Thermodynamics of unpaired terminal nucleotides on short RNA helixes correlates with stacking at helix termini in larger RNAs.

Free energies for stacking of unpaired nucleotides (dangling ends) at the termini of oligoribonucleotide Watson-Crick helixes (DeltaG(0)37,stack) depend on sequence for 3' ends but are always small for 5' ends. Here, these free energies are correlated with stacking at helix termini in a database of 34 RNA structures determined by X-ray crystallography and NMR spectroscopy. Stacking involving GA pairs is considered separately. A base is categorized as stacked by its distance from (相似文献   

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.     

Binding of complementary pentanucleotides to the anticodon loop of transfer RNA

The conformation of the anticodon loop of tRNA (yeast) was studied by detecting the most strongly binding pentanucleotide among the pentamers obtained by digestion of ribosomal RNA with T₁ RNase. This pentamer was identified as UUCAG which is complementary to the anticodon and the two pyrimidines on the 5′ side of the anticodon loop. Gel electrophoresis was used to detect binding. Control experiments employing other tRNA's showed that UUCAG formed a five base-pair complex with the tRNA. This indicates that the pentamer binds to the anticodon and the two pyrimidines to the 5′ side of it and lends support to a model for the tRNA loop which was recently proposed by Woese (1970).     

A Proposal For A Specific Double-Helical Structure In Which The Polynucleotide Strands Intercalate Instead of Forming Base-pairs

Abstract

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 3.3Å. Using these as repeat units one could generate a model for poly(dC) with parallel strands, having a turn angle of 30° and a base separation of 6.6Å 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 13.5Å, 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.     

Deciphering molecular aspects of interaction between anticancer drug mitoxantrone and tRNA

Mitoxantrone (1,4-dihydroxy-5,8-bis[[2-[(2-hydroxyethyl)amino]ethyl]amino]-9,10-anthracenedione) is a synthetically designed antineoplastic agent and structurally similar to classical anthracyclines. It is widely used as a potent chemotherapeutic component against various kinds of cancer and possesses lesser cardio-toxic effects with respect to naturally occurring anthracyclines. In the present study, we have investigated the binding features of mitoxantrone–tRNA complexation at physiological pH using attenuated total reflection-Fourier transform infrared (ATR-FTIR) spectroscopy, circular dichroism (CD) spectroscopy, isothermal titration calorimetry, and UV–visible absorption spectroscopic techniques. FTIR analysis reveals that mitoxantrone interacts mainly with heterocyclic base residues of tRNA along with slight external binding with phosphate–sugar backbone. In particular, mitoxantrone binds at uracil (C=O) and adenine (C=N) sites of biomolecule (tRNA). CD spectroscopic results suggest that there is no major conformational transition in native A-form of tRNA upon mitoxantrone–tRNA adductation except an intensification in the secondary structure of tRNA is evident. The association constant calculated for mitoxantrone–tRNA association is found to be 1.27?×?10⁵ M^?1 indicating moderate to strong binding affinity of drug with tRNA. Thermodynamically, mitoxantrone–tRNA interaction is an enthalpy-driven exothermic reaction. Investigation into drug–tRNA interaction can play an essential role in the rational development of RNA targeting chemotherapeutic agents, which also delineate the structural–functional relationship between drug and its target at molecular level.     

Specificity in DNA interactions: an nmr investigation of the interaction of propidium with oligodeoxyribonucleotides containing normal and G-T base pairs

The interaction of propidium with three self-complementary oligodeoxyribonucleotides has been investigated by ¹H- (base-pair imino proton assigned by 1D NOE and saturation transfer methods) and ³¹P-nmr as a function of ratio of propidium to oligomer (from zero to saturation) and temperature. The three oligomers are dTATATGCGCATATA (1), dTATATGTGCATATA (2), which has the same sequence as 1 except for the mismatched base pair at position 7, and dTATGTGCATA (3), which is a shortened version of 2. The imino proton chemical-shift changes of 1 on titration with propidium can be explained by the effects of the ring-current anisotropy of propidium at intercalation (3.4 Å) and next-neighbor sites (6.8 Å). The results indicate that propidium binds with neighbor exclusion but with no significant specificity for any intercalation site in the sequence of 1. The addition of propidium to 1 results in general downfield shifts of all ³¹P signals, as expected for a nonspecific intercalator. Imino and ³¹P-nmr spectra for 2 indicate that this oligomer forms a hydrogen-bonded G · T base pair at position 7 with little change in base pairing and stacking of base pairs 1–6 compared to 1. The results for addition of propidium to 2 and 3 are quite different than with 1. At low ratio only secondary shifts (6.8 Å) are seen for the G and T imino protons of base-pair 7 on addition of propidium. At higher ratios of propidium, the signals for these G and T protons are lost in 2 and severely broadened in 3, even at low temperature. The other potential intercalation sites in 2 and 3 appear to bind propidium strongly and without significant specificity as with 1. ³¹P spectra of 2 in the presence of propidium show the expected downfield shifts and broadening. Thus, the minor differences in local helix geometry in 1, and in 2 and 3, away from the G · T base pair do not significantly affect propidium intercalation specificity. Having one or two G · T base pairs at a site, however, makes intercalation in the standard manner significantly less favorable.     

The Crystal Structure of d(CCCCGGGG): A New A-Form Variant with an Extended Backbone Conformation

Abstract

The crystal structure of d(CCCCGGGG) has been determined at a resolution of 2.25Å. The oligomers crystallize as A-DNA duplexes occupying crystallographic two-fold axes. The backbone conformation is, in general, similar to that observed in previously reported crystal structures of A-DNA fragments, except for the central linkage, where it adopts an extended structure resulting from all trans conformation at the P-05′-C5′-C4′ bonds. This type of conformation facilitates interstrand stacking between the guanines at the C-G site. The local helix twist at this step is very small (25°) compared to an overall average of 33.5°. The unique structure of the C-G base-pair step, namely the extended backbone and the distinct stacking geometry, may be an important feature in the recognition mechanism between double- stranded DNA molecules and restriction endonucleases such as Msp I, which cuts the sequence CCGG very specifically with a rate unaffected by neighboring base pairs.     

Positioning of CCA-arms of the A- and the P-tRNAs towards the 28S rRNA in the human ribosome

Nucleotides of 28S rRNA involved in binding of the human 80S ribosome with acceptor ends of the A site and the P site tRNAs were determined using two complementary approaches, namely, cross-linking with application of tRNA^Asp analogues substituted with 4-thiouridine in position 75 or 76 and hydroxyl radical footprinting with the use of the full sized tRNA and the tRNA deprived of the 3′-terminal trinucleotide CCA. In general, these 28S rRNA nucleotides are located in ribosomal regions homologous to the A, P and E sites of the prokaryotic 50S subunit. However, none of the approaches used discovered interactions of the apex of the large rRNA helix 80 with the acceptor end of the P site tRNA typical with prokaryotic ribosomes. Application of the results obtained to available atomic models of 50S and 60S subunits led us to a conclusion that the A site tRNA is actually present in both A/A and A/P states and the P site tRNA in the P/P and P/E states. Thus, the present study gives a biochemical confirmation of the data on the structure and dynamics of the mammalian ribosomal pretranslocation complex obtained with application of cryo-electron microscopy and single-molecule FRET [Budkevich et al., 2011]. Moreover, in our study, particular sets of 28S rRNA nucleotides involved in oscillations of tRNAs CCA-termini between their alternative locations in the mammalian 80S ribosome are revealed.     

Knocking out a specific tRNA species within unfractionated Escherichia coli tRNA by using antisense (complementary) oligodeoxyribonucleotides

Methods for the preparation of an Escherichia coli tRNA mixture lacking one or a few specific tRNA species can be the basis for future applications of cell-free protein synthesis. We demonstrate here that virtually a single tRNA species in a crude E. coli tRNA mixture can be knocked out by an antisense (complementary) oligodeoxyribonucleotide. One out of five oligomers complementary to tRNA^Asp blocked the aspartylation almost completely, while minimally affecting the aminoacylation with other 13 amino acids tested. This `knockout' tRNA behaved similarly to the untreated tRNA in a cell-free translation of an mRNA lacking Asp codons.     

Alternative design of a tRNA core for aminoacylation

The core of Escherichia coli tRNA(Cys) is important for aminoacylation of the tRNA by cysteine-tRNA synthetase. This core differs from the common tRNA core by having a G15:G48, rather than a G15:C48 base-pair. Substitution of G15:G48 with G15:C48 decreases the catalytic efficiency of aminoacylation by two orders of magnitude. This indicates that the design of the core is not compatible with G15:C48. However, the core of E. coli tRNA(Gln), which contains G15:C48, is functional for cysteine-tRNA synthetase. Here, guided by the core of E. coli tRNA(Gln), we sought to test and identify alternative functional design of the tRNA(Cys) core that contains G15:C48. Although analysis of the crystal structure of tRNA(Cys) and tRNA(Gln) implicated long-range tertiary base-pairs above and below G15:G48 as important for a functional core, we showed that this was not the case. The replacement of tertiary interactions involving 9, 21, and 59 in tRNA(Cys) with those in tRNA(Gln) did not construct a functional core that contained G15:C48. In contrast, substitution of nucleotides in the variable loop adjacent to 48 of the 15:48 base-pair created functional cores. Modeling studies of a functional core suggests that the re-constructed core arose from enhanced stacking interactions that compensated for the disruption caused by the G15:C48 base-pair. The repacked tRNA core displayed features that were distinct from those of the wild-type and provided evidence that stacking interactions are alternative means than long-range tertiary base-pairs to a functional core for aminoacylation.     

Antisense oligonucleotides targeting universally conserved 26S rRNA domains of plant ribosomes at different steps of polypeptide elongation

A ribosome undergoes significant conformational changes during elongation of polypeptide chain that are correlated with structural changes of rRNAs. We tested nine different antisense oligodeoxynucleotides complementary to the selected, highly conserved sequences of Lupinus luteus 26S rRNA that are engaged in the interactions with tRNA molecules. The ribosomes were converted either to pre- or to posttranslocational states, with or without prehybridized oligonucleotides, using tRNA or mini-tRNA molecules. The activity of those ribosomes was tested via the so-called binding assay. We observed well-defined structural changes of ribosome's conformation during different steps of the elongation cycle of protein biosynthesis. In this article, we present that (i) before and after translocation, fragments of domain V between helices H70/H71 and H74/H89 do not have to interact with nucleotides 72-76 of the acceptor arm of A-site tRNA; (ii) helix H69 does not have to interact with DHU arm of tRNA in positions 25 and 26 after forming the peptide bond, but before translocation; (iii) helices H69 and H70 interact weakly with nucleotides 11, 12, 25, and 26 of A-site tRNA before forming a peptide bond in the ribosome; (iv) interactions between helices H80, H93 and single-stranded region between helices H92 and H93 and CCAend of P-site tRNA are necessary at all steps of elongation cycle; and (v) before and after translocation, helix H89 does not have to interact with nucleotides in positions 64-65 and 50-53 of A-site tRNA TPsiC arm.     

Active suppressor tRNAs with a double helix between the D- and T-loops

One of the most conserved elements of the tRNA structure is the reverse-Hoogsteen base-pair T54--A58 in the T-loop, which plays a major role in the maintenance of the standard L-shape conformation. Here, we present the results of in vivo selection of 51 active suppressor tRNA clones, none of which contains base-pair T54--A58. In 49 clones, we found two regions in the D and T-loops that are complementary to each other. This finding suggests the existence of an inter-loop double helix consisting of three base-pairs, which could have the same role as base-pair T54--A58 in the fixation of the juxtaposition of the two helical domains within the L-shape. From this point of view, the appearance of the inter-loop double helix represents a compensatory effect for the absence of base-pair T54--A58. The results shed new light on the role of different elements of the tRNA structure in the formation of the standard L-shape conformation and on the possibility of synonymous replacements of one arrangement by another in functional RNA molecules.     

INDEX TO SUBJECTS,Volume 2

Abstract

The effect of U(34) dethiolation on the anticodon-anticodon association between E.coli tRNA(Glu) and yeast tRNA(Phe) has been studied by the temperature jump relaxation technique. An important destabilization upon replacement of the thioketo group of s²U(34) by a keto group, was revealed by a lowering of melting temperature of about 20° C. The measured kinetic parameters indicated that this destabilization effect was originated in an increase of dissociation and a decrease of association rate constants by a factor of 4 to 5. Modifications in both stacking interactions and flexibility in the anticodon loop would be responsible for this effect.     

The structural geometry of co-ordinated base changes in transfer RNA

The tertiary structure of the central region of yeast tRNA^Phe is maintained by a trans-bonded G · C pair and by three hydrogen-bonding systems each involving three bases (“triples”). All other tRNA sequences which have four base pairs in the D stem and five nucleotides in the extra loop can conserve the triple base bonding arrangements and the trans-bonding of residues 15–48 so that the long helix formed by the TΨC and amino acid stems can be tied to the augmented D helix in the same way. The co-ordinated base changes and the alternative hydrogen-bonding schemes which make this possible are described in detail.     

Purification of a hybrid molecule composed of tyrosine transfer RNA and its complementary DNA sequence

The transducing bacteriophage φ80psu_III⁺ carries one structural Escherichia coli gene specifying tyrosine tRNA.The r strand of bacteriophage φ80psu_III⁺ was hybridized with E. coli transfer RNA and the hybrid digested with Neurospora crassa endonuclease. The analysis of the products of enzymic digestion demonstrated the release of a cistron-hybrid composed of tyrosine tRNA and its complementary DNA sequence. The cistron-hybrid was purified from unhybridized DNA by cesium sulphate density-gradient centrifugation and gel filtration.The ratio between tyrosine tRNA and its complementary DNA sequence in the final product was 1:1 as demonstrated by radioisotopic analysis. This purification represents a 30,000-fold enrichment of the E. coli genome for a specific DNA sequence.     

Thermodynamic and kinetic parameters of an oligonucleotide hairpin helix

The thermodynamics of the hairpin helix-single strand transition of A₆C₆U₆ has been analyzed by a staggering zipper model with consideration of single strand stacking. This analysis yields an enthalpy change of +11 kcal/mole for the formation of a first, isolated base pair. The stability constant of a first (intramolecular) base pair in A₆C₆U₆ is around 2 × 1O^?5 at 25°C, whereas a first (intermoleciilar) base pair in an A₆ · U₆ helix is characterised by a stability constant of about 4 × 10^?3M^?1 (25°C, extrapolated from A_n · V_n oligomer measurements). These data indicate a destabilizing effect of the C₆ loop.The rate constant of hairpin helix formation is 2 to 3 × 10⁴ sec^?1 associated with an activation enthalpy of +2.5 kcal/mote. The rate of helix dissociation of the A₆C₆U₆ hairpin is in the range of 10³ to lO⁵ sec^?1 with an activation enthalpy of 21 $\text{kcal}\text{mole}$. A comparison with the kinetic parameters obtained for A · U oligomer helices shows a specific influence of the C₆ loop due to the stacking tendency of the cytosine residues. This intluence is preferentially reflected in the relatively low value of the rate constant of helix formation.     

Laser light-scattering analysis of the dimerization of transfer ribonucleic acids with complementary anticodons

Photon-correlation spectroscopy is a powerful technique for measuring the translational diffusion coefficient of particles and macromolecules in solution. In the study described here, this technique was used to analyze a specific dimerization process involving the association of two tRNA molecules through complementary anticodons. The tRNAs used in the analysis were E. coli tRNA and yeast tRNA^Phe. The experimental data on the concentration dependence of the observed diffusion constants are shown to agree well with theoretical predictions. From these data, the equilibrium constant of the association reaction was determined for dimers formed over a wide range of temperatures and in several different solution conditions. In solutions of 0.1M ionic strength at 22°C, the equilibrium constants vary from 1 × 10⁵M^?1 in the absence of magnesium to 1.5 × 10⁶M^?1 in 10 mM Mg⁺². The enthalpy and entropy changes for dimer formation in the absence and presence, 5 and 10 mM, of magnesium have been obtained from the temperature dependence of the equilibrium constant. The results show that both ΔH and ΔS contribute to the free energy of binding and that their relative contributions are similar for each solution condition evaluated.     

Ab Initio molecular orbital study on the thermostability of the extreme thermophile tRNA: Role of the base stacking

In extremely thermophilic tRNA, ribosylthymine is replaced by 2-thioribosylthymine at the key site in tRNA. By means of the ab initio molecular orbital (MO) calculation using the 4–31G basis set, we evaluate how this replacement brings about an increment of stacking energy, and how this increment in stacking energy is responsible for the stability of the thermophile tRNA. Calculated stacking energy for G : s²T : Ψ is larger by 4·85 kJ/mol (1·16 kcal/mol) than that for G : T : Ψ. Taking account of the thermodynamical data of yeast tRNAs by Privalov & Filimonov (1978), such an increment in stacking energy seems to considerably contribute to the increase of the midpoint melting temperature (T_m) in the thermophile tRNA, although other factors such as hydrogen bonding, ribose puckering and magnesium ions can not be excluded. It is found that the dispersion force mainly contributes to the stacking energies for G : T : Ψ and G : s²T : Ψ, especially for the latter. From the decomposition of the SCF energy, electrostatic and charge transfer energies are found to contribute to the stabilization of the thermophile tRNA, though the contribution of the former is larger than the latter.