[Basic characteristics of a parallel dual DNA helix by scanning tunnel microscopy data].
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Biomedical subjects
Publications and source records attributed to Iu D Nechipurenko.
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In studies of interactions of ligands with nucleic acid molecules, S-shaped curves are often obtained. In this work we show that the sigmoidal shape of the curves is due to a competition of ligand molecules for DNA binding sites. If a ligand that binds to DNA can form two types of complexes with the binding constants K1 and K2 and binding site sizes L1 and L2, respectively, then in the event that K1 < K2 and L1 < L2, the dependence of the concentration of complexes of the first type on the concentration of the ligand added to solution can be S-shaped.
This study is a continuation of a series of papers dealing with topotecan interaction with double-stranded polydeoxyribonucleotides. We showed earlier that topotecan molecules form dimers in solution at concentration above 10(-5) (per base pair). Topotecan interaction with calf thymus DNA in solutions of low ionic strength was studied by fluorescence, circular dichroism, and linear flow dichroism. The data obtained indicate that topotecan forms two types of complex with DNA, DNA molecules combining with each other during formation of one of these complexes. The association constant of two topotecan-filled DNA molecules with each other was estimated at 10(4) M-1 (per base pair) in 1 mM sodium cacodylate buffer, pH 6.8, at 20 degrees C. A possibility of modulation of DNA topoisomerase I activity by topotecan due to complexation with several sites of a supercoiled DNA molecule is discussed.
A thermodynamic model of the formation of bridges consisting of alternating daunomycin molecules and copper ions and connecting neighboring nucleic acid molecules in a particle of a liquid crystalline dispersion was constructed. The model is based on the conception that ligands are adsorbed on lattices of reaction centers which are formed in a liquid crystal at a particular spatial arrangement of adjacent nucleic acid molecules (phasing). Equations were derived that describe typical experimentally obtained S-shaped dependences of bridge concentration on the concentration of copper ions and daunomycin molecules in an initial solution. It was shown that dependences of this kind take place in two variants of the adsorption model: when the binding of daunomycin with adjacent nucleic acid molecules is considered to be independent on the formation of bridges and when bridges compete with single daunomycin molecules for the sites on adjacent nucleic acid molecules.
The binding of daunomycin and copper ions to poly(I).poly(C) molecules fixed in a particle of a liquid-crystalline dispersion was studied. A thermodynamic model of adsorption was developed, which makes it possible to describe the formation of complexes of a particular kind, "bridges" that connect adjacent nucleic acid molecules fixed in a liquid crystal. The bridges represent chelate complexes, which incorporate the molecules of the antibiotic daunomycin and copper ions. Equations describing the dependence of the concentration of these bridges in solution on the concentration of their constituents were derived. The family of dependences of experimental amplitudes of bands in CD spectra typical of "bridge" structures on the concentration of copper ions represents a set of S-shaped curves, and, as the concentration of daunomycin in solution increases, the level of saturation of these curves increases. The analysis of experimental data with the use of this model suggests that the structures of this type compete with daunomycin molecules for the binding sites on poly(I).poly(C). By using this model, the energies of formation of bridge structures were calculated.
Formation of molecular construction that consists of double-stranded molecules of nucleic acids (or synthetic polynucleotides) located at the distance 30-50 A in the spatial structure of particles of their cholesteric liquidcrystalline dispersion and crosslinked by polymeric chelate bridges is described. The resulting superstructure, which possesses peculiar physicochemical properties, could be used as integral biosensor whose properties depend on temperature, the presence of chemical or biologically active compounds of different nature, etc.
Three variants of the model for the formation of "bridges" between the nucleic acid molecules fixed in the structure of particles of liquid-crystalline dispersions were considered. What the three variants have in common is that the bridges represent polymeric chelate cross-links consisting of alternating molecules of daunomycin and copper ions. The differences between the three variants are that in the first variant, the bridges begin and end with daunomycin molecules that form a complex by the mechanism of external binding with nucleic acids; in the second variant, the bridges begin and end with copper ions coupled with the pairs of bases of nucleic acids; and in the third variant, the bridges begin with the daunomycin molecule and end with the copper ion. For each variant, a mathematical model was constructed, which describes the formation of bridges, and equations of binding were derived. The results of calculations were compared with the experimental data. Within the framework of each variant, the values of the energy of interaction between the daunomycin molecule and the copper ion in the bridge, the energy of interaction of the daunomycin molecule with the nucleic acid, and the length of the bridge were varied. For all variants, those values of the parameters were chosen that fit best the experimental data. The theoretical curves obtained using the three variants of the model agree rather well with the family of experimental curves. The best agreement between the theoretical and experimental data was obtained when the polymeric chelate bridge includes more than two daunomycin molecules.
Models of adsorption were considered, which describe the binding of biologically active ligands on DNA templates. The binding is described most comprehensively and in greatest detail by the distribution function, which determines the probability of detecting the preset number of adsorbed ligands on the template. In the case of noncooperative binding, this function corresponds to the Gaussian distribution and is characterized by two quantities: the mean value of the occupation of the template by ligands and the dispersion of occupation. The accuracy of the occupation of the template by ligands is inversely proportional to dispersion. As the length of the template and the number of reaction sites covered by one ligand upon binding increase, the accuracy of the occupation of the template by ligands increases. An important characteristic of binding is the degree of coverage of the template by ligands. This characteristic represents the portion of template reaction sites covered by all ligands adsorbed on the template. If polycations are bound to nucleic acid molecules, the coverage of the template determines the transition of nucleic acids to a compact state. The degree of template coverage for extended ligands depends only slightly on the binding constant in a wide range of concentrations of a free ligand in solution. Different adsorption models are considered from the unified point of view. The classification of cooperative interactions for a wide class of systems is given, from situations when several ligands are bound on nucleic acid templates to a situation when templates change by the action of ligands and begin to interact with each other.
Due to noncooperative binding of ligands to DNA molecules, DNA molecules are in equilibrium with different numbers of adsorbed ligands. This equilibrium for a given concentration of the free ligand in the solution is characterized by the distribution function, which describes the probability of revealing the DNA molecule with a definite number of adsorbed ligands. If polycations act as ligands, DNA molecules with the number of ligands sufficient for neutralizing the charges on phosphates may undergo a phase transition. One example of this transition is the formation of liquid-crystalline dispersions during the binding of DNA to chitosan. We analyzed the binding of chitosan to DNA on the assumption that this binding is due to equilibrium adsorption. At a definite concentration of chitosan in solution, DNA molecules are in equilibrium with different numbers of adsorbed molecules of chitosan. If the number of adsorbed ligands exceeds some critical value, the DNA molecule covered with chitosan becomes capable of interacting with other DNA molecules. As a result of this interaction (attraction), liquid-crystalline dispersions can form. Equations describing the dependence of the concentration of DNA molecules on the concentration of the ligand in solution were derived. It was shown that, at given parameters of the model, it is possible to describe experimental data characterizing the formation of cholesteric liquid-crystalline dispersions. The analysis of the data makes it possible to reconstitute both the size of the binding site occupied by chitosan on the DNA and the energy of interaction of chitosan with DNA.
The regulation of gene expression is a basic problem of biology. In some cases, the gene activity is regulated by specific binding of regulatory proteins to DNA. In terms of statistical mechanics, this binding is described as the process of adsorption of ligands on the one-dimensional lattice and has a probability nature. As a random physical process, the adsorption of regulatory proteins on DNA introduces a noise to the regulation of gene activity. We derived equations, which make it possible to estimate this noise in the case of the binding of the lac repressor to the operator and showed that these estimates correspond to experimental data. Many ligands are able to bind nonspecifically to DNA. Nonspecific binding is characterized by a lesser equilibrium constant but a greater number of binding sites on the DNA, as compared with specific binding. Relations are presented, which enable one to estimate the probability of the binding of a ligand on a specific site and on nonspecific sites on DNA. The competition between specific and nonspecific binding of regulatory proteins plays a great role in the regulation of gene activity. Similar to the one-dimensional "lattice gas" of particles, ligands adsorbed on DNA produce "one-dimensional" pressure on proteins located at the termini of free regions of DNA. This pressure, an analog of osmotic pressure, may be of importance in processes leading to changes in chromatin structure and activation of gene expression.
The properties of nanoconstructions formed by double-stranded DNA molecules fixed in the structure of their liquid crystalline dispersions and cross-linked by nanobridges were described. The dependence of the optical properties of the nanostructures on various factors (DNA concentration, nanobridge components, etc.) was examined.
The temperature stability of nanoconstructions formed by double-stranded DNA molecules fixed in the structure of their liquid crystalline dispersions and cross-linked by nanobridges was determined. It was shown that the heating of nanoconstructions is accompanied by a decrease in the amplitude of the negative bands in the CD spectrum both at lambda approximately 310 and lambda approximately 505 nm. Temperature "melting curves" were derived and characterzed by T(M) values. The T(M) values at lambda approximately 310 and lambda approximately 505 nm coincided with each other but differed from the T(M) value characteristic of the DNA cholesteric liquid crystalline dispersion.
The effect of finite fragment length on the distribution pattern of bound protein along the DNA fragment is considered. If the size of the binding site for a ligand on DNA is comparable with the length of the DNA fragment fluctuations in the amount of ligand bound to the fragment create some difficulties for evaluating the distribution pattern of ligand on DNA. A mathematical approach is developed which enables one to calculate the distribution pattern of ligand on DNA provided that the number of bound ligand on the DNA fragment is known. Expression are also obtained to treat the effects of fluctuations in the number of ligand molecules bound to the DNA fragment on the distribution pattern of ligand. A new procedure is proposed which may be useful for locating the preferable binding sites for ligand on DNA on the basis of footprinting experiments.
The influence of different types of long-range interaction of ligands adsorbed on DNA on the helix-coil transition was theoretically considered. The contact interaction was shown to differ significantly from the long-rang one. It was shown also that even weak dependence of a long-range potential on a degree of helicity resulted in the strong changes of a DNA melting curve. This result allowed to understand the different experimental data on DNA melting in the presence of different substances which reduced AT-and GC-base pairs thermostability difference.
A model has been developed which allows description of the binding of antibiotics and dyes to a nucleic acid in which different regions are involved in the formation of a certain tertiary structure. Interactions between different segments of nucleic acid may contribute to the internal overall energy of the macromolecule. We consider the case when the tertiary structure and the internal energy of the macromolecule are altered upon binding of small molecules. These structural changes affect the shape of the binding isotherm of ligand to the nucleic acid. We obtain relations which permit to determine the dependence of the internal energy on the degree of binding of ligand to nucleic acid.