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Biomedical subjects

G Kraft

Publications and source records attributed to G Kraft.

At least 73 records · Page 4Linked to original sources

Track structure and DNA damage.

Heavy particles like protons or heavier ions are different in their biological efficiency when compared to sparsely ionizing radiation. These differences have been attributed to the different pattern of energy deposition in the track of the particles. In radiobiological models two different approaches are used for the characterization of the radiation quality: the continuous dose distribution of the various track structure models and the separation in small compartments inside the track which are used in microdosimetry. In a recent Monte Carlo calculation using the binary encounter approximation as input for the electron emission process, the radial distribution of the dose is calculated for heavy ions. The result of this calculation is compared to other models and used for a qualitative interpretation of the induction of DNA damage by particles.

DNA↗

On the parameterization of the biological effect in a mixed radiation field.

The exposure of astronauts and electronics to the cosmic radiation especially to the particle component pose a major risk to all space flights. Up to now it is not possible to quantify this risk within acceptable limits of accuracy. This uncertainty is not only caused by difficulties in the more or less exact prediction of the incidence of the cosmic radiation but depends also on the problem of the quantification of the radiation field and the correlation of the biological effect. Usually the biological action of a mixed radiation field is estimated as product of the measured dose with an average quality factor, the relative biological efficiency. Because of the large variation in energy and atomic number of the cosmic particles, average values of the quality factor are not precise for risk estimation. A more appropriate way to treat the biological effects of mixed radiation is the concept of particle fluence and action cross section.

Animals↗

Cell cycle delays induced by heavy ion irradiation of synchronous mammalian cells.

Cell cycle delays in V79 Chinese hamster cells induced by heavy ion exposure have been investigated using flow cytometry. Synchronous cell populations in G1, S and late-S G2/M phase were used, which were prepared by centrifugal elutriation. Cells were irradiated with particles from Z = 10 (neon) up to 96 (uranium) in the energy range from 2.4 to 17.4 MeV/u and the LET range from 415 to 16,225 keV/micron at the UNILAC at GSI, Darmstadt. For comparison, experiments with 250 kV X-rays were performed. For light particles like neon, cell cycle perturbations comparable with those after X-ray irradiation were found, and with increasing LET an increasing delay per particle traversal was observed. For the highest LET values extended delavy in G1, S and G2/M phase were detected immediately after irradiation. A large fraction of the cells remained in S or G2/M phase up to 48 h or longer after irradiation: they probably died in interphase. The prolongation of delays with increasing LET is in contrast with inactivation cross section measurements, where cross sections reach a plateau at LET values > 500 keV/micron. No significant cell age dependence of cycle delays was detected for the very high LET values. In addition to cell cycle delays, two effects related to the DNA content as determined by flow cytometry were found after irradiation with very high LET particles, that were attributed to cell fusion and drastic morphological changes of the cells. Estimations based on the dose deposited by a single particle hit in the cell nucleus and the actual number of hits show that the basic trend of the experimental results can be explained by the stochastic properties of particle radiation.

Animals↗

Influence of radiation quality on the expression of chromosomal damage.

The amount of chromosomal damage induced in synchronous V79 cells by either 250 kV X-rays or 4.6 MeV/u Ar ions (LET: 1850 keV/microns) was determined at five successive sampling times. The experiments show that the time course of the appearance of damaged cells is strongly influenced by radiation-induced cell cycle perturbations and mitotic delay and depends on radiation quality and dose. The yield of chromosomal damage was found to increase with sampling time, but this increase was more pronounced for Ar ions. Because of the observed differences in the yield time profiles induced by sparsely and densely ionizing radiation the contribution of each sample to the overall damage was considered, i.e. the total (time integrated) amount of damage was determined. The obtained data are interpreted in terms of differences in the spatial energy deposition by sparsely and densely ionizing radiation.

Animals↗

Magnetic resonance imaging signal changes in denervated muscles after peripheral nerve injury.

The evaluation of peripheral nerve disorders has traditionally relied on a clinical history, physical examination, and electrodiagnostic studies. Recent studies have used magnetic resonance imaging (MRI) to evaluate a variety of both nerve and muscle disorders. In this article, we describe the use of MRI, using short-tau inversion recovery (STIR) sequences, to evaluate muscle signal characteristics in a variety of peripheral nerve disorders. A total of 32 patients were studied, and 12 representative cases are discussed in detail. Increased STIR signal in muscle was seen in cases of severe axonotmetic injuries involving the transection of axons producing severe denervation changes on electromyography. The increased STIR signal in denervated muscles was seen as early as 4 days after the onset of clinical symptoms, which is significantly earlier than changes detected on electromyography. The MRI signal changes were reversible when the recovery of motor function occurred as a result of further muscle innervation. In cases of neurapraxic nerve injuries, characterized by conduction block without axonal loss, the STIR signal in muscle was normal. These findings show that MRI using STIR sequences provides a panoramic visual representation of denervated muscles useful in localizing and grading the severity of peripheral nerve injury secondary to either disease or trauma. MRI using STIR sequences may therefore play an important role in the prediction of clinical outcome and the formulation of appropriate therapy early after peripheral nerve injury.

Adolescent↗

Protection of DNA from high LET radiation by two OH radical scavengers, tris (hydroxymethyl) aminomethane and 2-mercaptoethanol.

The effect of high linear energy transfer (LET) radiation on DNA in vitro, both in protective and non-protective environments was investigated. Two hydroxyl radical scavengers, tris(hydroxymethyl) aminomethane and 2-mercaptoethanol, were compared for their ability to protect SV40 DNA from radiation damage over a wide LET range. At comparable OH scavenging capacities, significant differences were found between these protective agents, indicating that other, radical scavenger-dependent processes affected the extent to which the DNA was protected. In general, a decrease in single-strand breaks (SSBs) relative to double-strand breaks (DSBs) was observed as LET increased. This effect was more pronounced when a radioprotector was present. Comparison of the relative biological efficiency (RBE) of radiation damage as LET increased showed a peak of DSB production in the mid-LET range. These data agree with measurements made by Christensen et al. (1972). An explanation for this increase in DSB production efficiency has been proposed based on the particle track structure of high-LET radiation.

DNA Damage↗

Free radicals from polycrystalline pyrimidines and purines upon heavy ion bombardment at low temperatures: an electron spin resonance study.

The formation of free radicals in polycrystalline samples of the DNA constituents thymine, cytosine, and adenosine after bombardment with heavy ions at about 100 K was investigated by electron spin resonance (ESR) spectroscopy. Spectra were observed at 77 K after irradiation at 100 K, upon annealing to 300 K and after storage at 300 K. Individual radical patterns were isolated from the spectra by computer manipulation and assigned to structures by powder-simulations based on literature data. The spectra of thymine contain an allyl radical, the octet pattern of the 5-thymyl radical and contributions of the 6-yl radical formed by net hydrogen gain at carbon C5. The latter species is also present in cytosine which in addition displays the pattern due to H-addition at the carboxyl oxygen C2. Adenosine exhibits two H-addition radicals, one at C2, the other at C8. Additionally, the spectra of all DNA subunits studied contain as a radical component a Gaussian singlet of about 0.9 mT line width. The spectra obtained at low temperature already contain the secondary radicals but exhibit a large linewidth. This feature is attributed to dipolar coupling caused by radicals in close proximity.

Adenosine↗

DNA strand break induction and rejoining and cellular recovery in mammalian cells after heavy-ion irradiation.

The induction of intracellular DNA strand breaks by X rays and various heavy charged particles was measured by the alkaline unwinding and alkaline and neutral filter elution techniques. No variations in strand break induction were found between the different cell lines under investigation. For a given particle, both the LET and the particle energy determined the efficiency to induce DNA lesions. RBE values for the total amount of induced strand breaks were always less than 1. For DNA double-strand breaks (DSBs), RBE values only slightly greater than 1 were determined for particle radiation with an LET around 300 keV/microns. Intracellular DSB/SSB ratios were found to be equivalent to data reported for in vitro systems using radioprotective conditions [Christensen et al., Int. J. Radiat. Biol. 22, 457-477, 1972; Taucher-Scholz et al., Adv. Space Res. 12(2-3), (2)73-(2)80, 1992]. Strand break rejoining as an indicator of cellular repair processes was detected even after high-LET irradiation (LET < or = 10,000 keV/microns). However, both the half-times of rejoining and the fraction of residual DNA breaks increased with the atomic number of the particle. After particle irradiation with LET values beyond 10,000 keV/microns, no rejoining of DNA strand breaks was found.

Animals↗

Histologic evidence of myocardial damage in apparently healthy subjects with ventricular arrhythmias and myocardial dysfunction.

The association of ventricular arrhythmias and myocardial dysfunction could be considered an early step toward cardiomyopathy; therefore, we studied 28 patients in NYHA class I and II, characterized by complex ventricular arrhythmias (VA) on 24-h Holter monitoring and volumetric and/or contractile abnormalities on a standard two-dimensional echocardiogram (2-D echo). All patients underwent radioisotopic angiography, 20 patients complete hemodynamic study, and 15 patients endomyocardial biopsy. Ambulatory ECG monitoring showed the presence of frequent premature ventricular contractions in 14 patients (50%) and episodes of ventricular tachycardia in 16 patients (57%). 2-D echo showed mono- or biventricular enlargement and dyssynergies in 25 patients (89%) (left ventricle in 6, right ventricle in 11, both in 8). Two patients showed only left ventricle enlargement and one patient isolated left ventricular dyssynergies. Radioisotopic angiography showed mono- or biventricular ejection fraction reduction in 24 patients (85%) and regional dyssynergies in 24 patients (85%) in accordance with 2-D echo. Hemodynamic study showed in all patients normal coronary arteries, and right and left angiography confirmed enlargement and/or regional dyssynergies. Endomyocardial biopsy was abnormal in 11 of 15 patients: various degrees of hypertrophy, parcellar fibrosis, and adipogenic infiltration were found. Our preliminary data suggest that the simultaneous occurrence of ventricular arrhythmias and ventricular dyssynergies and/or enlargement in patients without apparent clinical heart disease may represent an early stage of dilated cardiomyopathy.

Adolescent↗

Irradiation increases proteolysis in erythrocyte ghosts: a spin label study.

X- and gamma-irradiation of human erythrocyte membranes (250-1000 Gy) was found to decrease the ratio of weakly to strongly immobilized signal height of membrane-bound maleimide spin label (Mal-6). Subsequent incubation of spin-labeled membranes at ambient temperature (21 degrees C) induced a progressive increase in this ratio, faster for membranes irradiated with low doses which was hampered by protease inhibitors. These results demonstrate that ionizing radiation stimulates proteolysis of erythrocyte membrane proteins by membrane-associated proteases.

Blood Proteins↗

LET, track structure and models. A review.

Swift heavy ions when penetrating through matter strip off those electrons having a smaller orbital velocity than the ion velocity. The remaining electrons screen the nuclear charge yielding an effective charge. The effective charge of the ions interacts predominantly with the target electrons causing excitation and ionizations of the target atoms. Using the Bethe Bloch formula for the energy loss combined with the Barkas formula for effective charge, the energy loss values as well as unrestricted and restricted linear transfer can be calculated within a few percent of accuracy. From the primary energy loss only a small fraction of 10% or less is transformed into excitation. The major part of the energy loss is used for the ionization of the target atoms and the emission of the corresponding electrons with a high kinetic energy. These electrons form the track around the trajectory of the primary ion in which two thirds of the primary energy is deposited by collisions of primary, secondary and later generations of electrons with the target molecules. In the electron diffusion process the energy is transported from the center of the track into the halo. The radial dose decreases with the square of the radial distance from the center. The diameter of the track is determined by the maximum range of the emitted electrons, i.e. by the maximum energy electrons. All ions having the same velocity i.e. the same specific energy produce electrons of the same energy and therefore tracks of the same diameters independent of the effective charge. But the dose inside the track increases with the square of the effective charge. Track structure models using this continuous dose distributions produce a better agreement with the experiment than models based on microdosimetry. The critical volume as used in microdosimetry is too large compared to the size of the DNA as critical structure inside the biological objects. Track structure models yield better results because the gross-structure of the track i.e. its lateral extension and the thin down toward the end of the track is included in these calculations. In a recent refinement the repair capacity of the cell has been included in a track structure model by using the complete shouldered x-ray survival curve as a template for the local damage produced by the particle tracks. This improved model yields presently the best agreement with the experiment.

Energy Transfer↗

Delta-electron emission in fast heavy ion atom collisions.

Biological damages such as mutations, chromosomal aberrations etc. are a consequence of biochemical changes mostly in the DNA. With ionizing radiation, these chemical changes are due to primary ionization events and secondary ionization effects caused by the primarily produced electrons. Differences in the biological response of densely ionizing radiation, like heavy charged particles, in comparison to sparsely ionizing radiation, such as X- or gamma-rays, are mainly due to the differences in the production of the so called delta-electrons. Therefore, the emission process of electrons i.e. the cross section for the primary ionization event as well as the energy and angular distribution of the emitted electrons should be understood in detail. The delta-electron emission processes occuring in fast heavy ion atom collisions are explained qualitatively. The different spectral structures of electron emission arising from either the target or the projectile are explained in terms of simple models of the kinetics of momentum transfer induced by the COULOMB forces. In collisions of very heavy ions with matter, high nuclear COULOMB forces are created. These forces lead to a strong polarization of the electronic states of the participated electrons. The effects of this polarization are discussed.

Argon↗

Direct radiation action of heavy ions on DNA as studied by ESR-spectroscopy.

The effects of heavy ions on the mechanisms of free radical formation in DNA-constituents as compared to low-LET irradiation are investigated by means of Electron Spin Resonance (ESR) spectroscopy. Dose-yield curves were measured at low (T < 100 K) and ambient temperatures in order to obtain the G-value, that is number of radicals formed per 100 eV absorbed energy. These G-values show a characteristic LET-dependence and are one to two orders of magnitude lower than for low-LET irradiation. Measurements on 2'Deoxycytidine at 300 K using combined heavy ion and X-ray irradiation methods suggested that this effect can be partially explained by a destruction of radicals during the irradiation.

Adenosine↗

Induction of DNA breaks in SV40 by heavy ions.

Simian virus (SV40) DNA was used to study the induction of DNA strandbreaks by heavy ions varying in LET. DNA was exposed to X-rays and to accelerated particles either in dilute solution or in the presence of different radical scavengers. Relative proportions of the intact supercoiled DNA, nicked form arising from single strand breaks (SSB) and linear molecules produced by double strandbreaks (DSB) were quantified on the base of their electrophoretic mobility in agarose gels. Cross sections for the induction of SSBs and DSBs were calculated from the slope of dose effect curves. Mercaptoethanol was found to protect more efficiently against DNA strand breakage than Tris. When the biological efficiency, i.e. the number of strand breaks per unit dose and molecule weight was evaluated as a function of LET, curves for SSB induction always showed a continuous decrease. For DSB induction, an increase in the yield of DSBs with a maximum around 500 keV/micrometer was observed in the presence of radical scavenger. This peak of biological efficiency gradually disappeared when the radiosensitivity of the system was increased, and was no longer apparent in the dilute buffer system, where DNA showed a high susceptibility to strand breakage. When the relative biological efficiency was plotted versus LET, the curve for DSB induction observed in a low radical scavenging environment paralleled the curve obtained for SSB induction.

DNA Damage↗

Induction of chromosome aberrations in mammalian cells after heavy ion exposure.

The induction of chromosome aberrations by heavy charged particles was studied in V79 Chinese hamster cells over a wide range of energies (3-100 MeV/u) and LET (20-16000 keV/micrometer). For comparison, X-ray experiments were performed. Our data indicate quantitative and qualitative differences in the response of cells to particle and x-ray irradiation. For the same level of cell survival the amount of damaged cells which can be observed is smaller in heavy ion (11.4 MeV/u Ar) irradiated samples. The highest yield of damaged cells is found 8 to 12 hours after particle irradiation and 4 hours after x-irradiation. Differences in the amount of damaged cells are attributed to cell cycle perturbations which interfere with the expression of damage. After heavy ion exposure the amount of cells reaching mitosis (mitotic index) decreases drastically and not all damaged cells reach mitosis within 48 hours after exposure. A portion of cells die in interphase. Cell cycle delays induced by x-ray irradiation are less pronounced and all cells reach the first post-irradiation mitosis within 24 hours after irradiation. Additionally, the damage produced by charged particles seems to be more severe. The disintegration of chromosomes was only observed after high LET radiation: an indication of the high and local energy deposition in the particle track. Only cross sections for the induction of chromosome aberrations in mitotic cells were reported in this paper because of the problems arising from the drastic cell cycle perturbations. In this case, cells were irradiated in mitosis and assayed immediately.

Animals↗

When is a family not a family?

Recent molecular investigations of the small-subunit rRNA gene sequences have indicated that established taxonomic hierarchies can be clearly at odds with the degree of evolutionary divergence (as inferred from molecular divergence) between supposedly equivalent taxa at every rank (i.e., species through class), both within and across biological divisions. This is particularly true between the Rhodophyta and the Phaeophyta, whose higher-order taxa appear under- and overinflated, respectively. We present two plausible alternatives that algal taxonomists might adopt in order to invoke discussion on their relative merits.

Eukaryota↗

Fluidity alterations induced by chemical modification of erythrocyte membrane proteins.

Using EPR technique we have examined the effect of chemical agents on pig erythrocyte membranes. Treatment of the erythrocyte membranes with SH-oxidizing and denaturing or specific for amino groups reagents affects both the membrane proteins and lipids. These results suggest that modified proteins may perturb the interactions of the membrane components and lead to alterations of the membrane organization in the polar region.

Animals↗

Heavy-ion effects on bacteria spores: the impact parameter dependence of the inactivation.

The impact parameter dependence of the inactivation of Bacillus subtilis-spores has been measured using a heavy-ion minibeam facility, which permits single-ion exposure of individual spores with a spatial accuracy of about 1 micron. The apparatus consists basically of a collimator and a microscope used to position the biological objects directly behind the collimator. Measurements were obtained for nickel, tin, and uranium ions at 1.4 MeV/u. for central hits the results show an inactivation probability of less than one with a continuous decrease in inactivation with increasing distance. Long-ranging effects which extend beyond the range of the delta electrons could not be confirmed.

Bacillus subtilis↗