Studies on formation and stability of the d[G(AG)5]* d[G(AG)5]·d[C(TC)5] and d[G(TG)5]* d[G(AG)5]· d[C(TC)5] triple helices

We have targeted the d[G(AG)₅] · d[C(TC)₅] duplex for triplex formation at neutral pH with either d[G(AG)₅] or d[G(TG)₅]. Using a combination of gel electrophoresis, uv and CD spectra, mixing and melting curves, along with DNase I digestion studies, we have investigated the stability of the 2:1 pur*pur · pyr triplex, d[G(AG)₅] * d[G(AG)₅] · d[C(TC)₅], in the presence of MgCl₂. This triplex melts in a monophasic fashion at the same temperature as the underlying duplex. Although the uv spectrum changes little upon binding of the second purine strand, the CD spectrum shows significant changes in the wavelength range 200–230 nm and about a 7 nm shift in the positive band near 270 nm. In contrast, the 1:1:1 pur/pyr*pur · pyr triplex, d[G(TG)₅] * d[G(AG)₅] · d[C(TC)₅], is considerably less stable thermally, melting at a much lower temperature than the underlying duplex, and possesses a CD spectrum that is entirely negative from 200 to 300 nm. Ethidium bromide undergoes a strong fluorescence enhancement upon binding to each of these triplexes, and significantly stabilizes the pur/pyr*pur · pyr triplex. The uv melting and differential scanning calorimetry analysis of the alternating sequence duplex and pur*pur · pyr triplex shows that they are lower in thermodynamic stability than the corresponding 10-mer d(G₃A₄G₃) · d(C₃T₄C₃) duplex and its pur*pur · pyr triplex under identical solution conditions. © 1997 John Wiley & Sons, Inc.     

Influence of base-pair changes and cooperativity parameters on the melting curves of short DNAs

Theoretical melting curves were calculated for four DNA restriction fragments, 157–257 base pairs (bp), and a series of hypothetical block DNAs with sequences d(C_2xA_xC_2x). d(C_2xT_xG_2x), 5 ? x ? 40. These DNAs provided a mixture of A·T/G·C sequence distributions with which to investigate the effects of parameters and base-pair changes on the melting of short DNAs. The sensitivity of DNA melting curves to changes in internal loop melting parameters σ and κ was examined. As Expected, theoretical melting curves of short DNAs with a quasirandom base-pair sequence vary little with changes in internal loop parameters. End melting dominates the transition behaviour of these moleucles. This was also observed for the block DNAs up to x = 22. Beyond this length, melting curves are highly sensitive to the internal loop parameters. Sensitivity is also predicted for a 157-bp fragment with a block distribution of A·T and G·C pairs. These results indicate that accurate evaluation of internal loop parameters is possible with short DNAs (100–200 bp) containing a G·C/A·T/G·C block distribution with at least 22 bp in each block. Duplex-to-single-strands dissociation parameters were reevaluated form experimental melting curve data of eight DNA fragments using a least squares fit approach. This analysis confirmed parameter values previously found with a simplified dissociation model. A Priori predictions are made on the effects of base-pair changes on the melting curves of three characterized DNA restriction fragments. Single base-pair changes are predicted to induce small but measurable changes in the melting curves. The characteristics of the altered melting curves depend on the location of the base-pair change.     

Tetraplex Formation of d(GGGGGTTTTT): 1H NMR Study in Solution

Abstract

The oligonucleotide d(G₅T₅) can in principle form a fully matched duplex with G · T pairing and/or a tetraplex. Non-denaturing gel electrophoresis, circular dichroism and NMR experiments show that the tetraplex is exclusively formed by this oligomer in solution. In the presence of its complementary strand d(A₅C₅) at low temperature, d(G₅T₅) forms the tetraplex over the normally expected Watson-Crick duplex. However, when d(G₅T₅) and d(A₅C₅) are mixed together in equimolar amounts and heated for several minutes at 85°C, and then allowed to cool, the product was essentially the Watson-Crick duplex. The lack of resolution in the 500 MHz ¹H NMR spectra and the presence of extensive spin diffusion do not allow us to derive a quantitative structure for the tetraplex from the NMR data. However, we find good qualitative agreement between the NOESY and MINSY data and a theoretically derived stereochemically sound structure in which the G's and T's are part of a parallel tetraplex.     

Studies on interaction between poly(L-lysine) and DNA of varied G + C contents

Interaction between polylysine and DNA's of varied G + C contents was studied using thermal denaturation and circular dichroism (CD). For each complex there is one melting band at a lower temperature t_m, corresponding to the helix–coil transition of free base pairs, and another band at a higher temperature t′_m, corresponding to the transition of polylysine-bound base pairs. For free base pairs, with natural DNA's and poly(dA-dT) a linear relation is observed between the t_m and the G + C content of the particular DNA used. This is not true with poly(dG)·poly(dC), which has a t_m about 20°C lower than the extrapolated value for DNA of 100% G + C. For polylysine-bound base pairs, a linear relation is also observed between the t′_m and the G + C content of natural DNA's but neither poly(dA-dT) nor poly(dG)·poly(dC) complexes follow this relationship. The dependence of melting temperature on composition, expressed as dt_m/dX_G·C, where X_G·C is the fraction of G·C pairs, is 60°C for free base pairs and only 21°C for polylysine-bound base pairs. This reduction in compositional dependence of T_m is similar to that observed for pure DNA in high ionic strength. Although the t′_m of polylysine-poly(dA-dT) is 9°C lower than the extrapolated value for 0% G + C in EDTA buffer, it is independent of ionic strength in the medium and is equal to the t_m⁰ extrapolated from the linear plot of t_m against log Na⁺. There is also a noticeable similarity in the CD spectra of polylysine· and polyarginine·DNA complexes, except for complexes with poly(dA-dT). The calculated CD spectrum of polylysine-bound poly(dA-dT) is substantially different from that of polyarginine-bound poly(dA-dT).     

Further studies on telestability in DNA. The synthesis and characterization of the duplex block polymers d(C20A10) - d(T10G20) and d(C20A15) - d(T15G20).

The synthesis and characterization of the duplex block polymers d(C20A10) - d(T10G20) and d(C20A15) - d(T15G20) are described. Thermal denaturation studies on these DNAs in the absence and presence of actinomycin, which binds only to the GC portions of these molecules, have confirmed and extended our previous observation that the properties of one region of a DNA can be influenced (telestabilized) by a remote region. In addition, the large scale synthesis of d(C15A15) - d(T15G15) is described.     

Laser Photofootprinting of d(C)·d(G)·d(G) Intramolecular Triplex

Abstract

Supercoiling-induced structural transition of the d(C₂₄GC₂₁,) · d(G₂₁CG₂₄) sequence in plasmid DNA in the presence of Mg²⁺ at neutral pH results in alterations of efficiencies of not only single-quantum (pyrimidine[6–4]pyrimidone adducts) but also two-quantum (alkalisensitive lesions of dG residues) photomodifications of nucleoside residues within this sequence. The generation of both types of photoreactions was achieved by the application of high-intensity laser UV radiation (intensity ～ 10¹¹ W/m², pulse duration ～ 10^?8 s, λ= 266 nm) for irradiation of a plasmid DNA The modification extent sufficient for analysis of photoreaction efficiency distributions along both strands of the insert (photofootprinting) was obtained by the action of a single nanosecond pulse of laser UV radiation. The pattern of a laser photofootprinting is consistent with the d(C) · d(G) · d(G) triplex formation in the presence of Mg²⁺ within the insert and shows some details of this triplex structure.     

Helix coil transitions of d (A)n·d(T)n,d(A-T)n·d(A-T)n,and d(A-A-T)n·d(A-T-T)n; evaluation of parameters governing DNA stability

The thermally induced helix-coil transitions of three A-T DNAs, d(A)_n·d(T)_n, d(A-T)_n·d(A-T)_n, and d(A-A-T)_n·d(A-T-T)_n, were studied. Experimental transition curves of the DNAs were analyzed using the loop entropy model of DNA melting. The calculation of the melting curve of d(A-A-T)_n·d(A-T-T)_n is presented using the integral equation formalism of Goel and Montroll. The aim of this work was to evaluate thermodynamic parameters which govern DNA stability and to test the theoretical model employed in the analysis. Our results show (1) an excellent over-all agreement between theory and experiment, (2) a loop entropy exponent k = 1.55 ± 0.05 provided the best fit to all the polymer transition curves, (3) the evaluated stacking free energies reflect the relative stability of the DNAs, and (4) the stacking energies of the ApA·TpT dimer evaluated from d(A)_n·d(T)_n and d(A-A-T)_n·d(A-T-T)_n differ. The last result is consistent with different conformations for the dimer in these two polymers.     

CD studies of double-stranded polydeoxynucleotides composed of repeating units of contiguous homopurine residues

Double-stranded synthetic polydeoxynucleotides of the general form poly[d(G_nC_n)] · poly[d(G_nC_n)], poly[d(G_nC)] · poly[d(GC_n)], and poly[d(A_nT_n)] · poly[d(A_nT_n)] have been synthesized. When n = 4 or larger, the CD spectra of polymers of the form poly[d(G_nC_n)] · poly[d(G_nC_n)] or poly[d(G_nC)] · poly[d(GC_n)] closely resemble the spectrum of poly[dG] · poly[dC], suggesting that a string of four continguous guanosine residues is sufficient to induce a conformation resembling that of the polypurine · polypyrimidine. With polymers of the form poly[d(A_nT_n)] · poly[d(A_nT_n)], however, the CD spectrum only gradually approaches that of poly[dA] · poly[dT].     

Molecular Dynamics Simulation of 7, 8-dihydro-8-Oxoguanine DNA

Abstract

To elucidate the effect of guanine lesion produced by the oxidative damage on DNA, 1 nanosecond molecular dynamics simulations of native and oxidized DNA were performed. The target DNA molecules are dodecamer duplex d(CGCGAATTCGCG)2 and its derivative duplex d(C₁G₂C₃(8-oxoG)₄A₅A₆T₇T₈C₉G₁₀C₁₁G₁₂)·d(C₁₃G₁₄C₁₅G₁₆A₁₇A₁₈T₁₉T₂₀C21_G22C₂₃G₂₄), which has one oxidized guanine, 7, 8-dihydro-8-oxoguanine (8-oxoG), at the fourth position. The local structural change due to the lesion of 8-oxoG and the global dynamic structure of the 8-oxoG DNA were studied. It was found that the 8-oxoG DNA remained structurally stable during the simulation due to newly produced hydrogen bonds around the (8-oxoG)₄ residue. However, there were distinguishable differences in structural parameters and dynamic property in the 8-oxoG DNA. The conformation around the (8- oxoG)₄ residue departed from the usual conformation of native DNA and took an unique conformation of ?-ζ in B_II conformation and χ in high anti orientation at the (8-oxoG)₄ residue, and adopted a very low helical twist angle at the C₃:G₂₂—(8-oxoG)₄:C₂₁ step. Further analysis by principal component analysis indicated that the formation of the hydrogen bonds around the (8-oxoG)₄ residue plays a role as a trigger for the conformational transition of the 8-oxoG DNA in the conformational space.     

Polarized Raman scattering from oriented single microcrystals of d(A5T5)2 and d(pTpT)

Polarized Raman spectra have been obtained from single microcrystals of the duplex of the decamer d(A₅T₅)₂ using a Raman microscope. This is the first report of Raman spectra from a crystal of a deoxyoligomer that contains only long, nonalternating sequences of adenine and thymine. Sequences containing d(A)_n and d(T)_n are of interest in view of recent suggestions that they induce bends in DNA and that they might exist in a nonstandard B-conformation. Polarized Raman spectra of a crystal of d(pTpT) have also been obtained. Both crystals display Raman bands whose intensities are very sensitive to the orientation of the crystal with respect to the direction of polarization of the incident laser beam. These spectra indicate that the helical axes of the oligonucleotides are parallel to the long axes of the crystals and that the d(A₅T₅)₂ is not appreciably bent in the crystal. The Raman spectrum from the d(pTpT) crystal indicates that all of the furanose ring puckers are in a C2′-endo configuration since only the C2′-endo marker band at 835 ± 5 cm^?1 is present. Crystals of d(A₅T₅)₂ show measurable Raman intensities in both the 838- and 816-cm^?1 bands. This indicates the presence of both the C2′-endo and C3′-endo, or possibly other non-C2′-endo, furanose conformations. The 816-cm^?1 band is weak so that only a small fraction of the residues are estimated to be in the non-C2′-endo conformation. In both the d(pTpT) and d(A₅T₅)₂ crystals the intensity of the bands due to vibrations of the backbone show only a small dependence on orientation of the crystals. This result is explained by the low symmetry of the puckered sugar rings. It is concluded that Raman spectra obtained from oligonucleotide crystals in which the orientation of the crystal axes to the laser polarization is not carefully controlled may contain intensity artifacts that are due to polarization effects.     

An analysis of the sequence dependence of the structure and energy of A- and B-DNA models using molecular mechannics

Molecular-mechanics calculations have been carried out on the base-paired hexanucleoside pentaphosphates d(TATATA)₂, d(ATATAT)₂, d(A₆)·d(T₆), d(CGCGCG)₂, d(GCGCGC)₂, and d(C₆)·d(G₆) in both A- and B-DNA geometries. The calculated relative energies of these polymers are consistent with the relative stabilities of the polymers found experimentally. In particular, the results of our calculations support the observation that the homopolymer d(A)_n·d(T)_n is more stable in a B-DNA conformation, while the homopolymer d(G)_n·d(C)_n is more stable in an A-DNA conformation. The molecular interactions responsible for these differential stabilities include both inter- and intrastrand base stacking, as well as base–phosphate interactions. While definitive experiments on the heteropolymer stabilities have not yet been carried out, the results of our calculations also suggest a greater stability of the purine-3′,5′-pyrimidine sequence over the pyrimidine-3′,5′-purine sequence in both the A- and B-conformations. The reason for this greater stability lies in the importance of the inherent directionality (5′ → 3′ vs 3′ → 5′) of phosphate–base and base–base interactions. The largest conformation change observed on energy refinement is sugar repuckering, which occurs mainly on pyrimidine-attched sugars and only in the B-DNA geometry. We suggest a molecular mechanism, specifically, differential base–sugar steric interactions involving neighboring sugars, to explain why this repuckering occurs more with d(A₆)·d(T₆) than with other isomers.     

Base-pair exchange kinetics of the imino and amino protons of the 3′-phenazinium tethered DNA-RNA duplex,r(5′GAUUGAA3′):d(5′TCAATC3′-Pzn), and their comparison with those of B-DNA duplex

The dynamics of the opening-closing of the constituent base-pairs as well as of the exchange kinetics of the base-paired imino and amino protons with water in a DNA-RNA hybrid, [^5′r(G¹A²U³U⁴G⁵A⁶A⁷)^3′]:^5′p[d(T⁸C⁹A¹⁰A¹¹T¹²C¹³)]^3′-Pzn] duplex (I), are reported here in details for the first time. The exchange kinetics of amino and imino protons in the DNA-RNA hybrid (duplex I) have been compared with identical studies on the following B-DNA duplexes: d(C¹G²T³A⁴C⁵G⁶)₂ (II), d[p(^5′T¹G²T³T⁴T⁵G⁶ G⁷C⁸)^3′]:d[p(^5′C⁹C¹⁰A¹¹A¹²A¹³C¹⁴A¹⁵)^3′] (III), d(C⁵G⁶C⁷G⁸A⁹A¹⁰T¹¹T¹²C¹³G¹⁴C¹⁵G¹⁶)₂ (IV) and d(C¹G²C³G⁴C⁵G⁶C⁷G⁸A⁹A¹⁰T¹¹T¹²C¹³G¹⁴C¹⁵G¹⁶C¹⁷G¹⁸C¹⁹G²⁰)₂ (V). This comparative study shows that the life-times τ_o of various base-pairs in the DNA-RNA hybrid (I) varies in the range of ∼ 1 ms, and they are quite comparable to those of the shorter B-DNA duplexes (II) and (III), but very different from the τ_o of the larger duplexes (IV) and (V): the τ_o for the base pair of T¹¹ and T¹² residues in the 20-mer (duplex V) are 2.9 ± 2.3 ms and 23.2 ± 8.9 ms, respectively, while the corresponding τ_o in the 12-mer (duplex IV) are 2.8 ± 2.2 ms and 17.4 ± 5.4 ms. It has also been shown that the total energy of activation (E_a) assessed from the exchange rates of both imino and amino protons, representing energetic contributions from both base-pair and helix opening-closing as well as from the exchange process of the imino protons from the open state with the bound water, is close to the E_a of the short B-DNA duplex (E_a ≈ 28–47 kcal/mol).     

Structural transition from antiparallel to parallel G-quadruplex of d(G4T4G4) induced by Ca2+

Guanine quadruplex (G-quadruplex) structures are formed by guanine-rich oligonucleotides. Because of their in vivo and in vitro importance, numerous studies have been demonstrated that the structure and stability of the G-quadruplex are dependent on the sequence of oligonucleotide and environmental conditions such as existing cations. Previously, we quantitatively investigated the divalent cation effects on the antiparallel G-quadruplex of d(G₄T₄G₄), and found that Ca²⁺ induces a structural transition from the antiparallel to parallel G-quadruplex, and finally G-wire formation. In the present study, we report in detail the kinetic and thermodynamic analyses of the structural transition induced by Ca²⁺ using stopped-flow apparatus, circular dichroism, size-exclusion chromatography (SEC) and atomic force microscopy. The quantitative parameters showed that at least two Ca²⁺ ions were required for the transition. The kinetic parameters also indicated that d(G₄T₄G₄) underwent the transition through multiple steps involving the Ca²⁺ binding, isomerization and oligomerization of d(G₄T₄G₄). The parallel-stranded G-wire structure of d(G₄T₄G₄), which is a well controlled alignment of numerous DNA strands with G-quartets, as the final product induced by Ca²⁺, was observed using SEC and atomic force microscopy. These results provide insight into the mechanism of the structural transition and G-wire formation and are useful for constructing a nanomaterial regulated by Ca²⁺.     

Further crystallographic evidence of NH· · ·π (system) and CO· · ·π (system) interactions: The structures of bis(diarylhydrazonecarbonyl)methylene derivatives [{ArPhCNNH—C(O)}2CH2] (Ar = Ph, 2‐C5H4N, 2‐C4H3S)

In this study are reported the syntheses of three bis(diarylhydrazonecarbonyl)methylene derivatives [{ArPhCNNH C(O)}₂CH₂] [Ar = 2 C₅H₄N (5), C₆H₅ (6), and 2‐C₄H₃S (7)], obtained by condensation of corresponding hydrazones with carbon suboxide, C₃O₂. The solid‐state self‐assembly of these carbonyl derivatives, giving rise to polymeric and dimeric networks, is described. In the formation of these structural features, in addition to N—H· · ·OC intermolecular hydrogen bonds, stabilizing intramolecular NH· · · π (systems) and intermolecular CO· · ·π (systems) interactions also seem to play an important role. Solution ¹H‐nmr data of compounds 5–7 indicate that the polymeric and dimeric structures are not maintained in solution and show the occurrence of keto‐enolic equilibria. © 1999 John Wiley & Sons, Inc. Biopoly 49: 541–549, 1999     

Skeletal ontogeny of the vertebral column and of the fins in shi drum Umbrina cirrosa (Teleostei: Perciformes: Sciaenidae), a new candidate species for aquaculture

The osteological development of the vertebral column and fins in shi drum Umbrina cirrosa was studied in order to improve knowledge for its introduction in Mediterranean aquaculture. The osteological development was studied in 171 individuals, of total length (L_T) from 2·7 to 30·2 mm that were reared under the mesocosm technique. Vertebral ontogeny starts at 3·4 and 4·0 mm L_T, with the formation of the first cartilaginous neural and haemal arches, and spines, respectively, and is completed with the full attainment of epicentrals (12·5 mm L_T). The formation of vertebral centra occurs between 4·1 and 7·4 mm L_T. Pectoral supports are the first fin elements to develop (3·0 mm L_T), followed by those of the caudal fin (3·8 mm L_T), pelvic fin (3·9 mm L_T) and finally by those of the dorsal and anal fins (4·5 mm L_T). The caudal fin is the first to develop fin rays and attain the full count of principal fin rays (4·5–6·8 mm L_T), but the last to be fully completed with the formation of procurrent fin rays (6·9–17·5 mm L_T). The next fins starting to present rays are the dorsal (5·3 mm L_T) and the pectoral fins (5·6 mm L_T), while the anal and pelvic fins are the last (5·7 mm L_T). Following the caudal principal fin rays (6·8 mm L_T), the dorsal, anal (6·9 mm L_T), pelvic (7·4 mm L_T) and pectoral fins (9·8 mm L_T) are the next with fully completed ray counts. Aggregation of qualitative changes, such as the appearance of cartilages, the beginning and the complement of the ossification process and the full complement of elements in U. cirrosa were measured as cumulative frequency counts. These measurements reveal three ontogenetic intervals: one very developmentally active period during early life stages (from 3 to 5·9 mm L_T), a second slower developmental period (from 6·0 to 8·9 mm L_T) and finally a period of ontogeny more focused on structure refinement up to metamorphosis and settlement (>9·0 mm L_T).     

Correlation of Tm and sequence of DNA duplexes with delta H computed by an improved empirical potential method

T_m values for 20 DNA duplexes with different repeating base sequences provided the data base for developing a rational and relatively simple methodology for computing apparent enthalpies for the helix → coil transitions of DNA helices, ΔH _calc. The computational variables and their range of acceptable values were selected on the basis of physically plausible arguments. Over 350,000 different combinations of the variables were tested for degree of fit. It was therby possible to find a combination giving a high degree of linear fit between T_m and ΔH _calc (correlation coefficient, 0.99), with T_m values deviating (on average) from the regression line by only ±2.17°C. Most of this uncertainty is attributed to experimental limitations, although computational approximations also contribute. With ΔH _calc for the melting of each of the unique complementary dinucleotide fragments computed by the method developed, it is possible to estimate T_m and (relative) ΔH _calc reliable for the melting of any particular DNA [with base pairs G(I)·C and A·T] given only its base sequence. The ΔH_calc values for the complementary dinucleotide fragments, together with statistical considerations, make it apparent that T_m of DNAs with repeating base sequence show only an approximate linear dependence on G·C content because A·T and G·G pairs do not contribute to helix stability independently of the base-pair sequence in which they occur. In fact, the nearestneighbor stacking interactions are so significant that certain complementary dinucleotide fragment sequences with 0,50, and 100% G·C content have the same stability.     

Molecular mechanical studies of base-pair opening in d(CGCGC):d(GCGCG), dG5·dC5, d(TATAT):d(ATATA), and dA5·dT5 in the B and Z forms of DNA

Molecular mechanical energy refinement of double-helical pentanucleotide tetra-phosphates, d(CGCGC):d(GCGCG), dG₅·dC₅, d(TATAT):d(ATATA), and dA₅ ·dT₅ geometries, are presented in order to examine the energy required to open the Nl(purine) …? N3(pyrimidine) distance (base-pair opening) of a Watson-Crick base pair from its normal value of 3 Å to a value of 6 Å. The structural consequences of forcing base-pair opening is sequence dependent. For both dA₅ ·dT₅ and d(TATAT):d(ATATA), forcing the Nl (AdeKN3 (Thy) distance of the central base pair to a value of 6 Å slides the bases perpendicular to the helix axis forming a low-energy non-Watson-Crick base pair having an adenine amine hydrogen …? thymine carbonyl oxygen hydrogen bond. The two GC sequences behave differently from both AT sequences and differently from each other. Forcing the Nl(Gua) …? N3(Cyt) distance to 6 Å leads to unconventional structures in which hydrogen bonds are formed between the separated bases and the bases above or below them. These structures appear to be trapped in true local minima 6–10 kcal/mol higher in energy than the Watson-Crick structures. Preliminary simulations on d(CGCGC):d(GCGCG) in the Z geometry suggest the reason the Z form may be more refractory to proton exchange than the B form, consistent with experimental observations.     

Molecular mechanical calculations on the interaction of ethidium cation with double-helical DNA

Molecular mechanical calculations were done on complexes of ethidium cation with various base-paired deoxydinucleoside monophosphates [(ApT)₂, (TpA)₂, (A₂ · T₂), (GpC)₂, (CpG)₂, and (G₂ · C₂)] and deoxyhexanucleoside pentaphosphates [(ATATAT)₂, (TATATA)₂, (A₆ · T₆), (GCGCGC)₂, (CGCGCG)₂, and G₆ · C₆]. Relative binding energies, sequence preferences, and conformational aspects of the intercalation complexes were studied. The most detailed models used (an all-atom force field) gave results in good agreement with previous calculations and experimental work. Less-sophisticated models did not perform as well.     

Interaction of poly(I)·poly(C) with trans-dichloro-diammine-platinum (II)

The covalent binding of trans-Pt (NH₃)₂Cl₂ to the double-stranded poly(I)·poly(C) follows three types of reactions, depending on r_b and the concentration of polynucleotide in the reaction mixture. At r_b ? 0.1, the principal reaction is coordination to poly(I), giving rise to some destabilization of the double strand, as shown by uv and CD spectra, and a decrease in T_m values, giving rise to free loops of poly(C). At higher r_b and low polynucleotide concentration, the free cytidine bases react with platinum bound on the complementary strand to form intramolecular (interstrand) crosslinks that restabilize the double-stranded structure. At high r_b and high polynucleotide concentration, while the above reaction still occurs, the predominant one is the formation of intermolecular crosslinks. Under no conditions has strand separation been observed.     

DNA binding of a spermine derivative: Spectroscopic study of anthracene-9-carbonyl-n1-spermine with poly[d(G-C)·(d(G-C))] and poly[d(A-T) · d(A-T)]

The binding of polyamines, including spermidine ( 1 ) and spermine ( 2 ), to poly[d(G-C) · d(G-C) ] was probed using spectroscopic studies of anthracene-9-carbonyl-N¹-spermine ( 3 ); data from normal absorption, linear dichroism (LD), and circular dichroism (CD) are reported. Ligand LD and CD for transitions located in the DNA region of the spectrum were used. The data show that 3 binds to DNA in a manner characteristic of both its amine and polycyclic aromatic parts. With poly [(dG-dC) · (dG-dC)], binding modes are occupied sequentially and different modes correspond to different structural perturbations of the DNA. The most stable binding mode for 3 with poly[d(G-C) · d(G-C)] has a site size of 6 ± 1 bases, and an equilibrium binding constant of (2.2 ± 1.1) × 10⁷ M^?1 with the anthracene moiety intercalated. It dominates the spectra from mixing ratios of approximately 133:1 until 6:1 DNA phosphate: 3 is reached. The analogous data for poly [d(A-T) · d(A-T)] between mixing ratios 36:1 and 7:1 indicates a site size of 8.3 ± 1.1 bases and an equilibrium binding constant of (6.6 ± 3.3) × 10⁵ M^?1. Thus, 3 binds preferentially to poly [d(G-C) · d(G-C)] at these concentrations. © 1994 John Wiley & Sons, Inc.