The structure of triple helical poly(U).poly(A).poly(U) studied by Raman spectroscopy

Using Raman spectroscopy, we examined the ribose-phosphate backbone conformation, the hydrogen bonding interactions, and the stacking of the bases of the poly(U).poly(A).poly(U) triple helix. We compared the Raman spectra of poly(U).poly(A).poly(U) in H2O and D2O with those obtained for single-stranded poly(A) and poly(U) and for double-stranded poly(A).poly(U). The presence of a Raman band at 863 cm-1 indicated that the backbone conformations of the two poly(U) chains are different in the triple helix. The sugar conformation of the poly(U) chain held to the poly(A) by Watson-Crick base pairing is C3' endo; that of the second poly(U) chain may be C2' endo. Raman hypochromism of the bands associated with base vibrations demonstrated that uracil residues stack to the same extent in double helical poly(A).poly(U) and in the triple-stranded structure. An increase in the Raman hypochromism of the bands associated with adenine bases indicated that the stacking of adenine residues is greater in the triple helix than in the double helical form. Our data further suggest that the environment of the carbonyls of the uracil residues is different for the different strands.     

The Study of Possible A and B Conformations of Alternating DNA Using a New Program for Conformational Analysis of Duplexes (CONAN)

Abstract

A new program, CONAN has been designed for CONformational ANalysis of oligonucleotide duplexes with natural and modified bases. It allows to model both regular DNA fragments with different types of symmetry and irregular ones including bends, junctions, mismatched pairs and base lesions. Computations and minimization of the energy are performed in a space of internal structural variables chosen to build start structure easier and conveniently analyze the results obtained. These internal structural variables determine mutual base-base and base-sugar arrangement and sugar puckering. The analytical closure procedure is applied both to sugar rings and to backbone fragments between adjacent sugars. For more effective energy minimization, analytical gradient is calculated. The CONAN was applied to the search for low-energy conformations of poly(dA-dT)·poly(dA-dT) and poly(dG-dC)·poly(dG-dC) duplexes. Extended regions of low-energy A and B conformations are revealed and characterized. These regions contain structures with different relative values of helical twist, τ, for pur-pyr and pyr-pur steps, namely, conformations with τ(pur-pyr)>τ(pyr-pur) and with τ(pur-pyr)<τ(pyr-pur). Two types of sugar puckering were found for B-form low-energy conformations, the first type with all C2′-endo sugar residues and the second one—;with C2′-endo purines and O1′-endo pyrimidines. The calculated conformations are compared with X-ray diffraction data for crystals and fibers and NMR data for solution.     

Structural studies of O6-methyldeoxyguanosine and related compounds: a promutagenic DNA lesion by methylating carcinogens.

O6-Methylation of guanine residues in DNA can induce mutations by formation of base mispairing due to the deprotonation of N(1). The electronic, geometric and conformational properties of three N(9)-Substituted O6-methylguanine derivatives, O6-methyldeoxyguanosine (O6mdGuo), O6-methylguanosine (O6mGuo) and O6, 9-dimethylguanine (O6mdGua), were investigated by X-ray and/or NMR studies. O6mdGuo crystallizes in the monoclinic space group P2(1) with cell parameters a = 5.267(1), b = 19.109(2), c = 12.330(2) A, beta = 92.45(1) degrees, V = 1239.8(3) A3, z = 4 (two nucleosides per asymmetric unit), and O6mGua in the monoclinic space group P2(1)/n with cell parameters a = 10.729(2), b = 7.640(1) c = 10.216(1) A, beta = 92.17(2) degrees, V = 836.7(2) A3, z = 4. The geometry and conformation of O6-methylguanine moieties observed in both crystals and are very similar. Furthermore, the molecular dimensions of the O6methylguanine residue resemble more closely those of adenine than those of guanine. The methoxy group is coplanar with the purine ring, the methyl group being cis to N(1). The conformation of O6-methylguanine nucleosides is variable. The glycosidic conformation of O6mdGuo is anti for molecule (a) and high-anti for molecule (b) in the crystal, while that of O6mGuo is syn [Parthasarathy, R & Fridey, S. M. (1986) Carcinogenesis 7, 221-227]. The sugar ring pucker of O6mdGuo is C(2')-endo for molecule (a) and C(1')-exo for molecule (b). The C(4')-C(5') exocyclic bond conformation in O6mdGuo is gauche- for molecule (a) but trans for molecule (b), in contrast with gauche+ for O6mGuo. The hydrogen bonds exhibited by O6-methylguanine derivatives differ from those in guanine derivatives; the amino N(2) and ring N(3) and N(7) atoms of O6-methylguanine residues are involved in hydrogen bonding. 1H-NMR data for O6mdGuo and O6mdGuo reveal the predominance of a C(2')-endo type sugar puckering. In O6mdGuo, however, a contribution of a C(1')-exo sugar puckering is significant. The NOE data also indicate that O6mdGuo molecules exist with nearly equal population for anti (including high anti) and syn glycosidic conformations. These observations and their biological implications are discussed.     

The crystal and molecular structure of 2'-deoxy-2'-fluoroinosine monohydrate.

The structure of the hydrate of 2'-deoxy-2'-fluoroinosine has been determined by single-crystal x-ray diffraction. The nucleoside crystallizes in space group P2(1)2(1)2(1) with unit cell dimensions, a = 33.291, b = 10. 871, c = 6.897A. There are two nucleosides and two water molecules in the asymmetric unit. The structure was solved by direct methods and refined to a residual R = 0.095. The two independent nucleosides in the asymmetric unit show different conformations about the glycosidic bond, while other structural details are similar. The base orientation to the sugar is syn in molecule A, whereas anti in molecule B. The exocyclic C(4')-C(5') bond conformation defined with respect to C(3')-C(4')-C(5')-O(5') is gauche+ in both molecules A and B. The sugar ring pucker defined by the pseudorotation phase angle P is a twisted conformation in both, C(3')-endo-C(4')-exo with P = 29 degrees in molecule A and C(4')-exo-C(3')-endo with P = 41 degrees in molecule B. It is shown by comparison with x-ray results of other 2'-fluoronucleosides and unmodified nucleosides including inosines that, in addition to a strong preference of the C(3')-endo type pucker, twisted conformations involving C(4')-exo puckering may be one of characteristic features of 2'-fluoronucleosides.     

Temperature dependence of the Raman spectrum of DNA. II. Raman signatures of premelting and melting transitions of poly(dA).poly(dT) and comparison with poly(dA-dT).poly(dA-dT).

The temperature dependence of the Raman spectrum of poly(dA).poly(dT) (dA: deoxyadenosine; dT: thymidine), a model for DNA containing consecutive adenine.thymine (A.T) pairs, has been analyzed using a spectrometer of high spectral precision and sensitivity. Three temperature intervals are distinguished: (a) premelting (10 < t < 70 degrees C), in which the native double helix is structurally altered but not dissociated into single strands; (b) melting (70 < t < 80 degrees C), in which the duplex is dissociated into single strands; and (c) postmelting (80 < t degrees C), in which no significant structural change can be detected. The distinctive Raman difference signatures observed between 10 and 70 degrees C and between 70 and 80 degrees C are interpreted in terms of the structural changes specific to premelting and melting transitions, respectively. Premelting alters the low-temperature conformation of the deoxyribose-phosphate backbone and eliminates base hydrogen bonding that is distinct from canonical Watson-Crick hydrogen bonding; these premelting perturbations occur without disruption of base stacking. Conversely, melting eliminates canonical Watson-Crick pairing and base stacking. The results are compared with those reported previously on poly(dA-dT).poly(dA-dT), the DNA structure consisting of alternating A.T and T.A pairs (L. Movileanu, J. M. Benevides, and G. J. Thomas, Jr. Journal of Raman Spectroscopy, 1999, Vol. 30, pp. 637-649). Poly(dA).poly(dT) and poly(dA-dT).poly(dA-dT) exhibit strikingly dissimilar temperature-dependent Raman profiles prior to the onset of melting. However, the two duplexes exhibit very similar melting transitions, including the same Raman indicators of ruptured Watson-Crick pairing, base unstacking and collapse of backbone order. A detailed analysis of the data provides a comprehensive Raman assignment scheme for adenosine and thymidine residues of B-DNA, delineates Raman markers diagnostic of consecutive A.T and alternating A.T/T.A tracts of DNA, and identifies the distinct Raman difference signatures for premelting and melting transitions in the two types of sequences.     

Poly(dA-dT) complexes with histone H1 and pancreatic ribonuclease: Specific base recognition evidenced by ultraviolet resonance Raman spectroscopy

The conformational changes of poly(dA-dT) from random coil to ordered structure with stacked bases produce important changes in the Raman line intensities (hypochromism) when the polymer is excited under the preresonance Raman conditions (λ excitation = 300 nm). Poly(dA-dT)–RNase and poly(dA-dT)–histone H1 interactions have been studied as models of mechanisms of destabilization and stabilization by proteins of the DNA secondary structure, respectively, following this intense preresonance Raman hypochromism. In addition, the specific variation of the intensity of the 1582-cm^?1 line of adenine is interpreted in terms of the interaction of the amino group with the RNase (thus involving the large groove). In the poly(dA-dT)–H1 complex, the intensity of the 1665-cm^?1 line of thymine increases. This increase appears to involve the C₂?O group of thymine, located in the narrow groove.     

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.     

The Structure of Triple Helical Poly(U)·Poly(A)·Poly(U) Studied by Raman Spectroscopy

Abstract

Using Raman spectroscopy, we examined the ribose-phosphate backbone conformation, the hydrogen bonding interactions, and the stacking of the bases of the poly(U)·poly(A) ·poly(U) triple helix. We compared the Raman spectra of poly(U)·poly(A)·poly(U) in H₂O and D₂O with those obtained for single-stranded poly(A) and poly(U) and for double-stranded poly(A)·poly(U). The presence of a Raman band at 863 cm^?1 indicated that the backbone conformations of the two poly(U) chains are different in the triple helix. The sugar conformation of the poly(U) chain held to the poly(A) by Watson-Crick base pairing is C3′ endo; that of the second poly(U) chain may be C2′ endo. Raman hypochromism of the bands associated with base vibrations demonstrated that uracil residues stack to the same extent in double helical poly(A)·poly(U) and in the triple-stranded structure. An increase in the Raman hypochromism of the bands associated with adenine bases indicated that the stacking of adenine residues is greater in the triple helix than in the double helical form. Our data further suggest that the environment of the carbonyls of the uracil residues is different for the different strands.     

Sequence specific conformation of a DNA decamer containing an adenine tract studied in solution by H-NMR spectroscopy

The decanucleotide duplex d(AAAACGTTTT)2 and a variety of phase-sensitive two-dimensional (2D) NMR experiments have been used to investigate the solution conformation of an adenine-tract and its junction with another DNA sequence. 2D nuclear Overhauser effect data confirm that the oligonucleotide has a general B-type DNA morphology but an array of unusual correlations implies that the adenine tract and the 5'-ApC junction have conformations more compatible with the modified X-ray structures recently reported for DNAs of similar sequence (Nelson, H.C.M., Finch, J.T., Luisi, B.F. and Klug, A. (1987) Nature 330, 221-226). The pattern and magnitude of interstrand NOEs from the adenine H2s to the sugar H1's of the complementary base to the 5'-neighbouring residue indicate that the A-T basepairs are highly propeller twisted and that the minor groove is narrowed, showing its greatest compression at the 3'-end of the tract at the 5'-ApC step. Quantifying spin-coupling interactions within the deoxyribose rings by analysing both 1D and high-resolution 2D DQF-COSY data reveals that the conformation of the purines is predominantly C2'-endo, with the pseudorotation phase angle P lying in the range 140-180 degrees. For the pyrimidines, however, there are distortions away from this standard B-type geometry with the data being best described by P values lying in the range 90-130 degrees (i.e., O4'-endo, C1'-exo). The sugar puckers of A1, T9 and T10 are dynamically distorted no doubt as a consequence of their positions at, or close to, the ends of the duplex. Thus the conformation of the adenine and thymine sugars within the oligo(dA) and oligo(dT) strands are different with an abrupt change in sugar puckering occurring at the 5'-ApC (5'-GpT) step. Peculiar chemical shifts values for A4H2, T7CH3 and sugar C5 H1', H2' and H2", together with a number of interresidue NOEs with unusual intensities, imply that there are also substantial modifications to basepair stacking interactions at this step. Taken as a whole, our data are consistent with the view that the conformational dislocation at the 5'-ApC dinucleotide results from a combination of slide and roll manoeuvres and that the junction between the AAAA and CG sequences is a potential nucleation site for DNA bending.     

Theoretical studies of cis-Pt(II)-diammine binding to duplex DNA

The binding of cis-Pt(II) diammine (cis-DP) to double-stranded DNA was studied with several kinked conformations that can accommodate the formation of a square planar complex. Molecular mechanics (MM) calculations were performed to optimize the molecular fit. These results were combined with quantum mechanical (QM) calculations to ascertain the relative energetics of ligand binding through water vs direct binding of the phosphate to the ammine and platinum, and to guide the selection of DNA conformations to model complex formation. Based on QM and MM calculations, models are proposed that may be characterized by several general features. A structure involving hydrogen bonding between each ammine and distinct adjacent phosphate groups, referred to as closed conformation (CC), has already been reported. This is also found in the crystal structure of small dimers. We report alternative conformations that may be important in platination of duplex DNA. They are characterized by an intermediate conformation (IC), involving hydrogen bonding between one ammine and phosphate group, and an open conformation (OC), without ammine phosphate hydrogen bonding. The IC and OC can be stabilized by water bridges in the space between the ammine and the phosphate groups. Sugar puckers alternate from the type C(2')-endo or C(1')-exo (S), to the type C(3')-endo or C(2')-exo (N), with intermediate types near O(1')-endo (O). In general, the sugar puckers alternate from S to N to S through the platinated region (3'-TpG*pG*p-5'), with the complexed strand exhibiting, (3')-S*-N*-S-(5') alternation, while the complementary strand shows either (3')-S*-N*-S-(5') or (3')-S*-N*-O-(5') alternation. In both the OC and IC, a hydrogen bond is found between the ammine and O4(T) on thymine (T) at the (3') end, adjacent to the complex site. There is a continuous range of backbone conformations through the platinated region which relate the OC to the IC. The models presented suggest that the dynamics of the binding of the cis-Pt(II)-diammines to adjacent N7(G) in double-stranded DNA may encompass several conformational possibilities, and that water bridges may play a roll in supporting open and intermediate conformations. Proton-proton distances are reported to assist in the experimental determination of conformations.     

Structural characterization of the 5' untranslated RNA of hepatitis C virus by vibrational spectroscopy

Raman and FTIR spectroscopy have been used to characterize the structure of 5'untranslated region (5'UTR, 342-mer RNA) of the HCV genome. The study of the 750-850 cm(-1) Raman spectral domain of the ribose-phosphate backbone reveals that the percentage of nucleobases involved in double helix-loop junctions is 19+/-1%, which is very close to that of a theoretical secondary structure model (18.7%) proposed on the basis of comparative sequence analysis and thermodynamic modelling. In addition, about 68+/-2% of the bases are helically ordered having C(3')-endo ribofuranose pucker. FTIR-monitored H/D exchange provides the following results: (a) base-paired guanine and cytosine nucleobases show the lowest rate of isotopic exchange, and some synchronous intensity changes of marker bands of A.U pair and single stranded adenine are consistent with the presence of A(*)A.U triplets; (b) the vibrational coupling between the ribose ether C-O stretching and 2'OH bending motions reveals that helical regions of 5'UTR RNA are characterized by hydrogen bonding between the 2'OH ribose groups and the ether oxygen atoms of neighbouring ribose residues.     

The poly dA strand of poly dA.poly dT adopts an A-form in solution: a UV resonance Raman study.

The study by resonance Raman spectroscopy with a 257 nm excitation wave-length of adenine in two single-stranded polynucleotides, poly rA and poly dA, and in three double-stranded polynucleotides, poly dA.poly dT, poly(dA-dT).poly(dA-dT) and poly rA.poly rU, allows one to characterize the A-genus conformation of polynucleotides containing adenine and thymine bases. The characteristic spectrum of the A-form of the adenine strand is observed, except small differences, for poly rA, poly rA.poly rU and poly dA.poly dT. Our results prove that it is the adenine strand which adopts the A-family conformation in poly dA.poly dT.     

Conformational analysis of arabinonucleosides and nucleotides. A comparison with the ribonucleosides and nucleotides.

Conformations of arabino nucleosides and nucleotides have been analyzed by semiempirical energy calculations. It is found that the change in the configuration of the O(2')-hydroxyl group in arabinoses compared to riboses exerts significant influence on the conformational priorities of the glycosyl and the exocyclic C(4')-C(5') bond torsions. While the anti conformations for the bases are preferred, the anti in equilibrium or formed from syn interconversion is considerably hampered compared to ribosides due to large energy barrier. Further the preferred anti glycosyl torsions are shifted to higher values for C(3')-endo puckers and in ribosides. While the gauche+ conformation around the C(4')-C(5') bond is favored for C(3')-endo arabinosides, it is strongly stabilized for C(2')-endo arabinosides only in the presence of the intrasugar hydrogen bond O(2')-H ... O(5'). The net attractive electrostatic interactions between the phosphate and the base stabilizes the preferred conformations of 5'-arabinonucleotides also.     

The propeller DNA conformation of poly(dA).poly(dT).

Physical properties of the DNA duplex, poly(dA).poly(dT) differ considerably from the alternating copolymer poly(dAT). A number of molecular models have been used to describe these structures obtained from fiber X-ray diffraction data. The recent solutions of single crystal DNA dodecamer structures with segments of oligo-A.oligo-T have revealed the presence of a high propeller twist in the AT regions which is stabilized by the formation of bifurcated (three-center) hydrogen bonds on the floor of the major groove, involving the N6 amino group of adenine hydrogen bonding to two O4 atoms of adjacent thymine residues on the opposite strand. Here we show that it is possible to incorporate the features of the single crystal analysis, specifically high propeller twist, bifurcated hydrogen bonds, and a narrow minor groove, as well as the close interstrand NMR signal between adenine HC2 and ribose HC1' of the opposite strand, into a model that is fully compatible with the diffraction data obtained from poly(dA).poly(dT).     

The crystal and molecular structure of 8-methyladenosine 3'-monophosphate dihydrate.

8-Methyladenosine 3'-monophosphate dihydrate was synthesized and crystallized in the monoclinic space group P21 with the unit cell dimensions: a = 9.095(2) A, b = 16.750(3) A, c = 5.405(2) A and beta = 97.61(3) degrees. The structure was determined by the application of the heavy atom method and refined to give a final R factor of 0.047. The pertinent conformations are as follows: the syn conformation about the glycosyl bond (chiCN = 216.8 degrees), the C(2')-endo sugar puckering with the displacement of 0.55 A; and the gauche-gauche conformation about the C(4')-C(5') bond capable of forming an intramolecular hydrogen bonding between N(3) of adenine base and O(5') of the hydroxymethylene group on the ribose. The molecule exists in the zwitterionic form with the N(1) of the adenine base protonated by a phosphate proton and is stabilized by three-dimensional networks of hydrogen bonding through the crystalline water molecules or directly between the adjacent nucleotide molecules; no base stacking was observed.     

Fibre and molecular structure of thymidylyl-3′,5′-deoxyadenosine

X-ray diffraction and molecular model building studies of an ordered structure of thymidylyl-3′,5′-deoxyadenosine which gives fibre-type diffraction patterns, are consistent with a seven-residues per turn, left-handed structure in which the adenine of one molecule and the thymine of the next are linked together by Hoogsteen type of hydrogen bonds. The structure thus resembles a macromolecule in which units are linked together by hydrogen bonds and stabilized by base stocking. Both nucleosides in the basic molecule are in the anti conformation and both sugar rings have C3′-endo puckers. The C5′-05′ bond of the deoxyadenosine is trans relative to C4′-C3′ and the conformations about the P-03′ and P-05′ bond are gauche^?, trans.     

Secondary structure of the hybrid poly(rA).poly(dT) in solution. Studies involving NOE at 500 MHz and stereochemical modelling within the constraints of NOE data

One-dimensional nuclear Overhauser effect (NOE) in nuclear magnetic resonance spectroscopy along with stereochemically sound model building was employed to derive the structure of the hybrid poly(rA).poly(dT) in solution. Extremely strong NOE was observed at AH2' when AH8 was presaturated; strong NOEs were observed at TH2'TH2' when TH6 was presaturated; in addition the observed NOEs at TH2' and TH2' were nearly equal when TH6 was presaturated. There was no NOE transfer to AH3' from AH8 ruling out the possibility of (C-3'-endo, low anti chi approximately equal to 200 degrees to 220 degrees) conformation for the A residues. The observed NOE data suggest that the nucleotidyl units in both rA and dT strands have equivalent conformations: C-2'-endo/C-1'-exo, anti chi approximately equal to 240 degrees to 260 degrees. Such a nucleotide geometry for rA/dT is consistent with a right-handed B-DNA model for poly(rA).poly(dT) in solution in which the rA and dT strands are conformationally equivalent. Molecular models were generated for poly(rA).poly(dT) in the B-form based upon the geometrical constraints as obtained from the NOE data. Incorporation of (C-2'-endo pucker, chi congruent to 240 degrees to 260 degrees) into the classical B-form resulted in severe close contacts in the rA chain. By introducing base-displacement, tilt and twist along with concomitant changes in the backbone torsion angles, we were able to generate a B-form for the hybrid poly(rA).poly(dT) fully consistent with the observed NOE data. In the derived model the sugar pucker is C-1'-exo, a minor variant of C-2'-endo and the sugar base torsion is 243 degrees, the remaining torsion angles being: epsilon = 198 degrees, xi = 260 degrees, alpha = 286 degrees, beta = 161 degrees and gamma = 72 degrees; this structure is free of any steric compression and indicates that it is not necessary to switch to C-3'-endo pucker for rA residues in order to accommodate the 2'-OH group. The structure that we have proposed for the polynucleotide RNA-DNA hybrid in solution is in complete agreement with that proposed for a hexamer hybrid in solution from NOE data and is inconsistent with the heteronomous model proposed for the fibrous state.     

Absolute configuration of Rp-uridine 3'',5''-cyclic phosphorothioate.

Triethylammonium uridine-3',5'-cyclic phosphorothioate crystallizes in space group P2(1)2(1)2(1), a = 7.177(1), b = 13.155(6), c = 21.114(7) A, C15H26N3O7PS, MW 423.4, Z = 4, dx = 1.41g/cm3. The crystal structure was solved by direct methods on the basis of 1493 counter X-ray diffraction data (CuK alpha) and refined to R = 5.1%. The configuration of the thiophosphate group is Rp; conformational parameters are: glycosyl torsion angle anti, -151.9(5) degrees, sugar pucker C(3')-endo with P = 27.3 degrees, vmax = 45.5 degrees, six-membered cycle in chair form. The bond distances in the non-esterified P-S and P-O suggest that the negative charge is distributed between the groups. As illustrated in this and other studies, P-O has a much higher affinity for hydrogen bonds than P-S, indicated here by interactions with triethyl-ammonium N-H and O(2')-H as donors. One additional hydrogen bond N(3)-H---0(4) ties the bases which form a ribbon-like structure. 0(2) and S are not engaged in hydrogen bonds. The triethylammonium ion is two-fold disordered.     

The structure of 3'-O-anthraniloyladenosine, an analogue of the 3'-end of aminoacyl-tRNA.

3'-O-Anthraniloyladenosine, an analogue of the 3'- terminal aminoacyladenosine residue in aminoacyl-tRNAs, was prepared by chemical synthesis, and its crystal structure was determined. The sugar pucker of 3'-O-anthraniloyladenosine is 2'-endo resulting in a 3'-axial position of the anthraniloyl residue. The nucleoside is insynconformation, which is stabilized by alternating stacking of adenine and benzoyl residues of the neighboring molecules in the crystal lattice. The conformation of the 5'-hydroxymethylene in 3'-O- anthraniloyladenosine is gauche-gauche. There are two intramolecular and two intermolecular hydrogen bonds and several H-bridges with surrounding water molecules. The predominant structure of 3'-O-anthraniloyladenosine in solution, as determined by NMR spectroscopy, is 2'-endo,gauche-gauche and anti for the sugar ring pucker, the torsion angle around the C4'-C5'bond and the torsion angle around the C1'-N9 bond, respectively. The 2'-endo conformation of the ribose in 2'(3')-O-aminoacyladenosine, which places the adenine and aminoacyl residues in equatorial and axial positions, respectively, could serve as a structural element that is recognized by enzymes that interact with aminoacyl-tRNA or by ribosomes to differentiate between aminoacylated and non-aminoacylated tRNA.     

The photoreactivity of T-A sequences in oligodeoxyribonucleotides and DNA.

Photoaddition between adjacent adenine and thymine bases occurs, with a quantum yield of approximately 5 X 10(-4) mol einstein-1, when d(T-A), dT-A, d(pT-A), d(T-A-T), d(T-A-T-A) and poly(dA-dT) are irradiated, at 254 nm, in aqueous solution. The photoadduct thus formed is specifically degraded by acid to the fluorescent heterocyclic base 6-methylimidazo[4,5-b]pyridin-5-one (6-MIP) with retention of C(8) of adenine and the methyl group of thymine. This reaction, coupled with either spectrofluorimetric or radiochemical assay of 6-MIP isolated by high voltage paper electrophoresis, has been used to demonstrate formation of the adenine-thymine photoadduct on UV irradiation of poly(dA-dT).poly(dA-dT) and both native and denatured DNA from calf thymus and E. coli. Estimated quantum yields for this new type of photoreaction in DNA show that it is substantially quenched by base pairing. Possible biological implications of the photoreaction are discussed.