Binding and reversible denaturation of double-stranded DNA by Ff gene 5 protein

The gene 5 protein (g5p) from Ff filamentous virus is a model single-stranded DNA (ssDNA) binding protein that has an oligonucleotide/oligosaccharide binding (OB)-fold structure and binding properties in common with other ssDNA-binding proteins. In the present work, we use circular dichroism (CD) spectroscopy to analyze the effects of amino acid substitutions on the binding of g5p to double-stranded DNA (dsDNA) compared to its binding to ssDNA. CD titrations of poly[d(A). d(T)] with mutants of each of the five tyrosines of the g5p showed that the 229-nm CD band of Tyr34, a tyrosine at the interface of adjacent protein dimers, is reversed in sign upon binding to the dsDNA, poly[d(A). d(T)]. This effect is like that previously found for g5p binding to ssDNAs, suggesting there are similarities in the protein-protein interactions when g5p binds to dsDNA and ssDNA. However, there are differences, and the possible perturbation of a second tyrosine, Tyr41, in the complex with dsDNA. Three mutant proteins (Y26F, Y34F, and Y41H) reduced the melting temperature of poly[d(A). d(T)] by 67 degrees C, but the wild-type g5p only reduced it by 2 degrees C. This enhanced ability of the mutants to denature dsDNA suggests that their binding affinities to dsDNA are reduced more than are their binding affinities to ssDNA. Finally, we present evidence that when poly[d(A). d(T)] is melted in the presence of the wild-type, Y26F, or Y34F proteins, the poly[d(A)] and poly[d(T)] strands are separately sequestered such that renaturation of the duplex is facilitated in 2 mM Na(+).     

Independent tyrosyl contributions to the CD of Ff gene 5 protein and the distinctive effects of Y41H and Y41F mutants on protein-protein cooperative interactions

The gene 5 protein (g5p) of the Ff virus contains five Tyr, individual mutants of which have now all been characterized by CD spectroscopy. The protein has a dominant tyrosyl 229-nm L(a) CD band that is shown to be approximately the sum of the five individual Tyr contributions. Tyr41 is particularly important in contributing to the high cooperativity with which the g5p binds to ssDNA, and Y41F and Y41H mutants are known to differ in dimer-dimer packing interactions in crystal structures. We compared the solution structures and binding properties of the Y41F and Y41H mutants using CD spectroscopy. Secondary structures of the mutants were similar by CD analyses and close to those derived from the crystal structures. However, there were significant differences in the binding properties of the two mutant proteins. The Y41H protein had an especially low binding affinity and perturbed the spectrum of poly[d(A)] in 2 mM Na(+) much less than did Y41F and the wild-type gene 5 proteins. Moreover, a change in the Tyr 229 nm band, assigned to the perturbation of Tyr34 at the dimer-dimer interface, was absent in titrations with the Y41H mutant under low salt conditions. In contrast, titrations with the Y41H mutant in 50 mM Na(+) exhibited typical CD changes of both the nucleic acid and the Tyr 229-nm band. Thus, protein-protein and g5p-ssDNA interactions appeared to be mutually influenced by ionic strength, indicative of correlated changes in the ssDNA binding and cooperativity loops of the protein or of indirect structural constraints.     

Effects of ssDNA sequences on non-sequence-specific protein binding

The circular dichroism (CD) spectra of single-stranded DNAs (ssDNAs) are significantly perturbed by the binding of single-stranded DNA binding proteins such as the Ff bacteriophage gene 5 protein (g5p) and the A domain of the 70 kDa subunit of human replication protein A (RPA70-A). These two proteins have similar OB-fold secondary structures, although their CD spectra at wavelengths below 250 nm differ greatly. The spectrum of g5p is dominated by a tyrosyl L(a) band at 229 nm, while that of RPA70-A is dominated by its beta secondary structure. Despite differences in their inherent spectral properties, these two proteins similarly perturb the spectra of bound nucleic acid oligomers. CD spectra of free, non-protein-bound ssDNAs are dependent on interactions of the nearest-neighboring nucleotides in the sequence. The CD spectra (per mol of nucleotide) of simple repetitive sequences 48 nucleotides in length and containing simple combinations of A and C are related by nearest-neighbor equations. For example, 3 x Deltaepsilon[d(AAC)(16)] = 3 x Deltaepsilon[d(ACC)(16)] + Deltaepsilon[d(A)(48)] - Deltaepsilon[d(C)(48)]. Moreover, nearest-neighbor equations relate the spectra of ssDNAs when they are bound by g5p, indicating that each type of perturbed nearest neighbor has a similar average structure within the binding site of the protein.     

CD measurements show that fd and IKe gene 5 proteins undergo minimal conformational changes upon binding to poly(rA)

Circular dichroism (CD) measurements were made on both fd and IKe gene 5 proteins in solution. The difference between the CD spectra of these two proteins was interpreted as being the result of an enhanced tyrosine contribution in the IKe gene 5 protein spectrum. There was no spectral evidence for significant alpha-helical structures in either of the two gene 5 proteins. CD measurements were also made on complexes of the two gene 5 proteins with poly(rA). The long-wavelength region (300-250 nm) of the CD spectra of both complexes was essentially like that of free poly(rA) at a high temperature. With the assumption that the poly(rA) components of the complexes had the same CD at all wavelengths as did free poly(rA) at a high temperature, it was possible to separate the CD spectra of the complexes into protein and nucleic acid components. Except for the tyrosine CD band at 229 nm, there were no significant changes in the CD bands of either protein upon binding to poly(rA). Thus, each protein appeared to maintain essentially the same overall secondary conformation when complexed with poly(rA) as when in its free state.     

Specificity of the Binding of fd Gene 5 Protein to Polydeoxyribonucleotides

Abstract

The long-wavelength circular dichroism (CD) changes induced by binding of fd gene 5 protein to the alternating DNA sequences poly[d(A-C)] and poly [d(C-T)] were similar to those induced by the protein complexed with the homopolymers poly[d(A)], poly[d(C)], and poly[d(T)]. The fd gene 5 protein showed different binding affinities for the various polymers. The affinity for the alternating sequences was not compositionally weighted with respect to the affinities for the homopolymers, indicating that both base composition and base sequence of the template are important for the binding of fd gene 5 protein.     

A.U and G.C base pairs in synthetic RNAS have characteristic vacuum UV CD bands.

The vacuum UV CD spectra of GpC, CpG, GpG, poly[r(A)], poly[r(C)], poly[r(U)], poly[r(A-U)], poly[r(G).r(C)], poly[r(A).r(U)], and poly[r(A-U).r(A-U)] were measured down to at least 174 nm. These spectra, together with the published spectra of poly[r(G-C).r(G-C)], CMP, and GMP, were sufficient to estimate the CD changes upon base pairing for four double-stranded RNAs. The vacuum UV CD bands of poly[r(A)], poly[r(C)], and the dinucleotides GpC and CpG were temperature dependent, suggesting that they were due to intrastrand base stacking. The dinucleotide sequence isomers GpC and CpG had very different vacuum UV CD bands, indicating that the sequence can play a role in the vacuum UV CD of single-stranded RNA. The vacuum UV CD bands of the double-stranded (G.C)-containing RNAs, poly[r(G).r(C)] and poly[r(G-C).r(G-C)], were larger than the measured or estimated vacuum UV CD bands of their constituent single-stranded RNAs and were similar in having an exceptionally large positive band at about 185 nm and negative bands near 176 and 209 nm. These similarities were enhanced in difference-CD spectra, obtained by subtracting the CD spectra of the single strands from the CD spectra of the corresponding double strands. The (A.U)-containing double-stranded RNAs poly[r(A).r(U)] and poly[r(A-U).r(A-U)] were similar only in that their vacuum UV CD spectra had a large positive band at 177 nm. The spectrum of poly[r(A).r(U)] had a shoulder at 188 nm and a negative band at 206 nm, whereas the spectrum of poly[r(A-U).r(A-U)] had a positive band at 201 nm. On the other hand, difference spectra of both of the (A.U)-containing polymers had positive bands at about 177 and 201 nm. Thus, the difference-CD spectra revealed CD bands characteristic of A.U and G.C base pairing. (ABSTRACT TRUNCATED AT 250 WORDS)     

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)     

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.     

Mercury-induced transitions between right-handed and putative left-handed forms of poly[d(A-T).d(A-T)] and poly[d(G-C).d(G-C)]

Poly[d(A-T).d(A-T)] and poly[d(G-C).d(G-C)], each dissolved in 0.1 M NaClO4, 5 mM cacodylic acid buffer, pH 6.8, experience inversion of their circular dichroism (CD) spectrum subsequent to the addition of Hg(ClO4)2. Let r identical to [Hg(ClO4)2]added/[DNA-P]. The spectrum of the right-handed form of poly[d(A-T).d(A-T)] turns into that of a seemingly left-handed structure at r greater than or equal to 0.05 while a similar transition is noted with poly[d(G-C).(G-C)] at r greater than or equal to 0.12. The spectral changes are highly cooperative in the long-wavelength region above 250 nm. At r = 1.0, the spectra of the two polymers are more or less mirror images of their CD at r = 0. While most CD bands experience red-shifts upon the addition of Hg(ClO4)2, there are some that are blue-shifted. The CD changes are totally reversible when Hg(II) is removed from the nucleic acids by the addition of a strong complexing agent such as NaCN. This demonstrates that mercury keeps all base pairs in register.     

Template specificities of Aclacinomycin B on the inhibition of DNA-dependent RNA synthesis in vitro

Summary The effect of Aclacinomycin B (ACM-B), an anthracycline antitumor antibiotic, on the DNA-dependent RNA synthesis using single- and double-stranded DNAs of known base content and sequence is studied. The data show that ACM-B effectively inhibits the double-stranded DNA-directed RNA synthesis with a preference of poly[d(A-T)] > poly[d(G-C)] > poly[d(I-C)]. In contrast, it has no inhibitory effect on the template function of single-stranded DNA (e.g. poly dA, poly dT, and poly dC). These results suggest that the mechanism of ACM-13 inhibition, like other anthracycline antibiotics, is by intercalation. In addition to the base specificity, there are also dramatic differences in inhibition depending on the base sequence in the DNA template. Thus, ACM-13 preferentially inhibits the alternating double-stranded copolymers over the double-stranded homopolymers; e.g. poly [d(A-T)] is inhibited to a greater extent than poly dA · poly dT and poly [d(G-C)] is inhibited more than poly dG · poly dC. Since the inhibition by ACM-13 can be totally abolished when assayed in excess amount of DNA, this result suggests that ACM-B inhibition of RNA synthesis is solely on the DNA template (which is in support of the intercalation model), and has ruled out the possibility that ACM-B may also exert an inhibitory effect on the activity of RNA polymerase per se.     

Circular dichroism of adenine and thymine containing synthetic polynucleotides

Circular dichroism (CD) spectra of poly(dA), poly(dT), poly(dA)·poly(dT), and poly[d(A-T)]·poly[d(T-A)] have been measured as a function of temperature. From these data difference spectra have been calculated by subtracting the spectrum measured at low temperature from the spectra measured at higher temperatures. The CD difference spectra obtained upon melting of the two double-stranded polymers are very similar. From a comparison of these difference spectra with calculated ones it is shown that optical transitions near 272 nm (on A) and 288 nm (most probably on T) are present. The premelting changes of the CD spectrum of poly[d(A-t)]·poly[d(T-A)] are due to a change in conformation in which the secondary structure goes from a C- to B-type spectrum by increasing the A-type nature of the polymer. Such a change is not observed for poly(dA)·poly(dT). Instead, a transition between two different B-type geometries occurs.     

Demonstration by ultraviolet resonance Raman spectroscopy of differences in DNA organization and interactions in filamentous viruses Pf1 and fd

Pf1, a class II filamentous virus, has been investigated by ultraviolet resonance Raman (UVRR) spectroscopy with excitation wavelengths of 257, 244, 238, and 229 nm. The 257-nm UVRR spectrum is rich in Raman bands of the packaged single-stranded DNA (ssDNA) genome, despite the low DNA mass (6%) of the virion. Conversely, the 229-nm UVRR spectrum is dominated by tyrosines (Tyr 25 and Tyr 40) of the 46-residue alpha-helical coat subunit. UVRR spectra excited at 244 and 238 nm exhibit Raman bands diagnostic of both viral DNA and coat protein tyrosines. Raman markers of packaged Pf1 DNA contrast sharply with those of the DNA packaged in the class I filamentous virus fd [Wen, Z. Q., Overman, S. A., and Thomas, G. J., Jr. (1997) Biochemistry 36, 7810-7820]. Interestingly, deoxynucleotides of Pf1 DNA exhibit sugars in the C2'-endo/anti conformation and bases that are largely unstacked, compared with C3'-endo/anti conformers and very strong base stacking in fd DNA; hydrogen-bonding interactions of thymine carbonyls are also different in Pf1 and fd. On the other hand, coat protein tyrosines of Pf1 exhibit Raman markers of ring environment identical to those of fd, including an anomalous singlet at 853 cm-1 in lieu of the canonical Fermi doublet (850/830 cm-1) found in globular proteins. The results indicate markedly different modes of organization of ssDNA in Pf1 and fd virions, despite similar environments for coat protein tyrosines, and suggest strong hydrogen-bonding interactions between DNA bases and coat subunits of Pf1 but not between those of fd. We propose that structural relationships between the protein coat and encapsidated ssDNA genome are also fundamentally different in the two assemblies.     

Electrostatic potential distribution of the gene V protein from Ff phage facilitates cooperative DNA binding: a model of the GVP-ssDNA complex.

The crystal structure of the gene V protein (GVP) from the Ff filamentous phages (M13, fl, fd) has been solved for the wild-type and two mutant (Y41F and Y41H) proteins at high resolution. The Y41H mutant crystal structure revealed crystal packing interactions, which suggested a plausible scheme for constructing the polymeric protein shell of the GVP-single-stranded DNA (ssDNA) complex (Guan Y, et al., 1994, Biochemistry 33:7768-7778). The electrostatic potentials of the isolated and the cooperatively formed protein shell have been calculated using the program GRASP and they revealed a highly asymmetric pattern of the electrostatic charge distribution. The inner surface of the putative DNA-binding channel is positively charged, whereas the opposite outer surface is nearly neutral. The electrostatic calculation further demonstrated that the formation of the helical protein shell enhanced the asymmetry of the electrostatic distribution. A model of the GVP-ssDNA complex with the n = 4 DNA-binding mode could be built with only minor conformational perturbation to the GVP protein shell. The model is consistent with existing biochemical and biophysical data and provides clues to the properties of GVP, including the high cooperatively of the protein binding to ssDNA. The two antiparallel ssDNA strands form a helical ribbon with the sugar-phosphate backbones at the middle and the bases pointing away from each other. The bases are stacked and the Phe 73 residue is intercalated between two bases. The optimum binding to a tetranucleotide unit requires the participation of four GVP dimers, which may explain the cooperativity of the GVP binding to DNA.     

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)].     

Interaction of the HMG1 protein with nucleic acids

Binding constants have been measured for the interaction of the protein HMG1 with native DNA, denatured DNA and a number of polynucleotides at near-physiological ionic strengths, using gel filtration and thermal denaturation. The interaction of HMG1 with DNA is shown to be noncooperative and reversible. Nucleic acids form the following series in order of increasing binding constants: poly(U) integral of poly(A) less than poly(dA) less than dsDNA integral of poly(dA) X poly(dT) integral of poly(dG) X poly(dC) much less than poly[d(A-T]) integral of ssDNA.     

Specificity of the binding of fd gene 5 protein to polydeoxyribonucleotides

The long-wavelength circular dichroism (CD) changes induced by binding of fd gene 5 protein to the alternating DNA sequences poly[d(A-C)] and poly[d(C-T)] were similar to those induced by the protein complexed with the homopolymers poly[d(A)], poly[d(C)], and poly[d(T)]. The fd gene 5 protein showed different binding affinities for the various polymers. The affinity for the alternating sequences was not compositionally weighted with respect to the affinities for the homopolymers, indicating that both base composition and base sequence of the template are important for the binding of fd gene 5 protein.     

fd gene 5 protein binds to double-stranded polydeoxyribonucleotides poly(dA.dT) and poly[d(A-T).d(A-T)]

Circular dichroism (CD) data indicated that fd gene 5 protein (G5P) formed complexes with double-stranded poly(dA.dT) and poly[d(A-T).d(A-T)]. CD spectra of both polymers at wavelengths above 255 nm were altered upon protein binding. These spectral changes differed from those caused by strand separation. In addition, the tyrosyl 228-nm CD band of G5P decreased more than 65% upon binding of the protein to these double-stranded polymers. This reduction was significantly greater than that observed for binding to single-stranded poly(dA), poly(dT), and poly[d(A-T)] but was similar to that observed for binding of the protein to double-stranded RNA [Gray, C.W., Page, G.A., & Gray, D.M. (1984) J. Mol. Biol. 175, 553-559]. The decrease in melting temperature caused by the protein was twice as great for poly[d(A-T).d(A-T)] as for poly(dA.dT) in 5 mM tris(hydroxymethyl)aminomethane hydrochloride (Tris-HCl), pH 7. Upon heat denaturation of the poly(dA.dT)-G5P complex, CD spectra showed that single-stranded poly(dA) and poly(dT) formed complexes with the protein. The binding of gene 5 protein lowered the melting temperature of poly(dA.dT) by 10 degrees C in 5 mM Tris-HCl, pH 7, but after reducing the binding to the double-stranded form of the polymer by the addition of 0.1 M Na+, the melting temperature was lowered by approximately 30 degrees C. Since increasing the salt concentration decreases the affinity of G5P for the poly(dA) and poly(dT) single strands and increases the stability of the double-stranded polymer, the ability of the gene 5 protein to destabilize poly(dA.dT) appeared to be significantly affected by its binding to the double-stranded form of the polymer.     

The CD of ligand-DNA systems. 2. Poly(dA-dT) B-DNA.

A systematic theoretical study of the CD of [poly(dA-dT)]2 and its complexes with achiral small molecules is presented. The CD spectra of [poly(dA-dT)]2 and of poly(dA):poly(dT) are calculated for various DNA structures using the matrix method. The calculated and experimental spectra agree reasonably well for [poly(dA-dT)]2 but less well for poly(dA):poly(dT). The calculated CD spectrum of [poly(dA-dT)]2 fails to reproduce the wavelength region of 205-245 nm of the experimental spectrum. This discrepancy can be explained by a magnetic dipole allowed transition contributing significantly to the CD spectrum in this region. The induced CD of a transition moment of a molecule bound to [poly(dA-dT)]2 is also calculated. As was the case for [poly(dG-dC)]2, the induced CD of a groove bound molecule is one order of magnitude stronger than that of an intercalated molecule. The calculations also show considerable differences between pyrimidine-purine sites and purine-pyrimidine sites. Both signs and magnitudes of the CD induced into ligands bound in the minor groove agree with experimental observations.     

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.     

Complex-Formation of Ethidium Bromide with Poly[d(A-T)]·Poly[d(A-T)]

Abstract

The interaction of Ethidium Bromide (EtBr) with double-stranded (ds-) and single-stranded (ss-) poly[d(A-T)] was studied in different ionic strengths solutions. Optical spectroscopy and Scatchard analysis results indicate that the ligand interacts to both helix and coiled structures of the polynucleotide by “strong” and “weak” binding modes. The association parameters (binding constant—K—and the number of nucleotides corresponding to a binding site—n) of the strong type of interaction were found to be independent of Na+ concentration. Weak interaction occurs at low ionic strength and/or high EtBr concentration. Estimated binding parameters of EtBr with ss- and ds-polynucleotide are in good agreement with those for EtBr-B-DNA complexes. Data obtained provided an evidence for a stacking interaction of EtBr with single stranded poly[d(A-T)].