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A study of rats liver DNA damages under the influence of X-ray radiation at a dose of 6.5 Gy(LD60) was carried out. The radioprotective properties of newly synthesized Cu(II) L-Schiff Histidinate complexes were also studied. The survival of rats was determined over a 30-day period after exposure to X-rays without pretreatment and also after preadministration of Cu(II) L-Histidinate-Schiff base complexes. The structural defects of rat's liver DNA were detected at 3, 7, 14, and 30 days post-irradiation extracted. The results obtained revealed that irradiation with a 6.5Gy dose in the control group degraded the characteristics of rat liver DNA in comparison to healthy DNA. On all investigated experimental days, a decrease in the melting temperature (Tm), a widening of the melting interval (ΔT), and a decrease in hypochromicity (Δh) were observed in the DNA samples of irradiated animals compared to the norm. The rat's pretreatment by Cu(II) L-Histidinate complexes 1 or 24 hours prior to irradiation improved DNA characteristics. Electrophoretic studies of DNA were in good agreement with the melting data. Based on the study results, it can be concluded that Cu(II) L-Histidinate complexes exhibit radioprotective properties under the studied conditions and can protect DNA from damage.

RESUMEN

We used circular dichroism spectroscopy, UV spectrophotometry, and differential scanning calorimetry to investigate pH-dependent structural transitions in an equimolar mixture of complementary G-rich d[5'-A(GGGTTA)3GGG-3'] (TelG) and C-rich d[3'-T(CCCAAT)3CCC-5'] (TelC) human telomeric DNA strands. Our studies were conducted at neutral (pH 7.0) and slightly acidic (pH 5.5 and 6.5) pH. We analyzed the melting thermodynamics of TelG and TelC and their equimolar mixture. Our analysis revealed that the preferred conformation of an equimolar mixture of TelG and TelC is the duplex. At pH 5.5, however, in addition to the duplex state, we observed a significant population of the i-motif state formed by TelC. Our results are consistent with the picture in which an increase in pH from 5.5 to 7.0 has little effect on the melting enthalpy of an isolated G-quadruplex while causing a strong reduction in the melting enthalpy of an isolated i-motif (the latter diminishes to 0 at pH 7.0). These effects summarily lead to a decrease in the contribution of the i-motif to the melting enthalpy of the mixture and, hence, an increase in the apparent melting enthalpy and overall stability of the duplex state.

RESUMEN

Binding of the antitumor compound cisplatin to DNA locally distorts the double helix. These distortions correlate with a decrease in DNA melting temperature (Tm). However, the influence of cisplatin on DNA stability is more complex because it decreases the DNA charge density. In this way, cisplatin increases the melting temperature and partially compensates for the destabilizing influence of structural distortions. The stabilization is stronger at low Na+ ion concentration. Due to this compensation, the total decrease in the DNA melting temperature after cisplatin binding is much lower than the decrease caused by the distortions themselves, especially at low [Na+]. It is shown in this study that, besides Na+ concentration, pH also strongly influences the value of a change in the melting temperature caused by cisplatin. In alkaline medium (pH=10.5-10.8), a fall in the melting temperature caused by platination is enhanced several times with respect to neutral medium. Such a stronger drop in Tm is explained by a decrease in pK values of base pairs caused by lowering the charge density under platination that facilitates proton release. At neutral pH, the proton release is low for both control and platinated DNA and does not influence the melting behavior. Therefore, lowering in the charge density under platination, besides stabilization, gives additional destabilization just in alkaline medium. Destabilization caused by structural distortions due to this pH induced compensation of stabilizing effect is more pronounced. In the presence of carbonate ion, destabilization caused by high pH value is strengthened. As a decrease in DNA charge density, interstrand crosslinking caused by cisplatin also increases the DNA stability due to loss in the entropy of the melted state. However, computer modeling of DNA stability demonstrates that interstrand crosslinks formed by cisplatin do not stabilize long DNA. It is shown that the increase in Tm caused by interstrand crosslinking itself is compensated for by a local destabilization of the double helix at the sites of location of interstrand crosslinks formed by cisplatin.

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We characterized the interactions of meso-tetrakis(4N-(2-hydroxyethyl)pyridinium-4-yl) porphyrin (TEtOHPyP4), meso-tetrakis(4N-allylpyridinium-4-yl) porphyrin (TAlPyP4), and meso-tetrakis(4N-metallylpyridinium-4-yl) porphyrin (TMetAlPyP4) with the poly(rA)poly(rU) and poly(rI)poly(rC) RNA duplexes between 18 and 45 degrees C by employing circular dichroism, light absorption, and fluorescence intensity spectroscopic measurements. Our results suggest that TEtOHPyP4 and TAlPyP4 intercalate into the poly(rA)poly(rU) and poly(rI)poly(rC) host duplexes, while TMetAlPyP4 associates with these RNA duplexes by forming outside-bound, self-stacked aggregates. We used our temperature-dependent absorption titration data to determine the binding constants and stoichiometry for each porphyrin-RNA binding event studied in this work. From the temperature dependences of the binding constants, we calculated the binding free energies, DeltaG(b), enthalpies, DeltaH(b), and entropies, DeltaS(b). For each RNA duplex, the binding enthalpy, DeltaH(b), is the most favorable for TEtOHPyP4 (an intercalator) followed by TAlPyP4 (an intercalator) and TMetAlPyP4 (an outside binder). On the other hand, for each duplex, external self-stacking of TMetAlPyP4 produces the most favorable change in entropy, DeltaS(b), followed by the intercalators TAlPyP4 and TEtOHPyP4. Thus, our results suggest that the thermodynamic profile of porphyrin-RNA binding may correlate with the binding mode. This correlation reflects the differential nature of molecular forces that stabilize/destabilize the two modes of binding-intercalation versus external self-stacking along the host duplex.

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In the present work fluctuations of number of ligands adsorbed on macromolecule are investigated. We have taken into account the adsorption and desorption of ligands under the circumstance of some adsorption centers fluctuations affected by medium fluctuation. The correlation function and spectral density of number of ligands adsorbed on macromolecule are calculated. The properties of these fluctuations which allow identifying a noisemaker are determined. It has been shown, thatfas andsluggis adsorption can be distinguished by properties of dispersion and spectral density. It has been also shown, that comparison of experimental and theoretical correlation functions (or spectral densities) allows to calculate constants of ligand - adsorption center binding and unbinding.

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Long-range interaction between all the ligands bound to DNA molecule may give rise to adsorption with the character of phase transition of the first kind (D. Y. Lando, V. B. Teif, J. Biomol. Struct & Dynam. 18, 903-911 (2000)). In this case, the binding curve, c(c(o)), is characterized by a sudden change of the relative concentration of bound ligands ((c)) at a critical concentration of free (unbound) ligands, c(o)=c(ocr), from a low c value to a high one where c(o) is molar concentration of free ligands. Such a transition might be caused by some types of DNA condensation or changes in DNA topology. For the study of the conditions necessary for adsorption with the character of phase transition, a calculation procedure based on the method of the free energy minimum is developed. The ligand size and two types of interactions between ligands adsorbed on DNA molecule are taken into consideration: long-range interaction between all the ligands bound to DNA and contact interactions between neighboring ligands. It was found that a) Stronger long-range interaction is required for longer ligands to induce phase transition that is occurred at greater c(ocr) values; b) Pure contact interaction between neighboring ligands can not itself initiate phase transition. However contact cooperativity strongly decreases the threshold value of energy of long-range interaction necessary to give rise to the transition.

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