Thermodynamics of the various forms of the dodecamer d(ATTACCGGTAAT) and of its constituent hexamers from proton nmr chemical shifts and UV melting curves: three-state and four-state thermodynamic models

Chemical shifts of base and H1' protons of the single-stranded hexamers d(ATTACC) and d(GGTAAT), of the 1:1 mixtures of these complementary hexamers, and of the self-complementary dodecamer d(ATTACCGGTAAT) were measured at various temperatures in aqueous solution. Four different sample concentrations were used in the case of the dodecamer and of the mixture of the complementary hexamers; the individual hexamers were measured at two different DNA concentrations. Absorbance temperature profiles at five different NaCl concentrations were measured for the dodecamer in order to quantify the effect of the ionic strength on the duplex formation. Under suitable conditions of nucleotide concentration, temperature, and ionic strength, the dodecamer adopts either a B-DNA duplex or a hairpin-loop structure. Chemical shift vs temperature profiles, constructed for all samples, were used to obtain thermodynamic parameters either for the various stacking interactions in the single strands or for the duplex or the hairpin-loop formation. In the analysis of the duplex formation of the hexamers, a two-state approach appeared too simple, because systematic deviations were revealed. Therefore, a new three-state model (DUPSTAK) was developed. In order to investigate the magnitude of error arising from the use of the two-state approach in cases where the DUPSTAK model appears more appropriate, a series of test calculations was made. The magnitude of error in the enthalpy and in the entropy of duplex melting is found to depend linearly upon the actual melting temperature and not upon the individual delta Hd degrees and delta Sd degrees values. Thermodynamic analysis of the chemical shift vs temperature profiles in D2O solution (no added salt) yields an average Tmd value of 341 K (1M DNA) and delta Hd degrees of - 121 kJ.mol-1 for the dimer/random-coil transition of the hexamer duplex d(ATTACC).d(GGTAAT). For the duplex in equilibrium random-coil transition of the 12-mer d(ATTACCGGTAAT) an average Tmd value of 336 K (1M DNA) and delta Hd degrees of -372 kJ.mol-1 are found. The hairpin/random-coil transition of d(ATTACCGGTAAT) is characterized by a rather large delta Hh degrees value, -130 kJ.mol-1, and an average Tmh value of 304 K.     

An NMR study of polymorphous behaviour of the mismatched DNA octamer d(m5C-G-m5C-G-A-G-m5C-G) in solution. The B-duplex and hairpin forms

By means of one- and two-dimensional NMR spectroscopy the solution structures of the partly self-complementary octamer d(m5C-G-m5C-G-A-G-m5C-G) were investigated. It is shown that this DNA fragment, under conditions of high DNA concentration (8 mM DNA) and/or high ionic strength prefers to adopt a duplex structure. At low DNA concentration (0.4 mM DNA), the duplex exists in a 1:1 slow equilibrium with a monomeric hairpin form. Addition of salt destabilizes the hairpin structure in favour of the dimer. At high temperatures the hairpin form, as well as the dimer structure, exist in a fast equilibrium with the random-coil form. For the hairpin/random-coil equilibrium a Tm of 329 K and a delta H degree of -121 kJ.mol-1 were deduced. These thermodynamic parameters are independent of the DNA concentration, as is expected for a monomeric structure. For the dimer to coil transition a Tm of 359 K (1 M DNA) and a delta H degree of -285 kJ.mol duplex-1 were derived. The thermodynamic data of the hairpin-coil transition mutually agree with those recently reported for the hairpin to random coil equilibrium of the DNA octamer d(m5C-G-m5C-G-T-G-m5C-G) [Orbons, L. P. M., van der Marel, G. A., van Boom, J. H. & Altona, C. (1987) J. Biomol. Struct. Dyns. 4, 939-963]. It is demonstrated that the dimer structure exhibits B-DNA characteristics, as is witnessed by the NOESY experiments and the analysis of the proton-proton coupling data. It is shown that the base-pair formation of the G x A mismatches is anti-anti. A comparison of 1H and 31P chemical-shift data of the title compound with those of a well-characterized B-DNA structure reveals large differences in the dm5C(3)-dG(4)-dA(5) part of the mismatched dimer structure. These differences apparently indicate some major local structural changes due to the incorporation of the G x A mismatches. Under the most extreme conditions used (i.e. up to 3 M NaCl or 75% CH3OH in the presence of 10 mM MgCl2) no Z-DNA structure was observed. It is shown that the structural features of the hairpin form of the title compound mimic those of the hairpin structure of d(m5C-G-m5C-G-T-G-m5C-G). An energy-minimized model of the hairpin form is given.     

Energetics of the hairpin to mismatched duplex transition of d(GCCGCAGC) on NaCl solution

We report Potential of Mean Force studies to describe the relative thermodynamic stabilities of d(GCCGCAGC) in a mismatched duplex and a hairpin monomer conformation in NaCl solution. The PMF calculations are combined with previous molecular mechanics and normal mode analysis in order to estimate the role of different components of the free energy in determining the relative stability of the duplex and hairpin structures. The high entropy associated with the loop region and the lack of minor groove phosphate-phosphate interactions in the hairpin compete against the gain in enthalpic contribution to the free energy due to base pairing in the mismatched duplex. The combined free energy calculations show that the hairpin is the most stable conformation at low salt and that a hairpin to duplex transition takes place at approximately 0.47 M NaCl. In addition, we studied the hairpin to partially stacked single helical conformation equilibrium at low salt. We found a small variation in transition temperature in salt concentration, delta Tm/delta log10(cs) approximately 2-3 degrees K/decade, in contrast to the duplex to hairpin or duplex to partially stacked single helix transition where the transition temperature exhibited marked dependence on salt concentration. This is in qualitative agreement with experimental data. Based on the Potential of Mean Force free energy calculation, the order of relative stability of the three-conformations studied varies with salt concentration. We observed the following orders of stability: stacked single helix greater than hairpin greater than duplex for cs less than 0.77 M NaCl; single helix greater than duplex greater than hairpin for 0.77 less than Cs less than 2.1 M; and duplex greater than hairpin greater than single strand for cs greater than 2.1 M. From the calculated PMF free energy curves in the NaCl concentration range, 0.012 less than cs less than 5.0 M, we can assign upper and lower bounds for the non-ionic differences in free energy between the duplex, hairpin, and stacked single helical states (at standard conditions: cs = 1.0 M, T = 25 degrees C, and 1 M oligomer concentration). We found that for delta G duplex single helix = G duplex - 2 x G single helix less than -7.38 Kcal/mol, the single helix is the least stable state. For the duplex-to-hairpin free energy difference in the range, -1.87 less than delta G duplex-hairpin less than 0.03 Kcal/mol, there will always be a salt-induced hairpin-to-duplex transition for 0.01 less than cs less than 1.6 M NaCl. If delta G duplex-hairpin less than -1.87, the duplex is always more stable than the hairpin; and for delta G duplex-hairpin greater than Kcal/mol, the hairpin state is always more stable than the duplex, for all salt concentrations.     

Influence of N6-methylation of residue A(5) on the conformational behaviour of d(C-C-G-A-A-T-T-C-G-G) in solution studied by 1H-NMR spectroscopy. 2. The hairpin form

The solution conformations of the oligonucleotides d(C-C-G-A-A-T-T-C-G-G) and d(C-C-G-A-m6A-T-T-C-G-G) as a function of temperature and sample concentration were investigated by means of 1H-NMR spectroscopy. The NMR spectra revealed that, at certain combinations of temperature and low sample and salt concentration, both compounds exist as a B-DNA-type duplex slowly (on the 1H-NMR time scale) interconverting with a monomeric species. From chemical shift data and imino-proton spectra, it is concluded that the monomeric species consists of a mixture of a hairpin form in rapid equilibrium with the random-coil form. The double-helical stem of the hairpin is formed by the six terminal cytidine and guanine residues, whereas the four core residues, -A-(m6)A-T-T-, partake in the loop. Thermodynamic analysis of the chemical shift of the resonances of the monomeric species vs temperature profiles of the two decamers and mutual comparison of these profiles indicate the following: the influence of N6-methylation of residue A(5) upon the local structure of the hairpin must be small; methylation decreases the stability of the duplex relative to the monomeric species: the temperature at which the fraction duplex equals 0.5 was found to be 312 K for the parent compound and 305 K for the methylated decamer at 2 mM sample concentration; methylation does not significantly alter the stability of the hairpin form relative to the random coil form: the Tm of the hairp----n equilibrium random-coil equilibrium is 308 K for the parent compound and 306 K for the methylated decamer. A higher fraction hairpin-like structure for the N6-methylated compound is observed under identical conditions of temperature and sample concentration: at 300 K, 2 mM sample concentration, the fraction hairpin form is 0.12 for d(C-C-G-A-A-T-T-C-G-G) and 0.20 for d(C-C-G-A-m6A-T-T-C-G-G). This finding appears to be a consequence of the reduced stability of the methylated dimeric species relative to the monomeric species, and to depend upon the sodium-ion concentration: it becomes more pronounced under low-salt conditions.     

Proton NMR study and conformational analysis of d(CGT), d(TCG) and d(CGTCG) in aqueous solution. The effect of a dangling thymidine and of a thymidine mismatch on DNA mini-duplexes

Proton NMR studies of d(CGT), d(TCG) and d(CGTCG) were carried out at 300 and 500 MHz. The temperature and concentration dependence of the chemical shifts of various resonances indicates duplex formation only in the cases of d(TCG) and d(CGTCG). It is concluded that d(TCG) forms a mini-duplex stabilized by a 5'-dangling thymine base. Thermodynamic parameters of the duplex-to-coil equilibrium of the d(TCG) duplex are: delta H0 = -22.3 kcal/mol and delta S0 = -70 cal/mol. K, which correspond to approximately 40% duplex formation at 0 degrees C in a 2 mM nucleotide solution. Comparison of these data with thermodynamic parameters given earlier [Borer, P.N., Dengler, B., Tinoco, I. and Uhlenbeck, O.C. (1974) J. Mol. Biol. 86, 843-853] leads to the conclusion that the dangling base stabilization observed here is approximately equivalent to the stabilization caused by one or two additional A . T base pairs. The chemical shift behaviour of various resonances in d(CGTCG) indicates duplex formation without looping out of the thymine bases. The T X T mismatch does not seem to disturb the helical structure to a large extent. Analysis of the vicinal proton-proton coupling constants of the three compounds yielded geometrical data for the sugar rings. The data are interpreted in terms of N and S pseudorotational ranges. It is shown that a distinct conformation-transmission effect is exerted by the guanosine residues in a 5'----3' direction.     

1H NMR assignment and melting temperature study of cis-syn and trans-syn thymine dimer containing duplexes of d(CGTATTATGC).d(GCATAATACG)

The preparation and spectroscopic characterization of duplex decamers containing site-specific cis-syn and trans-syn thymine dimers are described. Three duplex decamers, d(CGTATTATGC).d(GCATAATACG), d(CGTAT[c,s]TATGC).d(GCATAATACG), and d(CGTAT[t,s]TATGC).d(GCATAATACG), were prepared by solid-phase phosphoramidite synthesis utilizing cis-syn and trans-syn cyclobutane thymine dimer building blocks (Taylor et al., 1987; Taylor & Brockie, 1988). NMR spectra (500 MHz 2D 1H and 202 MHz 1D 31P) were obtained in "100%" D2O at 10 degrees C, and 1D exchangeable 1H spectra were obtained in 10% D2O at 10 degrees C. 1H NMR assignments for H5, H6, H8, CH3, H1', H2', and H2" were made on the basis of standard sequential NOE assignment strategies and verified in part by DQF COSY data. Comparison of the chemical shift data suggests that the helix structure is perturbed more to the 3'-side of the cis-syn dimer and more to the 5'-side of the trans-syn dimer. Thermodynamic parameters for the helix in equilibrium coil equilibrium were obtained by two-state, all or none, analysis of the melting behavior of the duplexes. Analysis of the temperature dependence of the T5CH3 1H NMR signal gave delta H = 44 +/- 4 kcal and delta S = 132 +/- 13 eu for the trans-syn duplex. Analysis of the concentration and temperature dependence of UV spectra gave delta H = 64 +/- 6 kcal and delta S = 178 +/- 18 eu for the parent duplex and delta H = 66 +/- 7 kcal and delta S = 189 +/- 19 eu for cis-syn duplex. It was concluded that photodimerization of the dTpdT unit to give the cis-syn product causes little perturbation of the DNA whereas dimerization to give the trans-syn product causes much greater perturbation, possibly in the form of a kink or dislocation at the 5'-side of the dimer.     

Duplex-tetraplex equilibrium between a hairpin and two interacting hairpins of d(A-G)10 at neutral pH.

d(A-G)10 forms two helical structures at neutrality, at low ionic strength a single-hairpin duplex, and at higher ionic strength a double-hairpin tetraplex. An ionic strength-dependent equilibrium between these forms is indicated by native PAGE, which also reveals additional single-stranded species below 0.3 M Na+, probably corresponding to partially denatured states. The equilibrium also depends upon oligomer concentration: at very low concentrations, d(A-G)10 migrates faster than the random coil d(C-T)10, probably because it is a more compact single hairpin; at high concentrations, it co-migrates with the linear duplex d(A-G)10 x d(C-T)10, probably because it is a two-hairpin tetraplex. Molecular weights measured by equilibrium sedimentation in 0.1 M Na+, pH 7, reveal a mixture of monomer and dimer species at 1 degree C, but only a monomer at 40 degrees C; in 0.6 M Na+, pH 7, only a dimer species is observed at 4 degrees C. That the single- and double-stranded species are hairpin helices, is indicated by preferential S1 nuclease cleavage at the center of the oligomer(s), i.e., the loop of the hairpin(s). The UV melting transition below 0.3 M Na+ or K+, exhibits a dTm/dlog[Na+/K+] of 33 or 36 degrees C, respectively, consistent with conversion of a two-hairpin tetraplex to a single-hairpin duplex with extrahelical residues. When [Na+/K+] > or = 0.3 M, dTm/dlog [Na+/K+] is 19 or 17 degrees C, respectively, consistent with conversion of a two-hairpin tetraplex directly to single strands. A two-hairpin structure stabilized by G-tetrads is indicated by differential scanning calorimetry in 0.15 M Na+/5 mM Mg2+, with deltaH of formation per mole of the two-hairpin tetraplex of -116.9 kcal or -29.2 kcal/mol of G-tetrad.     

A comparison of the hairpin stability of the palindromic d(CGCG(A/T)4CGCG) oligonucleotides.

The palindromic deoxyribonucleotides 5'-CGCGA-TATCGCG-3' and 5'-CGCGTTAACGCG-3' have been characterized by 1H NMR spectroscopy. The NMR data identified both B-DNA duplex conformations and hairpin conformations, the latter with loop regions consisting of the four central nucleotides. The resonances of the various conformations were assigned by use of two-dimensional NMR methods. The relative stability of the various conformations was investigated as a function of temperature, ionic strength and nucleotide concentration. The duplexes were found to be stabilized at high ionic strength and at low temperature, while the hairpins were stabilized at low ionic strength and at medium temperature. The thermodynamics of the duplex-hairpin and the hairpin-random coil transitions were examined, and compared to the other two oligonucleotide in the palindromic d(CGCG(A/T)4CGCG) oligonucleotide family. The relative stabilities of the duplex conformations with respect to the random coil conformations are similar for the d(CGCGAATTCGCG), d(CGCGATATCGCG) and d(CGCGTATACGCG) oligonucleotides. The duplex conformation of d(CGCGTTAACGCG) is less stable. The hairpin of d(CGCGTTAACGCG) seems also to be less stable relative to the random coil conformation than in the case of the other oligonucleotides at an equal oligonucleotide concentration. A cruciform intermediate between the duplex and hairpin conformations is suggested to explain some discrepancies observed in this work in case of the d(CGCGTTAACGCG) oligonucleotide. This is similar to what has been reported for the d(CGCGTATACGCG) oligonucleotide.     

Thermodynamic behaviour of the heptadecadeoxynucleotide d(CGCGCGTTTTTCGCGCG) forming B and Z hairpins in aqueous solution.

UV and CD data of the partially self-complementary heptadecadeoxynucleotide d(CGCGCGTTTTTCGCGCG), obtained as a function of temperature, salt and strand concentration, show that: at low NaCl and strand concentration the oligomer exhibits, on increasing the temperature, a biphasic thermal profile which is indicative of two structural transitions, from dimeric duplex to hairpin and from hairpin to coil; the loop stabilizes enthalpically both B and Z hairpin structures with respect to the corresponding unconstrained hexamer d(CGCGCG) by a few Kcal/mol; the oligomer undergoes a B-Z transition which appears to be complete, at 0 degree C, when induced by NaClO4; by contrast the B-Z transition induced by NaCl does not reach completeness even at salt saturation. The independence of the denaturation temperature, at high salt conditions, on the oligomer concentration indicates that the Z structure is present also in the hairpin.     

Kinetic and thermodynamic characterization of DNA duplex–hairpin interconversion for two DNA decamers: d(CAACGGGTTG) and d(CAACCCGTTG)

The duplex–hairpin interconversion of two DNA decamers, d(CAACGGGTTG) and d(CAACCCGTTG), has been characterized thermodynamically and kinetically by using uv-melting and nmr relaxation methods. Separately, each decamer shows slow exchange between hairpin and duplex conformations. The hairpin conformations have melting points of 47 and 50°C, respectively, and exhibit similar thermodynamic stabilities. The enthalpies of duplex formation, measured by nmr, were found to be very similar (ΔH_DH = 26 ± 3 kcal/mole) for both decanters at low salt concentrations (< 50 mM NaCl). However, as the salt concentration was increased the behavior of ΔH_DH, and kinetics is significantly different for each decamer. The d(CAACGGGTTG) decamer forms a duplex containing two central G·G mismatches at high salt and DNA concentration. Based upon the measurement of high interconversion activation energies and a decrease in hairpin formation rate with increasing salt, the interconversion between hairpin and duplex was concluded to proceed by complete strand dissociation. In contrast, the d(CAAC-CCGTTG) decamer was determined to form a duplex with two centrally located C·C mismatches at pH values less than 6.2, consistent with the formation of a hemiprotonated C⁺·C mismatch. At pH values greater than 6.4, the hairpin–duplex equilibrium is almost completely shifted toward the hairpin conformation at DNA concentrations of 0.5–7.0 mM and salt concentrations of 10–100 mM. The interconversion of duplex and hairpin conformations was ascertained by means of both kinetic and thermodynamic measurements to proceed by a slightly different mechanism than its complementary decamer. Although the interconversion proceeds by complete strand separation as suggested by high duplex-hairpin interconversion activation enthalpies, the increasing hairpin formation rate with increasing ionic strength as well as the ΔH_DH, dependence on sail indicate that an intermediate internally bulged duplex (no C⁺·C formation) is stabilized by increasing ionic strength. These data support an interconversion mechanism where an intermediate internally bulged duplex may be the rate limiting step before strand separation. © 1995 John Wiley & Sons, Inc.     

The duplex-hairpin conformational transition of d(CGCGCGATCGCGCG) and d(CGCGCGTACGCGCG): a thermodynamic and kinetic study

We have studied the duplex-hairpin conformational transition in two perfectly palindromic sequences, d(CGCGCGATCGCGCG)(I) and d(CGCGCGTACGCGCG)(II), by means of UV-melting, electrophoretic and T-jump experiments. Both tetradecamers exhibit biphasic thermal profiles. The lower temperature transition is concentration dependent whereas the higher temperature transition is not. The former transition has been characterized by gel electrophoresis and shows two distinct bands, whose intensity depends on temperature. This behavior is due to the occurrence of a slow premelting interconversion between the duplex and hairpin forms in both tetradecamers. The kinetics of hairpin formation from the duplex is studied by T-jump experiments. Relaxation spectra are well reproduced by a single relaxation time with rate constants characterized by a high temperature coefficient. In 10 mM NaCl, the duplex-hairpin conversion of I is characterized by an apparent activation energy of 96 +/- 6 kcal/mol, a value rather close to the expected denaturation enthalpy. In 1 mM NaCl a value slightly lower has been obtained. The rate of duplex-hairpin interconversion has been found to decrease as the salt concentration is raised. These data suggest that the transformation from the duplex to the hairpin form should imply a transition state with a simultaneous breaking of most base pairs, if not total strand separation.     

The Duplex-Harpin Conformational Transition of d(CGCGCGATCGCGCG) and d(CGCGCGTACGCGCG): A Thermodynamic and Kinetic Study

Abstract

We have studied the duplex-hairpin conformational transition in two perfectly palindromic sequences, d(CGCGCGATCGCGCG)(I) and d(CGCGCGTACGCGCG)(II), by means of UV-melting, electrophoretic and T-jump experiments. Both tetradecamers exhibit biphasic thermal profiles. The lower temperature transition is concentration dependent whereas the higher temperature transition is not. The former transition has been characterized by gel electrophoresis and shows two distinct bands, whose intensity depends on temperature. This behavior is due to the occurrence of a slow premelting interconversion between the duplex and hairpin forms in both tetradecamers. The kinetics of hairpin formation from the duplex is studied by T-jump experiments. Relaxation spectra are well reproduced by a single relaxation time with rate constants characterized by a high temperature coefficient. In 10 mM NaCl, the duplex-hairpin conversion of I is characterized by an apparent activation energy of 96 ± 6 kcal/mol, a value rather close to the expected denaturation enthalpy. In 1 mM NaCl a value slightly lower has been obtained. The rate of duplex-hairpin interconversion has been found to decrease as the salt concentration is raised. These data suggest that the transformation from the duplex to the hairpin form should imply a transition state with a simultaneous breaking of most base pairs, if not total strand separation.     

Complementary addressed modification of a hairpin-shaped model oligodeoxyribonucleotide

A hairpin-shaped oligodeoxyribonucleotide d(pTTGGCACGAGCAGCCAA) (I) was alkylated with the reagent d(TTGGG) greater than UCHRCl (RCl = -C6H5-N(CH3)-CH2-CH2Cl) complementary to the hairpin's stem. Thermodynamic parameters for the hairpin structure estimated from melting curves were: delta Hh = -125 +/- 17 kJ/mol, delta Sh = -380 +/- 84 J/mol.K; and for the reagent - target complex delta Hpx = -155 +/- 8 kJ/mol, delta Spx = -427 +/- 21 J/mol.K. Effective constants of association Kx of the oligonucleotide with the reagent were determined at 30 and 50 degrees from the concentration dependence of the reaction yield and were 1988 +/- 83 and 1239 +/- 58 M-1, respectively. Experimental values of Kx agreed with the values of Kx = Kpx/(1 + Kh), calculated with the use of the thermodynamic parameters.     

Right- and left-handed (Z) helical conformations of the hairpin d(C-G)5T4(C-G)5 monomer and dimer

The partial self-complementary 24-mer oligodeoxynucleotide d(C-G)5T4(C-G)5 forms a hairpin which can be enzymatically dimerized to a dumbbell structure. The blunt-ended nature of the hairpin is indicated by its ability to inhibit the T4 DNA ligase catalyzed joining of phi X174 HaeIII fragments. The hairpin monomer and dimer (dumbbell) undergo a reversible B to Z transition as shown by ultraviolet, circular dichroism, and 31P NMR spectroscopy. The Z form of the hairpin monomer and dimer is supported by monovalent ions (Na+), divalent ions (Mg2+ but not Mn2+), and dehydrating (ethanol) conditions. The conformational transition of d(C-G)5T4(C-G)5 monomer requires higher ionic or dehydrating conditions than those necessary for the corresponding linear oligomer d(C-G)5. The contribution of the loop (-T4-) of the hairpin to the apparent free energy change for the B to Z conformational transition at the midpoint was calculated to be 3.8 kJ mol-1.     

Spectroscopic analysis of DNA base-pair opening by Escherichia coli RNA polymerase. Temperature and ionic strength effects

The interaction of Escherichia coli RNA polymerase with poly[d(A-T)] and poly[d-(I-C)] was studied by difference absorption spectroscopy at temperatures, from 5 to 45 degrees C in the absence and presence of Mg2+. The effect of KCl concentration, at a fixed temperature, was studied from 12.5 to 400 mM. Difference absorption experiments permitted calculation of the extent of DNA opening induced by RNA polymerase and estimation of the equilibrium constant associated with the isomerization from a closed to an open RNA polymerase-DNA complex. delta H0 and delta S0 for the closed-to-open transition with poly[d(A-T)] or poly[d(I-C)] complexed with RNA polymerase are significantly lower than the values associated with the helix-to-coil transition for the free polynucleotides. For the RNA polymerase complexes with poly[d(A-T)] and poly[d(I-C)] in 50 mM KCl, delta H0 approximately 15-16 kcal/mol (63-67 kJ/mol) and delta S0 approximately 50-57 cal/K per mol (209-239 J/K per mol). The presence of Mg2+ does not change these parameters appreciably for the RNA polymerase-poly[d(A-T)] complex, but for the RNA polymerase-poly[d(I-C)] complex in the presence of Mg2+, the delta H0 and delta S0 values are larger and temperature-dependent, with delta H0 approximately 22 kcal/mol (92 kJ/mol) and delta S0 approximately 72 cal/K per mol (approx. 300 J/K per mol) at 25 degrees C, and delta Cp0 approximately 2 kcal/K per mol (approx. 8.3 kJ/K per mol). The circular dichroism (CD) changes observed for helix opening induced by RNA polymerase are qualitatively consistent with the thermally induced changes observed for the free polynucleotides, supporting the difference absorption method. The salt-dependent studies indicate that two monovalent cations are released upon helix opening. For poly[d(A-T)], the temperature-dependence of enzyme activity correlates well with the helix opening, implying this step to be the rate-determining step. In the case of poly[d(I-C)], the same is not true, and so the rate-determining step must be a process subsequent to helix opening.     

Human Ku antigen tightly binds and stabilizes a tetrahelical form of the Fragile X syndrome d(CGG)n expanded sequence

Hairpin and tetrahelical structures of a d(CGG)(n) sequence in the FMR1 gene have been implicated in its expansion in fragile X syndrome. The identification of tetraplex d(CGG)(n) destabilizing proteins (Fry, M., and Loeb, L. A.(1999) J. Biol. Chem. 274, 12797-12803; Weisman-Shomer, P., Naot, Y., and Fry, M. (2000) J. Biol. Chem. 275, 2231-2238) suggested that proteins might modulate d(CGG)(n) folding and aggregation. We assayed human TK-6 lymphoblastoid cell extracts for d(CGG)(8) oligomer binding proteins. The principal binding protein was identified as Ku antigen by its partial amino acid sequence and antigenicity. The purified 88/75-kDa heterodimeric Ku bound with similar affinities (K(d) approximately 1. 8-10.2 x 10(-9) mol/liter) to double-stranded d(CGG)(8).d(CCG)(8), hairpin d(CGG)(8), single-stranded d(CII)(8), or tetraplex structures of telomeric or IgG switch region sequences. However, Ku associated more tightly with bimolecular G'2 tetraplex d(CGG)(8) (K(d) approximately 0.35 x 10(-9) mol/liter). Binding to Ku protected G'2 d(CGG)(8) against nuclease digestion and impeded its unwinding by the tetraplex destabilizing protein qTBP42. Stabilization of d(CGG)(n) tetraplex domains in FMR1 by Ku or other proteins might promote d(CGG) expansion and FMR1 silencing.     

Specific DNA binding by the homeodomain Nkx2.5(C56S): detection of impaired DNA or unfolded protein by isothermal titration calorimetry

Titrations of specific 18-bp duplex DNA with the cardiac-specific homeodomain Nkx2.5(C56S) have utilized an ultrasensitive isothermal titration calorimeter (ITC). As the free DNA nears depletion, we observe large apparent decreases in the binding enthalpy when the DNA is impaired or when the temperature is sufficiently high to produce some unfolding of the free protein. Either effect can be attributed to refolding of the biopolymer that occurs as a result of stabilization due to the large favorable change in free energy on the homeodomain binding to DNA (-49.4 kJ/mol at 298 K). In either case, thermodynamic parameters obtained in such ITC experiments are unreliable. By using a lower temperature (85 vs. 95 degrees C) during the annealing of complementary DNA strands, damage of the 18-bp duplex DNA (T(m) = 72 degrees C) is avoided, and titrations with the homeodomain are normal at temperatures from 10 to 40 degrees C when >95% of the protein is folded. Under the latter conditions, the heat capacity plot is linear with a DeltaC(p) value of -0.80 +/- 0.03 kJ K(-1) mol(-1), which is more negative than that calculated from the burial of solvent accessible surface areas (-0.64 +/- 0.05 kJ K(-1) mol(-1)), consistent with water structures being at the protein-DNA interfaces.     

Hairpin structures in DNA containing arabinofuranosylcytosine. A combination of nuclear magnetic resonance and molecular dynamics

Nuclear magnetic resonance (NMR) and model-building studies were carried out on the hairpin form of the octamer d(CGaCTAGCG) (aC = arabinofuranosylcytosine), referred to as the TA compound. The nonexchangeable protons of the TA compound were assigned by means of nuclear Overhauser effect spectroscopy (NOESY) and correlated spectroscopy (COSY). From a detailed analysis of the coupling data and of the NOESY spectra the following conclusions are reached: (i) The hairpin consists of a stem of three Watson-Crick type base pairs, and the two remaining residues, T(4) and dA(5), participate in a loop. (ii) All sugar rings show conformational flexibility although a strong preference for the S-type (C2'-endo) conformer is observed. (iii) The thymine does not stack upon the 3' side of the stem as expected, but swings into the minor groove. (This folding principle of the loop involves an unusual alpha t conformer in residue T(4).) (iv) At the 5'-3' loop-stem junction a stacking discontinuity occurs as a consequence of a sharp turn in that part of the backbone, caused by the unusual beta + and gamma t torsion angles in residue dG(6). (v) The A base slides over the 5' side of the stem to stack upon the aC(3) residue at the 3' side of the stem in an antiparallel fashion. On the basis of J couplings and a set of approximate proton-proton distances from NOE cross peaks, a model for the hairpin was constructed. This model was then refined by using an iterative relaxation matrix approach (IRMA) in combination with restrained molecular dynamics calculations. The resulting final model satisfactorily explains all the distance constraints.     

Conformational screening of oligonucleotides by variable-temperature high performance liquid chromatography: dissecting the duplex-hairpin-coil equilibria of d(CGCGAATTCGCG)

This study probes the potential of variable-temperature high performance liquid chromatography (VT-HPLC) as a tool for dissecting and modulating nucleic acid structural transitions, using as a model the duplex-hairpin-coil transitions of d(CGCGAATTCGCG). It is demonstrated that VT-HPLC, combined with diode-array detection of the uv signal, enables, for the first time, a physical separation of spectroscopically distinct species that can be assigned to the duplex, hairpin, and coil forms of d(CGCGAATTCGCG). Although the species are spectroscopically distinguishable, they are not readily isolated. Hence, if fractions from the peaks for hairpin or duplex forms are collected and subsequently reinjected onto the cartridge, reequilibration occurs, and both hairpin and duplex peaks are observed. Area integration of the peaks corresponding to duplex and hairpin species provides a means to monitor the duplex to hairpin transition at effective concentrations in the nanomolar range, well below that accessible by conventional spectrophotometers. Concentration-dependent equilibrium constants, melting temperatures, and standard state enthalpies extracted from our measurements compare very well with previous literature results, and with our own results that take into account the effect of our solvent conditions [100 mM TEAA (triethylammonium acetate) and variable acetonitrile] on the melting behavior. By combining precise temperature control with separation based on size, physical behavior, and interaction free energies, VT-HPLC provides a powerful tool for both the modulation and the separation of nucleic acid conformations.     

Spectroscopic and calorimetric investigation on the DNA triplex formed by d(CTCTTCTTTCTTTTCTTTCTTCTC) and d(GAGAAGAAAGA) at acidic pH.

The equimolar mixture of d(CTCTTCTTTCTTTTCTTTCTTCTC) (dY24) and d(GAGAAGAAAGA) (dR11) [designated (dY24).(dR11)], forms at pH = 5 a DNA triplex, which mimicks the H-DNA structure. The DNA triplex was identified by the following criteria: (i) dY24 and dR11 co-migrate in a poly-acrylamide gel, with a mobility and a retardation coefficient comparable to those observed for an 11-triad DNA triplex, previously characterized in our laboratories (1); (ii) the intercalator ethidium bromide shows a poor affinity for (dR11).(dY24) at pH = 5, and a high affinity at pH = 8; (iii) the (dR11).(dY24) mixture is not a substrate for DNase I at pH = 5; (iv) the CD spectrum of (dR11).(dY24), at pH = 5, is consistent with those previously reported for triple-stranded DNA. The (dR11).(dY24) mixture exhibits a thermally induced co-operative transition, which appears to be monophasic, reversible and concentration dependent. This transition is attributed to the disruption of the DNA triplex into single strands. The enthalpy change of the triplex-coil transition was measured by DSC (delta Hcal = 129 +/- 6 kcal/mol) and, assuming a two-state model, by analysis of UV-denaturation curves (average of two methods delta HUV = 137 +/- 13 kcal/mol). Subtracting from delta Hcal of triplex formation the contributions due to the Watson-Crick helix and to the protonation of the C-residues, we found that each pyrimidine binding into the major groove of the duplex, through a Hoogsteen base pair, is accompanied by an average delta H = -5.8 +/- 0.6 kcal/mol. The effect on the stability of the (dR11).(dY24) triplex due to the substitution of a T:A:T triad with a T:T:T one was also investigated.