A monoclonal antibody specific for the duplex DNA poly[d(TC)].poly[d(GA)]

Although most duplex DNAs are not immunogenic some synthetic DNAs such as poly[d(Tm5C)].poly[d(GA)] are weakly immunogenic allowing the production of monoclonal antibodies. The specificity of one of these antibodies, Jel 172, was investigated in detail by a competitive solid-phase radioimmune assay. Jel 172 bound well to poly[d(TC)].poly[d(GA)] but not to other duplex DNAs such as poly[d(TTC)].poly[d(GAA)] and poly[d(TCC)].poly[d(GGA)]. The binding to poly[d(Br5UC)].poly[d(GA)] was enhanced while that to poly[d(TC)].poly[d(IA)] was decreased compared to poly[d(TC)].poly[D(GA)]. Thus, not only is the antibody very specific for a sequence of duplex DNA but it also appears to recognize functional groups in both grooves of the helix.     

Synthetic repeating sequence DNAs containing phosphorothioates: nuclease sensitivity and triplex formation.

More than twenty repeating sequence DNAs containing phosphorothioates were prepared from the appropriate dXTPs with DNA polymerase I. The Tms of the modified DNAs were all lower than the parent polymers. A phosphorothioate group 5' to a pyrimidine gave rise to a large decrease than 5' to a purine, e.g., poly(dA).poly(dT) = 50 degrees; poly(dsA).poly(dT) = 44 degrees; poly(dA).poly(dsT) = 33 degrees; and poly(dsA).poly(dsT) = 26 degrees. The presence of phosphorothioate groups had a dramatic effect on triplex formation; poly[d(TC)].poly[d(sGsA)] spontaneously dismutases to a triplex at pH 8 whereas triplex formation in poly[d(sTsC)].poly[d(GA)] was inhibited. Surprisingly poly(dsG).poly(dC) had a Tm which initially decreased with increasing ionic strength. Resistance to digestion with pancreatic DNAse I did not correlate with phosphorothioate content. Poly[d(AsT)], poly[d(TsC)].poly[d(sGA)] and poly[d(sTG)].poly[d(sCA)] were resistant whereas poly[d(sAT)] and poly[d(sTsTG)].poly[d(CsAsA)] were rapidly degraded. Thus phosphorothioate groups cause small conformational changes and may reveal new families of conformational polymorphisms.     

A monoclonal antibody to triplex DNA binds to eucaryotic chromosomes.

A monoclonal antibody (Jel 318) was produced by immunizing mice with poly[d(TmC)].poly[d(GA)].poly[d(mCT) which forms a stable triplex at neutral pH. Jel 318 did not bind to calf thymus DNA or other non pyrimidine.purine DNAs such as poly[d(TG)].poly[d(CA)]. In addition the antibody did not recognize pyrimidine.purine DNAs containing mA (e.g. poly[d(TC)].poly[d(GmA)]) which cannot form a triplex since the methyl group blocks Hoogsteen base-pairing. The binding of Jel 318 to chromosomes was assessed by immunofluorescent microscopy of mouse myeloma cells which had been fixed in methanol/acetic acid. An antibody specific for duplex DNA (Jel 239) served as a control. The fluorescence due to Jel 318 was much weaker than that of Jel 239 but binding to metaphase chromosomes and interphase nuclei was observed. The staining by Jel 318 was unaffected by addition of E. coli DNA but it was obliterated in the presence of triplex. Since an acid pH favours triplex formation, nuclei were also prepared from mouse melanoma cells by fixation in cold acetone. Again Jel 318 showed weak but consistent staining of the nuclei. Therefore it seems likely that triplexes are an inherent feature of the structure of eucaryotic DNA.     

Rotation of periphery methylpyridine of meso-tetrakis(n-N-methylpyridiniumyl)porphyrin (n = 2, 3, 4) and its selective binding to native and synthetic DNAs

By utilizing circular and linear dichroism, the binding mode of meso-tetrakis(n-N-methylpyridiniumyl)porphyrin (n = 2, 3, 4) to various DNAs was studied in this work. 2-N-(methylpyridiniumyl)porphyrin(o-TMPyP), in which rotation of the periphery pyridinium ring is prevented, exhibits similar spectral properties when bound to DNA, poly[d(G-C)(2)] and poly[d(A-T)(2)], suggesting a similar binding mode. Close analysis of the spectral properties led us to conclude that o-TMPyP sits in the major groove. However, both 3-N- and 4-N-(methylpyridiniumyl)porphyrin (m- and p-TMPyP), of which the periphery pyridinium ring is free to rotate, intercalate between the basepairs of DNA and poly[d(G-C)(2)]. In the presence of poly[d(A-T)(2)], m-TMPyP exhibits a typical bisignate excitonic CD spectrum in the Soret band, while p-TMPyP shows two positive CD bands. The excitonic CD spectrum of the m-TMPyP-poly[d(A-T)(2)] complex and the positive CD band of the o-TMPyP-poly[d(A-T)(2)] complex were not affected by the presence of the minor groove binding drug, 4',6-diamidino-2-phenylindole (DAPI), indicating that this porphyrin is bound in the major groove. In contrast, two positive CD bands of the p-TMPyP-poly[d(A-T)(2)] complex altered in the presence of DAPI. From the changes in CD spectrum and other spectral properties, a few possible binding modes for p-TMPyP to poly[d(A-T)(2)] are suggested.     

The analysis of circular dichroism spectra of natural DNAs using spectral components from synthetic DNAs

We have tested 21 different basis sets of synthetic DNA circular dichroism spectra and have slected one for use in spectral analyses of natural DNAs. This “standard” set consists of spectra of eight polymers: poly[d(A-A-T)·d(A-T-T)], poly[d(A-G-G)·d(C-C-T)], poly[d(A-T)·d(A-T)], poly[d(G-C)·d(G-C)], poly[d(A-G)·d(C-T)], poly[d(A-C)·d(G-T)], poly[d(A-T-C)·d(G-A-T)], and poly[d(A-G-C)·d(G-C-T)]. This basis set, applied according to the first-neighbor polymer procedure of Gray and Tinoco, allows a more uniformly accurate spectral analysis of six natural complex DNAs and eight (A+T)-rich satellite DNAs for base composition and first-neighbor frequencies than was previously possible. We find that spectra of poly[d(A)·d(T)] and/or poly[d(A-C-T-)·d(A-G-T)] are not generally required for good analysis results but we show in this and the following paper that these spectra are needed for the most accurate analyses of some satellite DNAs.     

Poly(pyrimidine) . poly(purine) synthetic DNAs containing 5-methylcytosine form stable triplexes at neutral pH

Poly(pyrimidine) . poly(purine) tracts have been discovered in the 5'-flanking regions of many eucaryotic genes. They may be involved in the regulation of expression since they can be mapped to the nuclease-sensitive sites of active chromatin. We have found that poly(pyrimidine) . poly(purine) DNAs which contain 5-methylcytosine (e.g. poly[d(Tm5C)] . poly[d(GA)]) will form a triplex at a pH below 8. In contrast, the unmethylated analogue, poly[d(TC)] . poly[d(GA)] only forms a triplex at pHs below 6. Synthetic DNAs containing repeating trinucleotides and poly[d(Um5C)] . poly[d(GA)] behave in a similar manner. Thus the stability of a triplex can be controlled by methylation of cytosine. This suggests a model for the regulation of expression based upon specific triplex formation on the 5'-side of eucaryotic genes.     

The binding of fd gene 5 protein to polydeoxynucleotides: evidence from CD measurements for two binding modes

Circular dichroism measurements were used to study the binding of fd gene 5 protein to fd DNA, to six polydeoxynucleotides (poly[d(A)], poly[d(T)], poly[d(I)], poly[d(C)], poly[d(A-T)], and the random copolymer poly[d(A,T)]), and to three oligodeoxynucleotides (d(pA)20, d(pA)7, and d(pT)7). Titrations of these DNAs with fd gene 5 protein were generally done in a low ionic strength buffer (5 mM Tris-HCl, pH 7.0 or 7.8) to insure tight binding, needed to obtain stoichiometric endpoints. By monitoring the CD of the nucleic acids above 250 nm, where the protein has no significant intrinsic optical activity, we found that there were two modes of binding, with the number of nucleotides covered by a gene 5 protein monomer (n) being close to either 4 or 3. These stoichiometries depended upon which polymer was titrated as well as upon the protein concentration. Single endpoints at nucleotide/protein molar ratios close to 3 were found during titrations of poly[d(T)] and fd DNA (giving n = 3.1 and 2.8 +/- 0.2, respectively), while CD changes with two apparent endpoints at nucleotide/protein molar ratios close to 4 and approximately 3 were found during titrations of poly[d(A)], poly[d(I)], poly[d(A-T)], and poly[d(A,T)] (with the first endpoints giving n = 4.1 4.0, 4.0, and 4.1 +/- 0.3, respectively). Calculations showed that the CD changes we observed during these latter titrations were consistent with a switch between two non-interacting binding modes of n = 4 and n = 3. We found no evidence for an n = 5 binding mode. One implication of our results is that the Brayer and McPherson model for the helical gene 5 protein-DNA complex, which has 5 nucleotides bound per protein monomer (G. Brayer and A. McPherson, J. Biomol. Struct. and Dyn. 2, 495-510, 1984), cannot be correct for the detailed solution structure of the complex. We interpreted the CD changes above 250 nm upon binding of the gene 5 protein to single-stranded DNAs to be the result of a slight unstacking of the bases, along with a significant alteration of the CD contributions of the individual nucleotides in the case of A-and/or T-containing DNAs. Interestingly, CD contributions attributed to nearest-neighbor interactions in free poly[d(A-T)], poly[d(A,T)], poly[d(A)], and poly[d(T)] were partially maintained in the CD spectra of the protein-saturated polymers, so that neighboring nucleotides, when bound to the protein at 20 degrees C, appeared to interact with one another in much the same manner as in the free polymers at 50 degrees C.(ABSTRACT TRUNCATED AT 250 WORDS)     

Binding mode of porphyrins to poly[d(A-T)(2)] and poly[d(G-C)(2)

We examined the binding geometry of Co-meso-tetrakis (N-methyl pyridinium-4-yl)porphyrin, Co-meso-tetrakis (N-n-butyl pyridinium-4-yl)porphyrin and their metal-free ligands to poly[d(A-T)(2)] and poly[d(G-C)(2)] by optical spectroscopic methods including absorption, circular and linear dichroism spectroscopy, and fluorescence energy transfer technique. Signs of an induced CD spectrum in the Soret band depend only on the nature of the DNA sequence; all porphyrins exhibit negative CD when bound to poly[d(G-C)(2)] and positive when bound to poly[d(A-T)(2)]. Close analysis of the linear dichroism result reveals that all porphyrins exhibit outside binding when complexed with poly[d(A-T)(2)], regardless of the existence of a central metal and side chain. However, in the case of poly[d(G-C)(2)], we observed intercalative binding mode for two nonmetalloporphyrins and an outside binding mode for metalloporphyrins. The nature of the outside binding modes of the porphyrins, when complexed with poly[d(A-T)(2)] and poly[d(G-C)(2)], are quite different. We also demonstrate that an energy transfer from the excited nucleo-bases to porphyrins can occur for metalloporphyrins.     

The alternating conformation of analogues of poly[d(AT)].

Synthetic DNAs were prepared containing 6-methyl adenine (m6A) in place of adenine and 5-ethyl uracil (Et5U) or 5-methoxymethyl uracil (Mm5U) in place of thymine. All three modifications destabilized duplex DNAs to varying degrees. The binding of ethidium was studied to analogues of poly[d(AT)]. There was no evidence of cooperative binding and the "neighbour exclusion rule" was obeyed in all cases although the binding constant to poly[d(m6AT)] was approximately 6 fold higher than to poly[d(AT)]. 31P NMR spectra were recorded in increasing concentrations of CsF. Poly[d(AEt5U)] showed two well-resolved signals separated by 0.55 ppm in 1 M CsF compared to 0.32 ppm for poly[d(AT)] under identical conditions. In contrast, poly[d(AMm5U)] and poly[d(m6AT)] showed two signals separated by 0.28 ppm and 0.15 ppm respectively, only when the concentration of CsF was raised to 2 M. The signals for poly[d(AT)] in 2 M CsF were better resolved and were separated by 0.41 ppm. These results suggest that minor modifications to the bases may have conformational effects which could be recognized by DNA-binding proteins.     

Structure of the alpha-form of poly[d(A)].poly[d(T)] and related polynucleotide duplexes

The alpha-form of poly[d(A)].poly[d(T)], observed in fibers at high (greater than 80%) relative humidity, is a 10-fold double-helical structure of pitch 3.2 nm. This new X-ray analysis shows that the two strands of the double helix are of the same kind conformationally and both B-like in containing C-2'-endo-puckered deoxyribose rings. Nevertheless, the two strands are different enough for the overall morphology of the duplex to resemble that of the heteromerous model for the drier (beta) form of poly[d(A)].poly[d(T)] in which one strand has C-2'-endo rings and the other C-3'-endo. Since the orientations of the bases in poly[d(A)].poly[d(T)] are persistently different from those of classical B-DNA it is likely that there will be local bending (about 10 degrees) at the junctions between general sequence tracts and the oligo[d(A)].oligo[d(T)] tracts that occur in some native DNAs. The conclusions about the structure of alpha-poly[d(A)].poly[d(T)] are reinforced by independent analyses of similar X-ray diffraction patterns from poly[d(A)].poly[d(U)] and poly[d(A-I)].poly[d(C-T)].     

A comparison of the circular dichroism spectra of synthetic DNA sequences of the homopurine . homopyrimidine and mixed purine- pyrimidine types.

We have obtained the ultraviolet circular dichroism spectra of two repeating trinucleotide DNAs, poly [d(A-G-G).d(C-C-T)] and poly[d(A-A-G).d(C-T-T)], that have all purines on one strand and all pyrimidines on the other. These spectra, together with spectra of other synthetic polymers, can be combined to give 3 first-neighbor calculations of the spectrum of poly[d(A).d(T)] and 2 first-neighbor calculations of the spectrum of poly [d(G).d(C)]. The results show (1) that first-neighbor calculations utilizing only spectra of homopurine.homopyrimidine DNA sequences are no more accurate than are similar calculations that involve spectra of mixed purine-pyrimidine sequences, demonstrating that double-stranded homopurine.homopyrimidine sequences do not obviously belong to a special class of secondary conformations, and (2) that the wavelength region above 250 nm in the CD spectra of synthetic DNAs is least predictable from first-neighbor equations, probably because this region is especially sensitive to sequence-dependent conformational differences.     

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)].     

Effect of cesium on the volume of the helix-coil transition of dA.dT polymers and their ligand complexes

The pressure dependence of the helix–coil transition of poly(dA)∙poly(dT) and poly[d(A-T)]·poly[d(A-T)] in aqueous solutions of NaCl and CsCl at concentrations between 10 and 200 mM is reported and used to calculate the accompanying volume change. We also investigated the binding parameters and volume change of ethidium bromide binding with poly(dA)∙poly(dT) and poly[d(A-T)]·poly[d(A-T)] in aqueous solutions of these two salts. The volume change of helix–coil transition of poly(dA)∙poly(dT) in Cs⁺-containing solutions differs by less than 1 cm³ mol^− 1 from the value measured when Na⁺ is the counter-ion. We propose that this insensitivity towards salt type arises if the counter-ions are essentially fully hydrated around DNA and the DNA conformation is not significantly altered by salt types. Circular dichroism spectroscopy showed that the previously observed large volumetric disparity for the helix–coil transition of poly[d(A-T)]·poly[d(A-T)] in solutions containing Na⁺ and Cs⁺ is likely result of a Cs⁺-induced conformation change that is specific for poly[d(A-T)]·poly[d(A-T)]. This cation-specific conformation difference is mostly absent for poly(dA)∙poly(dT) and EB bound poly[d(A-T)]·poly[d(A-T)].     

The stability of polypurine tetraplexes in the presence of mono- and divalent cations.

As with other guanine-rich sequences, poly[d(GGA)], poly[d(GA)] and poly[d(GAA)] probably form four-stranded or tetraplex structures. Thermal denaturation profiles were measured for these polymers at pH8 in the presence of Na+, NH4+, K+, Cs+, Mg2+, Ca2+ and Ba2+. For poly[d(GA)], Na+, NH4+, K+ stabilize the tetraplex to similar extents and the Tm increases with increasing ionic strength. In contrast the Tms with Mg2+, Ca2+ and Ba2+ are significantly different and reach maxima at about 5mM of cation. The tetraplex from poly [d(GAA)] behaves in a similar manner. Thermal denaturation profiles for poly[d(GGA)] yield transitions whose hyperchromicity depends both on the concentration and nature of the ion. A reversible cooperative transition is not observed at concentrations greater than 0.15M K+, 1mM Ca2+ or 0.3 mM Ba2+ and hysteresis is evident at some concentrations. These results are consistent with the idea that K+ and ions of a similar size can form a coordination complex with the 6-Keto group of eight guanines (G8-DNA). Unlike the tetraplex polymer this G8-DNA does not melt cooperatively.     

Volume and hydration changes of DNA-ligand interactions

We report the volumetric and other thermodynamic properties of ethidium bromide (EB), propidium iodide (PI) and daunomycin (DAU) intercalating with poly(dA).poly(dT), poly[d(A-T)].poly[d(A-T)], and poly[d(G-C)].poly[d(G-C)], respectively, as well as minor groove binder Hoechst 33258 binding with poly[d(A-T)].poly[d(A-T)]. The data were obtained using fluorescence titration and hydrostatic pressure measurements. Our thermodynamic data are combined with enthalpies from literature reports to analyze the thermodynamic characteristics of the different interactions. The differences are interpreted based on three processes related to hydration: I. burial of non-polar hydrophobic solvent accessible surface, II. burial of polar surface and formation of solute-solute H-bonds, and III. disruption of "structural" hydration. Sequence dependent conformational changes may also be important when comparing ligand binding to different DNA sequences. We conclude that a combination of different thermodynamic parameters, especially volume change, is essential in order to understand the role of hydration in the energetics of DNA-ligand interactions.     

The Binding of fd Gene 5 Protein to Polydeoxynucleotides: Evidence from CD Measurements for Two Binding Modes

Abstract

Circular dichroism measurements were used to study the binding of fd gene 5 protein to fd DNA, to six polydeoxynucleotides (poly(d(A)], poly[d(T)], poly[d(I)], poly[d(C)], poly[d(A-T)], and the random copolymer poly[d(A,T)]), and to three oligodeoxynucleotides (d(pA)₂₀, d(pA)₇, and d(pT)₇). Titrations of these DNAs with fd gene 5 protein were generally done in a low ionic strength buffer (5 mM Tris-HCl, pH 7.0 or 7.8) to insure tight binding, needed to obtain stoichiometric endpoints. By monitoring the CD of the nucleic acids above 250 nm, where the protein has no significant intrinsic optical activity, we found that there were two modes of binding, with the number of nucleotides covered by a gene 5 protein monomer (n) being close to either 4 or 3. These stoichiometrics depended upon which polymer was titrated as well as upon the protein concentration. Single endpoints at nucleotide/protein molar ratios close to 3 were found during titrations of poly[d(T)] and fd DNA (giving n = 3.1 and 2.8 ± 0.2, respectively), while CD changes with two apparent endpoints at nucleotide/protein molar ratios close to 4 and approximately 3 were found during titrations of poly[d(A)], poly[d(I)], poly[d(A-T)], and poly[d(A,T)) (with the first endpoints giving n = 4.1, 4.0, 4.0, and 4.1 ± 0.3, respectively). Calculations showed that the CD changes we observed during these latter titrations were consistent with a switch between two non- interacting binding modes of n = 4 and n = 3. We found no evidence for an n = 5 binding mode. One implication of our results is that the Brayer and McPherson model for the helical gene 5 protein-DNA complex, which has 5 nucleotides bound per protein monomer (G. Brayer and A. McPherson, J. Biomol Struct, and Dyn. 2, 495-510, 1984), cannot be correct for the detailed solution structure of the complex.

We interpreted the CD changes above 250 nm upon binding of the gene 5 protein to single-stranded DNAs to be the result of a slight unstacking of the bases, along with a significant alteration of the CD contributions of the individual nucleotides in the case of A- and/or T-containing DNAs, Interestingly, CD contributions attributed to nearest-neighbor interactions in free poly[d(A-T)], poly[d(A,T)], poly[d(A)], and poly[d(T)] were partially maintained in the CD spectra of the protein-saturated polymers, so that neighboring nucleotides, when bound to the protein at 20°C, appeared to interact with one another in much the same manner as in the free polymers at 50°C. Finally, we found that the protein tyrosyl CD band at 228.5 nm decreased 39-42% when the protein bound to poly[d(A)] or poly[d(T)], but this band decreased no more than 9% when the gene 5 protein bound to short A- or T-containing oligomers. Thus, at least one tyrosyl residue has a significantly altered optical activity only when the DNA substrate is long enough either to cause a transition to a different protein conformation or to allow additional protein-protein contacts between adjacent helical turns of the DNA-protein complex.     

Binding of ethidium ion to left-handed Z-RNA induces a cooperative transition to right-handed RNA at the intercalation site

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)     

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.     

The vacuum UV CD bands of repeating DNA sequences are dependent on sequence and conformation

CD spectra were obtained for eight synthetic double-stranded DNA polymers down to at least 175 nm in the vacuum uv. Three sets of sequence isomers were studied: (a) poly[d(A-C).d(G-T)] and poly[d(A-G).d(C-T)], (b) poly[d(A-C-C).d(G-G-T)] and poly[d(A-C-G).d(C-G-T)], and (c) poly[d(A).d(T)], poly[d(A-T).d(A-T)], poly[d(A-A-T).d(A-T-T)], and poly[d(A-A-T-T).d(A-A-T-T)]. There were significant differences in the CD spectra at short wavelengths among each set of sequence isomers. The (G.C)-containing sequences had the largest vacuum uv bands, which were positive and in the wavelength range of 180-191 nm. There were no large negative bands at longer wavelengths, consistent with the polymers all being in right-handed conformations. Among the set of sequences containing only A.T base pairs, poly[d(A).d(T)] had the largest vacuum uv CD band, which was at 190 nm. This CD band was not present in the spectra of the other (A.T)-rich polymers and was absent from two first-neighbor estimations of the poly[d(A).d(T)] spectrum obtained from the other three sequences. We concluded that the sequence dependence of the vacuum uv spectra of the (A.T)-rich polymers was due in part to the fact that poly[d(A).d(T)] exists in a noncanonical B conformation.     

Pressure-jump study of the kinetics of ethidium bromide binding to DNA

Pressure-jump chemical relaxation has been used to investigate the kinetics of ethidium bromide binding to the synthetic double-stranded polymers poly[d(G-C)] and poly[d(A-T)] in 0.1 M NaCl, 10 mM tris(hydroxymethyl)aminomethane hydrochloride, and 1 mM ethylenediaminetetraacetic acid, pH 7.2, at 24 degrees C. The progress of the reaction was followed by monitoring the fluorescence of the intercalated ethidium at wavelengths greater than 610 nm upon excitation at 545 nm. The concentration of DNA was varied from 1 to 45 microM and the ethidium bromide concentration from 0.5 to 25 microM. The data for both polymers were consistent with a single-step bimolecular association of ethidium bromide with a DNA binding site. The necessity of a proper definition of the ethidium bromide binding site is discussed: it is shown that an account of the statistically excluded binding phenomenon must be included in any adequate representation of the kinetic data. For poly[d(A-T)], the bimolecular association rate constant is k1 = 17 X 10(6) M-1 s-1, and the dissociation rate constant is k-1 = 10 s-1; in the case of poly[d(G-C)], k1 = 13 X 10(6) M-1 s-1, and k-1 = 30 s-1. From the analysis of the kinetic amplitudes, the molar volume change, delta V0, of the intercalation was calculated. In the case of poly[d(A-T)], delta V0 = -15 mL/mol, and for poly[d(G-C)], delta V0 = -9 mL/mol; that is, for both polymers, intercalation is favored as the pressure is increased.(ABSTRACT TRUNCATED AT 250 WORDS)