Influence of amino acid and peptide counterions on the conformation of DNA

We describe fibre diffraction studies on the interaction of DNA with different amino acids and peptides. The B form of DNA, with ten base-pairs per turn, is always found at high levels of humidity. We suggest that this pitch is observed because the DNA molecules are maintained in a straight position. In solution, the DNA molecules are bent and may have a larger pitch. The A form of DNA is never found upon dehydration. Instead, the B form may be either stabilized by the counterions or altered so that the number of base-pairs per helical turn decreases upon dehydration. Alteration is favoured either by small counterions that have a single charge or by large basic polypeptides and proteins. Stabilization is favoured by small counterions that have several charged groups. A third type of behaviour is found with some amino acids that contain hydrophobic groups, which destabilize the secondary structure of DNA, probably due to a modification of its intramolecular interactions. We have not detected any specific effect of amino acid side-chains, although the amino acid sequence has a clear influence on the interaction. We think that these observations are of interest in the pursuit of more detailed crystallographic studies on protein-DNA interactions.     

Conformations of duplex structures formed by oligodeoxynucleotides covalently linked to the intercalator 2-methoxy-6-chloro-9-aminoacridine

A family of covalent complexes between oligonucleotides and derivatives of the intercalating agent 9-amino acridine has been synthesized (Asseline, U., Thuong, N.T. and Helene, C. (1983) C.R.Acad. Sci. (Paris) 297 (III), 369-372) and studied (Lancelot, G., Asseline, U., Thuong, N.T., and Helene, C. (1985) Biochemistry 24, 2521-2529; Lancelot, G., Asseline, U., Thuong, N.T., and Helene, C. (1985) J. Biomol. Str. Dyn. 3, 913-921) with a view to understand nucleic acid-nucleic acid recognition. In order to understand the nature of interactions between the intercalator and the oligonucleotides in such complexes and the sensitivity of such interactions to the polymorphic form of the DNA, we have carried out molecular mechanics simulations on duplex deoxyoligonucleotides d(A)6.d(T)6 (A and B forms) and d(TATC).d(GATA) (B form) covalently bound to 2-methoxy-6-chloro-9-aminoacridine through a pentamethylene linker chain. Structures in which the acridine derivative is end stacked (at the 3' and 5' ends) and in which the dye is intercalated between the terminal base pairs (at both the ends) and between second and third base pairs from the 3' end are all of reasonably low energy in both A and B forms of DNA. Our studies on 3' end complexes find that in the B form, intercalation of the dye between the second and third base pairs is preferred over the other two modes of binding, while in the A form, intercalation between the terminal base pairs is preferred. In the 5' end A and B form complexes, outside stacking and intercalation between the terminal base pairs are preferred, respectively. Our calculations suggest the possibility that the presence of the dye attached covalently to the DNA can induce conformational transitions in the DNA. For example, intercalation of the dye two base pairs from the end could induce an A----B transition.     

Influence of alkali cation nature on structural transitions and reactions of biopolyelectrolytes

A general thermodynamic analysis is presented, describing how counterion species of different nature, but the same valency, influence polyelectrolyte transformations and reactions of the general form: PA1.B1-M(+)-->PA2.B2M+ + (B1 - B2)M+. Here PA1 and PA2 are two different states or structural forms of a polyanion, B1 and B2 are the number of M+ ions thermodynamically bound to the polyanions PA1 and PA2, respectively. The specific effects of the two counterions, M1+ and M2+, on this equilibrium can be simply related to the quotient of their selectivity constants, D2M2M1/D1M2M1, for the polyion states 1 and 2. We analyze how different monovalent counterions (particularly, sodium and potassium) affect polyelectrolyte reactions and transformations such as, e.g., the DNA helix-coil transition. Previous experimental results on the competition between DNA and the synthetic polyanion, poly(methacrylic acid), for binding to the synthetic polycation, poly(N-ethylvinylpyridinium), has been investigated with respect to sodium and potassium ion specificity, using our model. We also discuss the DNA-histone disassembly/assembly reaction modeled as a competition of two polyanions for binding to a polycation.     

Infrared linear dichroism investigations of deoxyribonucleic acid complexes with poly(L-arginine) and poly(L-lysine).

Complexes between DNAs from various sources and poly(L-lysine) and poly(L-arginine) were studied by means of infrared linear dichroism. The measurements of dichroic ratios allowed us to determine the orientation of the phosphate group of DNA in the complexes with basic polypeptides. At high relative humidities (higher than 90%, B form), the bisector of the less than OPO in the complexes forms an angle with respect to the helical axis which has a value lower by about 4 degrees than in the corresponding DNA sample. This change of orientation of the phosphate group of DNA indicates a modification of the B form upon binding of polylysine or polyarginine. The structural transitions B leads to A and B leads to C measured as a function of relative humidities were not affected by formation of complexes with both basic polypeptides. Similar results were obtained for complexes prepared by direct mixing or by salt gradient dialysis. The presence of A and C forms was observed in complexes of DNA with poly(L-lysine) and poly(L-arginine) at lower relative humidity. Thus, the conformational flexibility of DNA in complexes with polylysine and polyarginine is not changed despite a substantial increase in the Tm (melting temperature). These results are considered as a model for the understanding of interactions between DNA and histones particularly of the binding of the N-terminal fragment, lysine or arginine rich.     

A direct demonstration that the ethanol-induced transition of DNA is between the A and B forms: an X-ray diffraction study

DNA undergoes a reversible co-operative change in a number of its properties over a characteristic range of ethanol concentrations. This ethanol-induced transition of DNA has been studied by a number of groups, using circular dichroism as well as other assay techniques. There has been disagreement as to the species of DNA involved. We have used X-ray diffraction methods on DNA fibers exposed to an excess of solvent. The diffraction patterns serve as “fingerprints” to clearly show that the transition occurs between the B and A forms of DNA (at low and high ethanol concentrations, respectively) in agreement with the conclusions of some of the previous workers. At still higher ethanol concentrations, the diffraction pattern changes from that of the A form to that of a more disordered form.     

Characterization of intermediate conformational states in the B↔Z transitions of poly(dG?dC) · poly(dG?dC)

Time-dependent uv absorption and CD spectrum changes in salt-induced conformational B → Z and Z → B transitions of poly(dG? dC) · poly(dG? dC) were measured. This polynucleotide does not convert directly from a right-handed double-helical B form to a left-handed double-helical Z form, but goes through an intermediate, B* form, with the B → B* transition proceeding nearly instantaneously, and then transforms gradually to the Z form. Uv absorption spectra of these B and B* forms are nearly identical, but their CD spectra are quite different. The CD spectrum of the B* form is identical with that obtained for DNA in high salt solutions and is similar to a spectrum which for some time was thought to be a C form. These B and B* forms have the same number of base pairs per turn [Sprecher, C.A., Baase, W.A. & Johnson, Jr., W.C. (1979) Biopolymers 18 , 1009–1019]. Kinetic measurements showed that uv absorption and CD intensities at fixed wavelengths do not change in a simple exponential curve. However, both the uv absorption spectrum change in the B → Z transition and the CD spectrum change in the B* → Z transition, respectively, have isosbestic points. In the B → Z transition, no hyperchromicity can be observed. These results suggest that this B* form unfolding or premelting process is a rate-determining step in the B* → Z transition and makes it easy for the unfolded or premelted polynucleotide to almost immediately fold into the Z form. The double helix does not dissociate into single strands and transforms from the B* form to the Z form point-by-point along the chain in a soliton-like manner of with a small amount of open states in which the bases are unpaired. Also, in the Z → B transition, the polynucleotide does not convert directly from the Z to the B form, but goes through a B*-like form. In this transition, the uv-absorption spectra also have an isosbestic point. The reaction velocity in the Z → B transition is much faster than that in the B → Z transition. Possibly, the positive CD band between 265 and 310 nm in the B form comes from a n-π* transition due to an interaction of the bases with sugarphosphate groups.     

Conformational transitions of polynucleotides in the presence of rhodium complexes

We studied the effects of hexammine and tris(ethylene diamine) complexes of rhodium on the conformation of poly(dG-dC).poly(dG-dC) and poly(dG-m5dC).poly(dG-m5dC) using spectroscopic techniques and an enzyme immunoassay. Circular dichroism spectroscopic measurements showed that Rh(NH3)6(3+) provoked a B-DNA----Z-DNA----psi-DNA conformational transition in poly(dG-dC).poly(dG-dC). Using the enzyme immunoassay technique with a monoclonal anti-Z-DNA antibody, we found that the left-handedness of the polynucleotide was maintained in the psi-DNA form. In addition, we compared the efficacy of Rh(NH3)6(3+) and Rh(en)3(3+) to provoke the Z-DNA conformation in poly(dG-dC).poly(dG-dC) and poly(dG-m5dC.poly(dG-m5dC). The concentrations of Rh(NH3)6(3+) and Rh(en)3(3+) at the midpoint B-DNA----Z-DNA transition of poly(dG-dC).poly(dG-dC) were 48 +/- 2 and 238 +/- 2 microM, respectively. The psi-DNA form of poly(dG-dC).poly(dG-dC) was stabilized at 500 microM Rh(NH3)6(3+). With poly(dG-m5dC).poly(dg-m5dC), both counterions provoked the Z-DNA form at approximately 5 microM and stabilized the polynucleotide in this form up to 1000 microM concentration. These results show that trivalent complexes of Rh have a profound influence on the conformation of poly(dG-dC).poly(dG-dC) and its methylated derivative. Furthermore, the Rh complexes are capable of maintaining the Z-DNA form at concentration ranges far higher than that of other trivalent complexes. Our results also demonstrate that the efficacy of trivalent inorganic complexes to induce the B-DNA to Z-DNA transition of poly(dG-dC).poly(dG-dC) and poly(dG-m5dC).poly(dG-m5dC) is dependent on the nature of the ligand as well as the polynucleotide modification. Differences in charge density and hydration levels of counterions or base sequence- and counterion-dependent specific interactions between DNA and metal complexes might be possible mechanisms for the observed effects.     

Poly(L–lysine)–DNA interactions in NaCl solutions: B → C and B → ψ Transitions

Thermal denaturation and circular dichroism (CD) properties of poly(L -lysine)–DNA complexes vary greatly when these complexes are prepared differently, that is, whether by NaCl-gradient dialysis starting from 2.0 M NaCl or by direct mixing at low salt. These differing properties were investigated in more detail by examining complexes, made by direct mixing in the presence of various concentrations of NaCl, both before and after the NaCl was dialyzed out of the complex solution. The precipitation curves of DNA due to polylysine binding indicate that such binding is noncooperative at zero salt; from 0.1 up to 1.0 M NaCl they exhibit varying degrees of cooperatively. Starting from zero salt, as the NaCl concentration used for complex formation is increased, both the CD and the melting properties of the complexes are shifted from those of directly mixed at zero salt to those of reconstitution: in the CD spectra there is a gradual shift from a B → C transition to a B → ψ transition; thermal denaturation results show a gradual increase in the melting temperatures of both free DNA (t_m) and polylysine-bound DNA (t′_m). The progressive shift from B → C to B → ψ suggests a close relationship between these two transitions. Large aggregates of the complexes do not warrant the appearance of ψ-type CD spectra: ψ-spectra have been obtained in the supernatants of polylysine–DNA complexes made and measured at 1.0 M NaCl while slightly perturbed CD spectra in B → C transition have been observed in turbid solutions of fully covered complexes made at very low salt. If the complexes are made at intermediate salts and dialyzed to a very low salt, although up to 60% of the DNA is still bound by polylysine, the CD spectra of the complexes are shifted back to the B-type CD characteristic of pure DNA.     

A new approach to the characterization of the B and A forms of DNA by I.R. spectroscopy

The RNA conformational changes of B, A and C forms are reflected in the infrared absorption spectra in the region of 800 cm^?1 to 900 cm^?1 and allow one to investigate unoriented samples. The transition to the A form is characterized by the appearence of bands at about 870 cm^?1 and at 813 cm^?1 whereas the B and the C forms exhibit a band at 837 cm^?1, these bands undoubtedly arise from phosphate diester stretching vibrations and yield information about backbone conformation. The presence of these infrared bands provides a criterion for testing the simultaneous presence of two coexisting forms of DNA. It represents a useful method for structural studies of nucleic acid complexes such as protein-DNA for which it is difficult to obtain orientation.     

Conformational characteristics of deoxyribonucleic acid-butylamine complexes with C-type circular dichroism spectra. 2. A Raman spectroscopic study

The derivatives of calf thymus DNA in which n-butylamine is covalently attached as described in the preceding paper in this series [Chen, C. Y., Pheiffer, B. H., Zimmerman, S. B., & Hanlon, S. (1983) Biochemistry (preceding paper in this issue)] were examined by Raman spectroscopy. As previously mentioned, these complexes exhibit profoundly decreased rotational strengths of the positive band of the circular dichroism (CD) spectrum above 260 nm, with the most heavily substituted (ca. 0.12 mol of amine/mol of nucleotide) resembling that of DNA in 11 m LiCl. Raman spectra of all complexes and their controls in the form of either fibers at 98% relative humidity or gels at 40 mg/mL in 20 mM NaCl, pH 7, show typical B-type spectra with no evidence of significant amounts of C, A, Z, or disordered forms. We have thus concluded that the assignment of the nonconservative CD spectrum of DNA typically observed in concentrated electrolyte solutions to a C form is in error. Both these Raman data and the X-ray results reported in the previous paper indicate that the structure giving rise to the C CD spectrum has B-form backbone geometry.     

Molecular dynamics simulation of the DNA triplex d(TC)5.d(GA)5.d(C+T)5.

A molecular dynamics simulation of the DNA triple helix d(TC)5.d(GA)5.d(C+T)5 is described (C+ represents a protonated cytosine residue). The simulation has been performed using the program AMBER 3.1 and includes counterions and explicit solvent under periodic boundary conditions. Both the dynamic and time-averaged behaviour of the system has been analysed. Considerable deviations from the fibre-diffraction model for DNA triple helix structure are observed, including the repuckering of the purine strand sugars that has been identified in some nuclear magnetic resonance (n.m.r.) studies. The simulation suggests that this conformational change may be driven by the possibility of improved interactions between the phosphate groups of this strand and both the solvent and counterions. Several examples of a particular conformational transition are observed, involving correlated changes in the backbone angles alpha and gamma. These transitions provide a possible explanation for some unusual n.m.r. data that have been reported. The structure of the triple helix major groove also suggests an explanation for the observed stabilization of DNA triplexes by polyvalent cations, and their ability to interact with drugs that bind in the minor groove of DNA duplexes.     

DNA conformation and thermostability of aqueous solutions of beta-alanine and gamma-aminobutyric acid

It has been shown that at low concentrations of rare amino acids (from 10(-3) M to 10(-1) M of the substance) stechiometric complexes amino acid -- DNA are formed, which bring about partial substitution of counterions screening phosphate groups and to a change of spatial structure of DNA water molecules. The DNA-solvent molecular interactions are changed, accompanied by an abrupt decrease of helix-coil enthalpy transition which leads to the unwinding of DNA double helix. In the region of amino acid high concentrations (greater than 1-1,5 M) a rise of thermostability and winding of DNA double helix is observed. It has been established that B----C-like conformational transition stimulated by the rise of DNA thermostability is a result of counterions dehydration and the increase of effective ionic strength of the solution which is due to the rise of amino acid-zwitterions content in it.     

Structural investigations on DNA-protamine complexes.

Protamine·DNA complexes in film and in solution have been investigated by means of infrared linear dichroism, ultraviolet circular dichroism, and laser Raman spectroscopy. At high relative humidity and in solution both infrared linear dichroism and ultraviolet circular dichroism indicate the presence of a modified B form of DNA (designated as B* in our other papers^27,28,46). This modified B form is characterized by a change of the orientation of the \documentclass{article}\pagestyle{empty}\begin{document}$ \widehat{OPO} $\end{document} bisector angle by about 4° with respect to the helical axis when compared to the B form of DNA. At decreasing relative humidities the same modified B form is maintained and no structural transitions B → A (or B → C) normally occurring in free DNA were observed. The absence of the A form in these complexes was also confirmed by laser Raman scattering studies of protamine·DNA complexes. On the basis of these results, a model of the protamine·DNA complex is proposed, which suggests that the presence of apolar amino-acid residues, and probably the folding of the polypeptide chain, is responsible for preventing the B-to-A transition; this occurs either by protecting the high-humidity modified B form against dehydration or by steric interference of this protein probably located in one of the DNA grooves.     

The structure of nucleoprotein cores released from adenovirions.

The morphology, protein composition and DNA organization of nucleoprotein core complexes isolated from type 5 adenovirions have been examined by electron microscopy and biochemical techniques. The morphology of such core structures is in some ways strikingly similar to that exhibited by cellular chromatin. 'Native' core preparations contain compact and less highly-folded forms: the latter appear as thick fibres, 150-300A in diameter. Upon exposure to 0.4M NaCl, adenovirus cores undergo a transition to a beaded string form, reminiscent of nucleosomes. Of the three arginine-rich proteins, polypeptides V, VII and mu present in 'native' cores, only polypeptide VII remains associated with viral DNA in the presence of 0.4M NaCl. We therefore conclude that the nucleosome-like beads are constructed solely of polypeptide VII. The results of micrococcal nuclease digestion experiments suggest that polypeptide VII is sufficient to protect some 100-300bp of adenoviral DNA.     

A reduced set of coordinates for modeling DNA structures: (I). A B-to-A transition pathway driven by pseudorotational angle.

The A-DNA and the B-DNA are two well characterized polymorphous forms of DNA duplex. By using Metropolis Monte Carlo Simulations in a reduced coordinate space, we have shown that the B in equilibrium with A transitions can be induced by forcing pseudorotational angle (W) to change between C3'-endo and C2'-endo puckerings. The energy barrier for the transition pathway is less than 10 Kcal.mol-1. Base-pair parameters x-displacement (Dx) and roll (rho), which have the largest differences between the two forms of structures, cannot drive the transition. Our results support the view that the bistable states of the DNA duplex are due to the bistable structures of the sugar ring.     

Modulation of the B-A transition of DNA by potential antitumor antibiotics. Influence of the base composition of DNA

The B-A transition of DNA in oriented films of DNA-drug complexes is more or less restricted as a consequence of drug binding as revealed by infrared linear dichroism. A fraction of DNA is irreversibly locked into the B form. This behavior is described by the number of DNA base pairs "frozen" in the B form by one drug molecule. This quantity is dependent on the DNA sequence the drug is attached to. In this paper, drug complexes of oriented films of NaDNA with a GC content of 42% from calf thymus and a GC-rich DNA from Micrococcus lysodeikticus were compared. The restriction of the B-A transition of DNA complexes with two intercalating antibiotics, aclacinomycin A and violamycin BI, is not severely influenced by the base composition of DNA. By contrast, the strong groove binding oligopeptide antibiotics netropsin and distamycin A are much less effective to restrict the B-A transition of GC-rich DNA than of AT-rich DNA. This finding is in agreement with previous results by other methods which support a model based upon a strong preference of AT clusters by these two non-intercalating drugs.     

Influence of a Mechanical Tension on the B-C and B-C Conformational Transitions in DNA Fibres

Abstract

In the present fibre X-ray study we attempt to quantify the effect of a mechanical tension on the conformations, and transitions between the structural forms of DNA A simple experimental device has been realized in order to apply precise mechanical forces on DNA fibres during X-ray exposure. It is shown that, as the applied tension is increased, the B→A transition can be prevented as well as with a decrease of the sodium salt content A kind of distorted B form is then observed the helical parameters of which change with the relative humidity. On the contrary, the mechanical tension does not prevent the B→C transition; it only slows down the form change and improves the X-ray patterns up to a relative humidity of 0%.     

Adsorption of DNA to mica mediated by divalent counterions: a theoretical and experimental study

The adsorption of DNA molecules onto a flat mica surface is a necessary step to perform atomic force microscopy studies of DNA conformation and observe DNA-protein interactions in physiological environment. However, the phenomenon that pulls DNA molecules onto the surface is still not understood. This is a crucial issue because the DNA/surface interactions could affect the DNA biological functions. In this paper we develop a model that can explain the mechanism of the DNA adsorption onto mica. This model suggests that DNA attraction is due to the sharing of the DNA and mica counterions. The correlations between divalent counterions on both the negatively charged DNA and the mica surface can generate a net attraction force whereas the correlations between monovalent counterions are ineffective in the DNA attraction. DNA binding is then dependent on the fractional surface densities of the divalent and monovalent cations, which can compete for the mica surface and DNA neutralizations. In addition, the attraction can be enhanced when the mica has been pretreated by transition metal cations (Ni(2+), Zn(2+)). Mica pretreatment simultaneously enhances the DNA attraction and reduces the repulsive contribution due to the electrical double-layer force. We also perform end-to-end distance measurement of DNA chains to study the binding strength. The DNA binding strength appears to be constant for a fixed fractional surface density of the divalent cations at low ionic strength (I < 0.1 M) as predicted by the model. However, at higher ionic strength, the binding is weakened by the screening effect of the ions. Then, some equations were derived to describe the binding of a polyelectrolyte onto a charged surface. The electrostatic attraction due to the sharing of counterions is particularly effective if the polyelectrolyte and the surface have nearly the same surface charge density. This characteristic of the attraction force can explain the success of mica for performing single DNA molecule observation by AFM. In addition, we explain how a reversible binding of the DNA molecules can be obtained with a pretreated mica surface.     

A unified theory of the B-Z transition of DNA in high and low concentrations of multivalent ions

We showed recently that the high-salt transition of poly[d(G-C)]. poly[d(G-C)] between B-DNA and Z-DNA (at [NaCl] = 2.25 M or [MgCl(2)] = 0.7 M) can be ascribed to the lesser electrostatic free energy of the B form, due to better immersion of the phosphates in the solution. This property was incorporated in cylindrical DNA models that were analyzed by Poisson-Boltzmann theory. The results are insensitive to details of the models, and in fair agreement with experiment. In contrast, the Z form of the poly[d(G-m5C)] duplex is stabilized by very small concentrations of magnesium. We now show that this striking difference is accommodated quantitatively by the same electrostatic theory, without any adjustable parameter. The different responses to magnesium of the methylated and nonmethylated polymers do not come from stereospecific cation-DNA interactions: they stem from an experimentally derived, modest difference in the nonelectrostatic component of the free energy difference (or NFED) between the Z and B forms. The NFED is derived from circular DNA measurements. The differences between alkaline earth and transition metal ions are explained by weak coordination of the latter. The theory also explains the induction of the transition by micromolar concentrations of cobalt hexammine, again without specific binding or adjustable parameters. Hence, in the case of the B-Z transition as in others (e.g., the folding of tRNA and of ribozymes), the effect of multivalent cations on nucleic acid structure is mediated primarily by nonspecific ion-polyelectrolyte interactions. We propose this as a general rule for which convincing counter-examples are lacking.