1) Quercetin has a higher reduction potential compared with curcumin at three different pH settings and is comparable to Trolox at pH 7-9.5; 2) its TAC is 3.5 fold higher than curcumin; 3) it reduced LPS-induced ROS to near normal levels; 4) it reduced LPS-induced NO production. These data provide a physico-chemical basis for comparing antioxidants, with potential benefits individually or in combination.

The release of unaltered bases from irradiated DNA, hydrated between 2.5 and 32.7 mol of water per mole of nucleotide (gamma), was investigated using HPLC. The objective of this study was to elucidate the yield of the four DNA bases as a function of dose, extent of hydration, and the presence or absence of oxygen. The increase in the yield of radiation-induced free bases was linear with dose up to 90 kGy, except for the DNA with gamma = 2.5, for which the increase was linear only to 10 kGy. The yield of free bases as a function of gamma was not constant in either the absence or the presence of oxygen over the range of hydration examined. For DNA with gamma between 2.5 and 15, the yield of free bases was nearly constant under nitrogen, but decreased under oxygen. However, for DNA with gamma greater than 15, the yield increased rapidly under both nitrogen and oxygen. The yield of free bases was described by a model that depended on two factors: 1) a change in the DNA conformation from a mixture of the A and C conformers in vacuum-dried DNA to predominantly the B conformer in the fully hydrated DNA, and 2) the proximity of the water molecules to the DNA. Irradiation of the inner water molecules (gamma less than 15) was less efficient than irradiation of the outer water molecules (gamma greater than 15), by a factor of approximately 3.3, in forming DNA lesions that resulted in the release of an unaltered base. This factor is similar to the previously published relative efficiency of 2.8 with which hydroxyl radicals and base cations induce DNA strand breaks. Our irradiation results are consistent with the hypothesis that the G value for the first 12-15 water molecules of the DNA hydration layer is the same as the G value for the form of DNA to which it is bound (i.e., the pseudo-C or the B form). Thus we suggest that the release of bases originating from irradiation of the hydration water is obtained predominantly: (1) by charge transfer from the direct ionization of the first 12-15 water molecules of the primary hydration layer and (2) by the attack of hydroxyl radicals generated in the outer, more loosely bound water molecules.

The induction of base damage products in gamma-irradiated DNA, hydrated between 2.5 and 32.8 moles of water per mole of nucleotide (tau), was investigated using the gas chromatography/mass spectrometry-selected ion monitoring technique. In general, the yields of the measured base damage products were found to be dependent on the extent of the hydration when the DNA was irradiated under nitrogen. At low hydrations (tau < or = 13), the highest yields of the measured products were found for 7,8-dihydro-8-oxo-guanine, 5,6-dihydrothymine and, to a lesser extent, 2,6-diamino-4-oxo-5-formamidopyrimidine, products which are consistent with the base radicals found in low-temperature ESR studies. At higher hydrations (tau < or = 13), changes in DNA conformation and an increase in the attack of bulk water radicals on DNA play a significant role in the formation of radiation-induced DNA base damage products. Additional findings in our study include: (1) the sum of the yields of the products formed from electron-loss centers is greater than the sum of the yields of the products formed from electron-gain centers, indicating that there might be other electron-gain products which have not been identified; (2) the combined yield for the base damage products and the release of unaltered bases at tau < or = 13 is constant, implying that radiation damage in the tightly bound water molecules of the primary hydration layer causes DNA damage (quasi-direct effect) that is similar to the damage caused by direct ionization of the DNA (direct effect); and (3) the yields of the individual base damage products that were formed from electron-loss centers can be modeled on the basis of both the known reactions that lead to the formation of the initial charged base radicals in irradiated DNA, and the known reactions that involve the conversion of these initial DNA radicals into their respective nonradical end products.

No abstract

ESR spectroscopy at low temperatures is employed to investigate electron transfer within DNA doped with randomly spaced electron traps. The traps were introduced by careful bromination of DNA in ice-cooled aqueous solution. The procedure is shown by NMR and GC/MS techniques to modify thymine, cytosine, and guanine 2‘-deoxyribosides, transforming them into 5-bromo-6-hydroxy-5,6-dihydrothymine, T(OH)Br, 5-bromocytosine, CBr, and 8-bromoguanine, GBr, derivatives. The bromination products formed in molar ratio close to T(OH)Br/CBr/GBr = 0.2:1:0.23 and serve as internal electron scavengers on γ-irradiation. Paramagnetic products that result from electron scavenging in DNA by T(OH)Br and CBr units at 77 K have been identified by ESR as the 6-hydroxy-5,6-dihydrothymin-5-yl (TOH•) radical and the 5-bromocytosine σ* radical anion, CBr•-. Our quantitative estimates show that electron scavenging by T(OH)Br in bromine-doped DNA is over an order of magnitude more efficient than the more abundant CBr traps. This indicates that there is a high probability the electron survives encounters with the planar CBr traps through either transmission or reflection. The yields of electron scavenging by T(OH)Br moieties have been treated quantitatively considering the scavenging process as a competition between diffusion of electrons to T(OH)Br traps and their fixation on cytosines in the form of protonated radical anions. A mean displacement of the electron from its entry point evaluated using this model is about 11 bases at 77 K. After trapping at 77 K no further migration takes place until annealing to temperatures near 150 K and above. At these temperatures electron migration is activated and migration distances are found to increase with temperature likely through a hopping mechanism.

Dose-response curves were measured for the formation of direct-type DNA products in X-irradiated d(GCACGCGTGC)(2)prepared as dry films and as crystalline powders. Damage to deoxyribose (dRib) was assessed by HPLC measurements of strand break products containing 3' or 5' terminal phosphate and free base release. Base damage was measured using GC/ MS after acid hydrolysis and trimethylsilylation. The yield of trappable radicals was measured at 4 K by EPR of films X-irradiated at 4 K. With exception of those used for EPR, all samples were X-irradiated at room temperature. There was no measurable difference between working under oxygen or under nitrogen. The chemical yields (in units of nmol/J) for trapped radicals, free base release, 8-oxoGua, 8-oxoAde, diHUra and diHThy were G(total)(fr) = 618 +/- 60, G(fbr) = 93 +/- 8, G(8-oxoGua) = 111 +/- 62, G(8-oxoAde) = 4 +/- 3, G(diHUra) = 127 +/- 160, and G(diHThy) = 39 +/- 60, respectively. The yields were determined and the dose-response curves explained by a mechanistic model consisting of three reaction pathways: (1) trappable-radical single-track, (2) trappable-radical multiple-track, and (3) molecular. If the base content is projected from the decamer's GC:AT ratio of 4:1 to a ratio of 1:1, the percentage of the total measured damage (349 nmol/J) would partition as follows: 20 +/- 16% 8-oxoGua, 3 +/- 3% 8-oxoAde, 28 +/- 46% diHThy, 23 +/- 32% diHUra, and 27 +/- 17% dRib damage. With a cautionary note regarding large standard deviations, the projected yield of total damage is higher in CG-rich DNA because C combined with G is more prone to damage than A combined with T, the ratio of base damage to deoxyribose damage is approximately 3:1, the yield of diHUra is comparable to the yield of diHThy, and the yield of 8-oxoAde is not negligible. While the quantity and quality of the data fall short of proving the hypothesized model, the model provides an explanation for the dose-response curves of the more prevalent end products and provides a means of measuring their chemical yields, i.e., their rate of formation at zero dose. Therefore, we believe that this comprehensive analytical approach, combined with the mechanistic model, will prove important in predicting risk due to exposure to low doses and low dose rates of ionizing radiation.

Manganese (Mn) toxicity is partially mediated by reduced ATP production. We have used oxidation rate assays -a measure of ATP production -under rapid phosphorylation conditions to explore sites of Mn 2+ inhibition of ATP production in isolated liver, brain, and heart mitochondria. This approach has several advantages. First, the target tissue for Mn toxicity in the basal ganglia is energetically active and should be studied under rapid phosphorylation conditions. Second, Mn may inhibit metabolic steps which don't affect ATP production rate. This approach allows identification of inhibitions that decrease this rate. Third, mitochondria from different tissues contain different amounts of the components of the metabolic pathways potentially resulting in different patterns of ATP inhibition. Our results indicate that Mn 2+ inhibits ATP production with very different patterns in liver, brain, and heart mitochondria. The primary Mn 2+ inhibition site in liver and heart mitochondria, but not in brain mitochondria, is the F 1 F 0 ATP synthase. In mitochondria fueled by either succinate or glutamate + malate, ATP production is much more strongly inhibited in brain than in liver or heart mitochondria; moreover, Mn 2+ inhibits two independent sites in brain mitochondria. The primary site of Mn-induced inhibition of ATP production in brain mitochondria when succinate is substrate is either fumarase or complex II,

Antioxidants have been studied for their capacity to reduce the cytotoxic effects of radiation in normal tissues for at least 50 years. Early research identified sulfur-containing antioxidants as those with the most beneficial therapeutic ratio, even though these compounds have substantial toxicity when given in-vivo. Other antioxidant molecules (small molecules and enzymatic) have been studied for their capacity to prevent radiation toxicity both with regard to reduction of radiation-related cytotoxicity and for reduction of indirect radiation effects including long-term oxidative damage. Finally, categories of radiation protectors that are not primarily antioxidants, including those that act through acceleration of cell proliferation (e.g. growth factors), prevention of apoptosis, other cellular signaling effects (e.g. cytokine signal modifiers), or augmentation of DNA repair, all have direct or indirect effects on cellular redox state and levels of endogenous antioxidants. In this review we discuss what is known about the radioprotective properties of antioxidants, and what those properties tell us about the DNA and other cellular targets of radiation.