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.     

Conformational Analysis of a Hybrid DNA-RNA Double Helical Oligonucleotide in Aqueous Solution: d(CG)r(CG)d(CG) Studied by 1D- and 2D-1H NMR Spectroscopy

Abstract

The double helical structure of the self-complementary DNA-RNA-DNA hybrid d(CG)r(CG) d(CG) was studied in solution by 500 MHz ¹H-NMR spectroscopy. The non-exchangeable base protons and the (deoxy)ribose H1′, H2′ and H2″ protons were unambiguously assigned using 2D-J-correlated (COSY) and 2D-NOE (NOESY) spectroscopy techniques. A general strategy for the sequential assignment of ¹H-NMR spectra of (double) helical DNA and RNA fragments by means of 2D-NMR methods is presented.

Conformational analysis of the sugar rings of d(CG)r(CG)d(CG) at 300 K shows that the central ribonucleotide part of the helix adopts an A-type double helical conformation. The 5′- and 3′-terminal deoxyribose base pairs, however, take up the normal DNA-type conformation. The A-to-B transition in this molecule involves only one (deoxyribose) base pair. It is shown that this A-to-B conformational transition can only be accomodated by two specific sugar pucker combinations for the junction base pair, i.e. N·S (C3′-endo-C2′-endo, 60%, where the pucker given first is that assigned to the junction nucleotide residue of the strand running 5′ → 3′ from A-RNA to B-DNA) and S·S (C2′-endo-C2′-endo, 40%).     

Proton NMR study of the B----Z transition of d(CGm5CG)2 and d(CGm5CGCG)2: theory and experiment.

The magnetic shielding produced by the double helix in a B-DNA and a Z-DNA conformation is calculated for each non exchangeable proton of the oligodeoxynucleotides d(CGm5CG)2 and d(CGm5CGCG)2. The differences between the values obtained for the two helical forms are in good agreement with the variations of chemical shift measured when the salt concentration of the solution is changed from 0.1 M to 2 or 4 M. The analysis of the theoretical chemical shift variations shows that the large upfield shift observed for some of the protons of the cytidine residues is due to the sum of the ring current and local magnetic anisotropy effects of the guanines of the two nearest neighbours residues.     

The crystal structure of N4-methylcytosine.guanosine base-pairs in the synthetic hexanucleotide d(CGCGm4CG).

The structure of d(CGCGm4CG) were m4C = N4-methylcytosine has been determined by crystallographic methods. The crystals are multifaced prisms, with orthorhombic space group P2(1)2(1)2(1) and unit cell dimensions of a = 17.98, b = 30.77 and c = 44.75A. The asymmetric unit consists of one duplex of hexanucleotide and 49 waters. The R-factor is 0.189 for 1495 reflections with F > or = sigma(F) to a resolution limit of 1.8A. The double helix has a Z-DNA type structure which appears to be intermediate in structure to the two previously characterised structure types for Z-DNA hexamers. The two m4C.G base-pairs adopt structures that are very similar to those of the equivalent base-pairs in the structure of the native sequence d(CGCGCG) except for the presence of the methyl groups which are trans to the N3 atoms of their parent nucleotides and protrude into the solvent region. The introduction of the modified base-pairs into the d(CGCGCG) duplex appears to have a minimal effect on the overall base-pair morphology of the Z-DNA duplex.     

Comparison of the B- and Z-form hairpin loop structures formed by d(CG)5T4(CG)5

The partially self-complementary synthetic DNA oligonucleotide d(CG)5T4(CG)5 has been studied by using 1H and 31P NMR and circular dichroism. Results show that, under low-salt conditions (120 mM NaCl buffer), an intramolecular hairpin loop exists in which the double-helical stem region is B-form and the thymidine loop residues have predominantly southern (C2'-endo) sugar conformations. The thymidine glycosidic torsion angles are intermediate between syn and anti or exist as an equilibrium mixture of residues in the two extremes. NOESY data indicate that the structure of the loop region is very similar to that found for d(CG)2T4(CG)2 [Hare, D. R., & Reid, B. R. (1986) Biochemistry 25, 5341-5350]. Under high-salt conditions (6 M NaClO4 buffer), the dominant form (approximately equal to 85%) is an intramolecular hairpin structure in which the stem region forms a Z-form double helix. As in the B-form, the loop thymidine residues are intermediate between the syn and anti conformations or exist as an equilibrium mixture of the two, but the thymidine sugar conformations differ in that they are biased toward northern (C3'-endo) conformations.     

Electronic structure of DNA by DV-X alpha cluster calculations: II. d(GG).d(CC), d(CG)2, d(GC)2 A and B conformations. (Part 2) Sugars and bases

The electronic structure of d(GG).d(CC), d(CG)2, d(GC)2 which are stacked base pairs in the DNA double helix, are elucidated for both A and B conformations in detail by DV-X alpha cluster calculations. These three DNA double helix fragments are contracted from the same bases, G and C, but the electronic structures of the fragments for both A and B conformations are different from each other characteristically. There are some delicate differences in the admixture of the orbital components and the overlap populations of intra- and inter- strand stacked bases among the stacking isomers. On the other hand, the electronic states of sugars differ in the 5'-3' direction, but are not almost dependent on stacked base pairs.     

Electronic structure of DNA by DV-X alpha cluster calculations. I. d(GG).d(CC), d(CG)2, d(GC)2 A and B conformations

The electronic structure of d(GG).d(CC), d(CG)2, d(GC)2 which are stacked base pairs in the DNA double helix, are elucidated for both A and B conformations in detail by DV-X alpha cluster calculations. These three DNA double helix fragments are constructed from the same bases, G and C, but the electronic structure of the fragments for A and B conformations differs from each other characteristically. In particular, the electronic states of the O2 and O3 in phosphates differ drastically from each other, and might play a crucial role as recognition sites in various reaction processes concerning DNA. These differences are caused by the delicate differences in the admixture of the orbital components and the intra- and inter-bases interactions. Contour maps of the wavefunction of the HOMO and LUMO are compared among the stacking isomers.     

The effect of methylation of the 6 oxygen of guanine on the structure and stability of double helical DNA

The effect of methylation of the O-6 position of guanine in short segments of double helical DNA has been investigated by molecular mechanical simulations on the sequences d(CGCGCG)2, d(CGC[OMG]CG)2, d(CGT[OMG]CG)2, d(CGC[OMC]CG/(CGCGCG), d(CGC[OMG]CG/d(CGTGCG), d(CGCGAATTCGCG)2 and d(CGCGAATTC[OMG]CG)2. Guanines methylated at the O-6 position are found to form hydrogen bonds of roughly equal strength to cytosine and thymine. The optimum structure of these modified base pairs are not dramatically different from normal GC pairs, but both involve some bifurcation of the proton donors of cytosine (4NH2) or thymine (3NH) between the guanine N3 and O6 groups.     

Solution structure of RNA duplexes containing alternating CG base pairs: NMR study of r(CGCGCG)2 and 2'-O-Me(CGCGCG)2 under low salt conditions.

Structures of r(CGCGCG)2 and 2'-O-Me(CGCGCG)2 have been determined by NMR spectroscopy under low salt conditions. All protons and phosphorus nuclei resonances have been assigned. Signals of H5'/5" have been assigned stereospecifically. All 3JH,H and 3JP,H coupling constants have been measured. The structures were determined and refined using an iterative relaxation matrix procedure (IRMA) and the restrained MD simulation. Both duplexes form half-turn, right-handed helices with several conformational features which deviate significantly from a canonical A-RNA structure. Duplexes are characterised as having C3'-endo sugar pucker, very low base-pair rise and high helical twist and inclination angles. Helices are overwound with <10 bp per turn. There is limited inter-strand guanine stacking for CG steps. Within CG steps of both duplexes, the planes of the inter-strand cytosines are not parallel while guanines are almost parallel. For the GC steps this pattern is reversed. The 2'-O-methyl groups are spatially close to the 5'-hydrogens of neighbouring residues from the 3'-side and are directed towards the minor groove of 2'-O-Me(CGCGCG)2 forming a hydrophobic layer. Solution structures of both duplexes are similar; the effect of 2'-O-methylation on the parent RNA structure is small. This suggests that intrinsic properties imposed by alternating CG base pairs govern the overall conformation of both duplexes.     

Oligoaminonucleoside phosphoramidates. Oligomerization of dimers of 3''-amino-3''-deoxy-nucleotides (GC and CG) in aqueous solution.

The self-complementary 5'-phosphorylated dinucleoside 3' (N)----5' (P)-linked phosphoramidates with sequence GC (8a), CG (8b) and the tetranucleoside triphosphoramidate with sequence GCGC (10a) and CGCG (10b) have been synthesized and characterized by physicochemical and enzymatic methods. The dinucleosides 8a or 8b oligomerize in aqueous solution in the presence of a water-soluble carbodiimide. This process is efficient and regiospecific. In the case of GC it produces alternating 3' (N)----5' (P)-linked phosphoramidates up to 15 dimeric units in length with a yield in excess of 70%. The oligomerization of the CG isomer is much less efficient. The mechanism of oligomerization is discussed.     

B to Z transitions of the short DNA hairpins formed from the oligomer sequences: d[(CG)3X4(CG)3] (X = A, T, G, C).

Circular Dichroism (CD) spectra were collected as a function of sodium perchlorate concentration [NaClO4] for the set of DNA hairpins formed from the oligomer sequences d[(CG)3X4(CG)3] where X = A, T, G or C. Over the range in salt concentration from 0 to 4.0 M NaClO4, the CD spectra invert in a manner characteristic of the B to Z transition. A factor analysis routine is described and employed to determine the least number of basis spectra required to fit the measured spectra of each hairpin over the entire salt range examined. In every case, linear combinations of only two sub-spectra fit the experimental spectra of the hairpins with greater than 98% accuracy, indicating the spectrally monitored structural transitions are two-state. From the relative weights of the individual sub-spectra, B-Z transition curves are constructed. The transitions are analyzed in terms of a simple two-state equilibrium model which yields an evaluation of the transition free-energy, delta GB-Z, as a function of NaClO4 concentration. At 1.0 M NaClO4 and 21 degrees C, delta GB-Z = 5.4, 4.9, 3.6 and 2.3 kcal/mole for the G4, T4, A4 and C4 loop hairpins, respectively.     

Conformational stability of alternating d (CG) oligomers in high salt solution.

The conformation of d (CG)n oligomers with n = 2,3 has been studied in aqueous solution in the presence of high salt concentration. A minimum n value of three is necessary to obtain a left-handed Z-helix. When d (CG)3 is flanked by three non Z-helicogenic alternating AT sequences the left-handed helix is unstable and a B-type conformation is obtained also at high salt concentration.     

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.     

Discrimination between A-type and B-type conformations of double helical nucleic acid fragments in solution by means of two-dimensional nuclear Overhauser experiments

The solution structure of two double helical nucleic acid fragments, viz, r(CGCGCG) and d(CGCGCG), was probed by means of two-dimensional nuclear Overhauser effect spectroscopy. The two compounds were selected as models for the A-type and B-type double helical conformations, respectively, and it is shown that for each of the two model compounds the intensities of the NOE cross peaks between base- and H2' (deoxy)ribose proteins are qualitatively in correspondence with the relative NOE intensities expected on basis of the supposed duplex conformations. Thus our results indicate that NOE-data can be used to differentiate between A-and B-type double helical conformations in solution. Coupling constant data show that, except for G(6), all ribose rings in r(CGCGCG) adopt pure N (C3'-endo) conformations thereby manifesting that this molecule takes up a regular A-type double helical conformation in solution. In contrast, the deoxyribose rings in d(CGCGCG) retain conformational freedom in the duplex state, albeit that the N/S-equilibrium is biased towards the S (C2'-endo) sugar conformation. This finding indicates that in solution the B-DNA backbone is highly dynamic.     

Ethidium ion binds more strongly to a DNA double helix with a bulged cytosine than to a regular double helix

Thermodynamic parameters for ethidium intercalation were determined for the double helices formed by the oligonucleotides dCA6G + dCT6G, which form a normal helix, and dCA3CA3G + dCT6G, which form a double helix with the middle cytosine bulged outside of the helix. Ethidium intercalation was measured by monitoring the absorbance at 260 and 283 nm as a function of temperature for a number of concentrations of ethidium. The binding to the normal helix occurs equally at all the intercalation sites, with an enthalpy of binding of -8 kcal mol-1, an entropy of binding of -6 eu, and an equilibrium constant at 25 degrees C of 2.2 X 10(4) M-1. The binding to the bulged double helix was considerably stronger and is consistent with a model in which the intercalation sites on either side of the bulged base bind 10 times stronger than the other sites. Thus, there are two strong binding sites on the perturbed helix with equilibrium constants for binding of 2 X 10(5) M-1 at 25 degrees C in addition to five normal sites. Several other binding models were tested but did not fit the data satisfactorily.     

Interaction between the Z-type DNA duplex and 1,3-propanediamine: crystal structure of d(CACGTG)2 at 1.2 A resolution

The crystal structure of a hexamer duplex d(CACGTG)(2) has been determined and refined to an R-factor of 18.3% using X-ray data up to 1.2 A resolution. The sequence crystallizes as a left-handed Z-form double helix with Watson-Crick base pairing. There is one hexamer duplex, a spermine molecule, 71 water molecules, and an unexpected diamine (Z-5, 1,3-propanediamine, C(3)H(10)N(2)) in the asymmetric unit. This is the high-resolution non-disordered structure of a Z-DNA hexamer containing two AT base pairs in the interior of a duplex with no modifications such as bromination or methylation on cytosine bases. This structure does not possess multivalent cations such as cobalt hexaammine that are known to stabilize Z-DNA. The overall duplex structure and its crystal interactions are similar to those of the pure-spermine form of the d(CGCGCG)(2) structure. The spine of hydration in the minor groove is intact except in the vicinity of the T5A8 base pair. The binding of the Z-5 molecule in the minor grove of the d(CACGTG)(2) duplex appears to have a profound effect in conferring stability to a Z-DNA conformation via electrostatic complementarity and hydrogen bonding interactions. The successive base stacking geometry in d(CACGTG)(2) is similar to the corresponding steps in d(CG)(3). These results suggest that specific polyamines such as Z-5 could serve as powerful inducers of Z-type conformation in unmodified DNA sequences with AT base pairs. This structure provides a molecular basis for stabilizing AT base pairs incorporated into an alternating d(CG) sequence.     

Energetics of Z-DNA formation in poly d(A-T), poly d(G-C), and poly d(A-C) poly d(G-T).

The conformational change for the alternating purine-pyrimidine polydeoxyribonucleotides i.e. poly d(A-T), poly d(G-C), and poly d(A-C) poly d(G-T) from a right-handed conformation at room temperature to the left-handed Z-DNA like double helix at elevated temperatures has been studied by UV spectroscopy, Raman spectroscopy, and by adiabatic differential scanning microcalorimetry (DSC) in the presence of Na+ and Mg2+ or Ni2+ respectively as counterions. The differential UV spectra reveal through a hyperchromic shift at around 280nm and a hypochromic shift at 260nm that a conformational change to the left-handed conformation occurs. The Raman spectra clearly show characteristic changes, a drastic decrease of the band at 680cm-1 and the appearance of a new band at 628cm-1, due to the change of the purine bases to the syn conformation upon inversion of the helix-handedness. The course of the transition as function of temperature can be followed quantitatively by plotting the change in the excess heat capacity vs. temperature. The transition enthalpy delta H for the B- to Z-DNA transition per mole base pairs (mbp) amounts to 2.0 +/- 0.2kcal for poly d(G-C), to 4.0 +/- 0.4kcal for poly d(A-T), and to 3.1 +/- 0.3kcal for poly d(A-C) poly d(G-T). The enthalpy change due to the Z-DNA to coil transitions (per mole base pairs) amounts to 11kcal for poly d(G-C), 10.5kcal for poly d(A-T) and 11.3kcal for poly d(A-C) poly d(G-T).     

Cu(II)-binding properties of a cytochrome c with a synthetic metal-binding site: His-X3-His in an alpha-helix.

A metal-binding site consisting of two histidines positioned His-X3-His in an alpha-helix has been engineered into the surface of Saccharomyces cerevisiae iso-1-cytochrome c. The synthetic metal-binding cytochrome c retains its biological activity in vivo. Its ability to bind chelated Cu(II) has been characterized by partitioning in aqueous two-phase polymer systems containing a polymer-metal complex, Cu(II)IDA-PEG, and by metal-affinity chromatography. The stability constant for the complex formed between Cu(II)IDA-PEG and the cytochrome c His-X3-His site is 5.3 x 10(4) M-1, which corresponds to a chelate effect that contributes 1.5 kcal mol-1 to the binding energy. Incorporation of the His-X3-His site yields a synthetic metal-binding protein whose metal affinity is sensitive to environmental conditions that alter helix structure or flexibility.     

Fluorescence of meso-tetrakis(4-(carboxy)phenyl)porphine covalently bound to oligonucleotides d(CG)5 and d(TA)5

The amino-reactive derivative of tetraphenylporphine meso-tetrakis[4-(carboxy)phenyl]porphine (TCPP) was synthesized, which is characterized by a high molar absorption coefficient (epsilon 416 = 36,500 M-1.cm-1). TCPP was covalently attached to oligonucleotides d(CG)5 [d(CG)5-TCPP] and d(TA)5 [d(TA)5-TCPP]. The spectral characteristics of these complexes were studied in 0.01 M phosphate buffer, pH 7 at 23 degrees C. UV-visible absorption spectra of these complexes have a clearly pronounced Soret band at (414 +/- 1) nm for d(CG)5-TCPP and at (412 +/- 1) nm for d(TA)5-TCPP. The fluorescence spectra of these complexes have maxima at (648 +/- 2) nm for d(CG)5-TCPP and at (658 +/- 2) nm for d(TA)5-TCPP. In this study we also determined fluorescence quantum yields q and fluorescence lifetimes tau [q = 0.099 +/- 0.011, tau = (9.0 +/- 0.3) ns for d(CG)5-TCPP and q = 0.080 +/- 0.011, tau = (8.7 +/- 0.3) ns for d(TA)5-TCPP]. A temperature rise from 5 to 50 degrees C produced only slight (within 23%) emission changes in both samples studied. Taking into account: a) high fluorescence yields (q), b) weak dependence of q on temperature, c) weak q dependence of q on the oligonucleotide type, we conclude that TCPP may be used as a sensitive fluorescence label in DNA studies.     

Discrimination Between A-type and B-type Conformations of Double Helical Nucleic Acid Fragments in Solution by Means of Two-dimensional Nuclear Overhauser Experiments

Abstract

The solution structure of two double helical nucleic acid fragments, viz. r(CGCGCG) and d(CGCGCG), was probed by means of two-dimensional nuclear Overhauser effect spectroscopy. The two compounds were selected as models for the A-type and B-type double helical conformations, respectively, and it is shown that for each of the two model compounds the intensities of the NOE cross peaks between base- and H2′ (deoxy)ribose proteins are qualitatively in correspondence with the relative NOE intensities expected on basis of the supposed duplex conformations. Thus our results indicate that NOE-data can be used to differentiate between A- and B-type double helical conformations in solution.

Coupling constant data show that, except for G(6), all ribose rings in r(CGCGCG) adopt pure N (C3′-endo) conformations thereby manifesting that this molecule takes up a regular A-type double helical conformation in solution. In contrast, the deoxyribose rings in d(CGCGCG) retain conformational freedom in the duplex state, albeit that the N/S- equilibrium is biased towards the S (C2′-endo) sugar conformation. This finding indicates that in solution the B-DNA backbone is highly dynamic.