Sequence-Dependent Elasticity and Electrostatics of Single-Stranded DNA: Signatures of Base-Stacking

Base-stacking is a key factor in the energetics that determines nucleic acid structure. We measure the tensile response of single-stranded DNA as a function of sequence and monovalent salt concentration to examine the effects of base-stacking on the mechanical and thermodynamic properties of single-stranded DNA. By comparing the elastic response of highly stacked poly(dA) and that of a polypyrimidine sequence with minimal stacking, we find that base-stacking in poly(dA) significantly enhances the polymer’s rigidity. The unstacking transition of poly(dA) at high force reveals that the intrinsic electrostatic tension on the molecule varies significantly more weakly on salt concentration than mean-field predictions. Further, we provide a model-independent estimate of the free energy difference between stacked poly(dA) and unstacked polypyrimidine, finding it to be ∼−0.25 k_BT/base and nearly constant over three orders of magnitude in salt concentration.     

Is photocleavage of DNA by YOYO-1 using a synchrotron radiation light source sequence dependent?

The photocleavage of double-stranded and single-stranded DNA by the fluorescent dye YOYO-1 was investigated in real time by using the synchrotron radiation light source ASTRID (ISA, Denmark) both to initiate the reaction and to monitor its progress using Couette flow linear dichroism (LD) throughout the irradiation period. The dependence of LD signals on DNA sequences and on time in the intense light beam was explored and quantified for single-stranded poly(dA), poly[(dA-dT)₂], calf thymus DNA (ctDNA) and Micrococcus luteus DNA (mlDNA). The DNA and ligand regions of the spectrum showed different LD kinetic behaviors, and there was significant sequence dependence of the kinetics. However, in contrast to expectations from the literature, we found that poly(dA), mlDNA, low salt ctDNA and low salt poly[(dA-dT)₂] all had significant populations of groove-bound YOYO. It seems that this mode was predominantly responsible for the catalysis of DNA cleavage. In homopolymeric DNAs, intercalated YOYO was unable to cleave DNA. In mixed-sequence DNAs the data suggest that YOYO in some but not all intercalated binding sites can cause cleavage. It is also likely that cleavage occurs at transient single-stranded regions. The reaction rates for a 100 mA beam current of 0.5-μW power varied from 0.6 h⁻¹ for single-stranded poly(dA) to essentially zero for low salt poly[(dG-dC)₂] and high salt poly[(dA-dT)₂]. At the conclusion of the experiments with each kind of DNA, uncleaved DNA with intercalated YOYO remained.     

Molecular recognition of poly(A) by small ligands: an alternative method of analysis reveals nanomolar, cooperative and shape-selective binding

A few drug-like molecules have recently been found to bind poly(A) and induce a stable secondary structure (T_m ≈ 60°C), even though this RNA homopolymer is single-stranded in the absence of a ligand. Here, we report results from experiments specifically designed to explore the association of small molecules with poly(A). We demonstrate that coralyne, the first small molecule discovered to bind poly(dA), binds with unexpectedly high affinity (K_a >10⁷ M⁻¹), and that the crescent shape of coralyne appears necessary for poly(A) binding. We also show that the binding of similar ligands to poly(A) can be highly cooperative. For one particular ligand, at least six ligand molecules are required to stabilize the poly(A) self-structure at room temperature. This highly cooperative binding produces very sharp transitions between unstructured and structured poly(A) as a function of ligand concentration. Given the fact that junctions between Watson–Crick and A·A duplexes are tolerated, we propose that poly(A) sequence elements and appropriate ligands could be used to reversibly drive transitions in DNA and RNA-based molecular structures by simply diluting/concentrating a sample about the poly(A)-ligand ‘critical concentration’. The ligands described here may also find biological or medicinal applications, owing to the 3′-polyadenylation of mRNA in living cells.     

Effects of Escherichia coli SSB protein on the single-stranded DNA-dependent ATPase activity of Escherichia coli RecA protein: Evidence that SSB protein facilitates the binding of RecA protein to regions of secondary structure within single-stranded DNA

The effect that Escherichia coli single-stranded DNA binding (SSB) protein has on the single-stranded DNA-dependent ATPase activity of RecA protein is shown to depend upon a number of variables such as order of addition, magnesium concentration, temperature and the type of single-stranded DNA substrate used. When SSB protein is added to the DNA solution prior to the addition of RecA protein, a significant inhibition of ATPase activity is observed. Also, when SSB protein is added after the formation of a RecA protein-single-stranded DNA complex using either etheno M13 DNA, poly(dA) or poly(dT), or using single-stranded phage M13 DNA at lower temperature (25 °C) and magnesium chloride concentrations of 1 mm or 4 mm, a time-dependent inhibition of activity is observed. These results are consistent with the conclusion that SSB protein displaces the RecA protein from these DNA substrates, as described in the accompanying paper. However, if SSB protein is added last to complexes of RecA protein and single-stranded M13 DNA at elevated temperature (37 °C) and magnesium chloride concentrations of 4 mm or 10 mm, or to poly(dA) and poly(dT) that was renatured in the presence of RecA protein, no inhibition of ATPase activity is observed; in fact, a marked stimulation is observed for single-stranded M13 DNA. A similar effect is observed if the bacteriophage T4-coded gene 32 protein is substituted for SSB protein. The apparent stoichiometry of DNA (nucleotides) to RecA protein at the optimal ATPase activity for etheno M13 DNA, poly(dA) and poly(dT) is 6(±1) nucleotides per RecA protein monomer at 4 mm-MgCl₂ and 37 °C. Under the same conditions, the apparent stoichiometry obtained using single-stranded M13 DNA is 12 nucleotides per RecA protein monomer; however, the stoichiometry changes to 4.5 nucleotides per RecA protein monomer when SSB protein is added last. In addition, a stoichiometry of four nucleotides per RecA protein can be obtained with single-stranded M13 DNA in the absence of SSB protein if the reactions are carried out in 1 mm-MgCl₂. These data are consistent with the interpretation that secondary structure within the natural DNA substrate limits the accessibility of RecA protein to these regions. The role of SSB protein is to eliminate this secondary structure and allow RecA protein to bind to these previously inaccessible regions of the DNA. In addition, our results have disclosed an additional property of the RecA protein-single-stranded DNA complex: namely, in the presence of complementary base-pairing and at elevated temperatures and magnesium concentrations, a unique RecA protein-DNA complex forms that is resistant to inhibition by SSB protein.     

M-DNA is stabilised in G*C tracts or by incorporation of 5-fluorouracil

M-DNA is a complex between the divalent metal ions Zn²⁺, Ni²⁺ and Co²⁺ and duplex DNA which forms at a pH of ~8.5. The stability and formation of M-DNA was monitored with an ethidium fluorescence assay in order to assess the relationship between pH, metal ion concentration, DNA concentration and the base composition. The dismutation of calf thymus DNA exhibits hysteresis with the formation of M-DNA occurring at a higher pH than the reconversion of M-DNA back to B-DNA. Hysteresis is most prominent with the Ni form of M-DNA where complete reconversion to B-DNA takes several hours even in the presence of EDTA. Increasing the DNA concentration leads to an increase in the metal ion concentration required for M-DNA formation. Both poly(dG)•poly(dC) and poly(dA)•poly(dT) formed M-DNA more readily than the corresponding mixed sequence DNAs. For poly(dG)•(poly(dC) M-DNA formation was observed at pH 7.4 with 0.5 mM ZnCl₂. Modified bases were incorporated into a 500 bp fragment of phage λ DNA by polymerase chain reaction. DNAs in which guanine was replaced with hypoxanthine or thymine with 5-fluorouracil formed M-DNA at pHs below 8 whereas substitutions such as 2-aminoadenine and 5-methylcytosine had little effect. Poly[d(A5FU)] also formed a very stable M-DNA duplex as judged from T_m measurements. It is evident that the lower the pK_a of the imino proton of the base, the lower the pH at which M-DNA will form; a finding that is consistent with the replacement of the imino proton with the metal ion.     

Origin of the intrinsic rigidity of DNA

The intrinsic rigidities of DNA and RNA helices are generally thought to arise from some combination of vertical base-stacking interactions and intra-helix phosphate–phosphate charge repulsion; however, the relative contributions of these two types of interaction to helix rigidity have not been quantified. To address this issue, we have measured the rotational decay times of a ‘gapped-duplex’ DNA molecule possessing a central, single-stranded region, dT₂₄, before and after addition of the free purine base, N⁶-methyladenine (^meA). Upon addition of ^meA, the bases pair with the T residues, forming a continuous stack within the gap region. Formation of the gapped duplex is accompanied by a nearly 2-fold increase in decay time, to values that are indistinguishable from the full duplex control for monovalent salt concentrations up to 90 mM. These results indicate that at least 90% of the rigidity of the dT_n–dA_n homopolymer derives from base pair stacking effects, with phosphate–phosphate interactions contributing relatively little to net helix rigidity at moderate salt concentrations.     

Differences in melting behavior between homopolymers and copolymers of DNA: Role of nonbonded forces for GC and the role of the hydration spine and premelting transition for AT

Melting measurements of the mono-base-pair DNA polymers showed that the melting temperature T_m of the B-DNA homopolymer poly (dA ) · poly (dT) is higher than that of the copolymer poly [d(A-T)]. On the other hand, the T_mof the B-DNA homopolymer poly (dG) · poly (dC) is lower than that of the copolymer poly [d (G-C)]. From a structural point of view, the cross-strand base-stacking interaction in a DNA homopolymer is weaker than that in a DNA copolymer with the same base pair. One would then expect that all the DNA homopolymers are less stable than the copolymer with the same base pair. We find that the inversion of the melting order seen in the AT mono-base-pair DNA polymers is caused by the enhanced thermal stability of poly (dA) · poly (dT) from a well-defined spine of hydration attached to its minor groove. In this paper we employ the modified self-consistent phonon theory to calculate base-pair opening probabilities of four B-DNA polymers: poly(dA)-poly(dT), poly(dG) · poly(dC), poly[d(A-T)], and poly[d(G-C)] at temperatures from room temperature through the melting regions. Our calculations show that the spine of hydration can give the inverted melting order of the AT polymers as compared to the GC polymers in fair agreement with experimental measurements. Our calculated hydration spine disruption behavior in poly(dA) · poly(dT) at premelting temperatures is also in agreement with experimentally observed premelting transitions in poly (dA) · poly (dT). The work is in a sense a test of the validity of our models of nonbonded interactions and spine of hydration interactions. We find we have to develop the concept of a strained bond to fit observations in poly (dA) · poly(dT). The strained-bond concept also explains the otherwise anomalous stability of the hydration chain. © 1993 John Wiley & Sons, Inc.     

Controlling nucleic acid secondary structure by intercalation: effects of DNA strand length on coralyne-driven duplex disproportionation

Small molecules that intercalate in DNA and RNA are powerful agents for controlling nucleic acid structural transitions. We recently demonstrated that coralyne, a small crescent-shaped molecule, can cause the complete and irreversible disproportionation of duplex poly(dA)·poly(dT) into triplex poly(dA)·poly(dT)·poly(dT) and a poly(dA) self- structure. Both DNA secondary structures that result from duplex disproportionation are stabilized by coralyne intercalation. In the present study, we show that the kinetics and thermodynamics of coralyne-driven duplex disproportionation strongly depend on oligonucleotide length. For example, disproportionation of duplex (dA)₁₆·(dT)₁₆ by coralyne reverts over the course of hours if the sample is maintained at 4°C. Coralyne-disproportioned (dA)₃₂· (dT)₃₂, on the other hand, only partially reverts to the duplex state over the course of days at the same temperature. Furthermore, the equilibrium state of a (dA)₁₆·(dT)₁₆ sample in the presence of coralyne at room temperature contains three different secondary structures [i.e. duplex, triplex and the (dA)₁₆ self-structure]. Even the well-studied process of triplex stabilization by coralyne binding is found to be a length-dependent phenomenon and more complicated than previously appreciated. Together these observations indicate that at least one secondary structure in our nucleic acid system [i.e. duplex, triplex or (dA)_n self-structure] binds coralyne in a length-dependent manner.     

The binding affinity of Ff gene 5 protein depends on the nearest-neighbor composition of the ssDNA substrate

The Ff gene 5 protein (g5p) is considered to be a nonspecific single-stranded DNA binding protein, because it binds cooperatively to and saturates the Ff bacteriophage single-stranded DNA genome and other single-stranded polynucleotides. However, the binding affinity Komega (the intrinsic binding constant times a cooperativity factor) differs by over an order of magnitude for binding to single-stranded polynucleotides such as poly[d(A)] and poly[d(C)]. A polynucleotide that is more stacked, like poly[d(A)], binds more weakly than one that is less stacked, like poly[d(C)]. To test the hypothesis that DNA base stacking, a nearest-neighbor property, is involved in the binding affinity of the Ff g5p for different DNA sequences, Komega values were determined as a function of NaCl concentration for binding to six synthetic sequences 48 nucleotides in length: dA48, dC48, d(AAC)16, d(ACC)16, d(AACC)12, and d(AAACC)9A3. The binding affinities of the protein for these sequences were indeed found to be related to the nearest-neighbor compositions of the sequences, rather than to simple base compositions. That is, the g5p binding site, which is spanned by four nucleotides, discriminates among these sequences on the basis of the relative numbers of nearest neighbors (AA, CC, and AC plus CA) in the sequence. The results support the hypothesis that the extent of base stacking/unstacking of the free, nonbound ssDNA plays an important role in the binding affinity of the Ff gene 5 protein.     

Characterization of a Baculovirus-Encoded ATP-Dependent DNA Ligase

Sequence analysis of the Lymantria dispar multicapsid nucleopolyhedrovirus (LdMNPV) genome identified an open reading frame (ORF) encoding a 548-amino-acid (62-kDa) protein that showed 35% amino acid sequence identity with vaccinia virus ATP-dependent DNA ligase. Ligase homologs have not been reported from other baculoviruses. The ligase ORF was cloned and expressed as an N-terminal histidine-tagged fusion protein. Incubation of the purified protein with [α-³²P]ATP resulted in formation of a covalent enzyme-adenylate intermediate which ran as a 62-kDa labeled band on a sodium dodecyl sulfate-polyacrylamide gel. Loss of the radiolabeled band occurred upon incubation of the intermediate with pyrophosphate, poly(dA) · poly(dT)_12–18, or poly(rA) · poly(dT)_12–18, characteristics of a DNA ligase II or III. The protein was able to ligate a double-stranded synthetic DNA substrate containing a single nick and inefficiently ligated a 1-nucleotide (nt) gap but did not ligate a 2-nt gap. It was able to ligate short, complementary overhangs but not blunt-ended double-stranded DNA. In a transient DNA replication assay employing six plasmids containing the LdMNPV homologs of the essential baculovirus replication genes, a plasmid containing the DNA ligase gene was neither essential nor stimulatory. All of these results are consistent with the activity of type III DNA ligases, which have been implicated in DNA repair and recombination.     

Polymorphism of DNA double helices

Native DNA duplexes in fibers exist usually in one of three well-known (A, B and C) forms depending on relative humidity, type of cations and the amount of retained salt. To determine the precise influence of these factors and the effect of base composition, as well as base sequence, on DNA secondary structure, X-ray diffraction methods have been used to study all four synthetic DNA duplexes with repeated dinucleotide sequences, eight of the 12 with repeated trinucleotide sequences and seven analogues in which guanine was replaced with hypoxanthine. The results indicate that there are at least six additional allomorphs denoted by B′, C′, C″, D, E and S.The B′ form (h = 0.329 nm) observed for poly(dA) · poly(dT), poly(dI) · poly(dC) and poly[d(A-I)] · poly[d(C-T)] is a minor variant of the traditional B form (h = 0.338 nm) of native DNA. The two C-like forms C′ for poly[d(A-G-C)] · poly-[d(G-C-T)] and poly[d(G-G-T)] · poly[d(A-C-C)] and C″ for poly[d(A-G)] · poly-[d(C-T)] have, respectively, 9₁ and 9₂ symmetries which reflect repetition of trinucleotide and dinucleotide sequences, respectively. Although isocompositional with poly(dA) · poly(dT), the existence of the rather different D form (8₁) for poly[d(A-T)] · poly[d(A-T)] or for poly[d(A-A-T)] · poly[d(A-T-T)] is a clear demonstration of the sequence effect. The I · C pair generally mimics an A · T pair, but poly[d(I-I-T)] · poly[d(A-C-C)] provides a new (E) form with approximately 15₂ screw symmetry and with 〈h〉 = 0.325 nm and 〈t〉 = 48 dg per nucleotide. The S form (6₅) observed for poly[d(G-C)] · poly[d(G-C)] and poly[d(A-C)] · poly[d(G-T)] is an unusual left-handed polydinucleotide helix and is accessible to any alternating purine-pyrimidine sequence. In it the two nucleotides have quite different conformations and involve syn purine and anti pyrimidine nucleosides.     

Diadenosine 5′,5‴-P1,P4-tetraphosphate- (Ap4A-) mediated stimulation of DNA synthesis in extracts from Xenopus laevis oocytes

Diadenosine 5′,5‴-P¹,P⁴-tetraphosphate (Ap₄A) stimulates DNA synthesis in Xenopus laevis oocytes in the presence of activated DNA as template. Besides Ap₄A, other analogues such as Ap₃A, ATP and other derivatives are able to stimulate DNA polymerase activity. The effect of Ap₄A on DNA synthesis is observed with poly(dT) and poly(dT)-poly(dA) as templates, while no effect is found with poly(dA)(dT)_12–18 and poly(dC)(dG)_12–18. In the presence of a poly(dT) template, the oocyte extract is able to utilize Ap₄A as primer and to form a covalent bond between this dinucleotide and the nascent poly(dA) chain. An Ap₄A-binding protein present in the system has been purified and separated from DNA polymerase α-primase after phosphocellulose chromatography. After this separation, Ap₄A is no longer able to stimulate the polymerase activity, or to be utilized as primer by DNA polymerase α-primase.     

Characterization of 1,25-dihydroxyvitamin D3-receptor complex interactions with DNA by a competitive assay

To identify and assess the specificity of the 1,25-dihydroxyvitamin D₃ chick intestinal cytoplasmic receptor's nucleotide binding site, a competitive DNA-cellulose binding assay was utilized. Unlike other steroid hormone receptors, the 1,25-dihydroxyvitamin D₃-receptor complex binds homologous DNA at 4 °C and does not appear to undergo thermal- or salt-induced activation. Data are presented which suggest that receptor binding discriminates between double-stranded DNA and RNA but is not specific with respect to DNA base sequences. However, DNA base sequence selectivity by 1,25-dihydroxyvitamin D₃-receptor complexes is observed using synthetic polydeoxyribonucleotides, particularly, poly(dA-dT) · poly(dA-dT) and poly(dA) · poly(dT). Preference for double-stranded over single-stranded DNA was also observed. Consistent with this finding, both actinomycin D and ethidium bromide caused a dose-dependent inhibition of receptor binding to DNA-cellulose. It is concluded that the 1,25-dihydroxyvitamin D₃-receptor complex has specificity for AT-rich segments of double-stranded DNA and that this interaction is not merely electrostatic, but also involves hydrophobic interaction with the major and/or minor grooves of the DNA helix.     

Fluorescence studies of the complex formation between the gene 5 protein of bacteriophage M13 and polynucleotides

The binding characteristics of the interaction of gene 5 protein with polynucleotides, i.e. poly(dA), poly(dT) and M13 DNA, have been determined by following the quenching of the protein fluorescence. In general, the binding is highly co-operative and for the binding of the protein to poly(dA) and M13 DNA the co-operativity parameter ω is estimated to have values between 50 and 300. Under comparable experimental conditions, the intrinsic binding constant K_int is at least two orders of magnitude higher for poly(dT) than for poly(dA), while the value for M13 DNA is intermediate. For poly(dA), the binding has been studied as a function of ionic strength and temperature. From these experiments it can be concluded that ionic interactions as well as van der Waals interactions (e.g. stacking interactions) are important for the complex formation of the protein with polynucleotides. From a comparison of the binding of the protein to poly(dA) and poly(dT), it is concluded that stacking interactions in the polynucleotide have a negative influence on protein binding. This conclusion, in conjunction with the weak temperature dependence of K_int. indicates that ionic interactions play a major role in the stabilization of the protein-poly(dA) complex. The co-operativity factor ω is little or not dependent on the ionic strength or the type of polynucleotide involved in binding. It is determined by interactions between complexed protein molecules. These interactions are primarily non-electrostatic.The binding characteristics obtained for the gene 5 protein-polynucleotide complexes are compared with those we have found for the binding to small oligonucleotides. It appears that oligonucleotide and polynucleotide binding differ in many aspects; i.e. there is a difference in K_int, ω and the number of nucleotides covered. The validity of linear lattice binding theories is discussed in this context. By comparing the binding parameters found for the gene 5 protein with those of the Escherichia coli DNA binding protein I. it is possible to explain the displacement of the E. coli protein by the gene 5 protein that occurs in vivo.     

Microcalorimetric Investigation of DNA,poly(dA)poly(dT) and poly[d(A-C)]poly[d(G-T)] Melting in the Presence of Water Soluble (Meso tetra (4 N oxyethylpyridyl) Porphyrin) and its Zn Complex

Abstract

Thermodynamic parameters of melting process (δH_m, T_m, δT_m) of calf thymus DNA, poly(dA)poly(dT) and poly(d(A-C))·poly(d(G-T)) were determined in the presence of various concentrations of TOEPyP(4) and its Zn complex. The investigated porphyrins caused serious stabilization of calf thymus DNA and poly poly(dA)poly(dT), but not poly(d(A-C))poly(d(G-T)). It was shown that TOEpyp(4) revealed GC specificity, it increased T_m of satellite fraction by 24°C, but ZnTOEpyp(4), on the contrary, predominately bound with AT-rich sites and increased DNA main stage T_m by 18°C, and T_m of poly(dA)poly(dT) increased by 40 °C, in comparison with the same polymers without porphyrin. ZnTOEpyp(4) binds with DNA and poly(dA)poly(dT) in two modes—strong and weak ones. In the range of r from 0.005 to 0.08 both modes were fulfilled, and in the range of r from 0.165 to 0.25 only one mode—strong binding—took place. The weak binding is characterized with shifting of T_m by some grades, and for the strong binding T_m shifts by ～ 30–40°C. Invariability of ΔH_m of DNA and poly(dA)poly(dT), and sharp increase of T_m in the range of r from 0.08 to 0.25 for thymus DNA and 0.01–0.2 for poly(dA)poly(dT) we interpret as entropic character of these complexes melting. It was suggested that this entropic character of melting is connected with forcing out of H₂O molecules from AT sites by ZnTOEpyp(4) and with formation of outside stacking at the sites of binding. Four-fold decrease of calf thymus DNA melting range width ΔT_m caused by increase of added ZnTO- Epyp(4) concentration is explained by rapprochement of AT and GC pairs thermal stability, and it is in agreement with a well-known dependence, according to which ΔT～T_GC-T_AT for DNA obtained from higher organisms (L. V. Berestetskaya, M. D. Frank-Kamenetskii, and Yu. S. Lazurkin. Biopolymers 13, 193–205 (1974)). Poly (d(A-C))poly(d(G-T)) in the presence of ZnTOEpyp(4) gives only one mode of weak binding. The conclusion is that binding of ZnTOEpyp(4) with DNA depends on its nucleotide sequence.     

The interactions between the fluorescent dye thiazole orange and DNA

The interaction of the fluorescent dye thiazole orange (TO) with nucleic acids is characterized. It is found that TO binds with highest affinity to double-stranded (ds) DNA [log(K) ≈ 5.5 at 100 mM salt], about 5–10 times weaker to single-stranded polypurines, and further 10–1000 times weaker to single-stranded polypyrimidines. TO binds as a monomer to dsDNAs and poly(dA), both as a monomer and as a dimer to poly(dG) and mainly as a dimer to poly(dC) and poly(dT). The fluorescence quantum yield of TO free in solution is about 2 · 10⁻⁴, and it increases to about 0.1 when bound to dsDNA or to poly(dA), and to about 0.4 when bound to poly(dG). Estimated quantum yields of TO bound to poly(dC) and poly(dT) are about 0.06 and 0.01, respectively. The quantum yield of bound TO depends on temperature and decreases about threefold between 5 and 50°C. © 1998 John Wiley & Sons, Inc. Biopoly 46: 39–51, 1998     

Berberine–DNA complexation: New insights into the cooperative binding and energetic aspects

The equilibrium binding of the cytotoxic plant alkaloid berberine to various DNAs and energetics of the interaction have been studied. At low ratios of bound alkaloid to base pair, the binding exhibited cooperativity to natural DNAs having almost equal proportions of AT and GC sequences. In contrast, the binding was non-cooperative to DNAs with predominantly high AT or GC sequences. Among the synthetic DNAs, cooperative binding was observed with poly(dA).poly(dT) and poly(dG).poly(dC) while non-cooperative binding was seen with poly(dA–dT).poly(dA–dT) and poly(dG–dC).poly(dG–dC). Both cooperative and non-cooperative bindings were remarkably dependent on the salt concentration of the media. Linear plots of ln K_a versus [Na⁺] for poly(dA).poly(dT) and poly(dA–dT).poly(dA–dT) showed the release of 0.56 and 0.75 sodium ions respectively per bound alkaloid. Isothermal titration calorimetry results revealed the binding to be exothermic and favoured by both enthalpy and entropy changes in all DNAs except the two AT polymers and AT rich DNA, where the same was predominantly entropy driven. Heat capacity values (ΔCp^o) of berberine binding to poly(dA).poly(dT), poly(dA–dT).poly(dA–dT), Clostridium perfringens and calf thymus DNA were − 98, − 140, − 120 and − 110 cal/mol K respectively. This study presents new insights into the binding dependent base pair heterogeneity in DNA conformation and the first complete thermodynamic profile of berberine binding to DNAs.     

Molecular dynamics simulations and coupled nucleotide substitution experiments indicate the nature of A·A base pairing and a putative structure of the coralyne-induced homo-adenine duplex

Coralyne is an alkaloid drug that binds homo-adenine DNA (and RNA) oligonucleotides more tightly than it does Watson–Crick DNA. Hud’s laboratory has shown that poly(dA) in the presence of coralyne forms an anti-parallel duplex, however attempts to determine the structure by NMR spectroscopy and X-ray crystallography have been unsuccessful. Assuming adenine–adenine hydrogen bonding between the two poly(dA) strands, we constructed 40 hypothetical homo-(dA) anti-parallel duplexes and docked coralyne into the six most favorable duplex structures. The two most stable structures had trans glycosidic bonds, but distinct pairing geometries, i.e. either Watson–Crick Hoogsteen (transWH) or Watson–Crick Watson–Crick (transWW) with stability of transWH > transWW. To narrow down the possibilities, 7-deaza adenine base substitutions (dA→7) were engineered into homo-(dA) sequences. These substitutions significantly reduced the thermal stability of the coralyne-induced homo-(dA) structure. These experiments strongly suggest the involvement of N7 in the coralyne-induced A·A base pairs. Moreover, due to the differential effect on melting as a function of the location of the dA→7 mutations, these results are consistent with the N1–N7 base pairing of the transWH pairs. Together, the simulation and base substitution experiments predict that the coralyne-induced homo-(dA) duplex structure adopts the transWH geometry.     

Base-stacking and base-pairing contributions into thermal stability of the DNA double helix

Two factors are mainly responsible for the stability of the DNA double helix: base pairing between complementary strands and stacking between adjacent bases. By studying DNA molecules with solitary nicks and gaps we measure temperature and salt dependence of the stacking free energy of the DNA double helix. For the first time, DNA stacking parameters are obtained directly (without extrapolation) for temperatures from below room temperature to close to melting temperature. We also obtain DNA stacking parameters for different salt concentrations ranging from 15 to 100 mM Na⁺. From stacking parameters of individual contacts, we calculate base-stacking contribution to the stability of A•T- and G•C-containing DNA polymers. We find that temperature and salt dependences of the stacking term fully determine the temperature and the salt dependence of DNA stability parameters. For all temperatures and salt concentrations employed in present study, base-stacking is the main stabilizing factor in the DNA double helix. A•T pairing is always destabilizing and G•C pairing contributes almost no stabilization. Base-stacking interaction dominates not only in the duplex overall stability but also significantly contributes into the dependence of the duplex stability on its sequence.     

Calorimetric determination of the heat capacity changes associated with the conformational transitions of polyriboadenylic acid and polyribouridylic acid

The heat capacities of the single-stranded and double-stranded forms of polyadenylic acid, polyuridylic acid, and poly(uridylic and adenylic acid) were determined with a drop heat capacity calorimeter. In addition, the temperature dependence of the apparent partial heat capacity (?Cp) was measured with a newly developed differential scanning calorimeter. The calculated ΔCp at 28°C for the transition poly(A)·poly(A) ? 2 poly(A) was found to be 165 ± 24 cal/Kmol-base pair, compared with a value of 140 ± 28 for the transition poly(A)·poly(U) ? poly(A) + poly(U). The temperature dependence of ?Cp of single-stranded poly(U) was consistent with the conclusion that it is totally unstacked at temperatures above 15°C. The temperature dependence of ?Cp of single-stranded poly(A) was used to determine the base-stacking parameters for poly(A). The experimental results are consistent with a stacking enthalpy change of ?8.5 ± 0.1 kcal/mol bases and a cooperativity parameter σ of 0.57 ± 0.03 for the stacking of adenine bases. These results demonstrate that the heat capacity of single-stranded polynucleotides is greater than that of the double-stranded forms. This increased heat capacity is mainly the result of the temperature dependence of the base-stacking interactions in the single-stranded form.