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

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

Differential hydration of dA.dT base pairing and dA and dT bulges in deoxyoligonucleotides

The role of water in the formation of stable duplexes of nucleic acids is being studied by determining the concurrent volume change, heats, and counterion uptake that accompany the duplexation process. The variability of the volume contraction that we have observed in the formation of a variety of homoduplexes suggests that sequence and conformation acutely affect the degree of hydration. We have used a combination of densimetric and calorimetric techniques to measure the change in volume and enthalpy resulting from the mixing of two complementary strands to form (a) fully paired duplexes with 10 or 11 base pairs and (b) bulged decameric duplexes with an extra dA or dT unmatched residue. We also monitored absorbance vs temperature profiles as a function of strand and salt concentration for all four duplexes. Relative to the decamer duplex, insertion of an extra dA.dT base pair to form an undecamer duplex results in a favorable enthalpy of -5.6 kcal/mol that is nearly compensated by an unfavorable entropy term of -5.1 kcal/mol. This enthalpy difference correlates with a differential uptake of water molecules, corresponding to an additional hydration of 16 mol of water molecules/mol of base pair. Relative to the fully paired duplexes, both bulged duplexes are 12-16 degrees C less stable and exhibit marginally larger counterion uptake on forming the duplex. The enthalpy change is slightly lower for the T-bulge duplex and less still for the A-bulge duplex. The volume change results indicate that an unmatched residue increases the amount of coulombic and/or structural hydration. The combined results strongly suggest that the destabilizing forces in bulged duplexes are partially compensated by an increase in hydration levels.     

Thermodynamic parameters of the binding of retinol to binding proteins and to membranes

Retinol (vitamin A alcohol) is a hydrophobic compound and distributes in vivo mainly between binding proteins and cellular membranes. To better clarify the nature of the interactions of retinol with these phases which have a high affinity for it, the thermodynamic parameters of these interactions were studied. The temperature-dependence profiles of the binding of retinol to bovine retinol binding protein, bovine serum albumin, unilamellar vesicles of dioleoylphosphatidylcholine, and plasma membranes from rat liver were determined. It was found that binding of retinol to retinol binding protein is characterized by a large increase in entropy (T delta S degrees = +10.32 kcal/mol) and no change in enthalpy. Binding to albumin is driven by enthalpy (delta H degrees = -8.34 kcal/mol) and is accompanied by a decrease in entropy (T delta S degrees = -2.88 kcal/mol). Partitioning of retinal into unilamellar vesicles and into plasma membranes is stabilized both by enthalpic (delta H degrees was -3.3 and -5.5 kcal/mol, respectively) and by entropic (T delta S degrees was +4.44 and +2.91 kcal/mol, respectively) components. The implications of these finding are discussed.     

UV resonance Raman and circular dichroism studies of a DNA duplex containing an A(3)T(3) tract: evidence for a premelting transition and three-centered H-bonds.

The presence of A(n) and A(n)T(n) tracts in double-helical sequences perturbs the structural properties of DNA molecules, resulting in the formation of an alternate conformation to standard B-DNA known as B'-DNA. Evidence for a transition occurring prior to duplex melting in molecules containing A(n) tracts was previously detected by circular dichroism (CD) and calorimetric studies. This premelting transition was attributed to a conformational change from B'- to B-DNA. Structural features of A(n) and A(n)T(n) tracts revealed by X-ray crystallography include a large degree of propeller twisting of adenine bases, narrowed minor grooves, and the formation of three-centered H-bonds between dA and dT bases. We report UV resonance Raman (UVRR) and CD spectroscopic studies of two related DNA dodecamer duplexes, d(CGCAAATTTGCG)(2) (A(3)T(3)) and d(CGCATATATGCG)(2) [(AT)(3)]. These studies address the presence of three-centered H-bonds in the B' conformation and gauge the impact of these putative H-bonds on the structural and thermodynamic properties of the A(3)T(3) duplex. UVRR and CD spectra reveal that the premelting transition is only observed for the A(3)T(3) duplex, is primarily localized to the dA and dT bases, and is associated with base stacking interactions. Spectroscopic changes associated with the premelting transition are not readily detectable for the sugar-phosphate backbone or the cytosine and guanosine bases. The temperature-dependent concerted frequency shifts of dA exocyclic NH(2) and dT C4=O vibrational modes suggest that the A(3)T(3) duplex forms three-centered hydrogen bonds at low temperatures, while the (AT)(3) duplex does not. The enthalpy of this H-bond, estimated from the thermally induced frequency shift of the dT C4=O vibrational mode, is approximately 1.9 kJ/mol or 0.46 kcal/mol.     

Protoberberine Alkaloids Berberine,Palmatine, and Coralyne Binding to Poly(dT)⋅(Poly(dA)⋅Poly(dT)) Triplex: Comparative Structural Aspects and Energetics Profiles of the Interaction

The interaction of bioactive protoberberine alkaloids berberine, palmatine, and coralyne with the DNA triplex poly(dT)⋅(poly(dA)⋅poly(dT)) was studied using biophysical and calorimetric techniques. All three alkaloids bound the triplex cooperatively. Berberine and palmatine predominantly stabilized the triplex structure, while coralyne stabilized both triplex and duplex structures as inferred from optical thermal melting profiles. Fluorescence quenching, polarization, and viscometric studies hinted at an intercalative mode of binding for the alkaloids to the triplex, coralyne being more strongly intercalated compared to partial intercalation of berberine and palmatine. The overall affinity of coralyne was two order higher (2.29×10⁷ M ⁻¹) than that of berberine (3.43×10⁵ M ⁻¹) and palmatine (2.34×10⁵ M ⁻¹). Isothermal titration calorimetric studies revealed that the binding to the triplex was favored by negative enthalpy change (ΔH=−3.34 kcal/mol) with favorable entropy contribution (TΔS = 4.07 kcal/mol) for berberine, favored by almost equal negative enthalpy (ΔH =−3.88 kcal/mol) and entropy changes (TΔS = 3.37 kcal/mol) for palmatine, but driven by large enthalpy contributions (ΔH =−25.62 kcal/mol and TΔS =−15.21 kcal/mol) for coralyne. These results provide new insights on the binding of isoquinoline alkaloids to the DNA triplex structure.     

Thermodynamics of RNA duplexes with tandem mismatches containing a uracil-uracil pair flanked by C.G/G.C or G.C/A.U closing base pairs

The thermodynamics governing the denaturation of RNA duplexes containing 8 bp and a central tandem mismatch or 10 bp were evaluated using UV absorbance melting curves. Each of the eight tandem mismatches that were examined had one U-U pair adjacent to another noncanonical base pair. They were examined in two different RNA duplex environments, one with the tandem mismatch closed by G.C base pairs and the other with G.C and A.U closing base pairs. The free energy increments (Delta Gdegrees(loop)) of the 2 x 2 loops were positive, and showed relatively small differences between the two closing base pair environments. Assuming temperature-independent enthalpy changes for the transitions, (Delta Gdegrees(loop)) for the 2 x 2 loops varied from 0.9 to 1.9 kcal/mol in 1 M Na(+) at 37 degrees C. Most values were within 0.8 kcal/mol of previously estimated values; however, a few sequences differed by 1.2-2.0 kcal/mol. Single strands employed to form the RNA duplexes exhibited small noncooperative absorbance increases with temperature or transitions indicative of partial self-complementary duplexes. One strand formed a partial self-complementary duplex that was more stable than the tandem mismatch duplexes it formed. Transitions of the RNA duplexes were analyzed using equations that included the coupled equilibrium of self-complementary duplex and non-self-complementary duplex denaturation. The average heat capacity change (DeltaC(p)) associated with the transitions of two RNA duplexes was estimated by plotting DeltaH degrees and DeltaS degrees evaluated at different strand concentrations as a function of T(m) and ln T(m), respectively. The average DeltaC(p) was 70 +/- 5 cal K(-)(1) (mol of base pairs)(-)(1). Consideration of this heat capacity change reduced the free energy of formation at 37 degrees C of the 10 bp control RNA duplexes by 0.3-0.6 kcal/mol, which may increase Delta Gdegrees(loop) values by similar amounts.     

Effect of basic oligopeptides on the B-Z transition of poly(dG-dC). poly(dG-dC) in water-methanol solutions

The effect of basic oligopeptides (Lys-Ala-Ala)n (n = 1-5, 10) and (Lys-Leu-Ala)n (n = 1-4) on the B-Z transition of poly(dG-dC).poly(dG-dC) in water-methanol solutions was investigated using CD and uv spectroscopy. In the absence of peptides, the concentration of methanol at the midpoint of the B-Z transition is 64% at 25 degrees C. The transition is temperature dependent and the B conformation is preferred at higher temperatures. All peptides tested shift the midpoint of the B-Z transition to lower concentrations of methanol. For shorter peptides this effect increases with an increasing number of monomeric units, showing the importance of the number of positive charges in the peptide molecule. Al conditions of low methanol content, the trimer and tetramer of the (Lys-Leu-Ala)n series have a greater effect on the B-Z transition than the corresponding oligomers of the (Lys-Ala-Ala)n series. This indicates an important influence of the presence of hydrophobic groups in the peptide side chains on the binding. In the presence of peptides, the B-Z transition is also temperature dependent and the B conformation is preferred at higher temperatures. The addition of peptides results in an increase of the transition midpoint and of the transition width. These parameters were used for the calculation of the transition enthalpy delta HB-Z in 65% methanol, which is -1.15 +/- 0.25 kcal/base pair. Since the van't Hoff enthalpy delta HVH calculated from the temperature dependence of the B-Z transition in the absence of peptides is -130 kcal/mol, the length of the cooperative unit is about 110 base pairs. The results suggest that the mechanism of Z-DNA induction is similar but not identical with that involved in the action of metal cations in aqueous solution.     

Sequence dependence of the stability of RNA hairpin molecules with six nucleotide loops

Thermodynamic parameters are reported for hairpin formation in 1 M NaCl by RNA sequence of the types GCGXUAAUYCGC and GGUXUAAUYACC with Watson-Crick loop closure, where XY is the set of 10 possible mismatch base pairs. A nearest-neighbor analysis of the data indicates the free energy of loop formation at 37 degrees C varies from 3.1 to 5.1 kcal/mol. These results agree with the model previously developed [Vecenie, C. J., and Serra, M. J. (2004) Biochemistry 43, 11813] to predict the stability of RNA hairpin loops: DeltaG degrees (37L(n) = DeltaG degrees (37i(n) + DeltaG degrees (37MM) - 0.8 (if first mismatch is GA or UU) - 0.8 (if first mismatch is GG and loop is closed on the 5' side by a purine). Here, DeltaG degrees (37i(n) is the free energy for initiating a loop of n nucleotides, and DeltaG degrees (37MM) is the free energy for the interaction of the first mismatch with the closing base pair. Thermodynamic parameters are also reported for hairpin formation in 1 M NaCl by RNA sequence of the types GACGXUAAUYUGUC and GGUXUAAUYGCC with GU base pair closure, where XY is the set of 10 possible mismatch base pairs. A nearest-neighbor analysis of the data indicates the free energy of loop formation at 37 degrees C varies from 3.6 to 5.3 kcal/mol. These results allow the development of a model for predicting the stability of hairpin loops closed by GU base pairs. DeltaG degrees (37L(n) (kcal/mol) = DeltaG degrees (37i(n) - 0.8 (if the first mismatch is GA) - 0.8 (if the first mismatch is GG and the loop is closed on the 5' side by a purine). Note that for these hairpins, the stability of the loops does not depend on DeltaG degrees (37MM). For hairpin loops closed by GU base pairs, the DeltaG degrees (37i(n) values, when n = 4, 5, 6, 7, and 8, are 4.9, 5.0, 4.6, 5.0, and 4.8 kcal/mol, respectively. The model gives good agreement when tested against six naturally occurring hairpin sequences. Thermodynamic values for terminal mismatches adjacent to GC, GU, and UG base pairs are also reported.     

The thermodynamic contribution of the 5-methyl group of thymine in the two- and three-stranded complexes formed by poly(dU) and poly(dT) with poly(dA)

To assess the thermodynamic contribution of the 5-methyl group of thymine, we have studied the two-stranded helical complexes poly(dA).poly(dU) and poly(dA).poly(dT) and the three-stranded complexes--poly(dA).2poly(dU), poly(dA).poly(dT).poly(dU) and poly(dA).2poly(dT)--by differential scanning calorimetry, and uv optical melting experiments. The thermodynamic quantities associated with the 3 --> 2, 2 --> 1, and 3 --> 1 melting transitions are found to vary with salt concentration and temperature in a more complex manner than commonly believed. The transition temperatures, T(m), are generally not linear in the logarithm of concentration or activity of NaCl. The change in enthalpy and in entropy upon melting varies with salt concentration and temperature, and a change in heat capacity accompanies each transition. The poly(dA).2poly(dU) triple helix is markedly different from poly(dA).2poly(dT) in both its CD spectrum and thermodynamic behavior, while the poly(dA).poly(dT).poly(dU) triple helix resembles poly(dA).2poly(dT) in these properties. In comparing poly(dA).2poly(dT) with either the poly(dA).poly(dT).poly(dU) or the poly(dA).2poly(dU) triplexes, the substitution of thymine for uracil in the third strand results in an enhancement of stability against the 3 --> 2 dissociation of deltadeltaG degrees = -135 +/- 85 cal (mol A)(-1) at 37 degrees C. This represents a doubling of the absolute stability toward dissociation compared to the triplexes with poly(dU) as the third strand. The poly (dA).poly (dT) duplex is more stable than poly(dA).poly(dU) by deltadeltaG degrees = -350 +/- 60 cal (mol base pair)(-1) at 37 degrees C. Poly(dA).poly(dT) has 50% greater stability than poly(dA).poly(dU) as a result of the dT for dU substitution in the duplex.     

Thermodynamics-structure relationship of single mismatches in RNA/DNA duplexes

Thermodynamics of 66 RNA/DNA duplexes containing single mismatches were measured by UV melting methods. Stability enhancements for rG. dT mismatches were the largest of all mismatches examined here, while rU.dG mismatches were not as stable. The methyl group on C5 of thymine enhanced the stability by 0.12 approximately 0.53 kcal mol(-)(1) depending on the identity of adjacent Watson-Crick base pairs, whereas the 2'-hydroxyl group in ribouridine stabilized the duplex by approximately 0.6 kcal mol(-)(1) regardless of the adjacent base pairs. Stabilities induced by the methyl group in thymine, the 2'-hydroxyl group of ribouridine, and an nucleotide exchange at rG.dT and rU.dG mismatches were found to be independent of each other. The order for the mismatch stabilities is rG.dT > rU. dG approximately rG.dG > rA.dG approximately rG.dA approximately rA. dC > rA.dA approximately rU.dT approximately rU.dC > rC.dA approximately rC.dT, although the identity of the adjacent base pairs slightly altered the order. The pH dependence stability and structural changes were suggested for the rA.dG but not for rG.dA mismatches. Comparisons of trinucleotide stabilities for G.T and G.U pairs in RNA, DNA, and RNA/DNA duplexes indicate that stable RNA/DNA mismatches exhibit a stability similar to RNA mismatches while unstable RNA/DNA mismatches show a stability similar to that of DNA mismatches. These results would be useful for the design of antisense oligonucleotides.     

1H NMR and circular dichroism studies of the B and Z conformations of the self-complementary deoxyhexanucleotide d(m5C-G-C-G-m5-C-G): mechanism of the Z-B-coil transitions

The double-helical conformations of d(m5-C-G-C-G-m5-C-G) in aqueous solution were studied by circular dichroism and 1H NMR spectroscopy. In 0.1 M NaCl, only the B form is detected whereas the Z form is strongly predominant in 3 M NaCl. In the presence of 2 M NaCl, two resonance signals corresponding to the B and Z duplexes were observed for each proton below 50 degrees C, indicating a slow exchange between B and Z. However, the B-Z exchange becomes intermediate or fast in the 55-80 degrees C temperature interval. By contrast the exchange between B helix and single-stranded (or coil) forms is much faster for the same temperature conditions. The Z form is only detectable when the coil form is practically absent. With decreasing temperature the B form decreases in favor of the Z form. From proton line-width measurements under various experimental conditions, it was also shown that Z exchanges only with B, while the latter also exchanges with the single-stranded form (S): Z in equilibrium B in equilibrium S. The enthalpy value is about 8 +/- 1 kcal/mol for the B-Z transition and about 40 +/- 2 kcal/mol for the B-S dissociation (2 M NaCl solution). The activation energy is about 47 +/- 2 kcal/mol for the Z----B and 39 +/- 2 kcal/mol for the B----Z reaction. Very good agreement between the experimental results and computed data (based on the above kinetic reaction model) was found for the B, Z, and coil proportions. The B-Z transition of methylated d(C-G)n oligomers is only possible when the Watson-Crick hydrogen bonds between the CG base pairs are firmly maintained; otherwise, the transformation from B to Z would not occur, and B-S dissociation would take place instead.     

Thermodynamic, spectroscopic, and equilibrium binding studies of DNA sequence context effects in six 22-base pair deoxyoligonucleotides.

Effects of different end sequences on stability, circular dichroism spectra (CD), and enzyme binding properties were investigated for six 22-base pair, non-self-complementary duplex DNA oligomers. The center sequences of these deoxyoligonucleotides have 8-14 base pairs in common and are flanked on both sides by sequences differing in context and A-T content. Temperature-induced melting transitions monitored by differential scanning calorimetry (DSC) and ultraviolet absorbance were measured for the six duplexes in buffered 115 mM Na(+) solutions. Values of the melting transition enthalpy, DeltaH(cal), and entropy, DeltaS(cal), were obtained directly from DSC experiments. Melting transition parameters, DeltaH(vH) and DeltaS(vH), were also estimated from van't Hoff analysis of optical melting curves collected as a function of DNA concentration, assuming a two-state melting transition. Melting free energies (20 degrees C) of the six DNAs evaluated from DSC experiments ranged from -18.7 to -32.7 kcal/mol. van't Hoff estimates of the free energies ranged from -18.5 to -48.0 kcal/mol. With either method, the trends in free energy as a function of sequence were identical. Equilibrium binding by BamHI restriction endonuclease to the 22-base pair DNAs was also investigated. The central eight base pairs of all six molecules, 5'-A-GGATCC-A-3', contained a BamHI recognition sequence bounded by A-T base pairs. Magnesium free binding assays were performed by titering BamHI against a constant concentration of each of the deoxyoligonucleotide substrates and analyzing reaction products by gel retardation. Binding isotherms of the total amount of bound DNA versus protein concentration were constructed which provided semiquantitative estimates of the equilibrium dissociation constants for dissociation of BamHI from the six DNA oligomers. Dissociation constants ranged from 0.5 x 10(-)(9) to 12.0 x 10(-)(9) M with corresponding binding free energies of -12.5 to -10.6 (+/-0. 1) kcal/mol. An inverse relationship is found when binding and stability are compared.     

Thermodynamic analysis of the binding of component enzymes in the assembly of the pyruvate dehydrogenase multienzyme complex of Bacillus stearothermophilus

The peripheral subunit-binding domain (PSBD) of the dihydrolipoyl acetyltransferase (E2, EC 2.3.1.12) binds tightly but mutually exclusively to dihydrolipoyl dehydrogenase (E3, EC 1.8.1.4) and pyruvate decarboxylase (E1, EC 1.2.4.1) in the pyruvate dehydrogenase multienzyme complex of Bacillus stearothermophilus. Isothermal titration calorimetry (ITC) experiments demonstrated that the enthalpies of binding (DeltaH degrees ) of both E3 and E1 with the PSBD varied with salt concentration, temperature, pH, and buffer composition. There is little significant difference in the free energies of binding (DeltaG degrees = -12.6 kcal/mol for E3 and = -12.9 kcal/mol for E1 at pH 7.4 and 25 degrees C). However, the association with E3 was characterized by a small, unfavorable enthalpy change (DeltaH degrees = +2.2 kcal/mol) and a large, positive entropy change (TDeltaS degrees = +14.8 kcal/mol), whereas that with E1 was accompanied by a favorable enthalpy change (DeltaH degrees = -8.4 kcal/mol) and a less positive entropy change (TDeltaS degrees = +4.5 kcal/mol). Values of DeltaC(p) of -316 cal/molK and -470 cal/molK were obtained for the binding of E3 and E1, respectively. The value for E3 was not compatible with the DeltaC(p) calculated from the nonpolar surface area buried in the crystal structure of the E3-PSBD complex. In this instance, a large negative DeltaC(p) is not indicative of a classical hydrophobic interaction. In differential scanning calorimetry experiments, the midpoint melting temperature (T(m)) of E3 increased from 91 degrees C to 97.1 degrees C when it was bound to PSBD, and that of E1 increased from 65.2 degrees C to 70.0 degrees C. These high T(m) values eliminate unfolding as a major source of the anomalous DeltaC(p) effects at the temperatures (10-37 degrees C) used for the ITC experiments.     

Binding of urate and caffeine to hemocyanin of the lobster Homarus vulgaris (E.) as studied by isothermal titration calorimetry

Hemocyanin serves as an oxygen carrier in the hemolymph of the European lobster Homarus vulgaris. The oxygen binding behavior of the pigment is modulated by metabolic effectors such as lactate and urate. Urate and caffeine binding to 12-meric hemocyanin (H. vulgaris) was studied using isothermal titration calorimetry (ITC). Binding isotherms were determined for fully oxygenated hemocyanin between pH 7.55 and 8.15. No pH dependence of the binding parameters could be found for either effector. Since the magnitude of the Bohr effect depends on the urate concentration, the absence of any pH dependence of urate and caffeine binding to oxygenated hemocyanin suggests two conformations of the pigment under deoxygenated conditions. Urate binds to two identical binding sites (n = 2) each with a microscopic binding constant K of 8500 M(-1) and an enthalpy change DeltaH degrees of -32.3 kcal mol(-1). Caffeine binds cooperatively to hemocyanin with two microscopic binding constants: K(1) = 14 100 M(-1) and K(2) = 40 400 M(-1). The corresponding enthalpy changes in binding are as follows: DeltaH degrees (1) = -23.3 kcal mol(-1) and DeltaH degrees (2) = -27.1 kcal mol(-1). The comparison of urate and caffeine binding to the oxygenated pigment indicates the existence of two protein conformations for oxygen-saturated hemocyanin. Since effector binding is not influenced by protons, four different conformations are required to create a convincing explanation for caffeine and urate binding curves. This was predicted earlier on the basis of the analysis of oxygen binding to lobster hemocyanin, employing the nesting model.     

Thermodynamic stability of DNA tandem mismatches

The thermodynamics of nine hairpin DNAs were evaluated using UV-monitored melting curves and differential scanning calorimetry (DSC). Each DNA has the same five-base loop and a stem with 8-10 base pairs. Five of the DNAs have a tandem mismatch in the stem, while four have all base pairs. The tandem mismatches examined (ga/ga, aa/gc, ca/gc, ta/ac, and tc/tc) spanned the range of stability observed for this motif in a previous study of 28 tandem mismatches. UV-monitored melting curves were obtained in 1.0 M Na(+), 0.1 M Na(+), and 0.1 M Na(+) with 5 mM Mg(2+). DSC studies were conducted in 0.1 M Na(+). Transition T(m) values were unchanged over a 50-fold range of strand concentration. Model-independent enthalpy changes (DeltaH degrees ) evaluated by DSC were in good agreement (+/-8%) with enthalpy values determined by van't Hoff analyses of the melting curves in 0.1 M Na(+). The average heat capacity change (DeltaC(p)) associated with the hairpin to single strands transitions was estimated from plots of DeltaH degrees and DeltaS degrees with T(m) and ln T(m), respectively, and from profiles of DSC curves. The average DeltaC(p) values (113 +/- 9 and 42 +/- 27 cal x K(-1) x mol(-1) of bp), were in the range of values reported in previous studies. Consideration of DeltaC(p) produced large changes in DeltaH degrees and DeltaS degrees extrapolated from the transition region to 37 degrees C and smaller but significant changes to free energies. The loop free energy of the five tandem mismatches at 37 degrees C varied over a range of approximately 4 kcal x mol(-1) for each solvent.     

The DNA sequence at echinomycin binding sites determines the structural changes induced by drug binding: NMR studies of echinomycin binding to [d(ACGTACGT)]2 and [d(TCGATCGA)]2

The complexes formed between the cyclic octadepsipeptide antibiotic echinomycin and the two DNA octamers [d(ACGTACGT)]2 and [d(TCGATCGA)]2 have been investigated by using one- and two-dimensional proton NMR spectroscopy techniques. The results obtained for the two complexes are compared to each other, to the crystal structures of related DNA-echinomycin complexes, and to enzymatic and chemical footprinting results. In the saturated complexes, two echinomycin molecules bind to each octamer by bisintercalation of the quinoxaline moieties on either side of each CpG step. Binding of echinomycin to the octamer [d(ACGTACGT)]2 is cooperative so that only the two-drug complex is observed at lower drug-DNA ratios, but binding to [d(TCGATCGA)]2 is not cooperative. At low temperatures, both the internal and terminal A.T base pairs adjacent to the binding site in the [d(ACGTACGT)]2-2 echinomycin complex are Hoogsteen base paired (Gilbert et al., 1989) as observed in related crystal structures. However, as the temperature is raised, the internal A.T Hoogsteen base pairs are destabilized and are observed to be exchanging between the Hoogsteen base-paired and an open (or Watson-Crick base-paired) state. In contrast, in the [d(TCGATCGA)]2-2 echinomycin complex, no A.T Hoogsteen base pairs are observed, the internal A.T base pairs appear to be stabilized by drug binding, and the structure of the complex does not change significantly from 0 to 45 degrees C. Thus, the structure and stability of the DNA in echinomycin-DNA complexes depends on the sequence at and adjacent to the binding site. While we conclude that no single structural change in the DNA can explain all of the footprinting results, unwinding of the DNA helix in the drug-DNA complexes appears to be an important factor while Hoogsteen base pair formation does not.     

Adenine base unstacking dominates the observed enthalpy and heat capacity changes for the Escherichia coli SSB tetramer binding to single-stranded oligoadenylates.

Isothermal titration calorimetry (ITC) was used to test the hypothesis that the relatively small enthalpy change (DeltaHobs) and large negative heat capacity change (DeltaCp,obs) observed for the binding of the Escherichia coli SSB protein to single-stranded (ss) oligodeoxyadenylates result from the temperature-dependent adenine base unstacking equilibrium that is thermodynamically coupled to binding. We have determined DeltaH1,obs for the binding of 1 mole of each of dT(pT)34, dC(pC)34, and dA(pA)34 to the SSB tetramer (20 mM NaCl at pH 8.1). For dT(pT)34 and dC(pC)34, we found large, negative values for DeltaH1,obs of -75 +/- 1 and -85 +/- 2 kcal/mol at 25 degrees C, with DeltaCp,obs values of -540 +/- 20 and -570 +/- 30 cal mol-1 K-1 (7-50 degrees C), respectively. However, for SSB-dA(pA)34 binding, DeltaH1,obs is considerably less negative (-14 +/- 1 kcal/mol at 25 degrees C), even becoming positive at temperatures below 13 degrees C, and DeltaCp,obs is nearly twice as large in magnitude (-1180 +/- 40 cal mol-1 K-1). These very different thermodynamic properties for SSB-dA(pA)34 binding appear to result from the fact that the bases in dA(pA)34 are more stacked at any temperature than are the bases in dC(pC)34 or dT(pT)34 and that the bases become unstacked within the SSB-ssDNA complexes. Therefore, the DeltaCp,obs for SSB-ssDNA binding has multiple contributions, a major one being the coupling to binding of a temperature-dependent conformational change in the ssDNA, although SSB binding to unstacked ssDNA still has an "intrinsic" negative DeltaCp,0. In general, such temperature-dependent changes in the conformational "end states" of interacting macromolecules can contribute significantly to both DeltaCp,obs and DeltaHobs.     

Proton nuclear magnetic resonance investigation of the conformation and dynamics in the synthetic deoxyribonucleic acid decamers d(ATATCGATAT) and d(ATATGCATAT)

A variety of one-dimensional proton NMR methods have been used to investigate the properties of two synthetic DNA decamers, d(ATATCGATAT) and d(ATATGCATAT). These results, in conjunction with the results of two-dimensional NMR experiments, permit complete assignment of the base proton resonances. Low-field resonances were assigned by sequential "melting" of the A . T base pairs and by comparison of the spectra of the two decamers. Below 20 degree C spin-lattice relaxation is dominated by through-space dipolar interactions. A substantial isotope effect on the G imino proton relaxation is observed in 75% D2O, confirming the importance of the exchangeable amino protons in the relaxation process. A somewhat smaller isotope effect is observed on the T imino proton relaxation. At elevated temperatures spin-lattice relaxation of the imino protons is due to proton exchange with solvent. Apparent activation energies for exchange vary from 36 kcal/base pair for base pairs (3,8) to 64 kcal/mol for the most interior base pairs (5,6), indicating that disruption of part, or all, of the double helix contributes significantly to the exchange of the imino protons in these decamers. By contrast, single base pair opening events are the major low-temperature pathways for exchange from A X T and G X C base pairs in the more stable higher molecular weight DNA examined in other studies. The temperature dependence of the chemical shifts and line widths of certain aromatic resonances indicates that the interconversion between the helix and coil states is not in fast exchange below the melting temperature, Tm. Within experimental error, no differential melting of base pairs was found in either molecule, and both exhibited melting points Tm = 50-52 degrees C. Spin-spin and spin-lattice relaxation rates of the nonexchangeable protons (TH6, AH8, and AH2) are consistent with values calculated by using an isotropic rotor model with a rotational correlation time of 6 ns and interproton distances appropriate for B-family DNA. The faster decay of AH8 compared with GH8 is attributed to an interaction between the thymine methyl protons and the AH8 protons in adjacent adenines (5'ApT3'). The base protons (AH8, GH8, and TH6) appear to be located close (1.9-2.3 A) to sugar H2',2" protons.(ABSTRACT TRUNCATED AT 400 WORDS)     

Calorimetric and spectroscopic investigation of drug-DNA interactions. I. The binding of netropsin to poly d(AT)

We report the first calorimetric investigation of netropsin binding to poly d(AT). Temperature-dependent uv absorption, circular dichroism (CD), batch calorimetry, and differential scanning calorimetry (DSC) were used to detect, monitor, and thermodynamically characterize the binding process. The following results have been obtained: 1) Netropsin groove binding is accompanied by a large exothermic enthalpy of 9.2 kcal/mol of drug bound at 25 degrees C. This indicates that a large negative binding enthalpy may be a necessary but not a sufficient criterion for drug intercalation. We suggest that the exothermic binding might be correlated with specific H-bonding interactions. 2) From the difference in DSC transition enthalpies in the presence and absence of netropsin, we calculate a binding enthalpy of -10.7 kcal/mol of netropsin at 88 degrees C. 3) We calculate a positive delta S for netropsin binding to poly d(AT) at 25 degrees C. This positive entropy change may reflect netropsin-induced release of condensed cations and/or bound water. 4) The netropsin-saturated duplex monophasically melts 46 degrees C higher than the free duplex. The unsaturated duplex melts through two thermally-resolved transitions that correspond to netropsin-free and netropsin-bound regions. These two regions interact dynamically with no substantial influence on the thermal stabilities of the separate domains. 5) Netropsin binding decreases the cooperativity of the duplex to single strand transition.