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To determine the effectiveness of two UV spectra with different UVB components for cell kill and micronucleus induction in irradiated human HeLaxskin fibroblast (CGL1) hybrid cells and their progeny. To determine the presence of reactive oxygen species (ROS) in the progeny of the irradiated cells at various post-irradiation times and their relationship with induced delayed biological effects.A commercial solar ultraviolet simulator was used. Two different filters were employed: the first transmitted radiation with lambda284nm and the second radiation with lambda293nm. The resulting spectra have different UVB components (lambda between 284 and 320nm, 19 W/m(2), and between 293 and 320nm, 13 W/m(2)) and the same UVA component (lambda between 320 and 400nm, 135 W/m(2)). CGL1 cells were irradiated with various doses. Clonogenic survival and micronucleus formation were scored in the irradiated cells and their progeny. ROS were detected by incubation of cultures at various post-irradiation times with dichlorodihydrofluorescein diacetate followed by flow cytometric measurement of the final product, dichlorofluorescein.The biological effectiveness of the lambda284nm spectrum was higher by a factor of 3 compared to the lambda293nm spectrum for cell kill, and by a factor of 5 for micronucleus induction. No delayed cell death or micronucleus formation was found in the progeny of cells exposed to lambda293nm, while a large and dose-dependent effect was found in the progeny of cells exposed to lambda284nm for both of these endpoints. ROS levels above those in unirradiated controls were found only in the progeny of cells exposed to the lambda284nm spectrum.The spectrum with lambda284nm was more effective than that with lambda293nm for induction of cell kill and micronucleus formation in the directly irradiated cells as well as induction of delayed effects in the progeny in the form of delayed reproductive death and micronucleus formation. The presence of ROS in the progeny of the irradiated cells may be the cause of the delayed effects.

To determine the relative biological effectiveness (RBE) for initial and delayed inactivation of cells by a modulated proton beam suitable for the treatment of tumours of the eye, within the spread-out Bragg peak and in its distal declining edge.Human tumour SCC25 cells were irradiated with the 65 MeV proton beam at the Cyclotron Medicyc in Nice. Perspex plates of different thickness were used to simulate five positions along the beam line: 2mm corresponding to the entrance beam; 15.6 and 25 mm in the spread-out Bragg peak; 27.2 and 27.8mm for the distal edge. At each position clonogenic survival of the irradiated cells and of their progeny were determined at various dose values. 60Co gamma-rays were used as reference radiation.RBE values evaluated at the survival level given by 2 Gy of gamma-rays increased with increasing depth from close to 1.0 at the proximal to about 1.2 at the distal part of the peak. Within the declining edge it reached the value of about 1.4 at 27.2 and about 2 at 27.8 mm. For the progeny of irradiated cells, the RBE value ranged from 1.0 to 1.1 within the spread-out Bragg peak and then increased up to a value of 2.0 at the last position. The dose-effect curves for the progeny always had a larger shoulder than for the irradiated progenitors, their alpha parameters being lower by a factor of about 4 and their beta parameters always being higher. The alpha/beta ratio was about 50 Gy for the progenitors and about 6 Gy for their progeny. The incidence of delayed effects increased with dose and with the depth within the beam.RBE values for the inactivation of cells irradiated in the spread-out Bragg peak are compatible with the value currently assumed in clinical applications. In the distal declining edge of the beam, the RBE values increased significantly to an extent that may be of concern when the region of the treatment volume is close to sensitive tissues. The yield of delayed reproductive cell death was significant at each position along the beam line.

Measurements of C3H10T1/2 and V79 cell thickness were performed on living cells by confocal laser fluorescence microscopy. Thickness distributions are reported for cells growing as a monolayer (on mylar and glass) and suspended in their medium. Mean values for cells grown on mylar (corrected for refractive index effects) are 2.9 +/- 0.6 and 6.1 +/- 1.0 microm for C3H10T1/2 and V79 cells respectively. Mean values of the diameters of cells suspended in their medium are 13.0 +/- 1.6 and 9.3 +/- 1.4 microm for C3H10T1/2 and V79 respectively. Knowledge of cell thickness, as irradiated, is of central relevance for studying the relative biological effectiveness of low energy, poorly penetrating radiations. It can be concluded, from the measured cell thickness distributions, that with C3H10T1/2 cells grown on mylar, the LET variation through the whole cell is within 20% for protons and alpha-particles with energies down to 0.6 and 2.5 MeV respectively. From a comparison with thickness values reported in the literature for living or fixed embedded cells growing on plastic substrate, mean values between 2.4 and 3.4 microm and between 6 and 7.5 microm could be assumed for C3H10T1/2 cells and for the most widely used V79 cell lines respectively.

Survival and oncogenic transformation frequencies were determined through the cell cycle in hybrid cells (HeLa x human skin fibroblasts), exposed to 0.30 and 0.15 Gy 4.3 MeV (LET= 101 keV/microm) alpha-particles. The cells were synchronized by mitotic collection and irradiated at times ranging from 2 to 10 h after collection, corresponding to G1 and early S. At 0.30 Gy the highest value in the transformation frequency (1.6 +/- 0.3) x 10(-4) transformants/survivor, occurred 4 h after mitotic collection, corresponding to mid-G1 and was about twice as high as that for the asynchronous population (0.7 +/- 0.1) x 10(-4) transformants/survivor. A similar pattern was seen at 0.15 Gy albeit less marked. The results are similar to previous findings with C3H10T1/2 exposed to 0.30 Gy where (1.8 +/- 0.4) x 10(-4) and (0.8 +/- 0.4) x 10(-4) transformants/survivor were found in mid-G1 and in the asynchronous population respectively. The results of both these studies with 101 keV/microm alpha particles indicate that mid-G1 cells may be more sensitive than asynchronous cells by up to a factor of two. However, it is unlikely that such a factor is sufficient to represent the cell cycle 'hot spot' for transformation postulated to explain the inverse dose-rate effect.

(1). To determine the biological effectiveness of two solar ultraviolet (UVB) spectra with different lower wavelength thresholds for oncogenic transformation and micronucleus induction in CGL1 cells; (2). to investigate whether the action spectra for short- and long-term effects are similar; and (3). to investigate possible links between transformation and other delayed effects.Two spectra were derived from a solar UV simulator by using two filters: the first transmitted radiation with lambda284 nm, the second with lambda293 nm. The resulting spectra have the same UVA, but different UVB components (lambda between 284 and 320 nm, 19 W m(-2), and lambda between 293 and 320 nm, 13 W m(-2)). CGL1 cells were irradiated with 466 J m(-2) with lambda284 nm and 1582 J m(-2) with lambda293 nm. These doses were approximately equilethal. The endpoints examined were oncogenic transformation, and centromere-positive and -negative micronucleus frequencies in the directly irradiated cells and in transtheir progeny.At equilethal doses, the oncogenic transformation frequency in the directly irradiated cells was greater by a factor of at least 7 for lambda284 nm irradiation compared with lambda293 nm. The micronucleus induction frequency was also significantly higher with the lambda284 spectrum. Consistent with our previous findings, no delayed micronucleus formation was found in the progeny of cells exposed to lambda293 nm, while a threefold elevation above controls was seen in the progeny of cells exposed to lambda284 nm irradiation. This was also the case for formation of micronuclei with a centromere.It was found that: (1). for equilethal doses the lambda284 nm spectrum was more biologically effective than the lambda293 nm spectrum for induction of oncogenic transformation and micronucleus formation; and (2). the higher effectiveness of the lambda284 nm spectrum found at equilethal doses for delayed effects in the progeny of irradiated cells resembles that found for transformation. The results suggest that the UVB action spectrum for cell killing is different from that of some delayed effects, and from that of transformation.

Purpose To determine the RBE-LET relationship for C3H10T1/2 cell inactivation by protons in the LET range 11-33 keV/microm and to compare inactivation frequencies induced in C3H10T1/2 cells by protons and deuterons at two matching LET values in the range 11-20 keV/microm. Materials and methods C3H10T1/2 cells were irradiated with protons and deuterons at the radiobiological facility set up at the 7MV Van de Graaff accelerator at the LNL, Legnaro, Padova. Gamma rays from 60Co were used as reference radiation. Results Proton RBE values (alpha/alphagamma) for inactivation of C3H10T1/2 cells are constant around a value of 2 between 11 and 20 keV/microm and then rise sharply to reach a value of 4.2+/-1.0 at 33 keV/microm. Deuteron RBE values are 1.7+/-0.4 and 2.2+/-0.6 at LET values of 13 and 18 keV/microm respectively. Conclusions Proton RBE values with C3H10T1/2 cells are significantly larger than unity at LET values as low as 11 keV/microm. No difference in effectiveness for inactivation of C3H10T1/2 has been found between protons and deuterons at two LET values in the range 10-20 keV/microm.

The effects of cell density on transformation frequencies were studied in C3H10T1/2 cells exposed to 0.5 and 7 Gy of 200 kVp X-rays. Initial cell density strongly influenced transformation frequency; this decreased by a factor of between 4 and 10 when the initial seeding density was changed from 50 to 2500 cells/10 cm diameter Petri dish. The data were fitted with two equations: (a) an allometric function represented on a log-log scale by a straight line and (b) a sigmoidal function with plateaux between 50 and 250 cells/dish and above 600. The two curves are compared and their probabilities discussed. Our data indicate that the region between 50 and 250 cells/dish would be the most suitable region for dose-effect measurements. A study of the growth curves at 0.5 and 8.5 Gy shows that cell growth rates are not influenced by initial cell density.

Growth curves and size of the colonies of C3H10T1/2 cells exposed to low-LET radiation (31 MeV protons) were determined after 0, 1, 3, 5, and 7 Gy. The data show that: cell density at confluence was 3.3 x 10(4) cells/cm2; the initial division delay was very small; in the first 15 h the increase in the cell number was essentially the same at all doses; at 100 h the colony size distribution was very large, ranging from 0 to 7 generations, even within the control population. The temporal dependence of the growth properties of surviving and non-surviving cells was represented by the equation N = N0(Fe(a(t - dD] + (1 - F)ea/bD(1 - e - bD(1 - e - bD(t - dD]) where F is the surviving fraction, t the time of sampling, a the growth rate, d the division delay per unit dose, b the rate per unit of dose at which the non-surviving cells lose their ability to divide. The resulting values were: a = 0.029 +/- 0.002 h-1; b = 0.0041 +/- 0.0009 h-1 Gy-1 and d = 1 +/- 0.8 h Gy-1. It was found that growth curves are affected by non-surviving progeny up to 150, 200 and 250 h after irradiation at 3, 5 and 7 Gy, whereas at longer times the population consists essentially of progeny of surviving cells.