Conformation and dynamics of the Pribnow box region of the self-complementary d(C-G-A-T-T-A-T-A-A-T-C-G) duplex in solution

Nuclear magnetic resonance (NMR) has been used to monitor the conformation and dynamics of the d(C1-G2-A3-T4-T5-A6-T6-A5-A4-T3-C2-G1) self-complementary dodecanucleotide duplex (henceforth called Pribnow 12-mer), which contains a TATAAT Pribnow box and a central core of eight dA X dT base pairs. The exchangeable imino and nonexchangeable base protons have been assigned from one-dimensional intra and inter base pair nuclear Overhauser effect (NOE) measurements. Premelting conformational changes are observed at all the dA X dT base pairs in the central octanucleotide core in the Pribnow 12-mer duplex with the duplex to strand transition occurring at 55 degrees C in 0.1 M phosphate solution. The magnitude of the NOE measurements between minor groove H-2 protons of adjacent adenosines demonstrates that the base pairs are propeller twisted with the same handedness as observed in the crystalline state. The thymidine imino proton hydrogen exchange at the dA X dT base pairs has been measured from saturation recovery measurements as a function of temperature. The exchange rates and activation barriers show small variations among the four different dA X dT base pairs in the Pribnow 12-mer duplex.(ABSTRACT TRUNCATED AT 250 WORDS)     

NMR studies of the stable mismatch purine-thymine in the self-complementary d(CGPuAATTTCG) duplex in solution

One- and two-dimensional nuclear Overhauser effect experiments demonstrate that a single hydrogen bond between a T imino proton and purine N3 is sufficient to hold the base pair dPu.dT in d(CGPuAATTTCG) by a Watson-Crick fashion rather than a Hoogsteen type. In addition, the dPu.dT base pair is well stacked with neighboring base pairs. The spin-lattice relaxation measurements at 30 and 35 degrees C of two decamers, d(CGPuAATTTCG) and d(CGAAATTTCG), reveal that the elimination of two single hydrogen bonds of dA.dT base pairs (due to the substitution of adenine for purine) in the sequence results in an increase in the overall imino proton exchange rate from 7 to 36 s-1 at the site of mismatch.     

Helix-coil transition of the dG-dC-dG-dC self-complementary duplex and complex formation with daunomycin in solution.

The duplex-to-strand transition of the self-complementary sequence dG-dC-dG-dC has been probed at the exchangeable and nonexchangeable protons and backbone phosphates by high-resolution nmr spectroscopy. The Watson-Crick imino and amino hydrogen-bonded protons, as well as the exposed amino protons, could be followed through the duplex-to-strand transition and provide information on base-pair stability at the tetranucleotide duplex level. The magnitudes of the experimental upfield nonexchangeable base-proton chemical shifts on duplex formation are consistent with calculations based on base-pair overlap geometries of the B-DNA type. The variation of the ³¹P chemical shifts in dG-dC-dG-dC with temperature appear to monitor changes in the ω,ω′ rotation angles about the O? P bonds in the postmelting transition temperature region. The complex formed between the antitumor anthracycline antibiotic daunomycin and the dG-dC-dG-dC duplex was probed at the nucleic acid and the antibiotic resonances as a function of temperature. The experimental complexation shifts of the observable daunomycin resonances have put constraints on possible overlap geometries between the intercalating anthracycline ring and adjacent base pairs.     

Structure of a purine-purine wobble base pair in the decoding center of the ribosome

Here we report the crystal structures of I.C and I.A wobble base pairs in the context of the ribosomal decoding center, clearly showing that the I.A base pair is of an I(anti).A(anti) conformation, as predicted by Crick. Additionally, the structures enable the observation of changes in the anticodon to allow purine-purine base pairing, the 'widest' base pair geometry allowed in the wobble position.     

Extra thymidine stacks into the d(CTGGTGCGG).d(CCGCCCAG) duplex. An NMR and model-building study.

NMR and model-building studies were carried out on the duplex d(CTGGTGCGG).d(CCGCCCAG), referred to as (9+8)-mer, which contains an unpaired thymidine residue. Resonances of the base and of several sugar protons of the (9+8)-mer were assigned by means of a NOESY experiment. Interresidue NOEs between dG(4) and dT(5) as well as between dT(5) and dG(6) provided evidence that the extra dT is stacked into the duplex. Thermodynamic analysis of the chemical shift vs temperature profiles yielded an average TmD value of 334 K and delta HD of -289 kJmol-1 for the duplex in equilibrium random-coil transition. The shapes of the shift profiles as well as the thermodynamic parameters obtained for the extra dT residue and its neighbours again indicate that the unpaired dT base is incorporated inside an otherwise intact duplex. This conclusion is further supported by (a) the observation of an imino-proton resonance of the unpaired dT; (b) the relatively small dispersion in 31P chemical shifts (approximately 0.5 ppm) for the (9+8)-mer, which indicates the absence of t/g or g/t combinations for the phosphate diester torsion angles alpha/zeta. An energy-minimized model of the (9+8)-mer, which fits the present collection of experimental data, is presented.     

Base pairing structure in the poly d(G-T) double helix: wobble base pairs.

High resolution nuclear magnetic resonance (NMR) and ethidium bromide binding studies are used to demonstrate that poly d(G-T) forms an ordered double helical structure at low temperatures (below 24 degrees C in 0.3 M NaCl) in which G and T are hydrogen bonded together in a wobble base pair hydrogen bonding scheme as proposed earlier by Lezius and Domin. Alternative hydrogen bonding schemes involving the tautomeric form of either T or G, such as have been proposed to account for mutation rates in DNA synthesis, are eliminated.     

Kinetics and thermodynamics of double-helix formation of self-complementary deoxyribooctanucleotides d(TCTATAGA) and d(TAGATCTA).

Double-helix formation of self-complementary deoxyribooctanucleotides, d(TCTATAGA) and d(TAGATCTA), with identical nearest neighbor base pairs has been studied by means of UV melting and temperature-jump techniques. The self-complementary duplexes of both octanucleotides with identical nearest neighbors had similar stabilities: The stabilization energies of the octanucleotides at 25 degrees C were 5.8 kcal mol-1 for d(TCTATAGA) and 6.7 kcal mol-1 for d(TAGATCTA). On the kinetic curve the melting reactions finished within 20 ms for d(TCTATAGA) and 40 ms for d(TAGATCTA) at 20 degrees C. For both octanucleotides the rate constants of dissociation increased and the rate constants of association decreased with increasing temperature.     

Low temperature solution structures and base pair stacking of double helical d(CGTACG)(2)

Solution structures and base pair stacking of a self- complementary DNA hexamer d(CGTACG)(2) have been studied at 5, 10 and 15 degrees C, respectively. The stacking interactions among the center base pair steps of the DNA duplex are found to improve when the terminal base pairs became less stable due to end fraying. A new structural quantity, the stacking sum (Sigma(s)), is introduced to indicate small changes in the stacking overlaps between base pairs. The improvements in the stacking overlaps to maintain the double helical conformation are probably the cause for the observed temperature dependent structural changes in double helical DNA molecule. A detailed analysis of the helical parameters, backbone torsion angles, base orientations and sugar conformations of these structures has been performed.     

The conformation of the d(ACCCGGGT) duplex in aqueous solution

The nonexchangeable base and sugar protons of the octanucleotide d(ACCCGGGT)2 have been assigned using two dimensional homonuclear Hartmann-Hahn relayed spectroscopy (HOHAHA), double quantum filtered homonuclear correlation spectroscopy (DQFCOSY) and nuclear Overhauser spectroscopy (NOESY) in D2O at 12 degrees C. The observed NOE's between the base protons and their own H2' protons and between the base protons and the H2' protons of the 5' adjacent nucleotide and the observed coupling constants between the deoxyribose 1' and 2',2' protons indicate that this duplex assumes a right-handed B-type helix conformation in solution.     

Recognition of base pair inversions in duplex by chimeric (alpha,beta) triplex-forming oligonucleotides

DNA recognition by triplex-forming oligonucleotides (TFOs) is usually limited by homopurine-homopyrimidine sequence in duplexes. Modifications of the third strand may overcome this limitation. Chimeric alpha-beta TFOs are expected to form triplex DNA upon binding to non-regular sequence duplexes. In the present study we describe binding properties of chimeric alpha-beta oligodeoxynucleotides in the respect to short DNA duplexes with one, three, and five base pair inversions. Non-natural chimeric TFO's contained alpha-thymidine residues inside (GT) or (GA) core sequences. Modified residues were addressed to AT/TA inversions in duplexes. It was found in the non-denaturing gel-electrophoresis experiments that single or five adjacent base pair inversions in duplexes may be recognized by chimeric alpha-beta TFO's at 10 degrees C and pH 7.8. Three dispersed base pair inversions in the double stranded DNA prevented triplex formation by either (GT) or (GA) chimeras. Estimation of thermal stability of chimeric alpha-beta triplexes showed decrease in T(m) values as compared with unmodified complexes.     

Conformation and dynamics of Z-DNA oligomer duplex of d[(CG)3TATA(CG)3] in solution.

The conformation and dynamics of a DNA oligomer, d[(CG)3TATA(CG)3], in 4M NaClO4 (Z-TATA 16 mer) have been studied by 1H NMR. The principal results of our investigation are: (i) at low temperature d[(CG)3TATA(CG)3] exists as duplexes in both low (0.1M NaCl) and high (4M NaClO4) ionic strength solutions; (ii) CGCGCG segments undergo the B-to-Z transition in 4M NaClO4; (iii) even in 4M NaClO4 the TATA box exhibits non-Z-structures and possesses multiple conformations which are slowly exchanging on the NMR chemical shift difference time scale; and, (iv) the Z-type structure of the CGCGCG segments induced in 4M NaClO4 is more conformationally mobile than its B-type counterpart in 0.1M NaCl on the nanosecond time scale.     

1H NMR study of the solution structure of the self-complementary dodecanucleotide d(TGCA)3.

The deoxyoligonucleotide d(TGCA)3 is a candidate for exhibiting unusual conformations. Its 1H NMR spectrum under low salt conditions has been obtained at 400 MHz and assigned using two-dimensional NMR techniques. The sugar puckers and glycosidic torsions have been determined by inspecting the relative intensities of the intranucleotide NOEs and COSY crosspeaks. At low electrolyte concentration (100 mM NaCl) the molecule exists as a right-handed duplex with twelve Watson-Crick base-pairs and deoxyribose moieties assuming the O1'-endo to C1'-exo pucker.     

NMR study of self-paired parallel duplex of d(AAAAACCCCC) in solution.

The oligonucleotide d(A5C5) in solution forms a parallel self-duplex at neutral and low pH values. H2O NMR spectra at pH 5.1 indicate the presence of five imino resonances at lower temperatures; and the structure is stable up to 60 degrees C. These signals can arise only from the hemiprotonated C+.C pairs [Westhof, E. and Sundaralingham, M. (1980) Biochemistry 77, 1852-1856; Westhof, E. and Sundaralingham, M. (1980) J. Mol. Biol. 142, 331-361] and constitute the first direct observation of C+.C hemiprotonated pairs in solution. The cross peaks from H1's and more than five distinct AH8's in 500 MHz 1H 2D-NOESY spectra indicate that there are two conformationally different and energetically similar A-tracts. There is good qualitative agreement between NOESY data and two theoretically derived structures in which A-tracts are reverse Watson-Crick and reverse Hoogsteen base-paired, respectively.     

The solution structure of an oligonucleotide duplex containing a 2'-deoxyadenosine-3-(2-hydroxyethyl)- 2'-deoxyuridine base pair determined by NMR and molecular dynamics studies

Determination of the solution structure of the duplex d(GCAAGTC(HE)AAAACG)·d(CGTTTTAGACTTGC) containing a 3-(2-hydroxyethyl)-2′-deoxyuridine·deoxyadenine (HE·A) base pair is reported. The three-dimensional solution structure, determined starting from 512 models via restrained molecular mechanics using inter-proton distances and torsion angles, converged to two final families of structures. For both families the HE and the opposite A residues are intrahelical and in the anti conformation. The hydroxyethyl chain lies close to the helix axis and for one family the hydroxyl group is above the HE·A plane and in the other case it is below. These two models were used to start molecular dynamic calculations with explicit solvent to explore the hydrogen bonding possibilities of the HE·A base pair. The dynamics calculations converge finally to one model structure in which two hydrogen bonds are formed. The first is formed all the time and is between HEO4 and the amino group of A, and the second, an intermittent one, is between the hydroxyl group and the N1 of A. When this second hydrogen bond is not formed a weak interaction CH···N is possible between HEC7H2 and N1A21. All the best structures show an increase in the C1′–C1′ distance relative to a Watson–Crick base pair.     

Crystal structure of d(GCGAAAGCT) containing a parallel-stranded duplex with homo base pairs and an anti-parallel duplex with Watson-Crick base pairs

A DNA fragment d(GCGAAAGCT), known to adopt a stable mini-hairpin structure in solution, has been crystallized in the space group I4₁22 with the unit-cell dimensions a = b = 53.4 Å and c = 54.0 Å, and the crystal structure has been determined at 2.5 Å resolution. The four nucleotide residues CGAA of the first half of the oligomer form a parallel duplex with another half through the homo base pairs, C₂:C₂⁺ (singly-protonated between the Watson– Crick sites), G₃:G₃ (between the minor groove sites), A₄:A₄ (between the major groove sites) and A₅:A₅ (between the Watson–Crick sites). The two strands remaining in the half of the parallel duplex are split away in different directions, and they pair in an anti-parallel B-form duplex with the second half extending from a neighboring parallel duplex, so that an infinite column is formed in a head-to-tail fashion along the c-axis. It seems that a hexa-ammine cobalt cation supports such a branched and bent conformation of the oligomer. One end of the parallel duplex is stacked on the corresponding end of the adjacent parallel duplex; between them, the guanine base of the first residue is stacked on the fourth ribose of another duplex.     

i-motif solution structure and dynamics of the d(AACCCC) and d(CCCCAA) tetrahymena telomeric repeats

Using NMR methods, we have resolved the i-motif structures formed by d(AACCCC) and by d(CCCCAA), two versions of the DNA sequence repeated in the telomeric regions of the C-rich strand of tetrahymena chromosomes. Both oligonucleotides form fully symmetrical i-motif tetramers built by intercalation of two hemiprotonated duplexes containing four C•C⁺ pairs. The structures are extremely stable. In the tetramer of d(AACCCC), the outermost C•C⁺ pairs are formed by the cytidines of the 5′ ends of the cytidine tracts. A2 forms an A2•A2 (H6trans–N7) pair stacked to C3•C3⁺ and cross-strand stacked to A1. At 0°C, the lifetimes of the hemiprotonated pairs range from 1 ms for the outermost pair to ~1 h for the innermost pairs. The tetramer of d(CCCCAA) adopts two distinct intercalation topologies in slow conformational exchange. One, whose outermost C•C⁺ pairs are built by the cytidines of the 5′ end and the other by those of the 3′ end. In both topologies, the adenosine bases are fairly well stacked to the adjacent C•C⁺ pairs. They are not paired but form symmetrical pseudo-pairs with their H6cis amino proton and N1 nitrogen pointing towards each other.     

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.     

Sequence-dependent conformation of DNA duplexes. The AATT segment of the d(G-G-A-A-T-T-C-C) duplex in aqueous solution

The nonexchangeable base and sugar protons of the octanucleotide d(G-G-A-A-T-T-C-C) have been assigned by two-dimensional correlated (COSY) and nuclear Overhauser effect (NOESY) methods in aqueous solution. The assignments are based on distance connectivities of less than 4.5 A established from NOE effects between base and sugar protons on the same strand and occasionally between strands, as well as, coupling connectivities within the protons on each sugar ring. We observe the NOEs to exhibit directionality and are consistent with the d(G-G-A-A-T-T-C-C) duplex adopting a right-handed helix in solution. The relative magnitude of the NOEs between base and sugar H2' protons of the same and 5'-adjacent sugars characterizes the AATT segment to the B-helix type in solution.     

Structure, dynamics, and thermodynamics of mismatched DNA oligonucleotide duplexes d(CCCAGGG)2 and d(CCCTGGG)2

The structures and hydrogen exchange properties of the mismatched DNA oligonucleotide duplexes d(CCCAGGG)2 and d(CCCTGGG)2 have been studied by high-resolution nuclear magnetic resonance. Both the adenine-adenine and thymine-thymine mismatches are intercalated in the duplexes. The structures of these self-complementary duplexes are symmetric, with the two strands in equivalent positions. The evidence indicates that these mismatches are not stably hydrogen bonded. The mismatched bases in both duplexes are in the anti conformation. The mismatched thymine nucleotide in d(CCCTGGG)2 is intercalated in the duplex with very little distortion of the bases or sugar-phosphate backbone. In contrast, the bases of the adenine-adenine mismatch in d(CCCAGGG)2 must tilt and push apart to reduce the overlap of the amino groups. The thermodynamic data show that the T-T mismatch is less destabilizing than the A-A mismatch when flanked by C-G base pairs in this sequence, in contrast to their approximately equal stabilities when flanked by A-T base pairs in the sequence d(CAAAXAAAG.CTTTYTTTG) where X and Y = A, C, G, and T [Aboul-ela, F., Koh, D., & Tinoco, I., Jr. (1985) Nucleic Acids Res. 13, 4811]. Although the mechanism cannot be determined conclusively from the limited data obtained, exchange of the imino protons with solvent in these destabilized heteroduplexes appears to occur by a cooperative mechanism in which half the helix dissociates.