Formation of psi (+) and psi (-) DNA

DNA molecules can be organized into ordered aggregates of opposite handedness by complexation with polylysine and other polypeptides; we have investigated the conditions under which ψ(+) and ψ(?) structures are produced with double-helical synthetic polynucleotides. Both poly(dGdC)·poly(dGdC) and poly(dAdT)·poly(dAdT) readily form ψ(?) structures with polylysine, although the method of preparation can alter the CD spectra. The GC copolymer, which is more susceptible to conversion into A or Z conformers, forms ψ(+) structures with lysine–alanine copolypeptides more readily than the AT copolymer. Nucleotide base modifications that favor the Z structure, such as bromination and methylation, also favor ψ(+) formation, and the Co(NH₃)₆Cl₃ reagent that readily induces the Z structure also leads to ψ(+). Thus, the production of the ψ(+) structure seems to be frequently correlated with susceptibility to A or Z formation, although there are some cases in which the B conformer also leads to ψ(+). Polyethylene glycol generally produces a ψ(?) structure; the differentiation between ψ(+) and ψ(?) structures seems to require electrically charged polymers.     

Psi compaction of poly[d(AT)].poly[d(AT)]

The compaction of poly[d(A–T)] · poly[d(A–T)] by Co(III) is accompanied by the formation of ψ(+)- and ψ(-)-structures. The chirality of the ψ-structure depends on the Co(III) concentration, ionic strength, temperature, pH, and the chain length of the polymer. The two forms can be readily interconverted by manipulating these factors. Phase diagrams have been constructed that demonstrate the regions of stability of the enantiomers as a function of two variables, while other factors are held constant. At critical points in the phase diagram the two forms are in such unstable equilibrium that mechanical motion will cause ψ(+) ? ψ(-) interconversion. The formation of both ψ(+)- and ψ(-)-structures by the action of Co(III) on poly[d(A–T)] · poly[d(A–T)] contrasts markedly with the behavior of poly[d(G–C)] · poly[d(G–C)] in similar circumstances by forming only the ψ(+)-structure and that of native DNA to produce no ψ at all. Thus the base sequence is important in determining the structure of chirally associated DNA molecules.     

Thermodynamics of the B to Z transition in poly(dGdC)

The thermodynamics of the B to Z transition in poly(dGdC) was examined by differential scanning calorimetry, temperature-dependent absorbance spectroscopy, and CD spectroscopy. In a buffer containing 1 mM Na cacodylate, 1 mM MgCl₂, pH 6.3, the B to Z transition is centered at 76.4°C, and is characterized by ΔH_cal = 2.02 kcal (mol base pair)^?1 and a cooperative unit of 150 base pairs (bp). The t_m of this transition is independent of both polynucleotide and Mg²⁺ concentrations. A second transition, with ΔH_cal = 2.90 cal (mol bp)^?1, follows the B to Z conversion, the t_m of which is dependent upon both the polynucleotide and the Mg²⁺ concentrations. Turbidity changes are concomitant with the second transition, indicative of DNA aggregation. CD spectra recorded at a temperature above the second transition are similar to those reported for ψ(–)-DNA. Both the B to Z transition and the aggregation reaction are fully and rapidly reversible in calorimetric experiments. The helix to coil transition under these solution conditions is centered at 126°C, and is characterized by ΔH_cal = 12.4 kcal (mol bp)^?1 and a cooperative unit of 290 bp. In 5 mM MgCl₂, a single transition is seen centered at 75.5°C, characterized by ΔH_cal = 2.82 kcal (mol bp)^?1 and a cooperative unit of 430 bp. This transition is not readily reversible in calorimetric experiments. Changes in turbidity are coincident with the transition, and CD spectra at a temperature just above the transition are characteristic of ψ(–)-DNA. A transition at 124.9°C is seen under these solution conditions, with ΔH_cal = 10.0 kcal (mol bp)^?1 and which requires a complex three-step reaction mechanism to approximate the experimental excess heat capacity curve. Our results provide a direct measure of the thermodynamics of the B to Z transition, and indicate that Z-DNA is an intermediate in the formation of the ψ-(–) aggregate under these solution conditions.     

Carcinogen-Nucleic Acid Interactions: Equilibrium Binding Studies of Aflatoxins B1 and B2 with DNA and the Oligodeoxynucleotide d(ATGCAT)2

Abstract

Equilibrium binding is believed to play an important role in directing the subsequent covalent attachment of many carcinogens to DNA. We have utilized UV spectroscopy to examine the non-covalent interactions of aflatoxin B₁ and B₂ with calf thymus DNA, poly(dAdT):poly(dAdT), and poly(dGdC):poly(dGdC), and have utilized NMR spectroscopy to examine non-covalent interactions of aflatoxin B₂ with the oligodeoxynucleotide d(ATGCAT)₂. UV-VIS binding isotherms suggest a greater binding affinity for calf thymus DNA and poly(dAdT):poly(dAdT) than for poly(dGdC):poly(dGdC). Scatchard analysis of aflatoxin B₁ binding to calf thymus DNA in 0.1 M NaCl buffer indicates that binding of the carcinogen at levels of bound aflatoxin ? 1 carcinogen per 200 base pairs occurs with positive cooperativity. The cooperative binding effect is dependent on the ionic strength of the medium; when the NaCl concentration is reduced to 0.01 M, positive cooperativity is observed at carcinogen levels ? 1 carcinogen per 500 base pairs. The Scatchard data may be fit using a “two-site” binding model [L.S. Rosenberg, M J. Carvlin, and T.R. Krugh, Biochemistry 25, 1002–1008 (1986)]. This model assumes two independent sets of binding sites on the DNA lattice, one a high affinity site which binds the carcinogen with positive cooperativity, the second consisting of lower affinity binding sites to which non-specific binding occurs. NMR analysis of aflatoxin B₂ binding to d(ATGCAT)₂ indicates that the aflatoxin B₂/oligodeoxynucleotide complex is in fast exchange on the NMR time scale. Upfield chemical shifts of 0.1–0.5 ppm are observed for the aflatoxin B₂ 4-OCH₃, H5, and H6a protons. Much smaller chemical shift changes ? 0.06 ppm) are observed for the oligodeoxynucleotide protons. The greatest effect for the oligodeoxynucleotide protons is observed for the adenine H2 protons, located in the minor groove. Nonselective T₁ experiments demonstrate a 15–25 % decrease in the relaxation time for the adenine H2 protons when aflatoxin B₂ is added to the solution. This result suggests that aflatoxin B₂ protons in the bound state may be in close proximity to these protons, providing a source of dipolar relaxation. Further experiments are in progress to probe the nature of the aflatoxin B₁ and B₂ complexes with polymeric DNA and oligodeoxynucleotides, and to establish the relationship between the non-covalent DNA-carcinogen complexes observed in these experiments, and covalent aflatoxin B₁,-guanine N7 DNA adducts.     

Methylated Polyl(L-lysine): Conformational Effects and Interactions with Polynucleotides

Abstract

Methylated lysine, arginine and histidine residues are found in a number of proteins (for example, histones, non-histone chromosomal proteins, ribosomal proteins, calmodulin, cytochrome C, etc.). We are studying the effects of methylation on the conformations of poly(lysine) and of the effects of methylation of poly(lysine) and poly(arginine) on interactions with polynucleotides. The conformational properties of e-amino-methylated poly(lysine) differ from those of unmodified poly(lysine). Methylation increases resistance to thermally- induced and NaCl-induced changes in the CD spectrum. Guanidinium chloride increases (proportional to the degree of methylation) the extent of approach to the conformation in dispute as to its being a random coil or an extended helix. Methylation enhances aggregation in the helix-inducing solvent 0.5 M Ca(ClO₄)₂. With increasing methylation of poly(lysine), the conformation in dodecyl sulfate changes from β, to 50% α, to random coil at the maximum methylation.

Increasing methylation of poly(lysine) weakens the interaction with polynucleotides in respect to dissociation by salt, linearly with methyl content. Complexes of (dAdT)_n·(dAdT)_n with the polypeptides are increasingly stabilized to heat denaturation by progressive methylation. However, with a series of synthetic double-stranded RNA's and DNA's a more complex situation exists, Tm increasing or decreasing, depending on the base composition, sequence and type of sugar. Methylation of poly(lysine) and poly(arginine) can have opposite effects on Tm based on results with complexes with (dI)_n·(dC)_n. Methylated poly(lysine) affects the CD spectrum of polynucleotides, in a manner dependent on base composition and sequence. In some cases large positive or negative ψ-spectra are induced, which, in the case of (dGdC)_n·(dGdC)_n, can be positive or negative depending on the degree of methylation of the polypeptide and the salt concentration.

It is suggested that the biological effects of methylated proteins may be evoked by salt changes in the cell cycle, and that methylation can affect local interactions with nucleic acids and larger scale structure, and interactions with lipids.     

Conformational Peculiarities of Polynucleotides with a Nonrandom Base Sequence According to the 1H→ 3H Exchange Rate in C8H Groups of Purinic Residues

Abstract

We have determined the ¹H→³H exchange rate constants between water and C8H groups of purinic residues of alternating polynucleotides poly(dA-dT)·poly(dA-dT), poly(dG-dC)·poly(dG- dC) and poly(dA-dC)·poly(dG-dT) as well as homopolynucleotides poly(dA)·poly(dT) and poly(dG)·poly(dC) in aqueous solutions with high-salt concentrations (3 M NaCl and 4–6 M CsF), in water-ethanol (60%) solution and in 0.15 M NaCl at 25°C. The rate constants for adenine (k_A) and guanine (k_G) of polynucleotides were compared with corresponding constants for E.coli DNA, dGMP nd dAMP at the same conditions. The relation between exchange rates and conformations of polynucleotides permits the study of their conformational peculiarities in solution.

Of three alternating polynucleotides examined in 0.15 M NaCl the exchange retardation was observed only for poly(dA-dT)·poly(dA-dT) as compared with that in B-DNA, which is in good agreement with the B-alternating “wrinkled” DNA model. The conformations of poly(dG-dC)·poly(dG-dC) and poly(dA-dC)·poly(dG-dT), according to the exchange data obtained, are within the B form. For homopolynucleotides in 0.15 M NaCl, the k_A value for poly(dA)·poly(dT) is nearly the same as k_A for B-DNA, which indicates the similarity of their conformations, whereas the k_G value for poly(dG)·poly(dC) is 1.7-fold lower in comparison with the k_G value in B-DNA. This seems to be connected with the existence of B? A conformation equilibrium for poly(dG)·poly(dC) in solution.

The increase of NaCl concentration to 3 M results in a B→Z transition in the case of poly(dG-dC)·poly(dG-dC) and in the shift of B?A equilibrium towards the A-form in the case of poly(dG)·poly(dC), as is evidenced by alterations of their K_G values. Poly(dA-dT)·poly(dA-dT) in 6 M CsF and poly(dA-dC)·poly(dG-dT) in 4.3 M CsF maintain their inherent conformations in 0.15 M NaCl in spite of the fact that they are characterised by the “X-type” CD-spectrum at these conditions. According to the exchange data the conformation of poly(dA)·poly(dT) in 6 M CsF corresponds to the “heteronomous” DNA model or some other structure with lower accessibility of C8H groups of adenylic residues.     

Recognition of left-handed Z-DNA of short unmodified oligonucleotides under physiological ionic strength conditions

The left-handed Z-DNA form of the short unmodified alternating guanine-cytosine oligonucleotides, 5′-(dGdC)₂₄ and 5′-(dGdC)₁₈, was selectively detected under physiological ionic strength and pH conditions using the anionic nickel(II) porphyrin, NiTPPS. No spectroscopic signal was observed for NiTPPS with any right-handed oligonucleotides under identical conditions. The 48mer 5′-(dGdC)₂₄ Z-form was detected at concentrations as low as 100 nM. The binding of NiTPPS to the B- and Z-oligonucleotides was studied quantitatively by UV-vis absorption and circular dichroism spectroscopies. NiTPPS was found to be a universal DNA binder, with binding affinity and geometry depending on the ionic composition of the solution, rather than on the DNA helical twist. This is the first example of a successful spectroscopic detection of the Z-DNA of short unmodified oligonucleotides under physiological pH and ionic strength conditions.     

Study of salt effects on adenosine–polyuridylic acid interaction

Complex formation between poly(U) and adenosine in solutions of salts that stabilize (Na₂SO₄), destabilize (NaClO₄), or have little effect on the water structure (NaCl), as well as the poly(U)·poly(A) interaction in NaClO₄, was studied by equilibrium dialysis and uv spectroscopy. At 3°C and neutral pH, Ado·2 poly(U) is formed in 1M NaCl and 0.33M Na₂SO₄. In NaClO₄ solutions under the same conditions, an Ado·poly(U) was found over the whole range of salt concentration investigated (10 mM?1M), which has not been previously observed under any conditions. The Ado-poly(U) was also found in a NaCl/NaClO₄ mixture, the transition from the triple- to the double-helical complex occurring within a narrow range of concentration of added NaClO₄. In the presence of 1M NaCl this transition is observed on adding as little as 10 mM NaClO₄, i.e., at a [ClO]/[Cl^?] ratio of about 1:100. However, when NaClO₄ is added to a 1M solution of the stabilizing salt Na₂SO₄, no transition occurs even at a [ClO]/[SO] ratio of 1:4. Investigation of melting curves and uv spectra has shown that in an equimolar mixture of the polynucleotides, only a double-helical poly(U)·poly(A) exists in 1M NaClO₄ at low temperatures; this also holds for 1M NaCl. This changes to a triple-helical 2 poly(U)·poly(A) and then dissociates as the temperature increases. At low temperatures and the poly(U)/poly(A) concentration ratio of 2:1, a mixture of 2 poly(U)·poly(A) and poly(U)·poly(A) was observed in 1M NaClO₄, in contrast to the case of 1M NaCl. Thus, sodium perchlorate, a strong destabilizer of water structure, promotes formation of double-helical complexes both in the polynucleotide–monomer and the polynucleotide–polynucleotide systems. Beginning with a sufficiently high ionic strength (μ ? 0.9), a further increase in the salt molarity results in an increase of the poly(U)·adenosine melting temperature in both stabilizing and neutral salts and a decrease in the destabilizing salt. In Na₂SO₄ concentrations higher than 1.2M Ado·2 poly(U) precipitates at room temperature. Analysis of the binding isotherms and melting profiles of the complexes between poly(U) and adenosine according to Hill's model shows that the cooperativity of binding, due to adenosine stacking on poly(U), increases in the order NaClO₄ < NaCl < Na₂SO₄. The free energy of adenosine stacking on the template is similar to that of hydrogen bonding between adenosine and poly(U) and ranges from ?1 to ?2 kcal/mol. The values of ΔH_t [the effective enthalpy of adenosine binding to poly(U) next to an occupied site, obtained from the relationship between complex melting temperature and free monomer concentration at the midpoint of the transition] are ?14.2, ?18.3, and ?16.8 kcal/mol for 1M solutions of NaClO₄, NaCl, and Na₂SO₄, respectively. The results indicate that the effects of anions of the salts studied are related to water structure alterations rather than to their direct interaction with the complexes between poly(U) and adenosine.     

Adaptation to Water Stress in Wheat

Three experiments were designed to investigate to what extent adaptation to water stress take place. Wheat (Triticum aestivum L. cv. Kolibri) was grown in water culture at constant temperature, air humidity, and light intensity. When the plants were 16 days old, the potential of the root medium (ψ_r) was lowered by 1 bar every second day by means of polyethyleneglycol 1500 down to ?4 or ?7 bar and then remained at these levels. As a control one experiment was grown at ?0.7 bar. By regression it was found that when ψ_r was lowered by I bar, osmotic potential in leaf (ψ_π) decreased 1.46 bar, and leaf water potential (ψ_t) 0.68 bar, which mean an increase of turgor of 0.78 bar. At the same time the leaf water content did fall 0.30 g per g dry matter. Specific transpiration rate increased significantly after ψ_r was kept constant, but the increase in area of fresh leaves was strongly reduced due to wilting of old leaves. After an “adaptation” period during which ψ_r remained at ?0.7, ?4, and ?7 bar, respectively, for at least 1 week. ψ_r was altered so as to cover the range from 0 to ?14 bar and ψ_π, ψ_r, transpiration and diffusion resistance in stomata (r_s) were measured. The levels of ψ_π and ψ₁ were lower (more negative) and turgor potential higher in plants grown at low ψ_r. The transpiration in pre-stressed plants showed less sensitivity to the alteration of ψ_r than in the non-stressed plants. The values of ψ_r at which r_s increased greatly, were found to be about ?13, ?15, and ?18 bar for plants grown at ?0.7, ?4, and ?7 bar, respectively.     

Binding properties of Ru(II) polypyridyl complexes with poly(U)·poly(A)*poly(U) triplex: the ancillary ligand effect on third-strand stabilization

The binding properties of [RuL₂(mip)]²⁺ {where L is 1,10-phenanthroline (phen) or 4,7-dimethyl-1,10-phenanthrollne (4,7-dmp) and mip is 2′-(3″,4″-methylenedioxyphenyl)imidazo[4′,5′-f][1,10]phenanthroline} with regard to the triplex RNA poly(U)·poly(A)*poly(U) were investigated using various biophysical techniques and quantum chemistry calculations. In comparison with [Ru(4,7-dmp)₂(mip)]²⁺, remarkably higher binding affinity of [Ru(phen)₂(mip)]²⁺ for the triplex RNA poly(U)·poly(A)*poly(U) was achieved by changing the ancillary ligands. The stabilization of the Hoogsteen-base-paired third strand was improved by about 10.9 °C by [Ru(phen)₂(mip)]²⁺ against 6.6 °C by [Ru(4,7-dmp)₂(mip)]²⁺. To the best of our knowledge, [Ru(phen)₂(mip)]²⁺ is the first metal complex able to raise the third-strand stabilization of poly(U)·poly(A)*poly(U) from 37.5 to 48.4 °C. The results reveal that the ancillary ligands have an important effect on third-strand stabilization of the triplex RNA poly(U)·poly(A)*poly(U) when metal complexes contain the same intercalative ligands.     

Left-handed Z-DNA Helices in Polymers,Restriction Fragments,and Recombinant Plasmids

Abstract

Studies on DNA polymers, restriction fragments, and recombinant plasmids have revealed the following: A) A family of left-handed DNA conformations exists for (dC-dG)_n·(dC-dG)_n. The observation of a particular conformation is dependent on the salt, the salt concentration and dehydrating agent. B) In sodium acetate solutions, (dC-dG)_n·(dC-dG)_n forms left-handed, ψ(+)-condensed structures as detected by Raman spectroscopy and circular dichroism. C) (dT-dG)_n·(dC-dA)_n undergoes a right-to-left-handed transition only when reacted with AAF and at high salt concentrations. D) Transitions observed for polymer DNAs also are observed for restriction fragments containing both (dC-dG)·(dC-dG) and (dT-dG)·(dC-dA) sequences, but the transitions in the fragments generally require higher salt concentrations than observed for the polymers. E) Studies with recombinant plasmids containing (dC-dG) sequences from 10 to 58 bp in length demonstrate that left-handed Z-DNA segments can exist contiguous to B-DNA segments. F) Negative supercoil density (σ≤ ?0.072) is sufficient to convert the (dC-dG) regions in those plasmids into left-handed structures under physiological ionic conditions (200 mM NaCl). G) The favorable free energy contribution of methyla- tion in stabilizing the Z form in fragments and plasmids is approximately offset by the unfavorable free energy contributions of the B/Z junctions. H) S₁ and BAL 31 nucleases recognize aberrant structural features at the confluence of the B and Z regions. I) Detailed mapping of S₁ nuclease cleavage on supercoiled plasmids shows that the nuclease sensitive regions extend over at least five to ten bp. J) Even though the (dT-dG)_n·(dC-dA)_n polymer requires base modification and high salt conditions to undergo the R?L transition, supercoiling (σ ?0.07) can supply enough energy to allow a plasmid containing the intervening sequence of a human fetal globin gene with (dT-dG)·(dC-dA) sequences to undergo a R?L transition.     

The binding of Mg++ ions to polyadenylate, polyuridylate, and their complexes

The binding of Mg ⁺⁺ to polyadenylate (poly A), Polyuridylate(poly U), and their complexes, poly (A + U) and poly (A + 2U), was studied by means of a technique in which the dye eriochrome black T is used to measure the concentration of free Mg^?. The apparent binding constant K_X = [MgN]/[Mg⁺⁺][N], N = site for Mg⁺⁺ binding (the phosphate group of the nucleotide), was found to decrease rapidly as the extent of binding increased and, at low extents of binding, as the concentration of Na^? increased in poly A, poly (A + U), and poly (A + 2U), and somewhat less so in poly U. K_x is generally in the range 10⁴ > K_X > 10². The cause of these dependences is apparently, primarily, the displacement of Na⁺ by Mg⁺⁺ in poly U and poly (A + U) on the basis of the similarity of extents of displacement measured in this work and those measured potentiometrically. was calculated and was found to approach zero as the concentration of Na⁺ increased. In poly U, poly (A + U), and poly (A + 2U) at low ΔH′ v.H. > 0, about + 2 kcal/“mole.” In poly A, also at low salt, ΔH′ v.H. ≈ ?4 kcal/“mol” for the initial binding of Mg⁺⁺, and increases to +2 kcal/“mol” at saturation. This enthalpic variation probably accounts for the anticooperativity in the binding of Mg⁺⁺ not ascribable to the displacement of Na⁺⁺.     

Importance of DNA conformation in the reaction with cis-dichlorodiammine platinum (II)

Cis-dichlorodiammine platinum (II) has been reacted with synthetic polynucleotides either in B or in Z conformation. The binding of cis-dichlorodiammine platinum (II) stabilizes the Z conformation when reacted with poly (dG-m⁵dC) ·poly (dG-m⁵dC) in the Z conformation as shown by circular dichroism and by the antibodies to Z-DNA. On the other hand, the binding of cis-dichlorodiammine platinum (II) stabilizes a new conformation when reacted with poly(dG-dC)·poly(dG-dC) or poly (dG-m⁵dC)·poly(dG-m5dC) in the B conformation. The antibodies to Z-DNA bind to these platinated polynucleotides. In rabbits, the injection of platinated poly (dG-dC) poly (dG-dC) induces the synthesis of antibodies which recognize Z-DNA. In low salt conditions, the circular dichroism spectra of these platinated polynucleotides differ from those of B-DNA or Z-DNA. The characteristic³¹P nuclear magnetic resonance spectrum of Z-DNA is not detected. It appears only at high ionic strength, as a component of a more complex spectrum.     

A search for the ideal type I β-turn

In 1968 C. Venkatachalam (Biopolymers, Vol. 6, pp. 1425–1436) predicted the ideal forms of β-turns (type I, type II, etc.) based entirely on theoretical calculations. Subsequently, over a thousand x-ray structures of different globular proteins have been analyzed, with results suggesting that the most important form among the hairpin conformers is the type I β-turn. For the latter type of hairpin conformation, the original computations had predicted ϕ_i+1 = −60°, ψ_i+1 = −30°, ϕ_i+2 = −90°, and ψ_i+2 = 0° as backbone torsion angle values, and these have been used from that time as reference values for the identification of the type I β-turn. However, it has never been clarified whether these “ideal” backbone torsion angle values exist in real structures, or whether these torsion angles are only “theoretical values.” Using the most recent release of the Protein Data Bank (1994), a survey has been made to assign amino acid pairs that approach the ideal form of the type I β-turn. The analysis resulted in four sequences where the deviation from ideal values for any main-chain torsion angles was less than 2°. In order to determine whether such a backbone fold is possible only in proteins owing to fortuitous cooperation of different folding effects, or whether it occurs even in short peptides, various attempts have been made to design the optimal amino acid sequence. Such a peptide model compound adopting precisely the predicted torsion angle values [ϕ_i+1 = −60°, ψ_i+1 = −30°, ϕ_i+2 = −90°, and ψ_i+2 = 0°] could provide valuable information. The solid state conformation of cyclo[(δ) Ava-Gly-Pro-Thr (O¹Bu)-Gly] reported herein, incorporating the -Pro-Thr- subunit, yields values suggesting that the “ideal” type I β-turn is even possible for a peptide where there are no major environmental effects present. © 1996 John Wiley & Sons, Inc.     

Solvent-accessible surfaces of nucleic acids

Static solvent-accessible surface areas were calculated for DNA and RNA double helices of varied conformation, composition and sequence, for the single helix of poly(rC), and for a transfer RNA. The results show that for DNA and RNA double helices, two thirds of the water-accessible surface area become buried on double helix formation; phosphate oxygens retain near maximal exposure while the bases are 80% buried. Transfer RNA exposes slightly less surface per residue than does double-helical RNA, despite the presence of several additional “modified” groups, all of which are exposed significantly.When a probe corresponding to a single water molecule is used, both the total and atom type exposures are very similar for A-DNA and B-DNA, although marked differences appear in the major and minor groove exposures between the two conformations. For a given base-pair, the accessible surface area buried upon double-helical stacking is nearly constant (within 5%) for different sequences of neighboring base-pairs.For probes larger than single water molecules, there exist considerable differences in the total and atom type exposures of A-DNA and B-DNA. Conformational transitions between the A-DNA and B-DNA helical forms can thus be related to differences in the accessible areas for “structured” water, or a secondary hydration shell, rather than to interactions with individual water molecules of the primary hydration shell. The base-composition dependence of DNA helical conformation can be explained in terms of the opposing effects of thymine methyl groups of A · T base-pairs and the amino groups of G · C base-pairs upon the solvent within the grooves.The area calculations show that primarily the major groove of B-DNA and the minor groove of A-DNA have sufficient accessible surface area to be recognized by a probe size corresponding to the side-chains of amino acids.     

Modifications of the amide bond and conformational constraints in pseudopeptide analogues

We have investigated the conformational effects of modifying the amide group in model dipeptides. The N-methyl amide ψ[CO-NMe], N-hydroxy amide ψ[CO-N(OH)], N-amino amide ψ[ CO-N (NH₂)], retro amide ψ[ NH-CO], reduced amide in the neutral ψ[CH₂-NH] and protonated ψ[CH₂-N ⁺ H₂] state, and hydrazide ψ[CO-NH-NH] have been introduced as surrogates of the amide link in pseudopeptide derivatives of the Pro-Gly or Ala-Gly model dipeptides protected on both termini by an amide group. These compounds have been studied in solution by proton nmr and ir spectroscopy, and in the solid state by x-ray diffraction, giving an extended data set of experimental structural and conformational information on pseudopeptide sequences. The conformational effects depend both on the nature and the position of the modified amide link. Some modifications appear to have no intrinsic conformational induction (N-amino and retro amide), but destabilize any local folded structure by hydrogen-bond breaking. Because of the formation of strong intramolecular interactions, others are capable of stabilizing a β-turn (for example protonated reduced amide), or of inducing a particular local conformation such as a β- or γ-like turn (for example N-hydroxy amide). The particular geometry of the cis N-methyl amide and of the “hydrazino” proline favors the formation of a sharp turn of the main chain. All these structural data are of interest to the design of bioactive peptide mimics. © 1993 John Wiley & Sons, Inc.     

Interactions of metallic ions with DNA. V. DNA renaturation mechanism in the presence of Cu 2+

New experimental data were obtained by means of circular dichroism, melting, renaturation, and kinetic experiments, upon Cu²⁺ binding to DNA, poly dAT, and poly dGdC. They enable us to propose a model of binding giving a satisfactory explanation to all of the data found in the literature. Two types of binding sites are proposed: (a) a “sandwich” of Cu²⁺ between two adjacent G-C pairs giving a charge-transfer complex, and (b) a chelate between a phosphate group and a nitrogen atom of the bases (N₇ of guanine and N₃ of cytosine at room temperature, N₃ of adenine after thermal opening of A-T pair). Type (a) stabilizes the helix and keeps the two strands linked. Type (b) destabilizes the helix and explains why the kinetic rate of renaturation is the same as that of copper release.     

Induced CD of DNA intercalators: electric dipole allowed transitions

The induced CD of an electric dipole allowed transition of a DNA intercalator has been calculated using the “matrix method” and a set of DNA ππ* transitions recently adopted for calculating the CD of DNA by Rizzo and Schellman [(1984) Biopolymers 23 , 435–470]. The induced CD is strongly dependent on the angular orientation of the intercalator and only moderately dependent on its location within the intercalation pocket. The dependence of the CD on the orientation and location of the intercalator was studied for some representative conformations of di- and tetranucleotide duplexes of (dGdC) and (dAdT). The effect of alternative DNA transition moment directions was also tested. The orientation dependence compares well with the previously predicted 1-2 cos² γ dependence [B. Nordén and F. Tjerneld (1982) Biopolymers 21 , 1713–1734]. Measured induced CD spectra of methylene blue (MB) intercalated in double-stranded poly(dAdT), poly(dGdC), and calf-thymus DNA are discussed on the basis of the results of the calculations. Major differences between the induced CD spectra are likely to reflect different modes of intercalation for the different nucleotide sequences. In particular, the concluded geometry in solution for MB intercalated in poly(dAdT) differs significantly from the corresponding geometry found in dinucleotide–intercalator crystals.     

The beta conformation of polypeptides of valine, isoleucine, and threonine in solution and solid-state: optical and infrared studies.

Water-soluble polypeptides of L -valyl and L -isoleucyl residues flanked with DL -lysyl blocks [poly(DL Lys · HCl)_x–poly(L Val)_y–poly(DL Lys · HCl)_x, poly(DL Lys · HCl)_x–poly-(L Ile)_y–poly(DL Lys · HCl)_x] and homopoly(L -threonine) were prepared. The β conformation of these polymers in water, as well as in aqueous methanol, was confirmed by infrared spectroscopy and circular dichroism studies. The optical properties of these valyl and isoleucyl polypeptides were quite different from those of previously reported synthetic homopolypeptides in the β structure. Their differences could be explained by the presence of a “single extended β chain” without either intra- or interchain association.