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.     

Deoxydodecanucleotide heteroduplex d(TTTTATAATAAA). d(TTTATTATAAAA) containing the promoter Pribnow sequence TATAAT. I. Double-helix stability by UV spectrophotometry and calorimetry

Thermally induced structural transition in the d(TTTTATAATAAA) d(TTTATTATAAAA) heteroduplex is characterized by UV-spectroscopy and differential scanning calorimetry. At low salt (less than 0.1 M) the occurrence of a cooperative transition in the lower temperature range, followed by a broad transition connected with small increase in absorbance is observed. At high salt (greater than or equal to 0.2 M) a single, monophasic transition appears. Linear dependence of the latter on log of salt concentration (dTm:dlogM = 14.2 degrees C) and of 1/Tm on log of oligomer concentration [derived therefrom delta H (v.H.) = 77.1 kcal/mole (duplex)] allows relating it to the melting of the heteroduplex helix. The non-cooperative transition, independent of oligomer concentration and similar to that of the single chain, was attributed to melting of short hairpin helices upon heteroduplex dissociation. Calorimetric enthalpy: 75.6 kcal/mole (duplex) proved significantly lower than predicted from known calorimetric data for poly[d(AT)] and poly d(A) X poly d(T).     

Structural equilibria in RNA as revealed by 19F NMR

We have incorporated 5-fluorouridine into several sites within a 19-mer RNA modelled on the translational operator of the MS2 bacteriophage. The 19F NMR spectra demonstrate the different chemical shifts of helical and loop fluorouridines of the hairpin secondary structure. Addition of salt gives rise to a species in which the loop fluorouridine gains the chemical shift of its helical counterparts, due to the formation of the alternative bi-molecular duplex form. This is supported by UV thermal melting behaviour which becomes highly dependent on the RNA concentration. Distinct 19F NMR signals for duplex and hairpin forms allow the duplex-hairpin equilibrium constant to be determined under a range of conditions, enabling thermodynamic characterisation and its salt dependence to be determined. Mg2+ also promotes duplex formation, but more strongly than Na+, such that at 25 degrees C, 10 mM MgCl2 has a comparable duplex-promoting effect to 300 mM NaCl. A similar effect is observed with Sr2+, but not Ca2+ or Ba2+. Additional hairpin species are observed in the presence of Na+ as well as Mg2+, Ca2+, Sr2+ and Ba2+ ions. The overall, ensemble average, hairpin conformation is therefore salt-dependent. Electrostatic considerations are thus involved in the balance between different hairpin conformers as well as the duplex-hairpin equilibrium. The data presented here demonstrate that 19F NMR is a powerful tool for the study of conformational heterogeneity in RNA, which is particularly important for probing the effects of metal ions on RNA structure. The thermodynamic characterisation of duplex-hairpin equilibria will also be valuable in the development of theoretical models of nucleic acid structure.     

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.     

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.     

Free energy contributions of G.U and other terminal mismatches to helix stability

Thermodynamic parameters of helix formation were measured spectroscopically for seven hexaribonucleotides containing a GC tetramer core and G.U or other terminal mismatches. The free energies of helix formation are compared with those for the tetramer core alone and with those for the hexamer with six Watson-Crick base pairs. In 1 M NaCl, at 37 degrees C, the free energy of a terminal G.U mismatch is about equal to that of the corresponding A.U pair. Although other terminal mismatches studied add between -1.0 and -1.6 kcal/mol to delta G0 37 for helix formation, all are less stable than the corresponding Watson-Crick pairs. Comparisons of the stability increments for terminal G.U mismatches and G.C pairs suggest when stacking is weak the additional hydrogen bond in the G.C pair adds roughly -1 kcal/mol to the favorable free energy of duplex formation.     

Z helix-coil transition of d(C-Br8G-C-G-C-Br8G) studied by CD, 1H-NMR and IR spectroscopies

The conformation of d(C-Br8G-C-G-C-Br8G) in aqueous solution was studied by CD and 1H-NMR spectroscopy and in condensed phase by IR spectroscopy. Whether in 0.1 M or 3 M NaCl solution or in film the only double helical structure adopted by brominated d(C-G)3 oligomer is the Z form. The IR spectrum of the film presents all the characteristic absorptions of the Z conformation and in particular is indicative of a syn conformation for the central guanosine as well as for the brominated one. Imino proton resonances of d(C-Br8G-C-G-C-Br8G) demonstrating the duplex formation were observed up to 60 degrees C. It is interesting to note that the significant highfield shifts of the dC H5" exocyclic sugar protons characteristic of the non exchangeable proton spectra of d(C-G)3 containing 5-methyl dC residues in the Z form were also detected in the proton spectrum of brominated oligomer. Whereas formation of the Z helix of methylated d(C-G)3 oligomers dependent on the salt concentration was found to occur via the preliminary formation of a B helix even in 4 M NaCl solution, the Z helix of d(C-Br8G-C-G-C-Br8G) is obtained directly from the coil form. However, IR data suggest that in the Z form of d(C-Br8G-C-G-C-Br8G), the overlapping of the base planes should be slightly different in comparison with the stacking observed in d(C-G)3 crystals. The kinetic data (activation energy and lifetime) of the Z helix-coil transition of brominated d(C-G)3 are compared to those of the B helix-coil transition observed for methylated d(C-G)3 in 0.1 M NaCl solution while the thermodynamic data of these two reactions (enthalpy and midpoint temperature) are slightly different.     

Thermodynamic stability of the 5' dangling-ended DNA hairpins formed from sequences 5'-(XY)2GGATAC(T)4GTATCC-3', where X, Y = A, T, G, C

Expressions for the partition function Q (T) of DNA hairpins are presented. Calculations of Q (T), in conjunction with our previously reported numerically exact algorithm [T. M. Paner, M. Amaratunga, M. J. Doktycz, and A. S. Benight (1990) Biopolymers, 29, 1715-1734], yield a numerical method to evaluate the temperature dependence of the transition enthalpy, entropy, and free energy of a DNA hairpin directly from its optical melting curve. No prior assumptions that the short hairpins melt in a two-state manner are required. This method is then applied in a systematic manner to investigate the stability of the six basepair duplex stem 5'-GGATAC-3' having four-base dangling single-strand ends with the sequences (XY)2, where X, Y = A, T, G, C, on the 5' end and a T4 loop on the 3' end. Results show that all dangling ends of the sample set stabilize the hairpin against melting. Increases in transition temperatures as great as 4.0 degrees C above the blunt-ended control hairpin were observed. The hierarchy of the hairpin transition temperatures is dictated by the identity of the first base of the dangling end adjoining the duplex in the order: purine greater than T greater than C. Calculated melting curves of every hairpin were fit to experimental curves by adjustment of a single parameter in the numerically exact theoretical algorithm. Exact fits were obtained in all cases. Experimental melting curves were also calculated assuming a two-state melting process. Equally accurate fits of all dangling-ended hairpin melting curves were obtained with the two-state model calculation. This was not the case for the melting curve of the blunt-ended hairpin, indicating the presence of a four-base dangling-end drives hairpin melting to a two-state process. Q (T) was calculated as a function of temperature for each hairpin using the theoretical parameters that provided calculated curves in exact agreement with the experimentally obtained optical melting curves. From Q (T), the temperature dependence of the transition enthalpy delta H, entropy delta S, and free energy delta G were calculated for every hairpin providing a quantitative assessment of the effects of dangling ends on hairpin thermodynamics. Comparisons of our results are made with those of the Breslauer group [M. Senior, R. A. Jones, and K. J. Breslauer (1988) Biochemistry 27, 3879-3885] on the T2 5' dangling-ended d(GC)3 duplexes.(ABSTRACT TRUNCATED AT 400 WORDS)     

Conformational consequences of the incorporation of arabinofuranosylcytidine in DNA. An NMR study of the DNA fragments d(CGCTAGCG) and d(CGaCTAGCG) in solution

The self-complementary octamers d(CGCTAGCG) and d(CGaCTAGCG) (aC, arabinofuranosylcytidine) were studied by means of NMR spectroscopy. It is shown that d(CGaCTAGCG), under suitable conditions of oligonucleotide concentration, ionic strength and temperature, exclusively adopts a hairpin structure. However, under the same experimental conditions (5 mM DNA, no added salt, 295 K) d(CGCTAGCG) mainly adopts a B-DNA-type duplex. At lower temperatures (less than or equal to 290 K) the hairpin form of d(CGaCTAGCG) occurs in slow exchange with an intact B-DNA-type duplex. When the DNA concentration of d(CGCTAGCG) is dramatically reduced (less than or equal to 0.5 mM) the hairpin form becomes highly favoured at the expense of the dimer. Moreover, proton-chemical-shift considerations indicate that the structural features of the hairpin structure of d(CGCTAGCG) mimic, in part, those of the modified octamer d(CGaCTAGCG), i.e. a loop comprising only the two central residues with the thymine located into the minor groove (Pieters, J. M. L., de Vroom, E., van der Marel, G. A., van Boom, J. H., Koning, T. M. G., Kaptein, R. and Altona, C. unpublished results). Thermodynamic analysis of d(CGCTAGCG) yields an average Tmd value of 342 K (1 M DNA) and a delta Hod value of -266 kJ/mol for the dimer/coil transition and an average Tmh value of 321 K and delta Hoh - 102 kJ/mol for the hairpin/coil equilibrium. For the duplex/coil equilibrium of d(CGaCTAGCG) an average Tmd value of 336 K (1 M DNA) and delta Hod value of -253 kJ/mol are deduced. The hairpin/coil transition of d(CGaCTAGCG) is characterized by a delta Hoh value of -104 kJ/mol and an average Tmh value of 331 K. It is concluded that incorporation of an arabinofuranosylcytidine in the octamer d(CGaCTAGCG) results in stabilization of the hairpin form, whereas the dimer is destablized by two aC.dG base pairs.     

Effect of base-pair sequence on the conformations and thermally induced transitions in oligodeoxyribonucleotides containing only AT base pairs

Tm curves, CD spectra, and kinetics results of the self-complementary DNA dodecamers d(A6T6), d(A3T3A3T3), d(A2T2A2T2A2T2), d(ATATATATATAT), and d(T6A6) demonstrate that the thermal transitions of these oligomers at low salt concentration involve a hairpin intermediate. At high salt concentrations (greater than 0.1 M Na+) only a duplex to denatured-strand transition appears to occur. The temperature and salt-concentration regions of the transitions are very sequence dependent. Alternating-type AT sequences have a lower duplex stability and a greater tendency to form hairpins than sequences containing more nonalternating AT base pairs. Of the two nonalternating sequences, d(T6A6) is significantly less stable than d(A6T6). Both oligomers have CD curves that are very similar to the unusual CD spectrum of poly(dA).poly(dT). The Raman spectra of these two oligomers are also quite similar, but at low temperature, small intensity differences in two backbone modes and three nucleoside vibrations are obtained. The hairpin to duplex transition for the AT dodecamers was examined by salt-jump kinetics measurements. The transition is faster than transitions for palindromic-sequence oligomers containing terminal GC base pairs. Stopped-flow kinetics studies indicate that the transition is second order and has a relatively low activation energy. The reaction rate increases with increasing ionic strength. These results are consistent with a three-step mechanism for the hairpin to duplex reaction: (i) fraying of the hairpin oligomers' terminal base pairs, (ii) a rate-determining bimolecular step involving formation of a cruciform-type intermediate from two hairpin oligomers with open terminal base pairs, and (iii) base-pair migration and formation in the intermediate to give the duplex.     

Hairpin formation of d(CGCG-TA-CGCG), d(CGCG-TG-CGCG) and their cytosine methylated analogs

Hairpin formations of decamers d(CGCG-TA-CGCG), d(CGCG-TG-CGCG), and their m5dC analogs are evidenced by the existence of biphasic absorbance melting profiles in which the lower transition temperature increases with increasing oligomer concentration, whereas the higher melting temperature is concentration independent. The corresponding temperature dependent CD intensity at 285 nm exhibits a maximum around 55 degrees C. These observations are consistent with the interpretation that the lower temperature transition corresponds to the duplex to hairpin transformation while the melting of hairpins into single strands constitutes the higher temperature transition. The CD spectrum of the hairpin conformation appears to be characterized by a couplet with nearly equal positive and negative intensities at 285 and 255 nm, respectively, while a significantly smaller intensity at 285 nm is apparent for the duplex form. The hairpin conformation is suspected to contain a two-nucleotide loop. Titrations with NaCl further suggest that, in contrast to the TA sequence, the TG sequence with wobble base pairing favors Z formation under high salt conditions.     

Hairpin Formation of d(CGCG-TA-CGCG), d(CGCG-TG-CGCG) and Their Cytosine Methylated Analogs

Abstract

Hairpin formations of decamers d(CGCG-TA-CGCG), d(CGCG-TG-CGCG), and their m⁵dC analogs are evidenced by the existence of biphasic absorbance melting profiles in which the lower transition temperature increases with increasing oligomer concentration, whereas the higher melting temperature is concentration independent. The corresponding temperature dependent CD intensity at 285 nm exhibits a maximum around 55°C. These observations are consistent with the interpretation that the lower temperature transition corresponds to the duplex to hairpin transformation while the melting of hairpins into single strands constitutes the higher temperature transition. The CD spectrum of the hairpin conformation appears to be characterized by a couplet with nearly equal positive and negative intensities at 285 and 255 nm, respectively, while a significantly smaller intensity at 285 nm is apparent for the duplex form. The hairpin conformation is suspected to contain a two-nucleotide loop. Titrations with NaCl further suggest that, in contrast to the TA sequence, the TG sequence with wobble base pairing favors Z formation under high salt conditions.     

Conformation and dynamics of a left-handed Z-DNA hairpin: studies of d(CGCGCGTTTTCGCGCG) in solution

The physical properties of the DNA oligomer d(CGCGCGTTTTCGCGCG) in solvents containing 4 M NaClO4 and 0.1 M NaCl were investigated by proton NMR, optical melting, and circular dichroism spectroscopy. Results of these investigations are as follows: (i) The DNA hexadecamer exists as a unimolecular hairpin in either high or low salt. (ii) In high salt the stem region of the hairpin is in the left-handed Z conformation. (iii) In either high or low salt, the duplex stem of the hairpin is stabilized against melting by approximately 40 degrees C compared to the linear core duplex. The added stability of the hairpin is entropic in origin. (iv) In high salt, as the temperature is elevated, the equilibrium structure of the duplex stem of the hairpin shifts from the Z to the B conformation before melting. (v) In low salt, when the DNA duplex exists in the B conformation, attachment of a T4 single-strand loop to one end only slightly decreases (by 14%) the correlation time of the CH5-CH6 interproton vector. In high salt, when the DNA duplex exists in the Z conformation, the correlation time of the CH5-CH6 interproton vector decreases by 51%. Since these viscosity-corrected correlation times are taken to be indicators of duplex motions on the nanosecond time scale, this result directly suggests a larger amplitude of these motions is present in the duplex stem of the hairpin when it exists in the Z conformation.     

A test of the linear extrapolation of unfolding free energy changes over an extended denaturant concentration range.

Guanidine hydrochloride (GdnHCl) and thermally induced unfolding measurements on the oxidized form of Escherichia coli thioredoxin at pH 7 were combined for the purpose of assessing the functional dependence of unfolding free energy changes on denaturant concentration over an extended GdnHCl concentration range. Conventional analysis of GdnHCl unfolding exhibits a linear plot of unfolding delta G vs [GdnHCl] in the transition zone. In order to extend unfolding delta G measurements outside of that narrow concentration range, thermal unfolding measurements were performed using differential scanning calorimetry (DSC) in the presence of low to moderate concentrations of GdnHCl. The unfolding delta G values from the DSC measurements were corrected to 25 degrees C using the Gibbs-Helmholtz equation and mapped onto the delta G vs [GdnHCl] plot. The dependence of unfolding delta G on [GdnHCl] was found to be linear over the full denaturant concentration range, provided that the chloride ion concentration was kept at a threshold of greater than or equal to 1.5 M. In the DSC experiments performed in the presence of GdnHCl, chloride concentrations were maintained at 1.5 M by addition of appropriate amounts of NaCl. The linear extrapolation method (LEM) gives an unfolding free energy change in the absence of denaturant (delta G degrees N-U) in excellent agreement with the delta G determined by DSC measurement in 1.5 M NaCl. The various methods give a consensus unfolding delta G value of 8.0 kcal/mol at 25 degrees C in the absence of denaturant.(ABSTRACT TRUNCATED AT 250 WORDS)     

RNA hairpin loop stability depends on closing base pair.

Thermodynamic parameters are reported for hairpin formation in 1 M NaCl by RNA sequences of the type GGXAUAAUAYCC, where X and Y are CG, GC, AU, UA, GU, or UG. A nearest neighbor analysis of the data indicates the free energy change for loop formation at 37 degrees C, delta degrees Gl,37, averages 3.4 kcal/mol for hairpin loops closed with C.G, G.C, and G.U pairs. In contrast, delta G degree l,37 averages 4.6 kcal/mol for loops closed with A.U, U.A, or U.G pairs. Thus the stability of an RNA hairpin depends on the closing base pair. The hairpin with a GA mismatch that is formed by GGCGUAAUAGCC is more stable than the corresponding hairpin with an AA mismatch. Thus hairpin stability also depends on loop sequence. These effects are not included in current algorithms for prediction of RNA structure from sequence.     

Hairpin Formation In d-AAGCTTAAGCTT Under High Salt Conditions Shows Unusual Properties

Abstract

The hairpin-duplex equillibria of the dodecamer d-AAGCTTAAGCTT and interaction of the duplex form with a pentapeptide, KGWGK, has been studied. UV thermal transitions are monophasic at low salt but biphasic at higher salt concentrations. At 10^?5M or less oligomer concentration biphasic melting curves persist till 900 mM NaCl. The d(Tm)/d log(Na⁺) for the duplex form is 12 °C and for the hairpin is 18 °C. The ΔH and ΔS values for duplex formation are low(-25 Kcal/mole and—59 Cal/mole respectively). KGWGK binds to the duplex form with a binding constant K = 3.4×10⁵M^?1measured from fluorescence quenching of tryptophan. These unusual results are markedly different from that reported for d-AGATCT- AGATCT (Biochemistry 31, 6241–6245) and are discussed in ternis of sequence dependence of loop folding and cruciform extrusion pathway of hairpin formation.     

L-nucleotides and 8-methylguanine of d(C1m8G2C3G4C5LG6LC7G8C9G10)2 act cooperatively to promote a left-handed helix under physiological salt conditions

The structure and thermal stability of a hetero chiral decaoligodeoxyribonucleotide duplex d(C1m8 G2C3G4C5LG6LC7G8C9G10)d(C11m8G12C13G14C15LG16LC17G18C19G20) (O1) with two contiguous pairs of enantiomeric 2'-deoxy-L-ribonucleotides (C5LG6L/C15LG16L) at its centre and an 8-methylguanine at position 2/12 was analysed by circular dichroism, NMR and molecular modelling. O1 resolves in a left-handed helical structure already at low salt concentration (0.1 M NaCl). The central L2-sugar portion assumes a B* left-handed conformation (mirror-image of right-handed B-DNA) while its flanking D4-sugar portions adopt the known Z left-handed conformation. The resulting Z4-B2*-Z4 structure (left-handed helix) is the reverse of that of B4-Z2*-B4 (right-handed helix) displayed by the nearly related decaoligodeoxyribonucleotide d(mC1G2mC3G4C5L G6LmC7G8mC9G10)2, at the same low salt concentration (0.1 M NaCl). In the same experimental conditions, d(C1m8G2C3G4C5G6C7G8C9G10)2 (O2), the stereoregular version of O1, resolves into a right-handed B-DNA helix. Thus, both the 8-methylguanine and the enantiomeric step CLpGL at the centre of the molecule are needed to induce left-handed helicity. Remarkably, in the various heterochiral decaoligodeoxyribonucleotides so far analysed by us, when the central CLpGL adopts the B* (respectively Z*) conformation, then the adjacent steps automatically resolves in the Z (respectively B) conformation. This allows a good optimisation of the base-base stackings and base-sugar van der Waals interactions at the ZB*/B*Z (respectively BZ*/Z*B) junctions so that the Z4-B2*-Z4 (respectively B4-Z2*-B4) helix displays a Tm (approximately 65 degrees C) that is only 5 degrees C lower than the one of its homochiral counterpart. Here we anticipate that a large variety of DNA helices can be generated at low salt concentration by manipulating internal factors such as sugar configuration, duplex length, nucleotide composition and base methylation. These helices can constitute powerful tools for structural and biological investigations, especially as they can be used in physiological conditions.     

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.     

Spectroscopic studies of (m5dC-dG)3: thermal stability of B- and Z-forms.

The hexanucleoside pentaphosphate d(m5CpGpm5CpGpm5CpG) has been studied in solution by ultra-violet absorption, circular dichroism and 31P nuclear magnetic resonance under various experimental conditions. In 0.2 M NaClO4 at low temperature, an hexamer duplex is formed which has a B or B-like conformation. As the salt concentration is increased, a transition from a B-form to the Z-form occurs and is complete in 3 M NaClO4. In 3 M NaClO4, the behavior of the Z double helix is complex as a function of temperature. The variation of the circular dichroism at 295 nm is biphasic. A first transition occurs over a large range of temperature and corresponds to a conformational change due to a non-cooperative intramolecular process. Ultra-violet absorption and 31P nuclear magnetic resonance show that the new conformation arising from a distortion of the backbone is not similar to that observed in low salt conditions (B-form). At high hexanucleotide concentration, aggregates are formed. The second transition is cooperative and corresponds to the melting of a double stranded helix into single strands.