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C Altona

Publications and source records attributed to C Altona.

At least 37 records · Page 2Linked to original sources

Hairpin structures in DNA containing arabinofuranosylcytosine. A combination of nuclear magnetic resonance and molecular dynamics.

Nuclear magnetic resonance (NMR) and model-building studies were carried out on the hairpin form of the octamer d(CGaCTAGCG) (aC = arabinofuranosylcytosine), referred to as the TA compound. The nonexchangeable protons of the TA compound were assigned by means of nuclear Overhauser effect spectroscopy (NOESY) and correlated spectroscopy (COSY). From a detailed analysis of the coupling data and of the NOESY spectra the following conclusions are reached: (i) The hairpin consists of a stem of three Watson-Crick type base pairs, and the two remaining residues, T(4) and dA(5), participate in a loop. (ii) All sugar rings show conformational flexibility although a strong preference for the S-type (C2'-endo) conformer is observed. (iii) The thymine does not stack upon the 3' side of the stem as expected, but swings into the minor groove. (This folding principle of the loop involves an unusual alpha t conformer in residue T(4).) (iv) At the 5'-3' loop-stem junction a stacking discontinuity occurs as a consequence of a sharp turn in that part of the backbone, caused by the unusual beta + and gamma t torsion angles in residue dG(6). (v) The A base slides over the 5' side of the stem to stack upon the aC(3) residue at the 3' side of the stem in an antiparallel fashion. On the basis of J couplings and a set of approximate proton-proton distances from NOE cross peaks, a model for the hairpin was constructed. This model was then refined by using an iterative relaxation matrix approach (IRMA) in combination with restrained molecular dynamics calculations. The resulting final model satisfactorily explains all the distance constraints.

Base Sequence↗

Conformational consequences of the incorporation of arabinofuranosylcytidine in DNA. An NMR study of the DNA fragments d(CGCTAGCG) and d(CGaCTAGCG) in solution.

The self-complementary octamers d(CGCTAGCG) and d(CGaCTAGCG) (aC, arabinofuranosylcytidine) were studied by means of NMR spectroscopy. It is shown that d(CGaCTAGCG), under suitable conditions of oligonucleotide concentration, ionic strength and temperature, exclusively adopts a hairpin structure. However, under the same experimental conditions (5 mM DNA, no added salt, 295 K) d(CGCTAGCG) mainly adopts a B-DNA-type duplex. At lower temperatures (less than or equal to 290 K) the hairpin form of d(CGaCTAGCG) occurs in slow exchange with an intact B-DNA-type duplex. When the DNA concentration of d(CGCTAGCG) is dramatically reduced (less than or equal to 0.5 mM) the hairpin form becomes highly favoured at the expense of the dimer. Moreover, proton-chemical-shift considerations indicate that the structural features of the hairpin structure of d(CGCTAGCG) mimic, in part, those of the modified octamer d(CGaCTAGCG), i.e. a loop comprising only the two central residues with the thymine located into the minor groove (Pieters, J. M. L., de Vroom, E., van der Marel, G. A., van Boom, J. H., Koning, T. M. G., Kaptein, R. and Altona, C. unpublished results). Thermodynamic analysis of d(CGCTAGCG) yields an average Tmd value of 342 K (1 M DNA) and a delta Hod value of -266 kJ/mol for the dimer/coil transition and an average Tmh value of 321 K and delta Hoh - 102 kJ/mol for the hairpin/coil equilibrium. For the duplex/coil equilibrium of d(CGaCTAGCG) an average Tmd value of 336 K (1 M DNA) and delta Hod value of -253 kJ/mol are deduced. The hairpin/coil transition of d(CGaCTAGCG) is characterized by a delta Hoh value of -104 kJ/mol and an average Tmh value of 331 K. It is concluded that incorporation of an arabinofuranosylcytidine in the octamer d(CGaCTAGCG) results in stabilization of the hairpin form, whereas the dimer is destablized by two aC.dG base pairs.

Base Sequence↗

Conformational analysis of brominated pA2'-5'A2'-5'A analogs. An NMR and model-building study.

NMR and model-building studies were carried out on pA2'-5'A2'-5'A and analogs in which one or more of the A residues were replaced by 8-bromoadenosine. Chemical shifts, coupling constants and NOE data were used to obtain structural information. The N/S equilibrium constant of the ribose rings as well as the phase angles and puckering amplitudes were determined from the experimental coupling constants with the aid of an improved version of the PSEUROT program. Chemical shifts in combination with NOE data were used to monitor base-base interactions and the orientation of the bases (syn or anti). The combined data suggest that different types of stacking interactions are present in the various compounds. Bromination of the first or second residue in the trimers results in a preference for N-type sugar and syn orientation of the base in these residues. When A(3) is brominated, an S-type sugar conformation together with a syn orientation of the base is favoured at the 2' terminus. Energy-minimized models of the different stacking interactions are presented which fit the present collection of data. The possible correlation between biological activity of these compounds and their conformation is briefly discussed.

Adenosine↗

Conformational and thermodynamic consequences of the introduction of a nick in duplexed DNA fragments: an NMR study augmented by biochemical experiments.

NMR studies were carried out on various equimolar mixtures consisting of a combination of oligomers: d(ACGGCT) (I). d(pACGGCT) (Ia), d(TGCAGT) (II), d(AGCCGTACTGCA) (III), d(TGCAGTACGGCT) (IV). It is shown that I + II + III (MI) and Ia + II + III (M2) form stable duplexes with nicks in the centre of the respective double helices. A close analysis of the NOESY experiments of M1 and M2 revealed that these fragments form B-DNA type duplex structures. A comparison of the chemical-shift data of the nicked duplexes with those of the intact duplex of III + IV (M3) demonstrated that only small local distortions occur when a nick is introduced. The chemical-shift profiles of M1 and M3 were used to obtain the thermodynamic data for the duplex/coil transitions. The profiles of M1 were analysed by means of a new thermodynamic model (TRIDUP). From the calculated thermodynamic data of M1 and M3 it is concluded that the melting behaviour of M1 occurs cooperatively. A ligation experiment demonstrated that the relatively small substrate (M2) was almost completely joined after an overnight incubation at 14 degrees C.

Base Sequence↗

Thermodynamics of the various forms of the dodecamer d(ATTACCGGTAAT) and of its constituent hexamers from proton nmr chemical shifts and UV melting curves: three-state and four-state thermodynamic models.

Chemical shifts of base and H1' protons of the single-stranded hexamers d(ATTACC) and d(GGTAAT), of the 1:1 mixtures of these complementary hexamers, and of the self-complementary dodecamer d(ATTACCGGTAAT) were measured at various temperatures in aqueous solution. Four different sample concentrations were used in the case of the dodecamer and of the mixture of the complementary hexamers; the individual hexamers were measured at two different DNA concentrations. Absorbance temperature profiles at five different NaCl concentrations were measured for the dodecamer in order to quantify the effect of the ionic strength on the duplex formation. Under suitable conditions of nucleotide concentration, temperature, and ionic strength, the dodecamer adopts either a B-DNA duplex or a hairpin-loop structure. Chemical shift vs temperature profiles, constructed for all samples, were used to obtain thermodynamic parameters either for the various stacking interactions in the single strands or for the duplex or the hairpin-loop formation. In the analysis of the duplex formation of the hexamers, a two-state approach appeared too simple, because systematic deviations were revealed. Therefore, a new three-state model (DUPSTAK) was developed. In order to investigate the magnitude of error arising from the use of the two-state approach in cases where the DUPSTAK model appears more appropriate, a series of test calculations was made. The magnitude of error in the enthalpy and in the entropy of duplex melting is found to depend linearly upon the actual melting temperature and not upon the individual delta Hd degrees and delta Sd degrees values. Thermodynamic analysis of the chemical shift vs temperature profiles in D2O solution (no added salt) yields an average Tmd value of 341 K (1M DNA) and delta Hd degrees of - 121 kJ.mol-1 for the dimer/random-coil transition of the hexamer duplex d(ATTACC).d(GGTAAT). For the duplex in equilibrium random-coil transition of the 12-mer d(ATTACCGGTAAT) an average Tmd value of 336 K (1M DNA) and delta Hd degrees of -372 kJ.mol-1 are found. The hairpin/random-coil transition of d(ATTACCGGTAAT) is characterized by a rather large delta Hh degrees value, -130 kJ.mol-1, and an average Tmh value of 304 K.

Magnetic Resonance Spectroscopy↗

Toward a computer assisted analysis of NOESY spectra: a multivariate data analysis of an RNA NOESY spectrum.

A multivariate data-representation of a portion of the H-NOESY spectrum of an RNA octamer duplex was used to explore the possibility of using Principal Component Analysis and Partial Least Squares Discrimination for pattern recognition. In this case, it is found that the methods can: (i) distinguish slices containing signal from those containing only noise, (ii) locate slices containing overlapping signals, and (iii) in some cases to segregate slices with unique aspects such as those from terminal nucleotides, overlapping signals, purine-H8, pyrimidine-H6 and adenine-H2 containing slices. These properties can easily be included in a scheme to automate spectral analysis. The formulation described here does not distinguish patterns needed to automate sequential assignment of resonances in NOESY spectra of RNA.

Base Sequence↗

Alterations in the d(CpGpT) structure in solution as a result of [PtCl(diethylenetriamine)]+ binding.

The trinucleotide d(CpGpT) reacts with [PtCl(dien)]Cl (dien = diethylenetriamine) to yield as a single adduct Pt(dien)[d(CpGpT)-N7(2)]. The structure of this adduct in solution has been analysed with the aid of NMR spectroscopy and compared with that of the unmodified trinucleotide. A change in the population of the S conformer of the guanosine deoxyribose ring and a syn preference of the guanine residue are the most important changes occurring upon platination. As a result the dC-dG stack disappears, whereas the dG-dT stack is hardly affected. The CD spectra of both platinated and free d(CpGpT) confirm the different nature of the two molecules.

Binding Sites↗

Bulge-out structures in the single-stranded trimer AUA and in the duplex (CUGGUGCGG).(CCGCCCAG). A model-building and NMR study.

Model-building studies were carried out on the trimer AUA. Bulge-out structures which allow incorporation into a continuous RNA helix were generated and energy-minimized. All geometrical features obtained by previous NMR studies on purine-pyrimidine-purine sequences are accounted for in these models. One of the models was used to fit into a double helical fragment. Only minor changes were necessary to construct a central bulge-out in an otherwise intact duplex. NMR and model-building studies were performed on the duplex (CUGGUGCGG).(CCGCCCAG) which contains an unpaired uridine residue. NOE data, chemical-shift profiles and imino-proton resonances provided evidence that the extra U is bulged out of the duplex. The relatively small dispersion in 31P chemical shifts (approximately equal to 0.7 ppm) indicate the absence of t/g or g/t combinations for the phosphodiester angles zeta/alpha. An energy-minimized model of the duplex, which fits the present collection of data, is presented.

Base Composition↗

Influence of uracil on the conformational behaviour of RNA oligonucleotides in solution.

NMR studies were carried out on some alternating pyrimidine-purine sequences: the single-stranded tetramers CACA and UGUG and the self-complementary octamer CACAUGUG. Assignments, based upon COSY, homonuclear Hartmann-Hahn, and NOESY experiments, are given for the resonances of all base protons and of several sugar protons. Chemical shift vs temperature profiles were used to obtain thermodynamic parameters for the single-stranded stack in equilibrium with random coil and the duplex in equilibrium with random coil equilibria. The populations of N-type conformer of the ribose rings were estimated from the observed J1'2'. Comparisons with another alternating pyrimidine-purine sequence Um2(6)AUm2(6)A and with the deoxyribose counterparts d(CACA), d(TGTG) and d(CACATGTG) are given. Previous 1H-NMR investigations of Um2(6)AUm2(6)A revealed that the population of bulge-out structure diminishes compared to m2(6)AUm2(6)A due to the U(1)-m2(6)A(2) stacking interaction. In CACA a strong stacking proclivity (Tm = 310 K) together with a clear preference for N-type ribose is observed. However, the stacking interactions in UGUG are relatively less stable (Tm = 288 K) and a bias towards S-type sugar is present. Besides a small amount of stack, a significant contribution of bulge out structure is proposed for UGUG. We conclude that the nature of the pyrimidine base mainly determines the formation of bulge-out structures. The poor stacking properties of uracil now appear to be mainly responsible for this phenomenon. Comparison with the deoxyribose counterparts shows a reasonable agreement between the Tm values of CACA and d(CACA), whereas the Tm of UGUG (288 K) is much lower than the Tm of d(TGTG) (315 K). It is suggested that the absence of bulge-out structures in DNA purine-pyrimidine-purine sequences is related to the relatively strong stacking proclivity of dT residues compared to that of U residues. The Tm values (average 341 K) for the duplex in equilibrium with random coil transition obtained for each residue of CACAUGUG appear very similar. All ribose rings, except the G(8), adopt a pure N conformer in the duplex. This is taken to mean that the differences in conformational behaviour of the constituent tetramers disappear upon duplex formation.

Base Sequence↗

Extra thymidine stacks into the d(CTGGTGCGG).d(CCGCCCAG) duplex. An NMR and model-building study.

NMR and model-building studies were carried out on the duplex d(CTGGTGCGG).d(CCGCCCAG), referred to as (9+8)-mer, which contains an unpaired thymidine residue. Resonances of the base and of several sugar protons of the (9+8)-mer were assigned by means of a NOESY experiment. Interresidue NOEs between dG(4) and dT(5) as well as between dT(5) and dG(6) provided evidence that the extra dT is stacked into the duplex. Thermodynamic analysis of the chemical shift vs temperature profiles yielded an average TmD value of 334 K and delta HD of -289 kJmol-1 for the duplex in equilibrium random-coil transition. The shapes of the shift profiles as well as the thermodynamic parameters obtained for the extra dT residue and its neighbours again indicate that the unpaired dT base is incorporated inside an otherwise intact duplex. This conclusion is further supported by (a) the observation of an imino-proton resonance of the unpaired dT; (b) the relatively small dispersion in 31P chemical shifts (approximately 0.5 ppm) for the (9+8)-mer, which indicates the absence of t/g or g/t combinations for the phosphate diester torsion angles alpha/zeta. An energy-minimized model of the (9+8)-mer, which fits the present collection of experimental data, is presented.

Base Composition↗

Conformational analysis of the dinucleotides 5'-methylphospho-N6-dimethyladenylyl-uridine (mpm62A-U) and 5'methylphospho-uridylyl-N6-dimethyladenosine (mpU-m62A) and of the trinucleotide U-m62A-U. A nuclear magnetic resonance and circular dichroic study.

NMR and CD studies were carried out on the dinucleotides 5'-methylphospho-N6-dimethyladenylyl-uridine (mpm62-U) and 5'-methylphospho-uridylyl-N6-dimethyladenosine (mpU-m62A) and on the trinucleotide U-m62A-U. A detailed comparison is given of the conformational features of mpm62A-U and mpU-m62A with the corresponding 5'-nonphosphorylated dinucleotides m62A-U and U-m62A, respectively. The behaviour of the trinucleotide U-m62A-U is compared with the properties of the constituent dinucleotides U-m62A and mpm62A-U. Chemical-shift and CD data were used to determine the amount of stacking interactions. For each compound NMR spectra were recorded at two or three sample concentrations in order to separate intermolecular and intramolecular base-base interactions. The coupling constants of the ribose ring are interpreted in terms of the N/S equilibrium, and population distributions along the backbone angles beta, gamma and epsilon are presented. The combined data indicate a strong similarity between mpm62A-U and m62A-U both in degree and in mode of stacking. In contrast, the existence of different types of stacking interactions in mpU-m62A and U-m62A is suggested in order to explain the NMR and CD data. It is concluded that dinucleoside bisphosphates serve better as a model for the behaviour of trinucleotides than dinucleoside monophosphates. The trinucleotide U-m62A-U adopts a regular single-stranded stacked RNA structure with preference for N-type ribose and gamma+ and beta t backbone torsion angles. The difference in behaviour between the U-m62A- part of U-m62A-U and the dimer U-m62A is seen as a typical example of conformational transmission.

Adenine Nucleotides↗

Conformational analysis of the tetranucleotides m6(2)A-m6(2)A-U-m6(2)A(m6(2)A = N6-dimethyladenosine) and U-m6(2)A-U-m6(2)A and of the hybrid dA-r(U-A). A one- and two-dimensional NMR study.

A 1H-NMR investigation was carried out on the tetranucleotides U-m6(2)A-U-m6(2)A and m6(2)A-m6(2)A-U-m6(2)A (m6(2) = N6-dimethyladenosine) as well as on the hybrid trinucleotide dA-r(U-A). An extensive comparison with m6(2)A-U-m6(2)A and other relevant compounds is made. Previous proton NMR studies on trinucleotides have shown that purine-pyrimidine-purine sequences prefer to adopt a mixture of states which have as a common feature that the interior pyrimidine residue bulges out, whereas the flanking purine residues stack upon each other. A stacking interaction on the 3' side of the bulge is known to have no measurable effect on the bulge population. Chemical-shift data, ribose ring conformational analysis and information from NOE experiments now show unambiguously that the moderate U(1)-m6(2)A(2) stack in U-m6(2)A-U-m6(2)A diminishes the population of bulged-out structures in favour of a regular stack. This tendency towards conformational transmission in the downstream 5'----3' direction is fully confirmed by the fact that the strong m6(2)A(1)-m6(2)A(2) stack in the tetranucleotide m6(2)A-m6(2)A-U-m6(2)A virtually precludes the formation of bulged-out structures. The conformational characteristics of dA-r(U-A) appear comparable with those of m6(2)A-U-m6(2)A, which indicates that the presence of a 2'-hydroxyl group in the first purine residue is not a necessary prerequisite for the formation of a bulge.

Adenine Nucleotides↗

An NMR study of polymorphous behaviour of the mismatched DNA octamer d(m5C-G-m5C-G-A-G-m5C-G) in solution. The B-duplex and hairpin forms.

By means of one- and two-dimensional NMR spectroscopy the solution structures of the partly self-complementary octamer d(m5C-G-m5C-G-A-G-m5C-G) were investigated. It is shown that this DNA fragment, under conditions of high DNA concentration (8 mM DNA) and/or high ionic strength prefers to adopt a duplex structure. At low DNA concentration (0.4 mM DNA), the duplex exists in a 1:1 slow equilibrium with a monomeric hairpin form. Addition of salt destabilizes the hairpin structure in favour of the dimer. At high temperatures the hairpin form, as well as the dimer structure, exist in a fast equilibrium with the random-coil form. For the hairpin/random-coil equilibrium a Tm of 329 K and a delta H degree of -121 kJ.mol-1 were deduced. These thermodynamic parameters are independent of the DNA concentration, as is expected for a monomeric structure. For the dimer to coil transition a Tm of 359 K (1 M DNA) and a delta H degree of -285 kJ.mol duplex-1 were derived. The thermodynamic data of the hairpin-coil transition mutually agree with those recently reported for the hairpin to random coil equilibrium of the DNA octamer d(m5C-G-m5C-G-T-G-m5C-G) [Orbons, L. P. M., van der Marel, G. A., van Boom, J. H. & Altona, C. (1987) J. Biomol. Struct. Dyns. 4, 939-963]. It is demonstrated that the dimer structure exhibits B-DNA characteristics, as is witnessed by the NOESY experiments and the analysis of the proton-proton coupling data. It is shown that the base-pair formation of the G x A mismatches is anti-anti. A comparison of 1H and 31P chemical-shift data of the title compound with those of a well-characterized B-DNA structure reveals large differences in the dm5C(3)-dG(4)-dA(5) part of the mismatched dimer structure. These differences apparently indicate some major local structural changes due to the incorporation of the G x A mismatches. Under the most extreme conditions used (i.e. up to 3 M NaCl or 75% CH3OH in the presence of 10 mM MgCl2) no Z-DNA structure was observed. It is shown that the structural features of the hairpin form of the title compound mimic those of the hairpin structure of d(m5C-G-m5C-G-T-G-m5C-G). An energy-minimized model of the hairpin form is given.

Base Sequence↗

Influence of the base sequence on the conformational behaviour of DNA polynucleotides in solution.

NMR studies were carried out on samples of the non-self-complementary tetramers d(C-A-C-A), d(T-G-T-G), d(G-A-G-A) and d(T-C-T-C) and of 1:1 mixtures of the complementary tetramers d(C-A-C-A) X d(T-G-T-G) and d(G-A-G-A) X d(T-C-T-C) at two DNA concentrations and of the self-complementary octamers d(C-A-C-A-T-G-T-G) and d(G-A-G-A-T-C-T-C). Assignments, based upon one-dimensional NOE and homonuclear-decoupling and two-dimensional correlated and NOE spectroscopies are given of the resonances of most of the base and sugar protons. Chemical shift vs temperature profiles, constructed for all samples, yielded insight into the temperature- and concentration-dependent conformational behaviour of the compounds and were used to obtain thermodynamic parameters pertaining to the stacked-single-strand----random-coil and duplex----random-coil equilibria. Vicinal proton-proton couplings were analyzed in terms of the conformation of the deoxyribose rings in the single-stranded tetramers and duplexed octamers. The NOE patterns, chemical shift profiles, imino-proton resonances and coupling data revealed that the compounds adopt B-DNA-like structures. The ratio duplexed/stacked-single-strand/random coil depends upon external conditions as well as upon base sequence. The thermodynamic data indicate that: in terms of single-helical stacking, the R-R steps (Tm 321-328 K) appear more stable than the Y-R or R-Y steps (Tm 308-316 K) and the Y-Y steps score least (Tm 290-300 K), and the duplexes consisting of alternating, d(Y-R)n, strands are more stable, in terms of delta H degrees, compared to the d(R-R)n X d(Y-Y)n duplexes. The analyses of the couplings demonstrated that the sugars of the single-stranded tetramers and duplexed octamers occur as a blend of N- and S-type conformers, with a preference for the S-type (C2'-endo) sugar conformation: upon duplex formation, no significant shift in the N-type/S-type ratio was observed. The fraction S-type sugar conformation of a given residue, %S, in the stacked-single strands was found to depend upon the nature of its own base and that of the adjacent residues: sugars in an R-R stretch display high values of %S (90-100), whereas those in Y-Y stretches show relatively low values (approximately equal to 65).(ABSTRACT TRUNCATED AT 400 WORDS)

Base Sequence↗

Influence of N6-methylation of residue A(5) on the conformational behaviour of d(C-C-G-A-A-T-T-C-G-G) in solution studied by 1H-NMR spectroscopy. 1. The duplex form.

One- and two-dimensional NMR studies at 300 MHz and 500 MHz were carried out on the two oligonucleotides d(C-C-G-A-A-T-T-C-G-G) and d(C-C-G-A-m6A-T-T-C-G-G) in aqueous solution. NMR spectra were observed at 10 mM sample concentration over the temperature range 273-368 K. Assignments are given of the base, H1', H2', H2", H3' and of some H4' resonances, based upon a combination of two-dimensional correlation spectra (COSY) and two-dimensional nuclear Overhauser effect spectra (NOESY); imino-proton resonances were assigned with the aid of a two-dimensional NOE experiment. Chemical shift vs temperature profiles were constructed in order to gain insight into the influence of N6-methylation of residue A(5) on the temperature-dependent conformational behaviour of the decamer and to determine thermodynamic parameters for the duplex-to-coil transition. The NOESY spectra, the imino-proton spectra and the shift profiles of the two compounds, under conditions where each forms a B-DNA-type duplex, are very similar. This is taken to indicate that the influence of N6-methylation of residue A(5) on the local structure of the duplex must be small. However, the temperature dependence of the (non-)exchangeable proton resonances of the two compounds reveals that methylation slows down the duplex-single-strand exchange. Furthermore, a thermodynamic analysis of the two compounds indicates that N6-methylation slightly decreases the stability of the duplex relative to the monomeric forms (Tm is reduced from 332 K down to 325 K at 10 mM sample concentration). Proton-proton couplings were obtained by means of one-dimensional and two-dimensional NMR experiments and were used in a conformational analysis of the sugar ring of each residue of the two compounds in the duplex form. The analysis indicated that all sugar rings display conformational flexibility in the intact duplex: population S-type sugar conformation ranges from 70% to 100%. A more refined analysis of the sugar rings of the parent compound revealed a sequence-dependent variation of the sugar geometry. This variation does not follow well the trend predicted by the Calladine/Dickerson sigma 3-sum rule [Dickerson, R. E. (1983) J. Mol. Biol. 166, 419-441; Calladine, C. R. (1982) J. Mol. Biol. 161, 343-352]; moreover the actual variations appear to be smaller in solution than those expected on the basis of known X-ray structures.

Magnetic Resonance Spectroscopy↗

Influence of N6-methylation of residue A(5) on the conformational behaviour of d(C-C-G-A-A-T-T-C-G-G) in solution studied by 1H-NMR spectroscopy. 2. The hairpin form.

The solution conformations of the oligonucleotides d(C-C-G-A-A-T-T-C-G-G) and d(C-C-G-A-m6A-T-T-C-G-G) as a function of temperature and sample concentration were investigated by means of 1H-NMR spectroscopy. The NMR spectra revealed that, at certain combinations of temperature and low sample and salt concentration, both compounds exist as a B-DNA-type duplex slowly (on the 1H-NMR time scale) interconverting with a monomeric species. From chemical shift data and imino-proton spectra, it is concluded that the monomeric species consists of a mixture of a hairpin form in rapid equilibrium with the random-coil form. The double-helical stem of the hairpin is formed by the six terminal cytidine and guanine residues, whereas the four core residues, -A-(m6)A-T-T-, partake in the loop. Thermodynamic analysis of the chemical shift of the resonances of the monomeric species vs temperature profiles of the two decamers and mutual comparison of these profiles indicate the following: the influence of N6-methylation of residue A(5) upon the local structure of the hairpin must be small; methylation decreases the stability of the duplex relative to the monomeric species: the temperature at which the fraction duplex equals 0.5 was found to be 312 K for the parent compound and 305 K for the methylated decamer at 2 mM sample concentration; methylation does not significantly alter the stability of the hairpin form relative to the random coil form: the Tm of the hairp----n equilibrium random-coil equilibrium is 308 K for the parent compound and 306 K for the methylated decamer. A higher fraction hairpin-like structure for the N6-methylated compound is observed under identical conditions of temperature and sample concentration: at 300 K, 2 mM sample concentration, the fraction hairpin form is 0.12 for d(C-C-G-A-A-T-T-C-G-G) and 0.20 for d(C-C-G-A-m6A-T-T-C-G-G). This finding appears to be a consequence of the reduced stability of the methylated dimeric species relative to the monomeric species, and to depend upon the sodium-ion concentration: it becomes more pronounced under low-salt conditions.

Magnetic Resonance Spectroscopy↗

Conformational analysis of the deoxyribofuranose ring in DNA by means of sums of proton-proton coupling constants: a graphical method.

A graphical method is presented for the conformational analysis of the sugar ring in DNA fragments by means of proton-proton couplings. The coupling data required for this analysis consist of sums of couplings, which are referred to as sigma 1' (= J1'2' + J1'2''), sigma 2' (= J1'2' + J2'3' + J2'2''), sigma 2'' (= J1'2'' + J2''3' + J2'2'') and sigma 3' (= J2'3' + J2''3' + J3'4'). These sums of couplings correspond to the distance between the outer peaks of the H1', H2', H2'' and H3' [31P] resonances, respectively, (except for sigma 2' and sigma 2'' in the case of a small chemical shift difference between the H2' and H2'' resonances) and can often be obtained from 1H-NMR spectra via first-order measurement, obviating the necessity of a computer-assisted simulation of the fine structure of these resonances. Two different types of graphs for the interpretation of the coupling data are discussed: the first type of graph serves to probe as to whether or not the sugar ring occurs as a single conformer, and if so to analyze the coupling data in terms of the geometry of this sugar ring. In cases where the sugar ring does not occur as a single conformer, but as a blend of N- and S-type sugar puckers, the second type of graph is used to analyze the coupling data in terms of the geometry and population of the most abundant form. It is shown that the latter type of analysis can be carried out on the basis of experimental values for merely sigma 1',sigma 2' and sigma 2'', without any assumptions or restrictions concerning a relation between the geometry of the N- and S-type conformer. In addition, the question is discussed as to how insight can be gained into the conformational purity of the sugar ring from the observed fine structure of the H1' resonance. Finally, a comparison is made between experimental coupling data reported for single-stranded and duplex DNA fragments and covalent RNA-DNA hybrids on the one hand and the predicted couplings and sums of couplings presented in this paper on the other hand.

Computer Graphics↗

An NMR study of the polymorphous behavior of the mismatched DNA octamer d(m5C-G-m5C-G-T-G-m5C-G) in solution. The B, Z, and hairpin forms.

The polymorphism exhibited by the mismatched octamer d(m5C-G-m5C-G-T-G-m5C-G), as a function of the temperature, DNA concentration and ionic strength, was investigated by means of NMR spectroscopy. It is shown that this partly self-complementary DNA fragment, under conditions of low DNA concentration (0.4 mM) and low ionic strength, exclusively prefers to adopt a monomeric hairpin form, which consists of a stem of three Watson-Crick-type base pairs and a loop of only two residues. This in striking contrast with earlier intimations in literature, which postulated that in oligonucleotides loop formations containing only two residues are sterically impossible. Moreover, the hairpin form displays an unusual stability in comparison with previously reported hairpins. A Tm of 332 K and a delta H degree of -130 kJ.mol-1 were calculated for the hairpin to random coil transition. At high DNA concentration (8 mM) and/or upon the addition of sodium chloride the hairpin form occurs in slow exchange with a B-DNA dimer structure (approximately 20% at 270 K, no added salt), which comprises two central GxT-mismatched base pairs with the bases as major tautomers. At higher ionic strength (greater than 100 mM NaCl), or upon the addition of methanol, a third species appears, which is in slow exchange with both the B dimer and the hairpin form. This third species could be identified with a Z DNA form, comprising two GxT mismatches with the bases as major tautomers, with the guanine bases syn and the cytosine and thymine bases anti.

Base Composition↗