Molecular conformations and 8-CH exchange rates of purine ribo- and deoxyribonucleotides: investigation by Raman spectroscopy

The rate of deuterium exchange of the 8-CH group in a purine deoxyribonucleotide, is the same as the 8-CH exchange rate in the corresponding purine ribonucleotide, with the exception of 5′-nucleotides of guanine. The observed 20% slower rate of 8-CH exchange in 5′-dGMP versus 5′-rGMP, over the temperature range 50–80°C, are attributable to differences in molecular conformation, including differences in ring puckering of the furanose substituents. Minor differences in 8-CH exhange rates are observed between 5′-and cyclic (3′:5′)-deoxyribonucleotides of a given purine, which are similar to those observed previously between corresponding 5′- and cyclic ribonucleotides that have been attributed to the charge difference of their respective phosphate groups [Ferreira, S. A. & Thomas, G. J., Jr. (1981) J. Raman Spectrosc. 11 , 508–514]. The coupling of guanine and furanose ring structures in the 5′-nucleotides is also evident from the vibrational frequencies of the guanine ring, which are strongly dependent on the pucker of the attached furanose moiety. Raman difference spectroscopy clearly reveals the dependence of purine nucleotide spectra on sugar-ring pucker. In the case of GMP, the guanine characteristic ring breathing mode near 600–700 cm^?1 depends for its exact position and intensity on the proportion of C3′-endo (668 cm^?1) and C2′-endo (682 cm^?1) conformers in equilibrium with one another. The Raman intensity ratio I(668)/I(682) is proposed as a measure of the conformer ratio C3′-endo/C2′-endo in 5′-dGMP with possible application also to nucleic acids. Among cyclic nucleotides, differences in spectra of deoxyribo- and ribo- forms also appear to be related to differences of molecular conformation.     

A vibrational spectroscopic study of the self-association of 5′-GMP in aqueous solution

The Raman spectra of highly concentrated solutions of 5′-GMP at neutral and acid pH were recorded in order to better characterize the structure of the self-aggregates formed in these solutions and their melting behavior. Vibrational coupling of the C?O stretching vibrations in tetrameric units at neutral pH is shown to yield a characteristic pattern of two Raman bands at ca. 1730 and 1680 cm^?1 (1708 and 1664 cm^?1 in D₂O), and an iractive mode at 1678 cm^?1 in D₂O. From the intensity of the 1730-cm^?1 band, proportional to tetramer concentration, and that at 1485 cm^?1, which reflects the stacking of the bases, the thermal stability of the self-associates formed at neutral pH is shown to be higher for stacked tetramers. At acid pH, the melting of the helical aggregates responsible for the formation of a gel is preceded by the freeing of the hydrogen-bonded phosphate groups, accompanied by a change of conformation from C3′-endo to C2′-endo in some of the associated ribose units. Previous spectroscopic results suggesting the formation of tetramers as an intermediate step in the melting of the gel were not reproduced in this study.     

Determination of the molecular conformation of beta-D-O2,2'-cyclouridine in aqueous solution by proton magnetic resonance spectroscopy

The solution conformation of β-D -O²,2′-cyclouridine has been determined at 27 and 88°C in D₂O by proton magnetic resonance spectroscopy. The conformation is described in terms of a fixed syn-like sugar-base torsional angle, a type S furanose ring conformation (similar to 2′-endo), and a temperature-dependent exocyclic C(4)′–C(5′) rotamer population containing approximately 50% of the gauche-gauche form at 27°C. β-D -O²,2′-Cyclouridine 5′-phosphate likewise possesses a type S furanose ring conformation.     

Structure and Conformation of 5′-Chlorocyclocytidine,a Potent Inhibitor of Nucleic Acid Synthesis: X-Ray, 1H and 13C NMR Analyses

Abstract

The structure of the hydrochloride of 5′-chlorocyclocytidine, a potent inhibitor of DNA synthesis, was determined by X-ray crystallography. The nucleoside crystallizes in the orthorhombic space group P2₁2₁2₁ with cell dimensions a = 10.413(4), b = 13.236(5), c = 17.064(6) Å and with two independent molecules in the asymmetric unit (Z = 8). Atomic parameters were refined by full-matrix least squares to a final value of R = 0.053 for 2490 observed reflections. In both molecules the furanose ring has a C4′ endo/04′ exo (⁴ T ₀) pucker. In molecule A the orientation of the -CH₂Cl side chain is gauche. In molecule B the side chain is disordered: in 70% of these molecules the orientation is trans and in 30% it is gauche ⁺. ¹H NMR spectra indicate a conformational equilibrium between C4′ exo/04′ endo (₄ T ⁰) and C4′ endo/C3′ exo (⁴ ₃ T) with a population ratio of 38:62. All three side chain rotamers occur in solution, the trans orientation contributing most. ¹J(C, H) values for C1′ and C2′ are significantly higher than normal and can therefore be used as a diagnostic tool for the assignment of bridgehead carbon atoms in cyclonucleosides.     

Cytldlne Cyclic (3′, 5′) Monophosphate: Cyclic Nucleotide With a Non-Characteristic Ribose Ring Conformation

Abstract

Cytidine 3′,-5′-cyclic phosphate (cCMP) occurs in nature and has growth stimulatory activity on L-1210 cells. The initiation of cell growth by cCMP, under conditions where CAMP, cGMP and cUMP delay the onset of proliferation suggests that cCMP may play a regulatory role in the cell metabolism. It has been reported that in 3′,5′-cyclic nucleotides, the phosphate ring fused to the furanose ring resuicts the conformation of the furanose ring to the twist form C(3′) endo C(4′) exo (³T₄), in contrast to the C(2′) endo C(3′) endo (²T₃) and C(3′) endo C(2′) exo (³T₂) twist forms normally found in nucleotides and nucleosides. We have carried out an accurate crystal structure of cCMP and found that the furanose ring in cCMP has the C(3′) endo C(2′) exo conformation (³T₂), with a pseudo rotation amplitude (P) of 44° and phase angle τ_m of 12°. cCMP is in low anti conformation (X_CN = 15.4°) and O(5′) has the fixed g conformation. The phosphate ring is constrained to the chair conformation, as in other cyclic nucleotides. The two exocyclic P-O bond distances are short (1.489, 1.476Å) and the ring angle at N(3) is large (125.2°) suggesting that the molecule in the solid state is a zwitterion with a plus charge on N(3). The crystals are hydrated and highly unstable. The three water molecules are highly disordered in ten locations. The crystals of cCMP 3H₂O are hexagonal, a = 16.294(3), b = c = 11.099(4)Å, space group P6₁, final R value is 0.067 for 1620 reflections 230.     

Configurational effects on conformational properties of cyclic nucleotides. I. Theoretical calculations of conformer preferences in α-nucleoside 3′,5′ cyclic monophosphates

A comparative study has been made of the configurational effects on the conformational properties of α- and β-anomers of purine and pyrimidine nucleoside 3′,5′,-cyclic monophosphates and their 2′-arabino epimers. Correlation between orientation of the base and the 2′-hydroxyl group have been studied theoretically using the PCILO (Perturbative Configuration Interaction using Localized Orbitals) method. The effect of change in ribose puckering on the base-hydroxyl interaction has also been studied. The result show that steric repulsions and stabilizing effects of intramolecular hydrogen bonding between the base and the 2′-hydroxyl (OH) group are of major importance in determining configurations of α-anomers and 2′-arabino-β-epimers. For example, hydrogen bonding between the 2′-hydroxyl group and polar centers on the base ring is clearly implicated as a determinant of syn-anti preferences of the purine (adenine) or pyrimidine (uracil) bases in α-nucleoside 3′,5′-cyclic monophosphates. Moreover, barrier heights for interconversion between conformers are sensitive to ribose pucker and 2′-OH orientations. The result clearly show that a change in ribose-ring pucker plays an essential role in relieving repulsive interaction between the base and the 2′-hydroxyl group. Thus a C2′-exo-C3′-endo (₂T³) pucker is favored for α-anomers in contrast with the C4′-exo-C3′-endo (₄T³) from found in β-compounds.     

Synthesis of 4′-C-Methylnucleosides

Several 4′-C-methylnucleosides were prepared. ¹H-NMR studies on these nucleosides showed that they have the 3′-exo furanose ring conformation different from the 3′-endo conformation of natural nucleosides.     

Raman spectroscopic elucidation of DNA backbone conformations for poly(dG-dT).poly(dA-dC) and poly(dA-dT).poly(dA-dT) in CsF solution

Raman spectra have been recorded for poly(dG-dT) · poly(dA-dC) and poly(dA-dT) · poly(dA-dT) in low salt and at high concentrations of CsF. Poly(dG-dT) · poly(dA-dC) shows no change in the 682-cm^?1 guanine mode, demonstrating the absence of the Z-structure at high salt. The 790-cm^?1 phosphodiester symmetric stretch, however, shifts up 5 cm^?1 in 4.3M CsF, suggesting a slight conformational change, associated with ion binding or hydration changes. Poly(dA-dT) · poly(dA-dT) shows an additional broad band at 816 cm^?1, attributed to the phosphodiester modes associated with the C3′-endo deoxyribose units in the alternating B-structure. In this case, both the 841- and the 816-cm^?1 asymmetric phosphodiester stretches, associated with the C2′- and C3′-endo units, shift down on addition of CsF in a sequential manner. Correlation of this sequence with that previously observed for the two ³¹P-nmr resonances, establishes that the phosphodiester stretching frequencies depend on the conformation of the 5′-sugar, and not on the 3′-sugar.     

Molecular structure of the cis-syn photodimer of d(TpT) (cyanoethyl ester)

The three-dimensional structure was determined by x-ray crystallography for d(T[p](CE)T), a uv photoproduct of the cyanoethyl (CE) derivative of d(TpT), having the cis-syn cyclobutane (CB) geometry and the S-configuration at the chiral phosphorus atom. The crystals of C₂₃H₃₀N₅O₁₂P · 2H₂O belong to the orthorhombic space group P2₁2₁2₁ (Z = 4), with cell dimensions a = 11.596 Å, b = 14.834 Å, and c = 15.946 Å, containing two water molecules per asymmetric unit. The CB ring is puckered with a dihedral angle of 151°. The two pyrimidine bases are rotated by –29° from the position of direct overlap of their corresponding atoms. This represents a major distortion of DNA, since in DNA adjacent thymines are rotated by +36°. The pyrimidine rings are puckered with Cremer–Pople parameters for T[p] and in parentheses [p]T: Q: 0.24 Å (0.31 Å); θ: 123° (120°); ?: 141° (86°). These represent half-chairs designated as ⁶H₁ (T[p]) and ₆H⁵ ([p]T). The CB and pyrimidine ring conformations are interrelated, and we postulate that they execute a coupled interconversion in solution. The T[p] segment has the syn glycosyl conformation, a ²T₃ sugar pucker, and gauche^? conformation at C4′-C5′; the [p]T segment is anti, ³T₄, trans. The C5′-O5′ torsion of the [p]T unit is –124.5°, and the C3′-O3′ torsion of the T[p] unit is –152.9°. Bond angles and bond lengths involving the phosphorus atom are similar to those of other phosphotriesters. The P-O3′ and P-05′ torsion angles are –138.1° and 58.6°, respectively. Several intermolecular (but no intramolecular) hydrogen bonds are found in the crystal.     

Conformational characteristics of the trinucleoside diphosphate d(ApApA) from energy-minimization studies

Energy-minimization studies were carried out on the trinucleoside diphosphate d(ApApA). The potential energy contributions from nonbonded, electrostatic, hydrogen-bonding, and torsional interactions were minimized by treating the 13 relevant dihedral angles as simultaneous variables. For the C(3′)-endo trimer, 14 low-energy conformations are within 10 kcal/mol above the lowest energy found, compared to only 3 in the case of the C(2′)-endo trimer. This result shows the flexible character of the C(3′)-endo unit. The hairpin-type, loop-promoting conformer with (ω′,ω) = (101°, 59°) was found to be the most favored structure at the 3′-terminus of d(ApApA). The predicted U- and L-type bend conformers were found to lie within 5 kcal/mol, compared to the lowest energy B-DNA structure. The A-DNA and Watson-Crick DNA types of helical conformers also lie within very small energy barriers. The phosphate group at the 5′-end of the nucleotide residue has a definite influence on the base of the corresponding nucleotide, keeping it in the normal anti-region, and hence on the base-stacking property. The results are compared with the presently available experimental data, mainly with the tRNA^Phe crystal.     

A Raman spectroscopic study on 5′-rGMP gel and self-aggregate

In order to analyze the melting behavior of 5′-rGMP gel at acidic pH and self-aggregate near neutral pH we have obtained Raman spectra of aqueous solutions of 5′-rGMP at various temperatures. At low temperature the intensities of Raman peaks at 502, 585, 1083, 1179, 1322, 1366, 1487, and 1578 cm^?1 decrease due to the formation of ordered structure (Raman hypochromism). In contrast, the peaks at 671, 725, 813, and 1338 cm^?1 become stronger at low temperature (Raman hyperchromism). The Raman hyperchromism of the 671- and 813-cm^?1 peaks have been explained in terms of detailed structural models. Recently, the 668- and 682-cm^?1 peaks in the Raman spectrum of aqueous 5′-rGMP solution have been attributed to the guanine ring breathing vibrations in C3′- and C2′-endo conformers [Benevides, J. B., Lemur, D. & Thomas, G. J., Jr. (1984) Biopolymers 23 , 1011–1024]. On the basis of this information our Raman data can be interpreted to suggest that the continuous helix model of 5′-rGMP gel is right-handed. The 1487-cm^?1 peak intensity has been used to monitor the melting profies at several pHs. Near neutral pH the melting profile shows a single transition, whereas at acidic pH it shows two transitions. From these observations we propose possible pathways for the melting of 5′-rGMP gel formed at acidic pH and self-aggregate formed near neutral pH.     

Visualization of drug--nucleic acid interactions at atomic resolution. V. Structure of two aminoacridine--dinucleoside monophosphate crystalline complexes, proflavine--5-iodocytidylyl (3'-5') guanosine and acridine orange--5-iodocytidylyl (3'-5') guanosine

Acridine orange and proflavine form complexes with the dinucleoside monophosphate, 5-iodocytidylyl(3′–5′)guanosine. The acridine orange-iodoCpG² crystals are monoclinic, space group P2₁, with unit cell dimensions $\text{a = 14.36}\text{A}\text{?}\text{, b = 19.64}\text{A}\text{?}\text{, c = 20.67}\text{A}\text{?}$, β = 102.5 °. The proflavine-iodoCpG crystals are monoclinic, space group C2, with unit cell dimensions $\text{a = 32.14}\text{A}\text{?}\text{, b = 22.23}\text{A}\text{?}\text{, c = 18.42}\text{A}\text{?}$, β = 123.3 °. Both structures have been solved to atomic resolution by Patterson and Fourier methods, and refined by full matrix least-squares.Acridine orange forms an intercalative structure with iodoCpG in much the same manner as ethidium, ellipticine and 3,5,6,8-tetramethyl-N-methyl phenanthrolinium (Jain et al., 1977, Jain et al., 1979), except that the acridine nucleus lies asymmetrically in the intercalation site. This asymmetric intercalation is accompanied by a sliding of base-pairs upon the acridine nucleus and is similar to that observed with the 9-aminoacridine-iodoCpG asymmetric intercalative binding mode described in the previous papers (Sakore et al., 1977, Sakore et al., 1979). Basepairs above and below the drug are separated by about 6.8 Å and are twisted about 10 °; this reflects the mixed sugar puckering pattern observed in the sugar-phospate chains: C3′ endo (3′–5′) C2′ endo (i.e. each cytidine residue has a C3′ endo sugar comformation, while each guanosine residue has a C2′ endo sugar conformation), alterations in glycosidic torsional angles and other small but significant conformational changes in the sugar-phosphate backbone.Proflavine, on the other hand, demonstrates symmetric intercalation with iodoCpG. Hydrogen bonds connect amino groups on proflavine with phosphate oxygen atoms on the dinucleotide. In contrast to the acridine orange structure, base-pairs above and below the intercalative proflavine molecule are twisted about 36 °. The altered magnitude of this angular twist reflects the sugar puckering pattern that is observed: C3′ endo (3′–5′) C3′ endo. Since proflavine is known to unwind DNA in much the same manner as ethidium and acridine orange (Waring, 1970), one cannot use the information from this model system to understand how proflavine binds to DNA (it is possible, for example, that hydrogen bonding observed between proflavine and iodoCpG alters the intercalative geometry in this model system).Instead, we propose a model for proflavine-DNA binding in which proflavine lies asymmetrically in the intercalation site (characterized by the C3′ endo (3′–5′) C2′ endo mixed sugar puckering pattern) and forms only one hydrogen bond to a neighboring phosphate oxygen atom. Our model for proflavine-DNA binding, therefore, is very similar to our acridine orange-DNA binding model. We will describe these models in detail in this paper.     

Conformational properties of poly[d(G-T)].poly[d(C-A)] and poly[d(A-T)] in low- and high-salt solutions: NMR and laser Raman analysis

³¹P- and ¹H-nmr and laser Raman spectra have been obtained for poly[d(G-T)]·[d(C-A)] and poly[d(A-T)] as a function of both temperature and salt. The ³¹P spectrum of poly[d(G-T)]·[d(C-A)] appears as a quadruplet whose resonances undergo separation upon addition of CsCl to 5.5M. ¹H-nmr measurements are assigned and reported as a function of temperature and CsCl concentration. One dimensional nuclear Overhauser effect (NOE) difference spectra are also reported for poly[d(G-T)]·[d(C-A)] at low salt. NOE enhancements between the H8 protons of the purines and the C5 protons of the pyrimidines, (H and CH₃) and between the base and H-2′,2″ protons indicate a right-handed B-DNA conformation for this polymer. The NOE patterns for the TH3 and GH1 protons in H₂O indicate a Watson–Crick hydrogen-bonding scheme. At high CsCl concentrations there are upfield shifts for selected sugar protons and the AH2 proton. In addition, laser Raman spectra for poly[d(A-T)] and poly[d(G-T)]·[d(C-A)] indicate B-type conformations in low and high CsCl, with predominantly C2′-endo sugar conformations for both polymers. Also, changes in base-ring vibrations indicate that Cs⁺ binds to O2 of thymine and possibly N3 of adenine in poly[d(G-T)]·[d(C-A)] but not in poly[d(A-T)]. Further, ¹H measurements are reported for poly[d(A-T)] as a function of temperature in high CsCl concentrations. On going to high CsCl there are selective upfield shifts, with the most dramatic being observed for TH1′. At high temperature some of the protons undergo severe changes in linewidths. Those protons that undergo the largest upfield shifts also undergo the most dramatic changes in linewidths. In particular TH1′, TCH₃, AH1′, AH2, and TH6 all undergo large changes in linewidths, whereas AH8 and all the H-2′,2″ protons remain essentially constant. The maximum linewidth occurs at the same temperature for all protons (65°C). This transition does not occur for d(G-T)·d(C-A) at 65°C or at any other temperature studied. These changes are cooperative in nature and can be rationalized as a temperature-induced equilibrium between bound and unbound Cs⁺, with duplex and single-stranded DNA. NOE measurements for poly[d(A-T)] indicate that at high Cs⁺ the polymer is in a right-handed B-conformation. Assignments and NOE effects for the low-salt ¹H spectra of poly[d(A-T)] agree with those of Assa-Munt and Kearns [(1984) Biochemistry 23 , 791–796] and provide a basis for analysis of the high Cs⁺ spectra. These results indicate that both polymers adopt a B-type conformation in both low and high salt. However, a significant variation is the ability of the phosphate backbone to adopt a repeat dependent upon the base sequence. This feature is common to poly[d(G-T)]·[d(C-A)], poly[d(A-T)], and some other pyr–pur polymers [J. S. Cohen, J. B. Wouten & C. L Chatterjee (1981) Biochemistry 20 , 3049–3055] but not poly[d(G-C)].     

A and Z canonical conformations in d(CnGCGn) crystals characterized by microFTIR and microRaman spectroscopies

Two crystals d(C₂GCG₂) and d(C₅GCG₅) have been studied under microscope by Fourier transform ir spectroscopy and Raman spectroscopy. The x-ray diffraction study of the latter crystal had shown that the d(C₅GCG₅) sequence is the first DNA dodecamer known to adopt a canonical A conformation [N. Verdaguer, J. Aymami, D. Fernandez-Forner, I. Fita, M. Coll, T. Huynh-Dinh, J. Igolen, and J. A. Subirana (1991) Journal of Molecular Biology, Vol. 221, pp. 623–635]. Characteristic ir marker bands and Raman marker peaks of the A conformation have thus been obtained and are compared with previously proposed assignments correlated to fiber diffraction x-ray results obtained on polymers. The d(C₂GCG₂) sequence crystal had previously been studied in an intermediate form between B and Z [L. Urpi, J. P. Ridoux, J. Liquier, N. Verdagner, I. Fita, J. A. Subirana, F. Iglesias, T. Huynh-Dinh, J. Igolen, and E. Taillandier (1989) Nucleic Acids Research, Vol. 17, pp. 6669–6679]. In this paper we present results obtained from a crystal with this oligonucleotide in Z conformation. The effect of the crystallization conditions on the geometry of the obtained oligomer helix is discussed. The influence of the addition, to the central tetramer CGCG, of dC_n stretches (at the 5′ end) and dG_n stretches (at the 3′ end) of different lengths, on the conformational flexibility of the nucleic acid, is considered. © 1993 John Wiley & Sons, Inc.     

Polarized Raman spectrum of single crystal uridylyl (3′–5′) adenosine: Local Raman tensors of some functional groups

Polarized Raman scattering measurements have been made of a single crystal of uridylyl(3′–5′)adenosine (UpA) by the use of a Raman microscope with 488.0 nm excitation. The UpA crystal belongs to space group P2₁ (monoclinic), and Raman intensities I_aa, I_bb, and I_c′c′, have been determined for each Raman band. These intensities correspond to the aa, bb, and c′c′ components of the crystal Raman tensor, where c′ is defined as an axis perpendicular to the crystallographic a axis in the ac plane. From these experimental data, and by taking the known crystal structure into account, anisotropic and isotropic molecular Raman tensors have been calculated for the following 11 normal modes: ring stretching modes of the adenine residue (protonated) at 1560, 1516, 1330, and 715 cm⁻¹; ring stretching modes of the uracil residue at 1696, 1657, 1615, 1228, and 790 cm⁻¹; PO⁻₂ symmetric stretching mode at 1080 cm⁻¹; P(—)O single bond stretching mode at 801 cm₋₁. These pieces of information of the Raman tensors are considered to be useful for estimating the orientations of the DNA and RNA strands in a biological complex from a polarized Raman spectroscopic measurement of such a complex. © 1998 John Wiley & Sons, Inc. Biopoly 45: 135–147, 1998     

Synthesis and X-ray structure of a C5-C4-linked glucofuranose-oxazolidin-2-one

The formation of (4R)-4-carbamoyl-4-[(4R)-3-O-benzyl-1,2-O-isopropylidene-β-l-threofuranos-4-C-yl]-oxazolidin-2-one instead of expected imidazolidin-2,4-dione (hydantoin) derivative from 5-amino-5-cyano-5-deoxy-3-O-benzyl-1,2-O-isopropylidene-α-d-glucofuranose or 3-O-benzyl-1,2-O-isopropylidene-α-d-xylo-hexofuranos-5-ulose under Bucherer-Bergs reaction conditions is reported. Single crystal X-ray diffraction data revealed that ³T₄ is the prefered conformation for the furanose ring, while E₂ and ²T₁ conformations are adopted by the 1,3-dioxolane and 2-oxazolidinone five-membered rings, respectively.     

Visualization of drug--nucleic acid interactions at atomic resolution. VI. Structure of two drug--dinucleoside monophosphate crystalline complexes, ellipticine--5-iodocytidylyy (3'-5') guanosine and 3,5,6,8-tetramethyl-N-methyl phenanthrolinium--5-iodocytidylyl (3'-5') guanosine

Ellipticine and 3,5,6,8-tetramethyl-N-methyl phenanthrolinium form complexes with the dinucleoside monophosphate, 5-iodocytidylyl(3′–5′)guanosine. These crystals are isomorphous: ellipticine-iodoCpG² crystals are monoclinic, space group P2₁ with $\text{a = 13.88}\text{A}\text{?}\text{, b = 19.11}\text{A}\text{?}\text{, c = 21.42}\text{A}\text{?}$, β = 105.4; TMP-iodoCpG crystals are monoclinic, space group P2₁, with $\text{a = 13.99}\text{A}\text{?}\text{, b = 19.12}\text{A}\text{?}\text{, c = 21.31}\text{A}\text{?}$, β = 104.9 °. Both structures have been solved to atomic resolution by Patterson and Fourier methods, and refined by full matrix least-squares.The asymmetric unit in the ellipticine-iodoCpG structure contains two ellipticine molecules, two iodoCpG molecules, 20 water molecules and 2 methanol molecules, a total of 144 atoms, whereas, in the tetramethyl-N-methyl phenanthrolinium-iodoCpG complex, the asymmetric unit contains two TMP molecules, two iodoCpG molecules, 17 water molecules and 2 methanol molecules, a total of 141 atoms. In both structures, the two iodoCpG molecules are hydrogenbonded together by guanine-cytosine Watson-Crick base-pairing. Adjacent base-pairs within this paired iodoCpG structure are separated by about 6.7 Å; this separation results from intercalative binding by one ellipticine (or TMP) molecule and stacking by the other ellipticine (or TMP) molecule above or below the base-pairs. Base-pairs within the paired nucleotide units are related by a twist of 10 to 12 °. The magnitude of this angular twist is related to conformational changes in the sugar-phosphate chains that accompany drug intercalation. These changes partly reflect the mixed sugar puckering pattern observed: C3′ endo (3′–5′) C2′ endo (i.e. both iodocytidine residues have C3′ endo conformations, whereas both guanosine residues have C2′ endo conformations), and additional small but systematic changes in torsional angles that involve the phosphodiester linkages and the C4′C5′ bond.The stereochemistry observed in these model drug-nucleic acid intercalative complexes is almost identical to that observed in the ethidium-iodoUpA and -iodoCpG complexes determined previously (Tsai et al., 1975a,b,1977; Jain et al., 1977). This stereochemistry is also very similar to that observed in the 9-aminoacridine-iodoCpG and acridine orange-iodoCpG complexes described in the preceding papers (Sakore et al., 1979 Reddy et al., 1979). We have already proposed this stereochemistry to provide a unified understanding of a large number of intercalative drug-DNA (and RNA) interactions (Sobell et al., 1977a,b), and discuss this aspect of our work further in this paper.     

Effect of specific inhibitors on mitochondrial DNA replication in HeLa cells

The crystal structure of an orthorhombic form of 2′-0-methyl cytidine was determined from three dimensional X-ray diffraction data. The two molecules in each asymmetric unit have C2-$\text{endo}$ C3-$\text{exo}$ puckered furanose rings. This differs from the C3-$\text{endo}$ puckering observed for cytidine (1) and it may have some relevance to the kinks that appear at the two 2′-0-methylated nucleotides in the anticodon phosphate ester backbone of the phe tRNA structure (2). This work and other studies (3,4) show that the presence of a 2′-0-methyl group does not prevent the furanose moiety from adopting its most commonly observed configurations. 2′-0-methyl nucleotides make up a small percentage of the residues in HnRNA, rRNA, tRNA and mRNA and therefore their conformational nuances are of interest.     

A vibrational spectroscopic study of the self-association of polyinosinic acid and polyguanylic acid in aqueous solution

We have studied by Raman and ir spectroscopy the structure of self-associated polyinosinic acid and polyguanylic acid in aqueous solution. The results are consistent with the formation of a four-stranded complex, which melts cooperatively near 60°C in the case of poly (I) in the presence of K⁺ ions. The conformation of the ribose in both systems is mixed C2′-endo/C3′-endo, giving a structure that is intermediate between the extremes proposed previously from x-ray diffraction studies. Characteristic Raman bands for the C2′-endo ribose conformation in polyribonucleotides are identified. The four-stranded structure of poly (I) appears to be very flexible, with ≈15% of the tetrameric segments being disrupted and ≈30% of the ribose units adopting a disordered conformation prior to melting. This disordering process increases to ≈75% above the melting transition, with the remaining ≈25% of the ribose units keeping an ordered C2′-endo or C3′-endo conformation. © 1994 John Wiley & Sons, Inc.     

13C-labeled oligodeoxyribonucleotides: A solution study of a CCAAT-containing sequence at the nuclear factor I recognition site of human adenovirus

The solution behavior of the single-stranded CCAAT-containing octamer 1 , d(AGCCAATA), that comprises part of the nuclear factor I (NF-I) recognition site at the origin of replication of human adenovirus has been studied by nmr spectroscopy at 500 and 600 MHz. Proton resonance assignments for 1 were aided by selective ¹³C enrichment at C1′ of A₁ or A₅. High-resolution ¹³C-¹H heteronuclear multiple-bond coherence spectra of the ¹³C-labeled oligomers permitted the selective detection of furanosyl ring protons within each labeled residue due to short- and long-range ¹³C-¹H couplings to the enriched C1′. The resulting assignments provided firm starting points in the interpretation of double quantum filtered correlated spectra, yielding information supplemented by total correlated spectroscopy (TOCSY) and rotating frame nuclear Overhauser effect spectroscopic data to completely assign the ¹H-nmr spectrum of 1 and extract ³J_HH values for furanose con-formational analysis. Several ¹³C-¹H spin-coupling constants within the ¹³C-enriched A₁ or A₅ residues were measured from cross-peak shifts in TOCSY spectra, and their signs determined by inspection of the relative orientations of these shifts. ¹H-²-H and ¹³C-¹H spin-couplings both indicate a preference (> 75%) for south (C2′-endo) conformations by the furanosyl rings of 1 . © 1994 John Wiley & Sons, Inc.