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.     

Monte Carlo calculations of ion distributions surrounding the oligonucleotide d(ATATATATAT)2 in the B, A, and wrinkled D conformations.

We calculated the uni-univalent ion distributions around the oligonucleotide d(AT)5.d(AT)5 in the A, B and wrinkled D conformation using the Metropolis Monte Carlo method. All atoms were included in the oligonucleotide model with partial charges and hard sphere radii assigned to each atom. The univalent counter- and coions were modeled as hard spheres with radius 0.3 nm. The solvent was assigned a dielectric constant of 80, corresponding to a temperature of 298K. The counterion distribution surrounding each of the conformers and the distribution surrounding an impenetrable cylinder, were calculated for four salt concentrations. We found significant counterion density in the major groove of the A DNA while fewer counterions occupied the grooves of B DNA. In the wrinkled D DNA, where groove occupancy is sterically hindered, the ion distributions were identical to the distributions surrounding the impenetrable, cylindrical model. This suggests that excluded volume effects significantly influence the details of the ion distributions near the oligomer, while the detailed charge distributions of the oligomer affects the ion distributions only minimally. Although substantial variation in counterion density was observed near the oligomers of differing conformations, the total number of counterions located within a cylinder surrounding the oligomer bounded radially by 2.4 nm was independent of the conformation of the oligomer. Therefore, for this model system, the local univalent counterion distributions are extremely sensitive to the geometry of the oligonucleotide whereas the extent of neutralization of the oligoanion is insensitive to the conformation of the oligomer.     

The effect of the simple repeating d(CG.GC)n, d(CA.GT)n, and d(A.T)n DNA sequences on the nucleosomal organization of SV40 minichromosomes.

The effect of several simple repeating DNA sequences--d(CG.GC)5, d(CA.GT)30, and d(A.T)60--on the nucleosomal organization of the SV40 minichromosome is analyzed. These three different sequences were cloned at the Hpa II site of SV40 (position 346) which occurs at the 3' border of the nucleosome-free SV40 control region. Our results show that neither the d(A.T)60 sequence nor the d(CG.GC)5 sequence appear to have any relevant effect on the nucleosomal organization of the region of the minichromosome surrounding the inserted repeated sequence. Both sequences are hypersensitive to micrococcal nuclease cleavage in the minichromosome, indicating that they are not organized into nucleosomes. On the other hand, the d(CA.GT)30 sequence is found organized as nucleosomes and causes the delocation of nucleosomes in the minichromosomal region close to the inserted repeated sequence.     

Interpretation of DNA vibration modes: I--The guanosine and cytidine residues involved in poly(dG-dC).poly(dG-dC) and d(CG)3.d(CG)3

A normal coordinate analysis has been carried out on guanosine and cytidine residues appearing in oligo and polynucleotides by using a simplified valence force field that allows the vibrational spectra of 5'-dGMP and 2'-deoxycytidine molecules to be reproduced. The role of both C2'-endo and C3'-endo conformations on sugar pucker, as well as that of glycosidic torsion angle (X), on several characteristic vibration modes of these residues have been studied. The present calculations based on a non-redundant set of internal coordinates preserving the harmonic approximation of the potential field, allows us to explain quite satisfactorily the modifications of the vibrational spectra in the 1550-1250 cm-1 and 785-500 cm-1 regions, when the right----left-handed conformational transition occurs.     

Ultrapolymorphic DNA: B, A, Z, and Z* conformations of poly(dA-dC).poly(dG-dT)

The synthetic polynucleotide poly(dA-dC).poly(dG-dT) at low ionic strength is shown to undergo conformational changes in the presence of [tris(2-aminoethyl)amine]zinc(II) chloride (ZnN4). At 100 microM ZnN4, circular dichroism and 31P NMR spectra show the formation of Z DNA. With an increase of the concentration up to 600 microM, an A-like form is obtained, and at still higher concentration, the polynucleotide reverts to the original B form. Experiments on polynucleotide samples in which some sequence errors were observed showed that spermine was necessary as well as ZnN4 to induce the Z form. At higher concentrations of spermine and ZnN4, a second Z form (Z*) is observed. Raising the ionic strength inhibits the formation of the Z form, whereas the presence of ethylene glycol favors it.     

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.     

Interruptions of (CG)n sequences by GG, TG and CA need not prevent B to Z transition in solution.

Oligonucleotides containing alternating purines-pyrimidines with AT base pairs have been shown to exist in the Z-form preferably in solid state. We report that oligodeoxyribonucleotides with GG, TG and CA interruptions in their alternating CG sequences can undergo B to Z transition in solution in the absence of any chemical modification or topological constraint. The sequences, d(CGCGCGGCGCGC) and d(CGTGCGCACG) have been synthesised and shown to adopt Z- conformation in presence of millimolar concentrations of Ni2+ under low water activity conditions. Significance of GG, TG and CA interruptions in the B to Z transition is discussed.     

The A and B conformations of DNA and RNA subunits. Potential energy calculations for dGpdC

In order to obtain a molecular picture of the A and B forms of a DNA subunit, potential energy calculations have been made for dGpdC with C(3′)-endo and C(2′)-endo [or C(3′)-exo] sugar puckerings. These are compared with results for GpC. The global minima for dGpdC and GpC are almost identical. They are like A-form duplex DNA and RNA, respectively, with bases anti, the ω′, ω angle pair near 300°, 280°, and sugar pucker C(3′)-endo. For dGpdC, a B-form helical conformer, with sugar pucker C(2′)-endo and ω′ = 257°, ω = 298°, is found only 0.4 kcal/mol above the global minimum. A second low-energy conformation (2.3 kcal/mol) has ω′ = 263°, ω = 158° and ψ near 180°. This has dihedral angles like the original Watson–Crick model of the double helix. In contrast, for GpC, the C(2′)-endo B form is 6.9 kcal/mol above the global minimum. These theoretical results are consistent with experimental studies on DNA and RNA fibers. DNA fibers exist in both A and B forms, while RNA fibers generally assume only the A form. A low-energy conformation unlike the A or B forms was found for both dGpdC and GpC when the sugars were C(3′)-endo. This conformation—ω′,ω near 20°,80°—was not observed for C(2′)-endo dGpdC. Energy surface maps in the ω′,ω plane showed that C(2′)-endo dGpdC has one low-energy valley. It is in the B-form helical region (ω′ ～ 260°, ω ～ 300). When the sugar pucker is C(3′)-endo, dGpdC has two low-energy regions: the A-form helical region and the region with the minimum at ω′ = 16°, ω = 85°.     

Oligonucleotide duplexes containing CC(A/T)GG stimulate cleavage of refractory DNA by restriction endonuclease EcoRII

Some DNA species are resistant towards the restriction endonuclease EcoRII despite the presence of unmodified recognition sites. We show that 14 base-pair oligonucleotide duplexes containing the EcoRII recognition site 5'-CC(A/T)GG are cleaved by this enzyme and are able to stimulate EcoRII cleavage of such resistant DNA molecules (e.g. DNA of bacterial virus T3). A direct correlation between the concentration of oligonucleotide duplex molecules and the degree of EcoRII digestion of the primarily resistant DNA is observed. This indicates a stoichiometric rather than a catalytic mode of enzyme activation. An excess of DNA devoid of EcoRII sites ('non-site' DNA, e.g. MvaI-digested T7 DNA) does not interfere with the activity of EcoRII.     

Complete primary structure of rainbow trout type I collagen consisting of alpha1(I)alpha2(I)alpha3(I) heterotrimers.

The subunit compositions of skin and muscle type I collagens from rainbow trout were found to be alpha1(I)alpha2(I)alpha3(I) and [alpha1(I)](2)alpha2(I), respectively. The occurrence of alpha3(I) has been observed only for bonyfish. The skin collagen exhibited more susceptibility to both heat denaturation and MMP-13 digestion than the muscle counterpart; the former had a lower denaturation temperature by about 0.5 degrees C than the latter. The lower stability of skin collagen, however, is not due to the low levels of imino acids because the contents of Pro and Hyp were almost constant in both collagens. On the other hand, some cDNAs coding for the N-terminal and/or a part of triple-helical domains of proalpha(I) chains were cloned from the cDNA library of rainbow trout fibroblasts. These cDNAs together with the previously cloned collagen cDNAs gave information about the complete primary structure of type I procollagen. The main triple-helical domain of each proalpha(I) chain had 338 uninterrupted Gly-X-Y triplets consisting of 1014 amino acids and was unique in its high content of Gly-Gly doublets. In particular, the bonyfish-specific alpha(I) chain, proalpha3(I) was characterized by the small number of Gly-Pro-Pro triplets, 19, and the large number of Gly-Gly doublets, 38, in the triple-helical domain, compared to 23 and 22, respectively, for proalpha1(I). The small number of Gly-Pro-Pro and the large number of Gly-Gly in proalpha3(I) was assumed to partially loosen the triple-helical structure of skin collagen, leading to the lower stability of skin collagen mentioned above. Finally, phylogenetic analyses revealed that proalpha3(I) had diverged from proalpha1(I). This study is the first report of the complete primary structure of fish type I procollagen.     

DNA fragment conformations. A 1H-NMR conformational analysis of the d(G-G)-chelated platinum-oligonucleotide d(A-T-G-G)cisPt

The conformation of d(A-T-G-G) and d(A-T-G-G)cisPt has been investigated by 1H-NMR at 500 MHz and 90 MHz under various experimental conditions of temperature and concentration. Analysis of the coupling constants between the deoxyribose protons shows that all the sugar rings of d(A-T-G-G) adopt the S(C2'-endo) conformation most of the time. By contrast, in the platinated tetramer, d(A-T-G-G)cisPt, the N(C3'-endo) conformation is highly predominant for the internal dG residue while the S(C2'-endo) conformation is largely favoured for the other residues as in the case of the unplatinated compound. The relaxation time and nuclear Overhauser effect measurements indicate that the orientation of the two guanines of d(A-T-G-G)cisPt is anti in agreement with the previous results obtained for the dimers: r(G-G)cisPt, d(G-G)cisPt. On lowering the temperature from 80 degrees C to 20 degrees C, several proton resonances of d(A-T-G-G)cisPt exhibit large chemical shift and linewidth variations. The most spectacular temperature effect was observed for the internal dG(H1') and dT(H4') protons. All the delta = f(t) curves display a sigmoid form with the same mid-point temperature of 44 +/- 2 degrees C. This mid-point temperature together with the observed chemical shift and linewidth variations were found to be independent of the d(A-T-G-G)cisPt concentration. These results suggest that d(A-T-G-G)cisPt can adopt two different conformations depending on the temperature. The enthalpy for the transition between the high and low temperature conformations is about 84 kJ/mol.     

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%).     

Ligand modulation of [35S]GTPgammaS binding at human alpha(2A), alpha(2B) and alpha(2C) adrenoceptors

Affinities and efficacies of chemically diverse ligands--some of them used as clinical agents--were examined, employing [3H]RX821,002 and [35S]GTPgammaS binding assays, respectively, at human (h) cloned, halpha(2A), halpha(2B) and halpha(2C) adrenoceptors (AR) expressed in Chinese hamster ovary (CHO) cells. As compared to noradrenaline (NA, efficacy defined as 100%), the majority of the 13 agonists tested generally behaved as partial agonists. Amongst 18 antagonists, pK(B) and pK(i) values, which were highly correlated for each alpha(2)-AR subtype, failed to reveal any strikingly selective agents. Inverse agonist properties were not detected for any antagonist, consistent with a lack of constitutive activity suggested by the monophasic inhibition of [35S]GTPgammaS binding by GTPgammaS. These data should facilitate interpretation of experimental and clinical actions of adrenergic agonists. Moreover, they emphasize the continuing need for alpha(2)-AR subtype-selective antagonists in order to define further the roles and therapeutic relevance of halpha(2A)-, halpha(2B)-, and halpha(2C)-AR.     

In vivo assessment of the Z-DNA-forming potential of d(CA.GT)n and d(CG.GC)n sequences cloned into SV40 minichromosomes

Alternating repeated d(CA.GT)n and d(CG.GC)n sequences constitute a significant proportion of the simple repeating elements found in eukaryotic genomic DNA. These sequences are known to form left-handed Z-DNA in vitro. In this paper, we have addressed the question of the in vivo determination of the Z-DNA-forming potential of such sequences in eukaryotic chromatin. For this purpose, we have investigated the ability of a d(CA.GT)30 sequence and a d(CG.GC)5 sequence to form left-handed Z-DNA when cloned into simian virus 40 (SV40) minichromosomes at two different positions: the TaqI site, which occurs in the intron of the T-antigen gene, and the HpaII site, which is located in the late promoter region within the SV40 control region. Formation of Z-DNA at the inserted repeated sequences was analyzed through the change in DNA linkage associated with the B to Z transition. Our results indicate that regardless of: (1) the site of insertion (either TaqI or HpaII), (2) the precise moment of the viral lytic cycle (from 12 h to 48 h postinfection) and (3) the condition of incorporation of the SV40 recombinants to the host cells (either as minichromosomes or as naked DNA, relaxed or negatively supercoiled), neither the d(CA.GT)30 nor the d(CG.GC)5 sequence are stable in the left-handed Z-DNA conformation in the SV40 minichromosome. The biological relevance of these results is discussed.     

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).     

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.     

Conformational variation of the central CG site in d(ATGACGTCAT)2 and d(GAAAACGTTTTC)2. An NMR, molecular modelling and 3D-homology investigation.

The determination of the solution structure of two self-complementary oligomers d(ATGACGTCAT)2 (CG10) and d(GAAAACGTTTTC)2 (CG12), both containing the 5'-pur-ACGT-pyr-3' sequence, is reported. The impact of the base context on the conformation of the central CpG site has been examined by a combined approach of: (a) 2D 1H-NMR and 31P-NMR; (b) molecular mechanics under experimental constraints; (c) back-calculations of NOESY spectra and iterative refinements of distances; and (d) 3D-homology search of the central tetrad ACGT within the complete oligonucleotides. A full NMR study of each fragment is achieved by means of standard 2D experiments: NOESY, 2D homonuclear Hartmann-Hahn spectroscopy, double-quantum-filtered COSY and heteronuclear 1H-31P correlation. Sugar phase angle, epsilon-zeta difference angle and NOE-derived distances are input as experimental constraints to generate molecular models by energy minimization with the help of jumna. The morass program is used to iteratively refine the structures obtained. The similarity of the two ACGTs within the whole oligonucleotides is investigated. Both the decamer and the dodecamer adopt a B-like DNA conformation. However, the helical parameters within this conformational type are significantly different in CG12 and CG10. The central CpG step conformation is not locked by its nearest environment (5'A and 3'T) as seen from the structural analysis of ACGT in the two molecules. In CG12, despite the presence of runs of A-T pairs, CpG presents a high twist of 43 degrees and a sugar phase at the guanine of about 180 degrees, previously observed in other ACGT-containing-oligomers. Conversely, ACGT in CG10 exhibits strong inclinations, positive rolls, a flat profile of sugar phase, twist and glycosidic angles, as a result of the nucleotide sequence extending beyond the tetrad. The structural specificity of CG10 and its flexibility (as reflected by its energy) are tentatively related to the process of recognition of the cyclic AMP response element by its cognate protein.     

Influence of tetraalkyl ammonium ions on the structure of poly (rG-dC).poly (rG-dC): unexpected transitions among the Z, A and B conformations.

The conformation of the double-stranded, mixed ribodeoxyribo polynucleotide, poly (rG-dC).poly (rG-dC), has been examined in the presence of tetraalkyl ammonium ions. Tetramethyl ammonium ion stabilizes the "low salt" Z conformation (1) of the polymer from submillimolar to molar concentrations of the counterion. In the presence of tetraethyl and tetrapropyl ammonium ions the polymer exists in the low salt Z form up to 2 mM concentration of the counterions and then flips to the right hand helical A form. With tetrabutyl ammonium counterions the polymer is in an A conformation at low ion concentrations and converts to a B form at concentrations greater than thirty millimolar. These results are interpreted in terms of electrostatic and solvent interactions of the polynucleotide.     

Higher-order structure of bovine mitochondrial tRNA(Phe) lacking the 'conserved' GG and T psi CG sequences as inferred by enzymatic and chemical probing.

Bovine mitochondrial (mt) phenylalanine tRNA (tRNA(Phe)), which lacks the 'conserved' GG and T psi YCG sequences, was efficiently purified by the selective hybridization method using a solid phase DNA probe. The entire nucleotide sequence of the tRNA, including modified nucleotides, was determined and its higher-order structure was investigated using RNaseT2 and chemical reagents as structural probes. The D and T loop regions as well as the anticodon loop region were accessible to RNaseT2, and the N-3 positions of cytidines present in the D and T loops were easily modified under the native conditions in the presence of 10mM Mg2+. On the other hand, the nucleotides present in the extra loop were protected from the chemical modification under the native conditions. From the results of these probing analyses and a comparison of the sequences of mitochondrial tRNA(Phe) genes from various organisms, it was inferred that bovine mt tRNA(Phe) lacks the D loop/T loop tertiary interactions, but does have the canonical extra loop/D stem interactions, which seem to be the main factor for bovine mt tRNA(Phe) to preserve its L-shaped higher-order structure.