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The thermal stability of oligodeoxyribonucleotide duplexes containing deoxyinosine (I) residues matched with each of the four normal DNA bases were determined by optical melting techniques. The duplexes containing at least one I were obtained by mixing equimolar amounts of an oligonucleotide of sequence dCA3XA3G with one of sequence dCT3YT3G where X and Y were A, C, G, T, or I. Comparison of optical melting curves yielded relative stabilities for the I-containing standard base pairs in an otherwise identical base-pair sequence. I:C pairs were found to be less stable than A:T pairs in these duplexes. Large neighboring-base effects upon stability were observed. For example, when (X,Y) = (I,A), the duplex is eight-fold more stable than when (X,Y) = (A,I). Independent of sequence effects the order of stabilities is: I:C greater than I:A greater than I:T congruent to I:G. This order differs from that of deoxyguanosine which pairs less strongly with dA; otherwise each deoxyinosine base pair is less stable than its deoxyguanosine counterpart in the same sequence environment. Implications of these results for design of DNA oligonucleotide probes are discussed.

Phase-dependent forms of microscopy (such as phase contrast, interference, or polarization microscopy) have been used for many years; the amount of phase retardation produces images based mainly on index of refraction. We have developed a microscope that forms images that depend on small differences in extinction for different forms of incident polarized light. By modulating the polarization of light incident on the sample and digitally recording the difference in intensities of transmitted light, we obtain images which specifically reveal either ordered linear structures or chiral (right- or left-handed) structures. Linearly polarized light, incident alternately with two perpendicular directions of polarization, forms images of structures which have linear order or linear orientation. Right-handed and left-handed circularly polarized light incident alternately on a sample forms images of chiral structures. Structures with neither linear order nor chirality are essentially invisible. Thus, images based on linear dichroism, circular dichroism, and linear and circular differential scattering can be used to detect specific types of structures which may be difficult to observe by conventional methods. We have used such 'linear and circular differential imaging' to study the structure of the nucleolus (the site of RNA synthesis) in live primary spermatocytes of Drosophila when they are transcriptionally active or inactive. Some inactive nucleoli are bipartite, with two distinct structures visible by differential scattering of both linearly and circularly polarized light. The active nucleolus is a single domain; it is clearly distinguished from part of the Y chromosome, and it shows different internal structure with linearly and circularly polarized light. Thus, polarization-dependent images reveal structures which can be associated with the transcriptional activity of cells.

If an optically active (chiral) sample is placed in a microscope and illuminated with circularly polarized light, an image can be formed that is related to the circular dichroism of each feature of the sample. A theoretical investigation has been done for the circular differential image obtained by subtracting the images formed under right- and left-circularly polarized light. Two types of differential images are possible: (i) dark-field images formed from light reflected or scattered by the sample and (ii) bright-field images formed from light transmitted through the sample. The sign and magnitude of each feature in a circular differential image strongly depend on the structure of the sample. The dark-field circular differential images are most sensitive to large features with dimensions similar to the wavelength of illumination whereas the bright-field images are most sensitive to the short-range molecular order. Applications of circular differential imaging may include clinical fingerprinting of normal and transformed cells and structural analysis of individual cellular components.

Circular dichroism (CD) spectra in the vacuum UV region for different conformations of poly d(G-C) X poly d(G-C) and poly r(G-C) X poly r(G-C) are very characteristic. The CD of the RNA in the A-form (6 M NaClO4 and 22 degrees C) is very similar to that of the DNA in 80% alcohol where it is believed to be in the A-form. With the exception of the longest wavelength transition, the CD of the RNA in 6 M NaClO4 at 46 degrees C is similar to the CD of the DNA under conditions where it is believed to be in the Z-form (2 M NaClO4). This substantiates that poly r(G-C) X poly r(G-C) assumes a left-handed Z-conformation in 6 M NaClO4 above 35 degrees C. CD spectra for the left-handed Z-forms of both the RNA and DNA are characterized by an intense negative peak at 190-195 nm, a crossover at about 184 nm, and an intense positive peak below 180 nm. The right-handed A- and B-forms of RNA and DNA all have an intense positive peak in their CD spectra near 186 nm. The large difference in CD in the range 185-195 nm for right- and left-handed conformations of nucleic acids can be used to identify the sense of helix winding.

The diverse functions of RNA, which include enzymatic activities, regulatory roles in transcription and translation, are made possible by tertiary structure. Computer algorithms can predict the secondary structure of an RNA molecule using free-energy parameters for base pairing and stacking, loops and bulges. However, with the exception of transfer RNA, little is known about the structures and thermodynamics of interactions involved in the tertiary structure of RNA. Recently, it has been proposed that a novel form of RNA folding called pseudoknotting occurs at the 3' end of certain viral RNAs from plants. A pseudoknot involves intramolecular pairing of bases in a hairpin loop with a few bases outside the stem of the loop to form an additional stem and loop region (Fig. 1). If each stem contained a full helical turn, a true knot would be formed. We present evidence from single-strand specific (S1) and double-strand specific (V1) nuclease digestion, that a short RNA oligonucleotide (19 nucleotides long) adopts a stable pseudoknotted structure. The nuclease digestion and thermodynamic properties of this oligonucleotide were compared with those of oligonucleotides which form hairpin structures containing the two possible stem regions in the pseudoknot. These results show that appropriate sequences can form pseudoknots and indicate that pseudoknots are a significant type of local tertiary structure which must be considered in the folding of complex RNA molecules.

The structures of ZI- and ZII-form RNA and DNA oligonucleotides were energy minimized in vacuum using the AMBER molecular mechanics force field. Alternating C-G sequences were studied containing either unmodified nucleotides, 8-bromoguanosine in place of all guanosine residues, 5-bromocytidine in place of all cytidine residues, or all modified residues. Some molecules were also energy minimized in the presence of H2O and cations. Free energy perturbation calculations were done in which G8 and C5 hydrogen atoms in one or two residues of Z-form RNAs and DNAs were replaced in a stepwise manner by bromines. Bromination had little effect on the structures of the energy-minimized molecules. Both the minimized molecular energies and the results of the perturbation calculations indicate that bromination of guanosine at C8 will stabilize the Z forms of RNA and DNA relative to the nonbrominated Z form, while bromination of cytidine at C5 stabilizes Z-DNA and destabilizes Z-RNA. These results are in agreement with experimental data. The destabilizing effect of br5C in Z-RNAs is apparently due to an unfavorable interaction between the negatively charged C5 bromine atom and the guanosine hydroxyl group. The vacuum-minimized energies of the ZII-form oligonucleotides are lower than those of the corresponding ZI-form molecules for both RNA and DNA. Previous x-ray diffraction, nmr, and molecular mechanics studies indicate that hydration effects may favor the ZI conformation over the ZII form in DNA. Molecular mechanics calculations show that the ZII-ZI energy differences for the RNAs are greater than three times those obtained for the DNAs. This is due to structurally reinforcing hydrogen-bonding interactions involving the hydroxyl groups in the ZII form, especially between the guanosine hydroxyl hydrogen atom and the 3'-adjacent phosphate oxygen. In addition, the cytidine hydroxyl oxygen forms a hydrogen bond with the 5'-adjacent guanosine amino group in the ZII-form molecule. Both of these interactions are less likely in the ZI-form molecule: the former due to the orientation of the GpC phosphate away from the guanosine ribose in the ZI form, and the latter apparently due to competitive hydrogen bonding of the cytidine 2'-hydroxyl hydrogen with the cytosine carbonyl oxygen in the ZI form. The hydrogen-bonding interaction between the cytidine hydroxyl oxygen and the 5'-adjacent guanosine amino group in Z-RNA twists the amino group out of the plane of the base. This may be responsible for differences in the CD and Raman spectra of Z-RNA and Z-DNA.

The distribution of oriented, polymerized sickle cell hemoglobin (hemoglobin S) in erythrocytes is visualized with a microscope that produces an image proportional to linear dichroism. Monochromatic light alternately polarized along two perpendicular directions is incident on the sample. The image is focused on a diode array, and the digital output is used to form two images. One is the usual image proportional to the average transmitted light intensity of the two incident polarizations of light; the other is a linear differential image proportional to the linear dichroism of the sample. This quantitative image can specifically reveal oriented hemoglobin molecules with a sensitivity of about 4000 oriented molecules per picture element of the image.

Chemically induced dynamic nuclear polarization (CIDNP) has been observed from yeast tRNAPhe following reaction with photoexcited riboflavin. At 20 degrees C, several resonances of tRNA in the native form show polarization; previous work predicts that only guanosine and its derivatives in single-stranded regions are likely to become polarized [ McCord , E.F., Morden , K. M., Pardi , A., Tinoco , I., Jr., & Boxer, S. G. (1984) Biochemistry (preceding paper in this issue)]. The methyl protons of m22G -26 show strong negative spin polarization, indicating that this residue is accessible. The solvent accessibility of this residue has not been previously demonstrated. In addition, two positively polarized aromatic resonances are observed, which are likely due to two or more G(H8) protons, including those of G-20, m22G -26, and/or Gm-34. For temperatures below 50 degrees C, a negatively polarized signal in the aromatic region is shown to arise from cross relaxation with the methyl group protons of m22G -26. This indicates the proximity of an aromatic proton, probably H2 of A-44, to the methyl groups of m22G -26. At higher temperatures, the CIDNP spectra show polarization of several additional G resonances, including those of m2G -10. These changes in the CIDNP spectra reflect melting of the tertiary and secondary structure of the tRNA. This work is the first use of CIDNP to study a large nucleic acid molecule and exemplifies the value of this technique in probing single-stranded and solvent-accessible regions of tRNA.

The structures and hydrogen exchange properties of the mismatched DNA oligonucleotide duplexes d(CCCAGGG)2 and d(CCCTGGG)2 have been studied by high-resolution nuclear magnetic resonance. Both the adenine-adenine and thymine-thymine mismatches are intercalated in the duplexes. The structures of these self-complementary duplexes are symmetric, with the two strands in equivalent positions. The evidence indicates that these mismatches are not stably hydrogen bonded. The mismatched bases in both duplexes are in the anti conformation. The mismatched thymine nucleotide in d(CCCTGGG)2 is intercalated in the duplex with very little distortion of the bases or sugar-phosphate backbone. In contrast, the bases of the adenine-adenine mismatch in d(CCCAGGG)2 must tilt and push apart to reduce the overlap of the amino groups. The thermodynamic data show that the T-T mismatch is less destabilizing than the A-A mismatch when flanked by C-G base pairs in this sequence, in contrast to their approximately equal stabilities when flanked by A-T base pairs in the sequence d(CAAAXAAAG.CTTTYTTTG) where X and Y = A, C, G, and T [Aboul-ela, F., Koh, D., & Tinoco, I., Jr. (1985) Nucleic Acids Res. 13, 4811]. Although the mechanism cannot be determined conclusively from the limited data obtained, exchange of the imino protons with solvent in these destabilized heteroduplexes appears to occur by a cooperative mechanism in which half the helix dissociates.

The conformations of dinucleoside phosphates have been reexamined by semiempirical potential energy calculations. Conformations I, II, and III, proposed by Lee & Tinoco [Lee, C. H., & Tinoco, I., Jr. (1977) Biochemistry 16, 5403], are possible species after refinement of their structures by potential energy minimization. These three conformers can represent three types of dinucleoside phosphate species in solution. Dhingra et al. [Dhingra, M. M., Sarma, R. H., Giessner-Prettre, C., & Pullman, B. (1978) Biochemistry 17, 5815] had concluded that conformations of type II and III were unlikely or impossible. They favored conformations g-g- (equivalent to I), g+g+,g+t, and tg+; the last three conformations have little stacking and are calculated to be energetically less favorable by more than 5 kcal/mol. Common structures of the types I, II, and III are found for dinucleoside phosphates with different purine-pyrimidine sequences. The sequence dependence of the potential energy of these three conformers has been calculated. The experimental nuclear magnetic resonance data of dinucleoside phosphates are consistent with these three conformations.

The cis and trans isomers of dicationic bis(4-N-methylpyridyl)diphenylporphine show a much greater tendency to aggregate than similar tetracationic porphyrins. Upon binding to nucleic acids these aggregating dicationic porphyrins form long-range structures on the polymer template giving intense circular dichroism signals whose profile reports the helical sense of the DNA.

Calculated circular dichroism spectra are presented for double-stranded polynucleotides of regular sequences in A-RNA, A-DNA, B-DNA, and Z-DNA conformations. Quantum mechanical matrix method calculations were carried out in the near and vacuum ultraviolet regions. In the near UV, the calculated spectra agreed qualitatively with the measured spectra. However in the far and vacuum UV, the calculated CD compared nearly quantitatively with the experimental spectra. The calculations show that the sign of the CD in the vacuum UV, in contrast to that in the near UV, can be correlated with the handedness of the helix.

The kinetics of U-U-C-A binding to the dodecanucleotide (A-Cm-U-Gm-A-A-Y-A-psi-m5C-U-Gp) isolated from the anticodon region of yeast tRNA-Phe are similar to the kinetics of binding of U-U-C-A to intact tRNA-Phe. A large enhancement in binding constant over that predicted for U-U-C-A-U-G-A-A is observed for both the complexes of dodecanucleotide and tRNA-Phe with U-U-C-A. This strongly suggests that both the anticodon loop in tRNA-Phe and the dodecanucleotide can form four base pairs with U-U-C-A. Furthermore, the enhanced stability cannot be attributed to a special conformation of the anticodon loop, but instead the anticodon loop is probably flexible. A likely explanation for the increased binding is the effect of non-base-paired ends. This increased thermodynamic stability comes from a larger entropy gain rather than a larger enthalpy decrease.

The equilibrium binding of the ethidium cation (Etd+) to the right-handed A-form of poly-[r(C-G)], the B-form of poly[d(C-G)], and the left-handed Z-forms of Br-poly[r(C-G)] and Br-poly[d(C-G)] was investigated in 0.22 M NaCl by optical methods. Scatchard analysis indicates that Etd+ intercalates into right-handed forms of poly[r(C-G)] and poly[d(C-G)] in a noncooperative manner. Correlation of Etd+ absorbance binding isotherms and polynucleotide circular dichroism data indicates that drug binding to Br-poly[r(C-G) and Br-poly[d(C-G)] results in cooperative conversion from left-handed Z-forms to right-handed intercalated conformations. Approximate stoichiometries necessary to induce the left- to right-handed transitions are 1 Etd+/9 base pairs (bp) for Z-RNA and 1 Etd+/6 bp for Z-DNA. The apparent limiting binding stoichiometries are approximately 1 Etd+/3 bp for RNA and 1 Etd+/2 bp for DNA. The equilibrium binding constants for binding to the right-handed forms decrease in the order Br-poly[d(C-G)], Br-poly[r(C-G)], poly[d(C-G)], and poly[r(C-G)]. Thermodynamic parameters are obtained by van't Hoff analysis of Etd+ absorbance thermal dissociation data. Enthalpy values for all four polynucleotides are negative and of similar magnitude. Negative entropy values indicate that the binding processes are primarily enthalpically driven.(ABSTRACT TRUNCATED AT 250 WORDS)

The kinetics of double-strand formation were measured by using temperature-jump kinetic techniques for the DNA oligonucleotides dCA5G + dCT5G, the analogous RNA oligonucleotides rCA5G + rCU5G, and the hybrid rCA5G + dCT5G. The DNA oligonucleotides have a faster rate of recombination and a slower rate of dissociation at 12.0 degrees C than the RNA oligonucleotides; the hybrid has about the same recombination rate and a slightly faster dissociation rate than the RNA oligonucleotides. The activation energies for recombination for the DNA and RNA oligonucleotides are both near 0 kcal/mol. The difference in dissociation and recombination activation energies is consistent with the thermodynamic results obtained earlier. The relaxation process is composed of two exponential components for the RNA and hybrid oligonucleotides at temperatures of 12.0 degrees C and lower. One exponential component is observed for these oligonucleotides above 12.0 degrees C and for the DNA oligonucleotides at all temperatures.

The nonexchangeable base protons and the hydrogen-bonding NH--N imino protons were used to study the conformations and the helix--coil transitions in the following oligonucleotides: (I) dCT5G + dCA5G, (II) rCU5G + rCA5G, (III) dCT5 G + rCA5G, (IV) rCU5G + dCA5G. The first three mixtures all form stable double-helical structures at 5 degrees C, whereas IV forms a triple strand with an rCU5G:dCA5G 2:1 ratio. The chemical shifts of the imino protons in the double strands indicate that I, II, and III have different conformations in solution. For example, the hydrogen-bonded proton of one of the C.G base pairs is more deshielded (a 0.4-ppm downfield shift) in helix I than in helix II or III. This implies a significant change in helical parameters, such as the winding angle, the distance between base pairs, or overlap of the bases. The coupling constants of the H1' sugar protons show that helix I has 90% 2'-endo sugar conformation, whereas helix III has greater than 85% 3'-endo conformation for the observed sugar rings. The sugar pucker data are consistent with helix I having B-family geometry; III has A-family geometry. The chemical shifts of the nonexchangeable base protons in system I were followed with increasing temperature. The midpoints for the transitions, Tm's, for all the base protons were 28--30 degrees C; this indicates an all-or-none transition.

The solvent conditions that induce the formation of a left-handed Z form of poly[r(G-C)] have been extended to include 6.5 M NaBr at 35 degrees C and 3.8 M MgCl2 at room temperature. The analysis of the A----Z transition in RNA by circular dichroism (CD), 1H and 31P NMR, and Raman spectroscopy shows that two distinct forms of left-handed RNA exist. The ZR-RNA structure forms in high concentrations of NaBr and NaClO4 and exhibits a unique CD signature. ZD-RNA is found in concentrated MgCl2 and has a CD signature similar to the Z form of poly[d(G-C)]. The loss of Raman intensity of the 813-cm-1 A-form marker band in both the A----ZR-RNA and A----ZD-RNA transitions parallels the loss of intensity at 835 cm-1 in the B----Z transition of DNA. A guanine vibration that is sensitive to the glycosyl torsion angle shifts from 671 cm-1 in A-RNA to 641 cm-1 in both ZD- and ZR-RNA, similar to the B----Z transition in DNA in which this band shifts from 682 to 625 cm-1. Significant differences in the glycosyl angle and sugar pucker between Z-DNA and Z-RNA are suggested by the 16-cm-1 difference in the position of this band. The Raman evidence for structural difference between ZD- and ZR-RNA comes from two groups of bands: First, Raman intensities between 1180 and 1600 cm-1 of ZD-RNA differ from those for ZR-RNA, corroborating the CD evidence for differences in base-stacking geometry. Second, the phosphodiester stretching bands near 815 cm-1 provide evidence of differences in backbone geometry between ZD- and ZR-RNA.

NMR and circular dichroism studies of the duplex formed by the self-complementary DNA hexanucleotide d(C3G3) indicate that it is a B-type structure but differs from standard B-form. An analysis of NMR coupling constants within the deoxyribose moieties yields a 70% or greater contribution from pseudorotation phase angles corresponding to the C3'-exo conformation, a conformation similar to the C2'-endo conformation associated with B-form DNA. Intranucleotide interproton distances are consistent with a B-form structure, but some internucleotide distances are intermediate between A- and B-form structures. Circular dichroism spectra have B-form characteristics but also include an unusual negative band at 282 nm. The solution spectroscopic results are in contrast with X-ray crystallographic studies which find A-form structures for similar sequences.

The interactions of 4-nitroquinoline 1-oxide (NQO), a potent mutagen and carcinogen, with several self- and non-self-complementary deoxydinucleotides were probed by using absorption spectra of the charge transfer bands and 1H and 13C NMR spectra. Absorption spectra were analyzed by using Benesi-Hildebrand-type equations to yield stoichiometries and equilibrium constants of complex formation. Non-self complementary dimers form weak l:1 complexes [dpTpG:NQO, K(25 degrees C) = 22 M-1] while self-complementary dimers form strong 2:1 complexes [dpCpG)2:NQO, K(25 degrees C) = 2.2 X 10(4) M-2]. A mixture of dpTpG and dpCpA with NQO gives a 2:1 complexes [dpCpG)2:NQO, K(25 degrees C) = 2.2 X 10(4) M-2]. A mixture of dpTpG and dpCpA, K(25 degrees C) = 8.6 X 10(3) M-2]. Analyses of the changes in 13C and 1H NMR chemical shifts with complex formation gave approximate orientations for the intercalation of NQO with self-complementary dimer minihelixes. In the (dpCpG)2:NQO and (dpGpC)2:NQO complexes, the NO2 group of NQO probably lies in the major grove and the NO2, NO containing NQO ring is stacked near the purine imidazole ring. In the (dpTpA)2:NQO and (dpApT)2NQO complexes, the NO2 seems to project into the minor grove and the NQO benzenoid ring is over the purine imidazole ring.

Limited chemical bromination of poly[r(C-G)] (32% br8G, 26% br5C) results in partial modification of guanine C8 and cytosine C5, producing a mixture of A- and Z-RNA forms. The Z conformation in the brominated polynucleotide is stabilized at much lower ionic strength than in the unmodified polynucleotide. More extensive bromination of poly[r(C-G)] (greater than 49% br8G, 43% br5C) results in stabilization of a form of RNA having a Z-DNA-like (ZD) CD spectrum in low-salt, pH 7.0-7.5 buffers. Raising the ionic strength to 6 M NaBr or NaClO4 results in a transition in Br-poly[r(C-G)] to a Z-RNA (ZR) conformation as judged by CD spectroscopy. At lower ionic strength Z-DNA-like (ZD) and A-RNA conformations are also present. 1H NMR data demonstrate a 1/1 mixture of A- and Z-RNAs in 110 mM NaBr buffer at 37 degrees C. Nuclear Overhauser effect (NOE) experiments permit complete assignments of GH8, CH6, CH5, GH1', and CH1' resonances in both the A- and Z-forms. GH8----GH1' NOEs demonstrate the presence of both A- and Z-form GH8 resonances in slow exchange on the NMR time scale. The NMR results indicate that unbrominated guanine residues undergo transition to the syn conformation (Z-form). Raman scattering data are consistent with a mixture of A- and Z-RNAs in 110 mM NaCl buffer at 37 degrees C. Comparison with the spectrum of Z-DNA indicates that there may be different glycosidic torsion angles in Z-RNA and Z-DNA [Tinoco, I., Jr., Cruz, P., Davis, P., Hall, K., Hardin, C. C., Mathies, R. A., Puglisi, J. D., Trulson, M. O., Johnson, W. C., & Neilson, T. (1986) in Structure and Dynamics of RNA, pp 55-68, Plenum, New York].(ABSTRACT TRUNCATED AT 250 WORDS)

Seven dinucleoside monophosphates containing epsilonA (1,N6-ethenoadenosine) and 2'-O-methylcytidine were studied by 360-MHz proton magnetic resonance and compared with unmodified dimers and component monomers at 4, 20, 45, and 75 degrees C. These studies show that the dimers exhibit preference for the gg and g'g' conformations for the C-4'-C-5' and C-5'-O-5' bonds, respectively, and that dimerization induces an increase of the population and inflexibility of the 3'-endo conformations for the ribose ring. Three stacked (or stable) conformations for dimers, I, II, and III, in equilibrium with an unstacked (or open) form in solution, are suggested by dimerization shifts of ribose protons. Conformation I exhibits anti, gg, 3'-endo, phi' = 203 to approximately 211 degrees, omega' = 300 degrees, omega = 290 degrees, g'g', gg, 3'-endo, and anti conformation from the 5' end to the 3' end of the dimer. Conformation II shows anti, gg, 3'-endo, phi' = 203-211 degrees, omega = 30 degrees, omega = 100 degrees, g'g', gg, 3'-endo, and anti conformation. Conformation III is anti, gg, 2'-endo, phi' = 260 degrees, omega' = 50 degrees, omega = 220 degrees g'g', gg, 3'-endo, and anti (x approximately 100 degrees) conformation. The dimers, PupPu and PupPy, prefer conformations I and II, while PypPu and PypPy prefer conformation II. Introduction of epsilonA for the base of -pN induces an increase of conformations II and III, while the epsilonA substitution for the Np- residue induces an increase of conformation I. 2'-O-methylation of the Cp- residue of CpC decreases conformation I and increases conformation II. Based on the stable solution conformations of these dimers, a possible conformation of the anticodon loop is proposed, which is an alternative to the one observed in the crystal of tRNAPhe.

The deoxyoligonucleotide d(GGATGGGAG).d(CTCCCATCC) is a portion of the gene recognition sequence of transcription factor IIIA (TFIIIA). The crystal structure of this oligonucleotide was shown to be A-form (Mc Call, M., Brown, T., Hunter, W.N., and Kennard, O. 1986 Nature 322, 661-664). The present study employs NMR, optical, chemical and enzymatic techniques to investigate the solution structure of this DNA 9-mer. NMR COSY experiments indicate 16 of the 18 residues are predominantly south (C2'-endo) sugar conformation. NMR NOESY indicates glycosidic angles in the range predicted for B-form DNA as opposed to A-form. Related DNA and RNA self-complementary 18-mer sequences, d(GGATGGGAGC-TCCCATCC), with U substituted for T in RNA, were studied by circular dichroism. CD spectra support B-form structures for the DNA 9-mer and the DNA 18-mer, and A-form for the RNA 18-mer. High trifluoroethanol concentrations induce a B- to A-form transition in the DNA oligonucleotides. Enzymatic and chemical probes also illustrate significant differences between the DNA and the RNA oligonucleotides. We find no evidence to support an A-form conformation for the TFIIIA recognition sequence d(GGATGGGAG).d(CTCCCATCC) in solution.

The interactions of 4-nitroquinoline 1-oxide (NQO) with the four 5'-deoxyribonucleotides were probed using absorption spectra of the charge transfer bands and 1H and 13C nuclear magnetic resonance (NMR) spectra of nucleotide-NQO mixtures. Spectral data yielded equilibrium constants (K(dpG:NQO) = 16 M-1, K(dpA:NQO) = 12 M-1, K(dpT:NQO) = K(dpC:NQO) = 4 M-1) which suggest the preference of NQO for the guanine residue in a DNA. This is in agreement with the data of Okano, T., et al. [(1969) Gann 60, 295]. From 13C and 1H NMR data on nucleosides, a structure for the dpG:NQO complex is proposed.

Structures for all sequences containing less than 1790 nucleotides in the 2600 nucleotide late region of the SV40 virus have been computed and saved on magnetic tape. Previously the longest sequence whose secondary structure was calculated in a single computer run contained 950 nucleotides. In the past, analysis of long molecules required numerous repeated, partially overlapping computations on much shorter segments. The structure obtained for the late half of the SV40 is Y-shaped with two unequal arms. It has 52 short hairpins. Two long range interactions between nucleotides near 650 and 1350 and between 1450 and 2450 appear to play an important role. The first is within the 16S intron; the second is in the 3' exon. The 5' and 3' ends of the molecule are close to each other and are found in the major elongated stem in the vicinity of the fork.

The lifetimes for exchange of the imino protons in the dodecanucleotide d(C-G-C-G-A-A-T-T-C-G-C-G) upon binding of netropsin and/or actinomycin have been measured by proton nuclear magnetic resonance experiments. At high temperature these lifetimes were found to measure the lifetimes for opening of the base pairs in the double helix. Comparison of the opening rates in the dodecamer with those in the complex with netropsin (which binds at the -A-A-T-T- sequence) shows that there is not only a large kinetic stabilization of the A . T base pairs at the binding site but also a significant stabilization of the G . C base pairs adjacent to the netropsin binding site. For the complex with actinomycin, which intercalates at the G-C sites in the double strand, the lifetimes of the base pairs at the binding site increase upon binding of actinomycin, and the A . T base pairs in the central core are slightly kinetically destabilized by the actinomycin binding. The activation energies for exchange of the imino protons were also measured in the complexes and indicate that the mechanism for exchange of the imino protons is individual base-pair opening, where one base pair opens independently of the others. The effects of drug binding on the dynamics of individual base pairs in a double-stranded helix are discussed.

The relation between DNA polymerase fidelity and base pairing stability is investigated by using DNA primer-template duplexes that contain a common 9-base template sequence but have either correct (A.T) or incorrect (G.T, C.T, T.T) base pairs at the primer 3' terminus. Thermal melting and enzyme kinetic measurements are compared for each kind of terminus. Analysis of melting temperatures finds that differences between the free energy changes upon dissociation (delta delta Go) are only 0.2, 0.3, and 0.4 kcal.mol-1 (1 cal = 4.18 J) for terminal A.T compared to G.T, C.T, and T.T mispairs, respectively, at 37 degrees C. We show that enthalpy changes are directly correlated with entropy changes for normal and abnormal base pairs in DNA in aqueous solution and that delta delta Go values are small because of near cancellation of corresponding enthalpy and entropy components. The kinetics of elongating primer termini are measured with purified Drosophila DNA polymerase alpha. The matched A.T terminus is found to be extended approximately 200 times faster than a G.T mismatch and 1400 and 2500 times faster than C.T and T.T mismatches, respectively. Enzymatic discrimination against elongating mismatched termini is based mainly on Km rather than Vmax differences. From Km at 37 degrees C, we find delta delta Go values of 2.6-3.7 kcal.mol-1, about an order of magnitude greater than indicated by melting data. A similar measurement of nucleotide insertion kinetics has previously found rates of forming A.T base pairs to be 500 times greater than G.T mispairs and 20,000 times greater than C.T and T.T mispairs. Here also, Km differences are mainly responsible for discrimination and indicate even larger delta delta Go values (4.3-4.9 kcal.mol-1). Thus, free energy differences between correct and incorrect base pairs in the active site cleft of polymerase appear to be greater than 10 times as large as in aqueous medium. We explore the idea that a binding cleft that snugly fits correct base pairs and excludes water at the active site may amplify base-pair free energy differences by reducing entropy differences and increasing enthalpy differences sufficiently to account for nucleotide insertion and extension fidelity.

The thermal stabilities of oligodeoxyribonucleotide duplexes containing 2,6-diaminopurine (D) matched with each of the four normal DNA bases were determined by optical melting techniques. Comparison of optical melting curves yielded relative stabilities for the D-containing standard base pairs in an otherwise identical base-pair sequence. The D:T pair was found to be more stable than the A:T pair in dC3DG3:dC3TG3, as stable as the A:T in dCT3DT3G:dCA3TA3G, and less stable than the A:T in dCA3DA3G:dCT7G. The order of stabilities for X:Y in the DNA duplex dCA3XA3G:dCT3YT3G is: (A:T) greater than (T:D) congruent to (D:T) greater than or equal to (T:A) greater than (C:D) congruent to (D:A) congruent to (D:G) greater than or equal to (D:C) congruent to (G:D) congruent to (D:D) greater than or equal to (A:D). Implications of these results for design of DNA oligonucleotide probes are discussed.