in the substrate recognition specificity among the cerebellar tRNA methyltransferases of the icteric than among those of the nonicteric controls during the crucial 6–21 day period of cerebellar development.     

Internal Motions of Transfer RNA: A Study of Exchanging Protons by Magnetic Resonance36

Abstract

Proton exchange is a probe of macromolecular structure and kinetics. Its value is enhanced when the exchanging protons can be identified by nmr.

After dilution of tRNA-H₂O samples in D₂O, slowly exchanging imino protons are observed, with exchange times ranging from minutes to days. In many cases they originate from the dihydro-uracil region.

Most slow exchangers are sensitive to buffer catalysis. Extrapolation to infinite buffer concentration yields the life-time of the closed form, in a two-state model of each base-pair. As predicted by the model, the lifetime obtained by extrapolation is independent of the buffer. Typical lifetimes are 14 minutes for CGI 1 of yeast tRNA^Phe at 17°C, or 5 minutes for U8-A14 of yeast tRNA^Asp at 20°C, without magnesium. For most slow exchangers, magnesium increases the lifetime of the closed form, but moderately, by factors never more than five.

The exchange rates of other,fast-exchanging, imino protons, as determined by line-broadening, are found to depend on buffer concentration. Base-pair lifetimes are determined as above. For instance UA6 of yeast tRNA^Phe has a lifetime of 14 ms at 17°C. Base-pairs 4 and 6 have shorter lifetimes than the rest of the acceptor stem.

Imidazole is a good catalyst for proton exchange of both the long-and the short-lived base-pairs, whereas phosphate is not. Tris is efficient except for cases where, possibly, access is impeded by its size; magnesium reduces the efficiency of catalysis by tris buffer.

From the variation of exchange time vs buffer concentration, one determines the buffer concentration for which the exchange rate from the open state is equal to the closing rate. Remarquably, this concentration takes comparable values for most base-pairs, whether shortlived or long-lived.

Buffer effects have also been observed in poly(rA)-poly(rU), for which we derive a lifetime of 2.5 ms at 27°C, and in other polynucleotides. Some of the exchange times identified in the literature as base-pair lifetimes may instead reflect incomplete catalysis.     

Assignment of the low field proton nuclear magnetic resonance spectrum of yeast phenylalanine transfer RNA to specific base pairs

High-resolution proton nuclear magnetic resonance spectra at 220 and 300 MHz have been used to investigate the base-pairing structure of fragments of yeast tRNA^Phe, of chemically modified tRNA^Phe and of intact tRNA^Phe. To a very good approximation the positions of the fragment spectra are additive within 0·2 part per million, indicating that factors responsible for certain structural features in the intact molecule are already present in the smaller fragments (half molecules, hairpins and $\text{3}\text{4}$ molecules). A simple first-order ring-current shift theory taken in conjunction with the cloverleaf model for tRNA^Phe (RajBhandary et al., 1967) has been used to predict the low-field (? 15 to ?11 part per million) nuclear magnetic resonance spectra and make assignments of the resolved resonances to ring NH protons of specific base pairs. The general agreement between the predicted and observed spectra to within 0·2 part per million confirms in detail the cloverleaf model for the secondary structure of tRNA^Phe in solution. It is also established that ring-current shifts are the principal factor responsible for the wide range of shifts observed in the low-field spectra. As a result it is evident that the resonances are very sensitive to small changes in the secondary structure and in some cases changes in the interbase distance as small as 0·2 Å could easily be detected. It is also clear from the analysis that certain of the resonances are sensitive to the tertiary structure of the molecule and specific examples are discussed. As with our previous study, we find no evidence for any strong Watson-Crick type base pairs beyond those predicted by the cloverleaf structure.     

The Effect of Modification of Nucleotide-37 on the Interaction of Aminoacyl-tRNA with the A Site of the 70S Ribosome

To estimate the effect of modified nucleotide 37, the interaction of two yeast aminoacyl-tRNAs (Phe-tRNA^Phe _+Y and Phe-tRNA^Phe _–Y) with the A site of complex [70S · poly(U) · deacylated tRNA^Phe in the P site] was assayed at 0–20°C. As comparisons with native Phe-tRNA^Phe _+Y showed, removal of the Y base decreased the association constant of Phe-tRNA^Phe _–Y and the complex by an order of magnitude at every temperature tested, and increased the enthalpy of their interaction by 23 kJ/mol. When the Y base was present in the anticodon loop of deacylated tRNA^Phe bound to the P site of the 70S ribosome, twice higher affinity for the A site was observed for Phe-tRNA^Phe _–Y but not for Phe-tRNA^Phe _+Y. Thus, the modified nucleotide 3" of the Phe-tRNA^Phe anticodon stabilized the codon–anticodon interaction both in the A and P sites of the 70S ribosome.     

Crystal structure of human mitochondrial PheRS complexed with tRNA(Phe) in the active "open" state

Monomeric human mitochondrial phenylalanyl-tRNA synthetase (PheRS), or hmPheRS, is the smallest known enzyme exhibiting aminoacylation activity. HmPheRS consists of only two structural domains and differs markedly from heterodimeric eukaryotic cytosolic and bacterial analogs both in the domain organization and in the mode of tRNA binding. Here, we describe the first crystal structure of mitochondrial aminoacyl-tRNA synthetase (aaRS) complexed with tRNA at a resolution of 3.0 Å. Unlike bacterial PheRSs, the hmPheRS recognizes C74, the G1–C72 base pair, and the “discriminator” base A73, proposed to contribute to tRNA^Phe identity in the yeast mitochondrial enzyme. An interaction of the tRNA acceptor stem with the signature motif 2 residues of hmPheRS is of critical importance for the stabilization of the CCA-extended conformation and its correct placement in the synthetic site of the enzyme. The crystal structure of hmPheRS–tRNA^Phe provides direct evidence that the formation of the complex with tRNA requires a significant rearrangement of the anticodon-binding domain from the “closed” to the productive “open” state. Global repositioning of the domain is tRNA modulated and governed by long-range electrostatic interactions.     

The distance between the anticodon loops of two tRNAs bound to the 70 S Escherichia coli ribosome.

Using singlet-singlet energy transfer, we have measured the distance between the anticodons of two transfer RNAs simultaneously bound to a messengerprogramed Escherichia coli 70 S ribosome. The fluorescent Y base adjacent to the anticodon of yeast tRNA_Y^Phe serves as a donor. A proflavine (Pf) chemically substituted for the Y base in tRNA_Pf^Phe serves as an acceptor. By exploiting the sequential binding properties of 70 S ribosomes for two deacylated tRNAs, we can fill the strong site with either tRNA_Y^Phe or tRNA_Pf^Phe and then the weak site with the other tRNA. In both cases donor quenching and sensitized emission of the acceptor are observed. Analysis of these results leads to an estimate for the Y-proflavine distance of 18 ± 2 Å. This distance is very short and suggests strongly that the two tRNAs are simultaneously in contact with adjacent codons of the message. Separate experiments show that binding of a tRNA to the weak site does not perturb the environment of the hypermodified base of a tRNA bound to the strong site. This supports the assignment of the strong site as the peptidyl site. It also indicates that binding of the second tRNA proceeds without a change in the anticodon structure of a pre-existing tRNA at the peptidyl site.