Hydration and structure of hemiprotonated polycytidylic acid in films

Structural transitions of poly(rC)-Ka+ in humid films with different water content were studied by infrared spectroscopy and piezogravimetry. From analysis of the hydration isotherms and the dependence of spectral parameters (frequencies and intensities of the main bands) on n the hydration sites of the polynucleotide were determined (C2O, O4', N4H2, N1, PO2-, C2'OH). It was found that the transition of the polynucleotide from the unordered state to a double-stranded complex poly(rC+).poly(rC) occurs in the interval of n from 2 to 8. The value n = 8 corresponds to the total hydration of poly(rC). A model of hydration of poly(rC+).poly(rC) based on the experimental results and known X-ray parameters of this double helix complex is proposed. The most important feature of the model is the presence of single water bridges between PO2(-)-groups in the first hydration shell of each chain and triple water bridges between O4', N4H2 and C2'OH- atomic groups of opposite chains. The experimental results obtained and the proposed structure of hydration environment of poly(rC+).poly(rC) suggest that the stabilization of this complex is stabilized by the intra- and inter-chain water bridges and hydrogen bonds between pairs of cytosine bases.     

500-MHz 1H NMR study of poly(dG).poly(dC) in solution using one-dimensional nuclear Overhauser effect

Secondary structures of poly(dG).poly(dC) and poly(dG).poly(dm5C) in solution are determined by nuclear Overhauser effect (NOE) measurements on GH8-deuterated and -nondeuterated DNAs with low presaturation pulse lengths (10-25 ms) and low-power and prolonged accumulations in the range of 50,000-72,000 scans. Under these conditions, the NOE difference spectra were free from diffusion. Primary NOEs between base protons GH8/CH6 and sugar protons H1', H2'/H2', and H3' suggest that in poly(dG).poly(dC) both guanine and cytosine nucleotides adopt a C3'-endo, low anti X = 200-220 degrees conformation. Computer modeling of the NOE data enable identification for the first time, in terms of the geometry of the nucleotide repeat, handedness, and helix geometry, of the structure of poly(dG).poly(dC) to be the A form, and the derived structure for the polymer duplex is very close to the single crystal structure of the double-helical d-GGGGCCCC [McCall, M., Brown, T., & Kennard, O. (1985) J. Mol. Biol. 183, 385-396]. Similar nuclear Overhauser effect data on poly(dG).poly(dm5C) revealed that G and m5C adopt a C2'endo, anti X = 240-260 degrees conformation, which indicates that this DNA exhibits the B form in solution. In summary, the results presented in this paper demonstrate that methylation of cytosines in poly(dG).poly(dC) causes A----B transition in the molecule.     

A solid-state deuterium NMR investigation of conformation and order in magnetically oriented [d(CGCGAATTCGCG)]2

Solid-state deuterium NMR has been used to investigate the oriented liquid crystal phase of the hydrated oligonucleotide [d(CGCGAATTCGCG)]2. Previous investigations have shown that the helix axis is aligned perpendicular to the magnetic field, while at reduced temperatures motion about the helix axis is eliminated. Synthetic oligonucleotide samples incorporating different labeled nucleosides, [2"-2H]-2'-deoxyadenosine, [methyl-2H]thymidine, [8-2H]-2'-deoxyguanosine, and [8-2H]-2'-deoxyadenosine, permitted investigation of both the base and sugar conformation and ordering in the aligned phase. From line-shape analysis of the purine-labeled samples the orientation of the base C8 C-D bond with respect to the helix axis was determined to be theta = 90 degrees with a distribution of sigma total = 20 degrees, which is comparable to the orientation of theta = 90 degrees, sigma total = 15 degrees, with an oriented fraction P = 0.7 found for the C3 symmetry axis of the methyl-labeled dodecamer. The orientation of the sugar 2" C-D bond with respect to the helix axis is theta = 22 degrees with a distribution of sigma total = 15 degrees in agreement with the expected C2'-endo sugar conformation. The fraction of C3'-endo was also investigated and from analysis of line shape cannot exceed 20%. These results, though preliminary in nature, illustrate the application of this aligned phase for structural investigations.     

Poly(2-amino-8-methyladenylic acid). Competing structural and energetic effects of substituents

The ribopolynucleotide poly(2-amino-8-methyladenylic acid), (r2NH2(8)MeA)n, has been synthesized, and its physical and chemical properties have been examined. The study reveals competing effects on these properties of the 2-NH2 and 8-Me substituents. In marked contrast to the analogous (r8MeA)n, the new polymer readily interacts to form double helixes with complementary pyrimidine polynucleotides. Triple helixes are not formed. The 8-Me group is strongly destabilizing for helix formation (delta Tm approximately 65 degrees C), presumably by favoring a syn conformation, which blocks heteroduplex formation with ribohomopolymers. The 2-NH2 substituent stabilizes helixes in the ribo series by about 30 degrees C in Tm by forming a third interbase hydrogen bond. We suggest that the free energy from the 2-NH2 interaction drives the syn-anti equilibrium to the purine polymer to the anti form present in the double helix. CD spectra of the homopolymers (r2NH2A)n and (r2NH2(8)MeA)n are completely different, reflecting major differences of conformation. The double helixes formed by these polymers with (rT)n and (rBrU)n, on the other hand, have closely similar CD spectra, supporting our proposal of a major change in conformation of (2NH2(8)MeA)n on going from single strand to double helix.     

Spectroscopic studies on the structure of poly(8-bromoadenylic acid): Effect of glycosidic torsion angle on the conformation and flexibility in polyribonucleotides

The helix–coil transition and conformational structure of poly(8-bromoadenylic acid) [poly(8BrA)] have been investigated using ¹H- and ¹³C-nmr, CD, and ir spectroscopy. The results have been compared with the structure of the related 5′-mono- and polynucleotides. The chemical shifts of H(2′), H(3′), C(2′), and C(3′) nmr signals show an interesting correlation with both the puckering of ribose ring and glycosidic bond torsion angle. Poly(8BrA) shows an upfield shift of the C(3′) signal and a downfield shift of the H(3′) signal compared to the chemical shifts in poly(A). These shifts are consistent with a C(3′) endo-syn conformation for poly(8BrA). A similar effect has been reported previously and is also observed here on the C(2′) and H(2′) signals when the preferred conformation is C(2′)endo-syn (e.g., in 5′-8BrAMP). The chemical-shift parameters thus act as a probe for studying syn ? anti and N ? S equilibria in solutions. The three-bond ¹H-′¹³C coupling constants between H(1′) and C(8) and C(4) have been measured in poly(8BrA) and 5′-8BrAMP and their structural implications have been discussed. The observed preference of a C(3′)endo-syn conformation for poly(8BrA), coupled with other evidence, throws doubt on the validity of a correlation previously reported whereby a syn conformation is associated with a C(2′)endo ribose pucker. The backbone conformation of randomly coiled poly(8BrA) is very similar to the structures found in polyribonucleotides: poly(A) and poly(U). All three polymers show strong preferences for the backbone angles found in RNA helices. The CD spectrum of poly(8BrA) has a striking relationship to that of poly(A). The signs of all extrema are inverted, and the magnitudes are related by a constant factor. We suggest that these differences result from a change in the angle between coupled transition moment vectors in the two polymers. Infrared spectra of poly(8BrA) in H₂O and D₂O solution are reported for the frequency range below 1400 cm^?1. The antisymmetric >PO stretching vibration is observed at an unusually low frequency in the helix (1214 cm^?1). The symmetric >PO stretch occurs at ～1095 cm^?1 but is not resolved from a ring vibration near this frequency. A conformationally sensitive band, characteristic of helical RNA structures, is observed at 817 cm^?1 and disappears when the helix is melted. This observation confirms the conclusion that ordered poly(8BrA) has a regular helical structure with an RNA backbone conformation. A stereochemical explanation is provided for the failure of poly(8BrA) (or other syn polymers) to form double helices with anti-polyribonucleotides.     

Plant prolyl hydroxylase recognizes poly(L-proline) II helix

Substrate specificity of a prolyl hydroxylase from Vinca rosea suspension-cultured cells was studied using synthetic oligo(L-proline)s and their t-butyloxycarbonyl derivatives (Pron and Boc-Pron; n = 2-8) as peptidyl substrates. All peptides with a residual number of 5 or greater served as substrates in the enzyme reaction at 30 degrees C, after the preincubation of the enzyme and peptides at 0 degrees C prior to addition of cofactors and cosubstrate. Under the same conditions, the hydroxylation of Pro5 reached a plateau within 10 min, but that of Boc-Pro8 and poly(L-proline) increased linearly up to 40 min. If the preincubation temperature was raised to 30 degrees C, only Pro5 among the peptides was unable to serve as a substrate. The optimum temperature of the enzyme was 30 degrees C toward Boc-Pro8 and poly(L-proline) but it decreased to 15 degrees C using Pro5. These data suggest that the enzyme can bind Pro5 only at low temperature. Poly(L-proline) and Boc-Pron (n greater than or equal to 5) in aqueous solution are known to have a left-handed helical structure (poly(L-proline) II helix). Moreover, Pro5 was indicated as forming this helix below 10 degrees C. Accordingly, the enzyme recognizes the poly(L-proline) II helix, that is, the secondary structure of a substrate rather than the primary structure.     

An unusual C-H...O hydrogen bond mediated reversal of polypeptide chain direction in a synthetic peptide helix

An unusual C-terminal conformation has been detected in a synthetic decapeptide designed to analyze the stereochemistry of helix termination in polypeptides. The crystal structure of the decapeptide Boc-Leu-Aib-Val-Ala-Leu-Aib-Val-(D)Ala-(D)Leu-Aib-OMe reveals a helical segment spanning residues 1-7 and helix termination by formation of a Schellman motif, generated by (D)Ala(8) adopting the left-handed helical (alpha(L)) conformation. The extended conformation at (D)Leu(9) results in a compact folded structure, stabilized by a potentially strong C-H. O hydrogen bond between Ala(4) C(alpha)H and (D)Leu(9) CO. The parameters for C-H. O interaction are Ala(4) C(alpha)H. O=C (D)Leu(9) distance 3.27 A, C(alpha)-H. O angle 176 degrees, and O. H(alpha) distance 2.29 A. This structure suggests that insertion of contiguous D-residues may provide a handle for the generation of designed structures containing more than one helical segment folded in a compact manner.     

1H NMR study of an ethidium dimer poly(dA-dT) complex: evidence of a transition between bis and monointercalation

Comparative 1H NMR and optical studies of the interaction between poly(dA-dT), ethidium bromide (Et) and ethidium dimer (Et2) in 0.7 M NaCl are reported as a function of the temperature. Denaturation of the complexes followed at both polynucleotide and drug levels leads to a biphasic melting process for poly(dA-dT) complexed with ethidium dimer (t1/2 = 75 degrees C; 93 degrees C) but a monophasic one in poly(dA-dT): ethidium bromide complex (t1/2 = 74 degrees C). In both cases drug signals exhibit monophasic thermal dependence (Et = 81 degrees C; Et2 = 95 degrees C). Evidence is presented showing that the ethidium dimer bisintercalates into poly(dA-dT) in high salt, based on the observation that i) dimer and monomer ring protons exhibit similar upfield shifts upon DNA binding, ii) upfield shifts of DNA sugar protons are twice as large with the dimer than with ethidium bromide. Comparison between native DNA fraction and bound drug fraction indicates that ethidium covers, n = 2.5-3 base pairs. The dimer bisintercalates and covers, n = 5.7 base pairs when the helix fraction is high but as the number of available sites decreases the binding mode changes and the drug monointercalates (n = 2.9).     

Interaction of transition metal ions with Z form poly d(A-C).poly d(G-T) and poly d(A-T) studied by I.R. spectroscopy.

Interactions between Ni2+, Co2+ and purine bases have been studied by I.R. spectroscopy in the case of double stranded regularly alternating purine-pyrimidine polynucleotides poly d(A-T), poly d(A-C).poly d(G-T) and poly d(G-C). The spectra of polynucleotide films have been recorded in hydration and salt content conditions which correspond to the obtention of the classical right-handed (A,B) and left-handed (Z) helical conformations. Selective deuteration of the 8C site of purines has been obtained and is used to detect interactions between the transition metal ions and the adenine or guanine bases. The spectral region between 1500 and 1250 cm-1 corresponding to base in-plane vibrations and involving also the glycosidic linkage torsion is discussed in detail. The selective interaction between the transition metal ion and the 7N site of the purine base is considered to be partly responsible for the stabilization of the base in a syn conformation, which favours the adoption by the polynucleotide (poly d(G-C), poly d(A-C).poly d(G-T) or poly d(A-T)) of a Z type conformation.     

Crystal structure of the topoisomerase II poison 9-amino-[N-(2-dimethylamino)ethyl]acridine-4-carboxamide bound to the DNA hexanucleotide d(CGTACG)2.

The structure of the complex formed between d(CGTACG)(2) and the antitumor agent 9-amino-[N-(2-dimethylamino)ethyl]acridine-4-carboxamide has been solved to a resolution of 1.6 A using X-ray crystallography. The complex crystallized in space group P6(4) with unit cell dimensions a = b = 30.2 A and c = 39.7 A, alpha = beta = 90 degrees, gamma = 120 degrees. The asymmetric unit contains a single strand of DNA, 1. 5 drug molecules, and 29 water molecules. The final structure has an overall R factor of 19.3%. A drug molecule intercalates between each of the CpG dinucleotide steps with its side chain lying in the major groove, and the protonated dimethylamino group partially occupies positions close to ( approximately 3.0 A) the N7 and O6 atoms of guanine G2. A water molecule forms bridging hydrogen bonds between the 4-carboxamide NH and the phosphate group of the same guanine. Sugar rings adopt the C2'-endo conformation except for cytosine C1 which moves to C3'-endo, thereby preventing steric collision between its C2' methylene group and the intercalated acridine ring. The intercalation cavity is opened by rotations of the main chain torsion angles alpha and gamma at guanines G2 and G6. Intercalation perturbs helix winding throughout the hexanucleotide compared to B-DNA, steps 1 and 2 being unwound by 8 degrees and 12 degrees, respectively, whereas the central TpA step is overwound by 17 degrees. An additional drug molecule, lying with the 2-fold axis in the plane of the acridine ring, is located at the end of each DNA helix, linking it to the next duplex to form a continuously stacked structure. The protonated N,N-dimethylamino group of this "end-stacked" drug hydrogen bonds to the N7 atom of guanine G6. In both drug molecules, the 4-carboxamide group is internally hydrogen bonded to the protonated N-10 atom of the acridine ring. The structure of the intercalated complex enables a rationalization of the known structure-activity relationships for inhibition of topoisomerase II activity, cytotoxicity, and DNA-binding kinetics for 9-aminoacridine-4-carboxamides.     

Helix-forming tendencies of amino acids depend on the restrictions of side-chain rotamer conformations: crystal structure of the tripeptide GAI in two crystalline forms.

In our attempts to design crystalline alpha-helical peptides, we synthesized and crystallized GAI (C11H21N3O4) in two crystal forms, GAI1 and GAI2. Form 1 (GAI1) Gly-L-Ala-L-Ile (C11H21N3O4.3H2O) crystals are monoclinic, space group P2(1) with a = 8.171(2), b = 6.072(4), c = 16.443(4) A, beta = 101.24(2) degrees, V = 800 A3, Dc = 1.300 g cm-3 and Z = 2, R = 0.081 for 482 reflections. Form 2 (GAI2) Gly-L-Ala-L-Ile (C11H21N3O4.1/2H2O) is triclinic, space group P1 with a = 5.830(1), b = 8.832(2), c = 15.008(2) A, alpha = 102.88(1), beta = 101.16(2), gamma = 70.72(2) degrees, V = 705 A3, Z = 2, Dc = 1.264 g cm-3, R = 0.04 for 2582 reflections. GAI1 is isomorphous with GAV and forms a helix, whereas GAI2 does not. In GAI1, the tripeptide molecule is held in a near helical conformation by a water molecule that bridges the NH3+ and COO- groups, and acts as the fourth residue needed to complete the turn by forming two hydrogen bonds. Two other water molecules form intermolecular hydrogen bonds in stabilizing the helical structure so that the end result is a column of molecules that looks like an incipient alpha-helix. GAI2 imitates a cyclic peptide and traps a water molecule. The conformation angles chi 11 and chi 12 for the side chain are (-63.7 degrees, 171.1 degrees) for the helical GAI1, and (-65.1 degrees, 58.6 degrees) and (-65.0 degrees, 58.9 degrees) for the two independent nonhelical molecules in GAI2; in GAI1, both the C gamma atoms point away from the helix, whereas in GAI2 the C gamma atom with the g+ conformation points inward to the helix and causes sterical interaction with atoms in the adjacent peptide plane. From these results, it is clear that the helix-forming tendencies of amino acids correlate with the restrictions of side-chain rotamer conformations. Both the peptide units in GAI1 are trans and show significant deviation from planarity [omega 1 = -168(1) degrees; omega 2 = -171(1) degrees] whereas both the peptide units in both the molecules A and B in GAI2 do not show significant deviation from planarity [omega 1 = 179.3(3) degrees; omega 2 = -179.3(3) degrees for molecule A and omega 1 = 179.5(3) degrees; omega 2 = -179.4(3) degrees for molecule B], indicating that the peptide planes in these incipient alpha-helical peptides are considerably bent.     

Structure of d(T)n.d(A)n.d(T)n: the DNA triple helix has B-form geometry with C2'-endo sugar pucker.

The polynucleotide helix d(T)n.d(A)n.d(T)n is the only deoxypolynucleotide triple helix for which a structure has been published, and it is generally assumed as the structural basis for studies of DNA triplexes. The helix has been assigned to an A-form conformation with C3'-endo sugar pucker by Arnott and Selsing [1974; cf. Arnott et al. (1976)]. We show here by infrared spectroscopy in D2O solution that the helix is instead B-form and that the sugar pucker is in the C2'-endo region. Distamycin A, which binds only to B-form and not to A-form helices, binds to the triple helix without displacement of the third strand, as demonstrated by CD spectroscopy and gel electrophoresis. Molecular modeling shows that a stereochemically satisfactory structure can be build using C2'-endo sugars and a displacement of the Watson-Crick base-pair center from the helix axis of 2.5 A. Helical constraints of rise per residue (h = 3.26 A) and residues per turn (n = 12) were taken from fiber diffraction experiments of Arnott and Selsing (1974). The conformational torsion angles are in the standard B-form range, and there are no short contacts. In contrast, we were unable to construct a stereochemically allowed model with A-form geometry and C3'-endo sugars. Arnott et al. (1976) observed that their model had short contacts (e.g., 2.3 A between the phosphate-dependent oxygen on the A strand and O2 in the Hoogsteen-paired thymine strand) which are generally known to be outside the allowed range.(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

Structural and conformational analysis of pentostatin (2'-deoxycoformycin), a potent inhibitor of adenosine deaminase

X-ray, NMR and molecular mechanics studies on pentostatin (C11H16N4O4), a potent inhibitor of the enzyme adenosine deaminase, have been carried out to study the structure and conformation. The crystals belong to the monoclinic space group P21 with the cell dimensions of a = 4.960(1), b = 10.746(3), c = 11.279(4)A, beta = 101.18(2) degrees and Z = 2. The structure was solved by direct methods and difference Fourier methods and refined to an R value of 0.047 for 997 reflections. The trihydrodiazepine ring is nonplanar and adopts a distorted sofa conformation with C(7) deviated from the mean plane by 0.66A. The deoxyribose ring adopts a C3'-endo conformation, different from coformycin where the sugar has a C2'-endo conformation. The observed glycosidic torsion angle (chi = -119.5 degrees) is in the anti range. The conformation about the C(4')-C(5') bond is gauche+. The conformation of the molecule is compared with that of coformycin and 2-azacoformycin. 1 and 2D NMR studies have been carried out and the dihedral angles obtained from coupling constants have been compared with those obtained from the crystal structure. The conformation of deoxyribose in solution is approximately 70% S and 30% N. Molecular mechanics studies were performed to obtain the energy minimized conformation, which is compared with X-ray and NMR results.     

Circular dichroism studies of the interaction of a limited hydrolysate of T4 gene 32 protein with T4 DNA and poly[d(A-T)].poly[d(A-T)].

gp32 I is a protein with a molecular weight of 27 000. It is obtained by limited hydrolysis of T4 gene 32 coded protein, which is one of the DNA melting proteins. gp32 I itself appears to be also a melting protein. It denatures poly[d(A-T)].poly[d(A-T)] and T4 DNA at temperatures far (50-60 degrees C) below their regular melting temperatures. Under similar conditions gp32 I will denature poly[d(A-T).poly[d(A-T)] at temperatures approximately 12 degrees C lower than those measured for the intact gp32 denaturation. For T4 DNA gp32 shows no melting behavior while gp32 I shows considerable denaturation (i.e., hyperchromicity) even at 1 degree C. In this paper the denaturation of poly[d(A-T)].poly[d(A-T)] and T4 DNA by gp32 I is studied by means of circular dichroism. It appears that gp32 I forms a complex with poly[d(A-T)]. The conformation of the polynucleotide in the complex is equal to that of one strand of the double-stranded polymer in 6 M LiCl. In the gp32 I DNA complex formed upon denaturation of T4 DNA, the single-stranded DNA molecule has the same conformation as one strand of the double-strand T4 DNA molecule in the C-DNA conformation.     

Spatial configuration of ordered polynucleotide chains. V. Conformational energy estimates of helical structure

Semiempirical potential energy functional used previously to account successfully for the mean-square unperturbed dimensions and nmr coupling constants of randomly coiling polynucleotides are used, after modifications, to account for base stacking and interstrand hydrogen bonding, and to evaluate the conformational energies of single- and double-stranded polynucleotide helices. Attention is focused upon the variety of A-genus helices with local backbone conformations resembling the known double-helical structures of RNA. Distinct structural differences between single- and double-stranded helices are predicted from the energy calculations. A second point of interest is the apparent failure of two conformationally identical left-handed polynucleotide chains to form a left-handed duplex. The third major observation of the study is the wide morphological variety of theoreticaly allowed right-handed polynucleotide duplexes. In addition to the familiar double helix stabilized by horizontal base stacking and hydrogen bonding, an unusual vertical double helix is predicted to form between complementary bases fixed in the unusual but not energetically forbidden high anti glycosyl conformation. Experimental results bearing upon the theoretical predictions are discussed.     

Helical epitope of the group B meningococcal alpha(2-8)-linked sialic acid polysaccharide.

The immunological properties of the group B meningococcal alpha(2-8)-linked sialic acid polysaccharide have been rationalized in terms of a model where the random coil nature of the polymer can be described by the presence of local helices. The conformational versatility of the alpha NeuAc(2-8)alpha NeuAc linkage has been explored by NMR studies at 600 MHz in conjunction with potential energy calculations for colominic acid, an alpha(2-8)NeuAc polymer, and the trisaccharide alpha NeuAc(2-8)alpha NeuAc(2-8)beta NeuAc. Potential energy calculations were used to estimate the energetically favorable conformers and to describe the wide range of helices which the polymer can adopt. No unique conformer was found to satisfy all NMR constraints, and only ensemble averaged nuclear Overhauser enhancements could correctly simulate the experimental data. Conformational differences between the polymer and the trisaccharide could be best explained in terms of slight changes in the relative distribution of conformers in solution. Similar helical parameters for the alpha(2-8)NeuAc polymer and poly(A) were proposed as the basis for their cross-reactivity to a monoclonal antibody IgMNOV. The unusual length dependency for binding of oligosaccharide to group B specific antibodies was postulated to arise from the recognition of a high-order local helix with an extended conformation which was not highly populated in solution.     

Reversible helix/coil transitions of left-handed Z-DNA structures. Comparison of the thermodynamic properties of poly(dG).poly(dC), poly[d(G-C)].poly[d(G-C)], and poly(dG-m5dC).poly(dG-m5dC)

In contrast to poly(dG).poly(dC), which remains in the B-DNA conformation under all experimental conditions the polynucleotides with the strictly alternating guanine/cytosine or guanine/5'-methylcytosine sequences can change from the classical right-handed B-DNA structure to the left-handed Z-DNA structure when certain experimental conditions such as ionic strength or solvent composition are fulfilled. Up to now the investigation of the helix/coil transition of left-handed DNA structures was not possible because the transition temperature exceeds 98 degrees C. By applying moderate external pressure to the surface of the aqueous polymer solution in the sample cell the boiling point of the solvent water is shifted up the temperature scale without shifting the transition temperature, so that we can measure the helix/coil transition of the polynucleotides at all experimental conditions applied. It can thus be shown that the Z-DNA/coil transition is cooperative and reversible. The Tm is 125 degrees C for poly(dG-m5dC).poly(dG-m5dC) in 2mM Mg2+, 50mM Na+, pH 7.2 and 115 degrees c for poly[d(G-C)].poly[d(G-C)] in 3.04M Na+. The transition enthalpy per base pair was determined by the help of an adiabatic scanning microcalorimeter.     

Interactions between an anthracycline antibiotic and DNA: molecular structure of daunomycin complexed to d(CpGpTpApCpG) at 1.2-A resolution

The crystal structure of a daunomycin-d(CGTACG) complex has been solved by X-ray diffraction analysis and refined to a final R factor of 0.175 at 1.2-A resolution. The crystals are in a tetragonal crystal system with space group P4(1)2(1)2 and cell dimensions of a = b = 27.86 A and c = 52.72 A. The self-complementary DNA forms a six base pair right-handed double helix with two daunomycin molecules intercalated in the d(CpG) sequences at either end of the helix. Daunomycin in the complex has a conformation different from that of daunomycin alone. The daunomycin aglycon chromophore is oriented at right angles to the long dimension of the DNA base pairs, and the cyclohexene ring A rests in the minor groove of the double helix. Substituents on this ring have hydrogen-bonding interactions to the base pairs above and below the intercalation site. O9 hydroxyl group of the daunomycin forms two hydrogen bonds with N3 and N2 of an adjacent guanine base. Two bridging water molecules between the drug and DNA stabilize the complex in the minor groove. In the major groove, a hydrated sodium ion is coordinated to N7 of the terminal guanine and the O4 and O5 of daunomycin with a distorted octahedral geometry. The amino sugar lies in the minor groove without bonding to the DNA. The DNA double helix is distorted with an asymmetrical rearrangement of the backbone conformation surrounding the intercalator drug. The sugar puckers are C1,C2'-endo, G2,C1'-endo, C11,C1'-endo, and G12,C3'-exo. Only the C1 residue has a normal anti-glycosyl torsion angle (chi = -154 degrees), while the other three residues are all in the high anti range (average chi = -86 degrees). This structure allows us to identify three principal functional components of anthracycline antibiotics: the intercalator (rings B-D), the anchoring functions associated with ring A, and the amino sugar. The structure-function relationships of daunomycin binding to DNA as well as other related anticancer drugs are discussed.     

On the recognition of helical RNA by cobra venom V1 nuclease

The V1 nuclease from cobra venom preferentially hydrolyzes double helical RNA and has been used extensively for detecting RNA secondary structure. To increase the utility of this enzyme as an RNA structure probe, we have investigated its properties and substrate specificity, using assays for polynucleotide hydrolysis based on fluorescent polynucleotide derivatives. Enzymatic activity requires both Na+ and Mg2+, with optima at 100 and 0.3 mM, respectively. From the sharp decrease in enzyme activity above 100 mM Na+ we estimate that 3-4 ionic interactions between the protein and polynucleotide phosphates take place. Analysis of products remaining after extensive V1 digestion also shows that the minimum size substrate is 4-6 nucleotides long. Helical RNAs and DNAs have Michaelis constants a factor of 3-10 times lower than most single-stranded RNAs. However, poly(epsilon A) has a Michaelis constant equal to the best synthetic double helices tested and is hydrolyzed at a rate comparable to helical RNA. The major V1 cutting sites in yeast tRNAPhe have Michaelis constants lower than any synthetic polymers. These data suggest that V1 nuclease recognizes any 4-6-nucleotide segment of polynucleotide backbone with an approximately helical conformation, but does not require that the bases be paired in a helix. A few single-stranded V1 cleavage sites are known in tRNA and rRNA, and their structures are consistent with the suggested V1 recognition site.