Determination of the kinetics of deuteration of DNA.RNA hybrids by ultraviolet spectroscopy

The kinetics of the hydrogen-deuterium exchange reactions of poly(dA).poly(rU) and poly(rA).poly(dT) has been examined, at pH 7.0 and at various temperatures in the 15-35 degrees C range, by stopped-flow ultraviolet spectrophotometry. For comparison, the deuteration kinetics of poly[d(A-T)].poly[d(A-T)] and poly(rA).poly(rU) has been reexamined. At 20 degrees C, the imino deuteration (NH----ND) rates of the two hybrid duplexes were found to be 1.5 and 1.8 s-1, respectively. These are nearly equal to the imino deuteration rates of poly[d(A-T)].poly[d(A-T)] (1.1 s-1) and poly(rA).poly(rU) (1.5 s-1) but appreciably higher than that of poly(dA).poly(dT) (0.35 s-1). It has been suggested that a DNA.RNA hybrid, an RNA duplex, and the AT-alternating DNA duplex have in general higher base-pair-opening reaction rates than the ordinary DNA duplex. The amino deuteration (NH2----ND2) rates, on the other hand, have been found to be 0.25, 0.28, and 0.33 s-1, respectively, for poly(dA).poly(rU), poly(rA).poly(dT), and poly[d(A-T)].poly[d(A-T)], at 20 degrees C. These are appreciably higher than that for poly(rA).poly(rU) (0.10 s-1). In general, the equilibrium constants (K) of the base-pair opening are considered to be greatest for the DNA.RNA hybrid duplex (0.05 at 20 degrees C), second greatest for the RNA duplex (0.02 at 20 degrees C), and smallest for the DNA duplex (0.005 at 20 degrees C), although the AT-alternating DNA duplex has an exceptionally great K (0.07 at 20 degrees C). From the temperature effect on the K value, the enthalpy of the base-pair opening was estimated to be 3.0 kcal/mol for the DNA.RNA hybrid duplex.     

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

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

UV irradiation of nucleic acids: formation, purification and solution conformational analysis of the '6-4 lesion' of dTpdT

Irradiation of dTpdT with 300 kJ/m2 of 254 nm produces numerous photo-products, one of which labeled dT6pd4T[1] was purified by HPLC. dT6pd4T has a UV spectrum (H20, pH 7) with lambda max = 326 nm and lambda min = 265 nm, and a P-31 NMR resonance at -3.46 ppm (normal dTpdT occurs at -4.01 ppm; TMP, 30 degrees C). 2-D COSY NMR spectra facilitated proton resonance assignments and 2-D NOESY spectra aided analysis of spatial orientation. Carbon-13 and proton-coupled P-31 NMR spectra of dT6pd4T were also obtained. These analyses indicate: C5=C6 of dT6p- is saturated and the -pd4T base is more aromatic; the dT6p- base possesses a configuration of 5R, 6S; dT6p- and -pd4T have anti-type glycosidic conformations; furanose conformation of dT6p- is mainly C3'-endo and that of -pd4T exists in a C3'-endo in equilibrium C3'-exo; exocyclic bonds gamma (C5'-C4'), beta (05'-C5') and epsilon (C3'-03') are non-classical rotamers; dihedral angle about epsilon (C3'-03') is smaller relative to dTpdT.     

Hydration of dA.dT polymers: role of water in the thermodynamics of ethidium and propidium intercalation

We report differences in the interaction of two structurally similar phenanthroline intercalators, ethidium and propidium, with poly(dA).poly(dT) and poly[d(A-T)] as a function of ionic strength based on titration microcalorimetry, fluorescence titration, and hydrostatic pressure measurements. Both ethidium and propidium bind more strongly to poly[d(A-T)].poly[d(A-T)] than to poly(dA).poly(dT). Ethidium intercalation into the latter polymer displays titrations with positive cooperativity; this is not found with propidium. The enthalpy of intercalation (delta H degrees) is exothermic for both dyes with poly[d(A-T)].poly[d(A-T)]; however, the value of this parameter is nearly zero in the case of poly(dA).poly(dT). The molar volume change (delta V degrees) accompanying dye intercalation is negative under all conditions for poly[d(A-T)].poly[d(A-T)] whereas it is positive for poly(dA).poly(dT). The changes observed in delta V degrees correlate well with the entropy changes derived from the titration and calorimetric data for this reaction. The results, interpreted in terms of the relative hydration of these two polymers, are consistent with a higher extent of hydration of poly(dA).poly(dT) relative to poly[d(A-T)].poly[d(A-T)].     

Kinetics of hydrogen-deuterium exchange in adenosine 5'-monophosphate, adenosine 3':5'-monophosphate, and poly(riboadenylic acid) determined by laser-Raman spectroscopy.

Pseudo-first-order rate constants governing the deuterium exchange of 8-CH groups in adenosine 5'-monophosphate, adenosine 3':5'-monophosphate, and poly(riboadenylic acid) (poly(rA)) were determined as a function of temperature in the range 20-90 degrees C by means of laser-Raman spectroscopy. For 5'-rAMP, the logarithm of the rate constant exhibits a strictly linear dependence on reciprocal temperature, i.e., kpsi = Ae-Ea/RT, with A = 2.3 X 10(14) hr-1 and Ea = 24.2 +/- 0.6 kcal/mol. For cAMP, above 50 degrees C, kpsi is nearly identical in magnitude and temperature dependence to that of 5'-rAMP. However, below 50 degrees C, isotope exchange in cAMP is much more rapid than in 5'-rAMP, characterized by a lower activation energy (17.7 kcal/mol) and frequency factor (9.6 X 10(9) hr-1). Exchange in poly(rA) is considerably slower than in 5'-rAMP at all temperatures, but like cAMP the in k vs. 1/T plot may be divided into high temperature and low temperature domains, each characterized by different Arrhenius parameters. Above 60 degrees C, poly(rA) gives Ea = 22.0 kcal/mol and A = 3.2 X 10(12) hr-1, while below 60 degrees C, Ea = 27.7 kcal/mol and A = 1.8 X 10(16) hr-1. Thus, increasing the temperature above 60 degrees C does not diminish the retardation of exchange in poly(rA) vis a vis 5'-rAMP. These results indicate that the distribution of electrons in the adenine ring of cAMP is altered by lowering the temperature below 50 degrees C, although no similar perturbation occurs for 5'-rAMP. Retardation of exchange in poly(rA) is most probably due to base stacking at lower temperatures and to steric hindrance from the ribopolymer backbone at higher temperatures. We also report the spectral effects of deuterium exchange on the vibrational Raman frequencies of 5'-rAMP, cAMP, and poly(rA) and suggest a number of new assignments for the 5' and cyclic ribosyl phosphate groups.     

Infrared and Raman studies show that poly(dA).poly(dT) and d(AAAAATTTTT)2 exhibit a heteronomous conformation in films at 75% relative humidity and a B-type conformation at high humidities and in solution

The decadeoxynucleotide d(AAAAATTTTT)2 in duplex form and the double-helical polynucleotide poly(dA).poly(dT) have been studied by Raman and infrared (IR) spectroscopy under a variety of environmental conditions. The IR spectra have been taken of cast films and compared to the IR spectra of the alternating poly(dA-dT), which shows clear B-genus and A-genus vibrational spectra under conditions of high (greater than 92%) and low (75%) relative humidity (RH). From the IR data, it is shown that d-(AAAAATTTTT)2 and poly(dA).poly(dT) adopt a B-genus conformation in films with high water content. When the relative humidity of the film is decreased, the IR spectra reflect a gradual evolution of the geometry of both d(AAAAATTTTT)2 and poly(dA).poly(dT) into a form intermediate between the B genus and A genus, but the IR spectrum of a pure A genus has not been obtained. In these DNAs at 75% RH, the IR bands of adenosine have the same frequencies as those found in poly(dA-dT) at 75% RH where the local furanose conformation is C3' endo/anti, but the thymidine frequencies do not resemble those of poly(dA-dT) at 75% RH but rather those of poly(dA-dT) at high humidities. It is concluded that both poly(dA).poly(dT) and d(AAAAATTTTT)2 adopt a fully heteronomous duplex geometry in cast films at low humidity. For studies in aqueous solution the Raman effect was employed. As a model for the heteronomous conformation in solution, the duplex poly(rA).poly(dT) was used.(ABSTRACT TRUNCATED AT 250 WORDS)     

Salt induced B----A transition of poly(dG).poly(dC) and the stabilization of A form by its methylation.

Raman spectra of poly(dG).poly(dC) have been observed in aqueous solutions at various ionic strengths, [NaCl] = 0.03 to 4 M, and at different temperatures, 10 to 60 degrees C. At 30 degrees C, and at [NaCl] = 0.03 M, it was found to have a B-form (with O4'endo-anti guanosine and C2'endo-anti cytidine), whereas, at [NaCl] = 4 M, an A form (with C3'endo-anti guanosine and C3'endo-anti cytidine). At 30 degrees C and [NaCl] = 1 M, namely at an intermediate state, a fraction of this molecules was considered to have a "heteronomous A" form (with O4'endo-anti guanosine and C3' endo-anti cytidine). At 60 degrees C and [NaCl] = 1 M, it assumes the B form, and at 10 degrees C and [NaCl] = 1 M, the A form. Cytosine-5-methylation was found to cause a marked stabilization of the A form. Even at [NaCl] = 0.1 M (at 30 degrees C), a substantial portion of poly(dG).poly(dm5C) was found to have a heteronomous form, in which the dG atrand is in the B form and the dC an A form; it never assumes a complete B form.     

Sequence-dependant polymorphism of DNA duplex in solutions

Raman spectra of six synthetic polydeoxyribonucleotide duplexes with different base sequences have been examined in aqueous solutions with different salt or nucleotide concentrations. Detailed conformational differences have been indicated between B and Z forms of poly[d(G-C)] X poly[d(G-C)], between B forms of poly[d(G-C)] X poly[d(G-C)] and poly[d(G-m5C)] X poly[d(G-m5C)], between A and B forms of poly(dG) X poly(dC), between B and "CsF" forms of poly[d(A-T)] X poly[d(A-T)], between B forms of poly[d(A-U)] X poly[d(A-U)] and poly[d(A-T)] X poly[d(A-T)], and between low- and high-salt (CsF) forms of poly(dA) X poly(dT). The Raman spectrum of calf-thymus DNA in aqueous solution was also observed and was compared with the Raman spectra of its fibers in A, B, and C forms.     

Unique requirements for template primers of DNA polymerase beta from rat ascites hepatoma AH130 cells.

The optimal condition for the rat DNA polymerase beta activity with (rA)n . (dT)12-18 as a template-primer was determined. The activity was remarkably affected by the concentration of the primer, (dT)12-18' and the mixing ratio of (dT)12-18 to (rA)n. DNA polymerase beta requires higher primer concentration (Km = 11.1 microM with respect to 3'-OH of the primer) than DNA polymerase gamma (Km = 0.04 microM) or oncornaviral DNA polymerase (Km = 0.08 microM) and the enzyme represented the maximum activity in the base ratio of 2:1 with (dT)12-18 and (rA)n suggesting the difference in reaction mechanisms of these enzymes. Under the optimized conditions, the specific activity of the near homogeneous preparation of DNA polymerase beta was 1,000,000 units per mg protein.     

Temperature dependence of the volumetric parameters of drug binding to poly[d(A-T)].Poly[d(A-T)] and Poly(dA).Poly(dT)

We report the temperature and salt dependence of the volume change (DeltaVb) associated with the binding of ethidium bromide and netropsin with poly(dA).poly(dT) and poly[d(A-T)].poly[d(A-T)]. The DeltaV(b) of binding of ethidium with poly(dA).poly(dT) was much more negative at temperatures approximately 70 degrees C than at 25 degrees C, whereas the difference is much smaller in the case of binding with poly[d(A-T)].poly[d(A-T)]. We also determined the volume change of DNA-drug interaction by comparing the volume change of melting of DNA duplex and DNA-drug complex. The DNA-drug complexes display helix-coil transition temperatures (Tm several degrees above those of the unbound polymers, e.g., the Tm of the netropsin complex with poly(dA)poly(dT) is 106 degrees C. The results for the binding of ethidium with poly[d(A-T)].poly[d(A-T)] were accurately described by scaled particle theory. However, this analysis did not yield results consistent with our data for ethidium binding with poly(dA).poly(dT). We hypothesize that heat-induced changes in conformation and hydration of this polymer are responsible for this behavior. The volumetric properties of poly(dA).poly(dT) become similar to those of poly[d(A-T)].poly[d(A-T)] at higher temperatures.     

Novel properties of DNA polymerase beta with poly(rA).oligo(dT) template-primer.

Purified DNA polymerase beta of calf thymus can utilize poly(rA).oligo(dT) as efficiently as poly(dA).oligo(dT) or activated DNA as a template primer. The poly(rA).oligo(dT)-dependent activity of DNA polymerase beta was found to differ markedly from the DNA-dependent activity of the same enzyme (with either activated calf thymus DNA or poly(dA).(dT)10) in the following respects. 1) Poly(rA)-dependent activity was strongly inhibited by natural DNA from various sources or synthetic deoxypolymer duplexes at very low concentrations (less than 0.5 microgram/ml) at which the DNA-dependent activity was affected to a much smaller extent, if at all. 2) Poly(rA)-dependent activity was inhibited by N-ethylmaleimide more strongly than DNA-dependent activity measured at 37 degrees C, while it was resistant to this reagent at 26 degrees C. 3) The curves of the activity versus substrate concentration were sigmoidal in the poly(rA)-dependent reaction but hyperbolic in the activated DNA-dependent reaction. A kinetic study suggested that the association of beta-enzyme protomers may be required to copy the poly(rA) strand.     

A solution structure for poly(rA).poly(dT) with different furanose pucker and backbone geometry in rA and dT strands and intrastrand hydrogen bonding of adenine 8CH

Equilibrium Raman spectra show that A- and B-form phosphodiester backbone geometries are both present in the solution structure of the RNA.DNA hybrid poly(rA).poly(dT) and that these arise from C3'-endo-rA and C2'-endo-dT nucleosides, respectively. Raman dynamic measurement of deuterium exchange of adenine 8CH groups reveals (i) a single kinetic class of rA conformers and (ii) extraordinary retardation of 8CH exchange in this class--more than 100-fold slower than in canonical DNA structures. The equilibrium and kinetic results, in conjunction with model building, indicate an unusual intrastrand hydrogen bond involving adenosine donor (8C-H) and acceptor (5'O) groups and a double-helical conformation in solution similar to that proposed for fibers at high relative humidity [Zimmerman, S. B., & Pheiffer, B. H. (1981) Proc. Natl. Acad. Sci. U.S.A. 78, 78-82]. In fibers of poly(rA).poly(dT) at low relative humidity, the Raman spectra indicate a conventional A-helix structure.     

Conformational transitions of duplex and triplex nucleic acid helices: thermodynamic analysis of effects of salt concentration on stability using preferential interaction coefficients.

For order-disorder transitions of double- and triple-stranded nucleic acid helices, the midpoint temperatures Tm depend strongly on a +/-, the mean ionic activity of uniunivalent salt. Experimental determinations of dTm/d ln a +/- and of the enthalpy change (delta H(o)) accompanying the transition in excess salt permit evaluation of delta gamma, the stoichiometrically weighted combination of preferential interaction coefficients, each of which reflects thermodynamic effects of interactions of salt ions with a reactant or product of the conformational transition (formula; see text) Here delta H(o) is defined per mole of nucleotide by analogy to delta gamma. Application of Eq. 1 to experimental values of delta H(o) and Tm yields values of delta gamma for the denaturation of B-DNA over the range of NaCl concentrations 0.01-0.20 M (Privalov et al. (1969), Biopolymers 8,559) and for each of four order-disorder transitions of poly rA.(poly rU)n, n = 1, 2 over the range of NaCl concentrations 0.01-1.0 M (Krakauer and Sturtevant (1968), Biopolymers 6, 491). For denaturation of duplexes and triplexes, delta gamma is negative and not significantly dependent on a +/-, but delta gamma is positive and dependent on a +/- for the disproportionation transition of poly rA.poly rU duplexes. Quantitative interpretations of these trends and magnitudes of delta gamma in terms of coulombic and excluded volume effects are obtained by fitting separately each of the two sets of thermodynamic data using Eq. 1 with delta gamma PB evaluated from the cylindrically symmetric Poisson-Boltzmann (PB) equation for a standard model of salt-polyelectrolyte solutions. The only structural parameters required by this model are: b, the mean axial distance between the projections of adjacent polyion charges onto the cylindrical axis; and a, the mean distance of closest approach between a salt ion center and the cylindrical axis. Fixing bMS and aMS for the multi-stranded (ordered) conformations, we determined the corresponding best fitted values of bSS and aSS for single-stranded RNA and DNA. The resulting best fitted values of aSS are systematically less than aDS by 2-4 A. Uncertainty in the best-fitted values of bSS is significantly lower than in the aSS, because bMS is known with relatively high precision and because the larger uncertainty in aMS has a relatively small effect on the best-fitted values of bSS:bSS = 3.2 +/- 0.6 A for single-stranded poly rA and poly rU; and bSS = 3.4 +/- 0.2 A for single-stranded DNA.(ABSTRACT TRUNCATED AT 400 WORDS)     

Investigations on the dynamic structures of adenine- and thymine-containing DNA.

The structures of poly(dA-dT), poly(dA-dBr5U) and of poly(dA).poly(dT) have been investigated in solution and in fibers, by Raman spectroscopy. Both the alternating poly(dA-dT), poly(dA-dBr5U) and non-alternating poly(dA).poly(dT) exhibit, in the region of sugar phosphate backbone vibrations, two bands of almost equal intensity at about 841 cm-1 and 817 cm-1. The analysis of the characteristic bands of thymine residues that are sensitive to sugar puckers gives indication of a significant displacement from the C(2')-endo conformer suggesting the adoption of alternative conformers such as O(4')-endo. In contrast, the diagnostic Raman bands for the sugar pucker of adenine residues suggest, instead, predominant adoption of C(2')-endo conformations. These Raman results are compatible with rapid dynamic changes of sugar puckers between C(2')-endo and O(4')-endo for the thymidine (and uridine) residues, whereas in adenine residues the sugar puckers fluctuate around the C(2')-endo pucker in all synthetic DNA molecules studied. Molecular dynamics simulations, performed on six different starting models using two distance-dependent dielectric functions epsilon(r) = 4 r and a sigmoidal dependence), all gave similar dynamic behavior in agreement with these Raman data and their interpretation. The mean calculated pseudorotation phases of the adenine residues are systematically higher (around C(2')-endo) than those of the thymine residues (close to O(4')-endo-C(1')-exo). Besides, the mean lifetimes of the thymine residues are 1.5 to 2.0-fold higher in the O(4')-endo than in the C(2')-endo domain, while those of the adenine residues are two to threefold higher in the C(2')-endo than in the O(4')-endo domain. In the Raman spectra of the alternating poly(dA-dBr5U), the splitting of a band into two components arising from the two contributions of ApBr5U and Br5UpA provides strong evidence for a repeating dinucleotide structure in solution. The calculated twist values averaged over the simulation runs are also systematically higher in the 5'T-A3' step (39 degrees) than in the 5'A-T3' step (33 degrees). Simultaneously, the calculated roll values are positive in the 5'T-A3' step (6 degrees) and negative in the 5'A-T3' step (-9 degrees), while the propeller twist values are about the same (-11 degrees to -16 degrees). On the other hand, in the homopolymer, the average twist value is close to 36 degrees with the roll angle close to 0 degrees and large propeller twist values (-20 degrees).     

Copper insertion facilitates water-soluble porphyrin binding to rA.rU and rA.dT base pairs in duplex RNA and RNA.DNA hybrids

The binding of the copper(II) complex of water-soluble meso-tetrakis(N-methylpyridinium-4-yl)porphyrin (TMPyP) to double-helical polynucleotides has been studied by optical absorption, circular dichroism (CD), and resonance Raman spectroscopic methods. The target polymers were RNA and RNA.DNA hybrids consisting of rA.rU, rI.rC, rA.dT, and rI.dC base pairs. Relative to the metal-free H(2)TMPyP [Uno, T., Hamasaki, K., Tanigawa, M., and Shimabayashi, S. (1997) Inorg. Chem. 36, 1676-1683], CuTMPyP binds to poly(rA).poly(dT) and poly(rA).poly(rU) with a greatly increased binding constant. The external self-stacking of the porphyrin on the surface of the polymers was evident from the strong conservative-type induced CD signals. The signal intensity correlated almost linearly with the number of stacking sites on the polymer except for poly(rA).poly(dT), which showed extraordinarily strong CD signals. Thus, the bound porphyrin may impose an ordered architecture on the polymer surface, the stacking being facilitated by the more planar nature of the CuTMPyP than the nonmetal counterpart. Resonance Raman spectra of the stacked CuTMPyP were indistinguishable from those of the intercalated one with positive delta(Cbeta-H) and negative delta(Cm-Py) bending shifts, and hence the stacked porphyrins are suggested to adopt a similar structure to that of intercalated ones. Porphyrin flattening by copper insertion opens a new avenue for medical applications of porphyrins, blocking biological events related to RNA and hybrids in malignant cells.     

Difference in the mechanisms of poly(dT) synthesis by DNA polymerases beta and gamma.

Poly(dT) products which were synthesized depending on (rA)n . (dT)12-18 as a template . primer by mammalian DNA polymerases beta and gamma were analyzed by alkaline sucrose gradient centrifugation. The size of the population of poly(dT) chains synthesized by DNA polymerase beta increased slowly and consistently during incubation up to at least 30 min. On the other hand, the product size with DNA polymerase gamma reached the final size (7 s) within 5 min and the number of products increased during further incubation. Comparison of product number per enzyme molecule suggests that DNA polymerase beta acts on multiple primers in a distributive fashion while DNA polymerase gamma completes poly(dT) chains of large size in a one-by-one fashion.     

Determination of nucleic acid backbone conformation by 1H NMR.

In DNA or RNA duplexes, the six-bond C3'-O3'-P-O5'-C5'-C4'-C3' backbone linkage connecting adjacent residues contains six torsion angles (epsilon, zeta, alpha, beta, gamma, delta) but only four protons. This seriously limits the ability to define the backbone conformation by NMR using purely 1H-1H distance geometry (DG) methods. The problem is further compounded by the inability to assign two of the four backbone protons, namely the poorly resolved H5' and H5' protons, and invariably leads to DG structures with poorly defined backbone conformations. We have developed and tested a reliable method to constrain the beta, gamma, and epsilon (and indirectly alpha and zeta) backbone torsion angles by lower-bound NOE distances to unassigned H5'/H5' resonances combined with either 1H line widths or the conservative use of sigma J measurements; the method relies only on 1H 2-D NMR data, does not involve any structural assumptions, and leads to much improved backbone convergence among DG structures. The C4'-C5' torsion angle gamma is constrained by lower-bound NOE distances from H2' and from H6/H8 to any H5'/H5', as well as by sigma JH4, coupling measurements in the 3.9-4.4 ppm region; delta is constrained by H1'-H4' NOE distances and by H3'-H4' and H3'-H2' J couplings in COSY data; epsilon is partially constrained by H3' line width and/or further constrained by subtracting the minimum possible sigma JH3'-H from the observed sigma JH3' (COSY) to arrive at the maximum possible JH3'-P, which is then converted to H3'-P distance bounds. The angle beta is partially constrained via H5'-P and H5'-P distance bounds consistent with the maximum H5'-P and H5'-P J couplings derived from the observed H5' and H5' line widths, while alpha and zeta are indirectly constrained by lower distance bounds on the observed (n)H1' to (n + 1)H5'/H5' NOEs combined with the prior partial constraints on beta, gamma, delta, and epsilon. The combined effects of these additional constraints in determining distance geometry structures have been demonstrated using a 12-base duplex, [d(GCCGTTAACGGC)]2. Coordinate RMSDs per atom between structures refined with these constraints from random-embedded DG structures, from ideal A-DNA, and from B-DNA starting structures were less than 0.4 A for the central 8 base pairs indicating good convergence. All backbone angles for the central 8 base pairs are very well constrained with less than 10 degrees variation in any of the 48 torsion angles.     

Theoretical studies of DNA-RNA hybrid conformations.

Molecular modelling has been used to probe the conformational preferences of double stranded DNA-RNA hybrids. As might be expected, the sugars of the DNA strand have higher conformational flexibility, but, for the majority of the repetitive sequences studied, these sugars prefer a C2-endo pucker, while ribose sugars uniformly adopt a C3-endo pucker. This gives rise to a strongly heteronomous duplex conformation. One exception to this rule involves the thymidine strand of poly(dT).poly(rA), which marginally prefers a C3-endo pucker. Our study further indicates that the DNA strands of the hybrids favour backbone torsions in the canonical B domain, rather than the modified values proposed on the basis of fibre diffraction studies. Backbone conformational transitions can nevertheless be induced leading to an alpha gamma-flip (alpha:gamma, g-/g(+)-->t/t) or to the alpha beta gamma-flip form proposed from fibre studies (alpha:beta:gamma, g-/t/g(+)-->t/g+/t). The latter transition is also found to be linked to BI-->BII transitions (epsilon:zeta, t/g(-)-->g-/t).     

Poly(dA).poly(dT) exists in an unusual conformation under physiological conditions: propidium binding to poly(dA).poly(dT) and poly[d(A-T)].poly[d(A-T)]

The binding of propidium to poly(dA).poly(dT) [poly(dA.dT)] and to poly[d(A-T)].poly[d(A-T)] [poly[d(A-T)2]] has been compared under a variety of solution conditions by viscometric titrations, binding studies, and kinetic experiments. The binding of propidium to poly[d(A-T)2] is quite similar to its binding to calf thymus deoxyribonucleic acid (DNA). The interaction with poly(dA.dT), however, is quite unusual. The viscosity of a poly(dA.dT) solution first decreases and then increases in a titration with propidium at 18 degrees C. The viscosity of poly[d(A-T)2] shows no decrease in a similar titration. Scatchard plots for the interaction of propidium with poly(dA.dT) show the classical upward curvature for positive cooperativity. The curvature decreases as the temperature is increased in binding experiments. A van't Hoff plot of the observed binding constants yields an apparent positive enthalpy of approximately +6 kcal/mol for the propidium-poly(dA.dT) interaction. Propidium binding to poly[d(A-T)2] shows no evidence for positive cooperativity, and the enthalpy change for the reaction is approximately -9 kcal/mol. Both the magnitude of the dissociation constants and the effects of ionic strength are quite similar for the dissociation of propidium from poly(dA-T)2] and from poly[d(A-T)2], suggesting that the intercalated states are similar for the two complexes. The observed association reactions, under pseudo-first-order conditions, are quite different. Plots of the observed pseudo-first-order association rate constant vs. polymer concentration have much larger slopes for propidium binding to poly[d(A-T)2] than to poly(dA.dT).(ABSTRACT TRUNCATED AT 250 WORDS)