Increased complexity of radiation-induced chromosome aberrations consistent with a mechanism of sequential formation.

Complex chromosome aberrations (any exchange involving three or more breaks in two or more chromosomes) are effectively induced in peripheral blood lymphocytes (PBL) after exposure to low doses (mostly single particles) of densely ionising high-linear energy transfer (LET) alpha-particle radiation. The complexity, when observed by multiplex fluorescence in situ hybridisation (m-FISH), shows that commonly four but up to eight different chromosomes can be involved in each rearrangement. Given the territorial organisation of chromosomes in interphase and that only a very small fraction of the nucleus is irradiated by each alpha-particle traversal, the aim of this study is to address how aberrations of such complexity can be formed. To do this, we applied theoretical "cycle" analyses using m-FISH paint detail of PBL in their first cell division after exposure to high-LET alpha-particles. In brief, "cycle" analysis deconstructs the aberration "observed" by m-FISH to make predictions as to how it could have been formed in interphase. We propose from this that individual high-LET alpha-particle-induced complex aberrations may be formed by the misrepair of damaged chromatin in single physical "sites" within the nucleus, where each "site" is consistent with an "area" corresponding to the interface of two to three different chromosome territories. Limited migration of damaged chromatin is "allowed" within this "area". Complex aberrations of increased size, reflecting the path of alpha-particle nuclear intersection, are formed through the sequential linking of these individual sites by the involvement of common chromosomes.

Chromosome breakpoint distribution of damage induced in peripheral blood lymphocytes by densely ionizing radiation.

PURPOSE: To assess the chromosomal breakpoint distribution in human peripheral blood lymphocytes (PBL) after exposure to a low dose of high linear energy transfer (LET) alpha-particles using the technique of multiplex fluorescence in situ hybridization (m-FISH). MATERIALS AND METHODS: Separated PBL were exposed in G0 to 0.5 Gy 238Pu alpha-particles, stimulated to divide and harvested approximately 48 - 50 hours after exposure. Metaphase cells were assayed by m-FISH and chromosome breaks identified. The observed distribution of breaks were then compared with expected distributions of breaks, calculated on the assumption that the distribution of breaks is random with regard to either chromosome volume or chromosome surface area. RESULTS: More breaks than expected were observed on chromosomes 2 and 11, however no particular region of either chromosome was identified as significantly contributing to this over-representation. The identification of hot or cold chromosome regions (pter,p,cen,q,qter) varied depending on whether the data were compared according to chromosome volume or surface area. CONCLUSIONS: A deviation from randomness in chromosome breakpoint distribution was observed, and this was greatest when data were compared according to the relative surface area of each individual chromosome (or region). The identification of breaks by m-FISH (i.e., more efficient observation of interchanges than intrachanges) and importance of territorial boundaries on interchange formation are thought to contribute to these differences. The significance of the observed non-random distribution of breaks on chromosomes 2 and 11 in relation to chromatin organization is unclear.

Regulation of the apoptotic response to radiation damage in B cell development.

B lymphocyte precursor cells are ultrasensitive to DNA damage induced by irradiation and drugs and die by apoptosis at very low levels of exposure. Previous studies have shown that this high level sensitivity is p53-dependent, associated with very low level expression of Bcl-2 protein and can be reversed by expression of a bcl-2 transgene. We show here that transition from the pro-B to pre-B and then mature B cell stages of murine lymphopoiesis is accompanied by changes in proliferating cells in sensitivity to X-irradiation induced apoptosis and that this is paralleled by variation in the ratio of anti-(Bcl-2/Bcl-chiL) to pro-(Bax) apoptotic proteins. These are however not fixed or invariant features of developmental stage as they can be modulated by interactions via adhesive interactions with stromal cells, stromal proteins and growth factors. We interpret these data in the context of the stringent developmental regulation of clonal lymphopoiesis and the contingency programming of cells that have extensive proliferative potential with a very low threshold for apoptosis following DNA damage.

Carcinogenicity of radon/radon decay product inhalation in rats--effect of dose, dose rate and unattached fraction.

PURPOSE: The effects of inhalation of radon/radon decay products at different total doses, dose rates and 'unattached' fractions were investigated in a life span study in rats. MATERIALS AND METHODS: 1574 rats inhaled radon/radon decay products in a purpose-built recirculating exposure system that provided stable/reproducible exposure conditions. 501 were maintained as controls. RESULTS: Lung tumour incidences were significantly elevated in most exposed groups. The study power was insufficient to resolve the shape of the dose and dose rate response curves, but combination of this data with that from other studies demonstrated that for high cumulative exposures, the lifetime excess absolute risk increases with increasing exposure durations and for low cumulative exposures the opposite trend occurs. Exposure did not increase leukaemia incidences. A small number of non-lung tumour types including mammary fibroadenoma showed elevated incidences in some exposed groups, however not consistently across all exposure groups and showed no dose or dose rate relationship. CONCLUSIONS: Radon/radon decay product exposure caused excess lung tumours in rats along with limited non-lung effects. The results are consistent with the findings that at low cumulative exposures decreasing exposure concentrations or protracting the time over which the dose is delivered, reduces lung tumour risk. At higher levels, decreasing exposure concentrations or protracting exposure time increases lung tumour risk.

A comparison of peribulbar and retrobulbar anesthesia for vitreoretinal surgical procedures.

OBJECTIVE: To compare the efficacy of retrobulbar and peribulbar anesthetic techniques for vitreoretinal surgical procedures. DESIGN: Prospective, randomized, double-blind study. SETTING: A large university teaching hospital. PARTICIPANTS: One hundred sixteen consecutive patients who were scheduled for vitreoretinal surgical procedures. METHODS: Patients who were undergoing vitreoretinal surgical procedures were divided into four separate groups, depending on the type of surgical procedure planned. Equal numbers of patients in each group of patients who were undergoing a surgical procedure were randomly assigned to either the retrobulbar or peribulbar block-treated group. Anesthesia, akinesia, need for block supplementation, and patient acceptance were measured. RESULTS: Both retrobulbar and peribulbar anesthetic techniques provided equal levels of akinesia and analgesia, with each requiring intraoperative supplementation in 32%. CONCLUSION: Peribulbar block can be expeditiously and efficiently used for a full range of vitreoretinal surgical procedures.

Comment on the ratio of chromosome-type dicentric interchanges to centric rings for track-clustered compared with random breaks.

Evidence has been published suggesting that the ratio of chromosome-type dicentric interchanges to centric rings (D/R or F) is significantly lower for neutrons than for X or gamma rays, and it is proposed that a low D/R could be used as a "fingerprint" for high-LET radiations. One explanation offered for this observation is that the closely spaced, clustered breaks confined to linear tracks will favor intrachanges, as opposed to interchanges, leading to a lower D/R, while the more scattered, random breaks of low-LET radiations will favor the reverse situation and elevate the D/R. We have tested this suggestion empirically by constructing various modeled tracks and grids of breaks which satisfy the proposed conditions. These have then been superimposed, in random orientation, on an array of hexagons, representing a planar section through the interphase arm domains of 14 polarized, metacentric, G1-phase chromosomes, and the D/R computed from the interaction of break clusters with the arms. The ratios recovered were essentially the same for the four different break distributions tested, and we conclude that, for this simple model, the determinant of the D/R is the arm arrangement in the array, rather than the disposition of the breaks.

The spatial and temporal distribution of inhaled UO2 particles in the respiratory tract of the rat. I. Pulmonary tissue.

An analysis is described of the mass distribution of inhaled UO2 particles in the pulmonary tissue of rats by random sampling of fields in autoradiographs of histological sections. The degree of nonrandomness is compared between fields, between sections, and between lobes and interpreted in terms of the physical distribution of UO2. The error in the estimate of the mean number of charged-particle tracks from UO2 per field in the pulmonary tissue by selective tissue sampling is related to the degree of nonrandomness of the UO2 distribution. Estimates of this error in the lungs from nine animals range from 5.2 to 8.4%. When estimating this error, it is concluded that, in the case of the rat, sections should be taken at intervals of 3 mm or less throughout the lobes.

Dependence of the yield of DNA double-strand breaks in Chinese hamster V79-4 cells on the photon energy of ultrasoft X rays.

Induction of DNA DSBs by low-LET radiations reflects clustered damage produced predominantly by low-energy, secondary electron "track ends". Cell inactivation and induction of DSBs and their rejoining, assayed using pulsed-field gel electrophoresis, were determined in Chinese hamster V79-4 cells irradiated as a monolayer with characteristic carbon K-shell (CK) (0.28 keV), aluminum K-shell (AlK) (1.49 keV), and titanium K-shell (TiK) (4.55 keV) ultrasoft X rays under aerobic and anaerobic conditions. Relative to (60)Co gamma rays, the relative biological effectiveness (RBE) for cell inactivation at 10% survival and for induction of DSBs increases as the photon energy of the ultrasoft X rays decreases. The RBE values for cell inactivation and for induction of DSBs by CK ultrasoft X rays are 2.8 +/- 0.3 and 2.7 +/- 0.3, respectively, and by TiK ultrasoft X rays are 1.5 +/- 0.1 and 1.4 +/- 0.1, respectively. Oxygen enhancement ratios (OERs) of approximately 2 for cell inactivation and induction of DSBs by ultrasoft X rays are independent of the photon energy. The time scale for rejoining of DNA DSBs is similar for both ultrasoft X rays and 60Co gamma rays. From the size distribution of small DNA fragments down to 0.48 kbp, we concluded that DSBs are induced randomly by CK and AlK ultrasoft X rays. Therefore, ultrasoft X rays are more efficient per unit dose than gamma radiation at inducing DNA DSBs, the yield of which increases with decreasing photon energy.

Irradiation of DNA with 193 nm light yields formamidopyrimidine-DNA glycosylase(Fpg) protein-sensitive lesions.

Irradiation of aqueous solutions of plasmid DNA (pUC18) at pH 7.6 with 193 nm laser light results in low yields of prompt single strand breakage (air-saturated sample phi ssh = [1.5 +/- 0.1] x 10(4), argon-saturated sample phi ssh = [0.9 +/- 0.1] x 10(4). Treatment of the irradiated DNA samples with Escherichia coli formamidopyrimidine-DNA glycosylase (Fpg) protein results in an approximate 20-fold increase in the yield of single strand break-age (air-saturated sample phi fpg = [33.1 +/- 3.1] x 10(-4), argon-saturated sample phi fpg = [23.8 +/- 2.6] x 10(-4). This result indicates that 193 nm light induces other modification(s) (most likely of the purine moieties) that are 20 times more abundant than prompt strand breakage within the DNA matrix.

Susceptibility to radiation-induced leukaemia/lymphoma is genetically separable from sensitivity to radiation-induced genomic instability.

PURPOSE: To determine whether there is a relationship between the genetics underlying the susceptibility to radiation-induced leukaemia in CBA/H (acute myeloid leukaemia, AML) and C57BL/6 (thymic lymphoma, TL) mice, and the genetics underlying the sensitivity of CBA/H (sensitive) and C57BL/6 (resistant) mice to radiation-induced chromosomal instability. MATERIALS AND METHODS: CBA/H, (CBA/H x C57BL/6)F1, F1 x CBA/H, F1 x C57BL/6 and F1 x F1 mice were exposed to a single acute dose of 3.0 Gy X-rays. AML and TL were diagnosed over the subsequent 30 months. RESULTS: There was no statistically significant difference in the incidence of AML in F1, F1 x F1, F1 x CBA/H and F1 x C57BL/6 mice, which was approximately 50% that in CBA/H mice. AML susceptibility is therefore a dominant polygenic trait, and both susceptibility and resistance (variable penetrance) CBA/H and C57BL/6 loci are involved. The incidence of TL in the FM and F1 x CBA/H mice was negligible, indicating that TL susceptibility is a recessive trait. As the TL incidence in the F1 x C57BL/6 mice was about half that in C57BL/6 mice, one recessive locus is probably involved. CONCLUSIONS: AML susceptibility in CBA/H mice is a dominant trait in contrast to the recessive inheritance of CBA/H sensitivity to radiation-induced chromosomal instability. TL-susceptibility in C57BL/6 is a recessive trait in contrast to the dominant inheritance of C57BL/6 resistance to radiation-induced chromosomal instability.

Chromosome 2 hypersensitivity and clonal development in murine radiation acute myeloid leukaemia.

Acute myeloid leukaemias induced by ionizing radiation in mouse are characterized by chromosome (chr) 2 aberrations. While it is known that chr 2 aberrations form early and in abundance post-irradiation, unequivocal evidence for hypersensitivity of chr 2 in the first post-irradiation mitoses is lacking. Here it is established that chromosomal aberrations detected in bone marrow cells by chromosome painting are induced in all mice at an approximately 2-fold greater frequency in chr 2 by comparison with chrs 1 and 3 at 24 and 48 h following in vivo whole-body X-irradiation. Long-term follow up studies (to 15 months post-irradiation) indicated that chromosomal hypersensitivity is accounted for largely by the existence of hot-spots for aberration formation on sensitive chromosomes. Analysis of clonal developments suggested that chr 2 aberrant clones are selected for entry into the proliferating bone marrow cell compartment in preference to cells with other aberrations and that these clones in general have a higher proliferative potential. However, neither the induction of chr 2 aberrations nor the presence of a chr 2 aberrant clone specifically predict the development of AML in an individual irradiated mouse. Nonetheless these events or sub-groups of these events are necessary for AML development.

X-ray-induced simple, pseudosimple and complex exchanges involving two distinctly painted chromosomes.

PURPOSE: To detect simple, pseudosimple and complex chromosome exchanges in X-ray-induced aberrations involving two distinctly painted chromosomes. Each visibly complex two-paint exchange was analysed to determine the number of breaks and chromosomes necessary to derive the pattern. In addition, the number of associated paint junctions was scored to assess the frequency of non-reciprocal exchanges. MATERIALS AND METHODS: Metaphase spreads were prepared from a human primary fibroblast cell line irradiated with 2, 4 and 6 Gy 250kV X-rays. FISH-painting was performed with distinctly labelled probes for chromosomes 1 and 2, and a pancentromeric probe. RESULTS: From a total of 78 two-paint exchanges observed, 35 were apparently simple, with no additional counterstain chromatin, and 43 were visibly complex with two-colour painting, of which 23 contained at least one pseudosimple exchange. A detailed analysis of the number of two-paint colour junctions showed that at least 50% of the visibly complex exchange patterns involved non-reciprocal exchanges. The simple and complex exchange dose-response curves were considered to be linear and curvilinear respectively. CONCLUSION: The frequency of non-reciprocal rejoining events within complex exchanges is consistent with an interaction model based on the free exchange of multiple break-ends. In addition, the simple and complex exchanges have distinct dose-response curves, in agreement with previous data for single-painted exchanges corrected for pseudosimples.

In vivo chromosomal instability and transmissible aberrations in the progeny of haemopoietic stem cells induced by high- and low-LET radiations.

PURPOSE: To study stable and unstable chromosomal aberrations in the haemopoietic cells of CBA/H mice after exposure to both high- and low-LET radiations. MATERIALS AND METHODS: Chromosomal aberrations were scored in the clonal progeny of X-, alpha- or non-irradiated short-term repopulating stem cells using the spleen colony-forming unit (CFU-S) assay, 12 days post-transplantation and in the bone marrow reconstituted by X-, neutron- or non-irradiated exogenous (transplanted) or endogenous (X- or neutron whole-body-irradiated) long-term repopulating stem cells for up to 24 months. RESULTS: Chromosomal instability was demonstrated in 3-6% of cells in all cases. After transplantation of X- or neutron-irradiated bone marrow approximately 8% of cells with stable aberrations were recorded at all times. After 3Gy X- or 0.5 Gy neutron- whole-body irradiation stable aberrations were detected in approximately 17 and 5% of cells respectively. CONCLUSIONS: Chromosomal instability induced in vitro can be transmitted in vivo by transplantation of haemopoietic stem cells exposed to high- or low-LET radiations. Comparable instability can be induced and shown to persist for the remaining lifetime after whole-body irradiation. There was no direct relationship between the expression of stable and unstable aberrations and significant interanimal variation in the expression of both stable and unstable aberrations.

Investigation of lung tumour induction in BALB/cJ mice following paternal X-irradiation.

Evidence of an enhanced incidence of lung tumours (benign adenomas and adenocarcinomas) was sought in the BALB/cJ mouse following paternal germ cell X-irradiation. In a series of replicate studies spanning approximately 1 year, males were exposed to single, acute X-ray doses of 0, 250 and 500 cGy. In each of the 2 consecutive weeks immediately thereafter they were placed with two females to generate progeny that were derived from irradiated post-meiotic cells (spermatozoa to late spermatids). These animals were then examined at 8 or 12 months for lung tumours. While the proportion of fertile females and mean litter size was affected by the radiation, showing a dose-dependent, dominant lethal response, and while cases of mutant offspring were detected, the paternal radiation did not affect lung tumour incidence in the offspring. The incidence did not vary significantly between germ cell stages irradiated (week of mating), sex of offspring, or radiation dose. However, significant differences between lung tumour incidence (mostly representing benign adenomas) were found between different replicates, these being high at the start of the study, declining and then rising to yet higher levels at its close. The finding that lung tumour incidence in BALB/cJ mice is not affected by paternal germ cell irradiation does not accord with Nomura's reports using other strains of mice. This, in turn, weakens biological support for a causal association between the raised incidence of childhood leukaemia and non-Hodgkin lymphoma near Sellafield and the father's recorded radiation exposure during employment by the nuclear industry.

Effectiveness of 0.28 keV carbon K ultrasoft X-rays at producing simple and complex chromosome exchanges in human fibroblasts in vitro detected using FISH.

PURPOSE: To study the effects of carbon K ultrasoft X-rays, which produce a single photoelectron with a track length of < 7 nm, on the production of structural chromosome-type changes. MATERIALS AND METHODS: Untransformed human fibroblasts (HF12) were irradiated in G1 phase. Aberrations were analysed using fluorescence in situ hybridization using multi-coloured chromosome specific DNA probes for chromosomes 1 and 2 and an alpha-satellite pan-centromeric probe. RESULTS: CK X-rays have a high efficiency per unit absorbed dose for producing simple and complex exchanges. Mean absorbed doses of 0.33-1.31 Gy produce simple exchanges with a predominantly linear dose dependency, and visibly complex exchanges increased by more than the power 2 of the dose, with no evidence of a linear component. The proportion of exchanges that are visibly complex ranged from 9% to 46%. CONCLUSIONS: The linear response for simple exchanges provides further support to the hypothesis that damaged DNA may be able to interact with undamaged DNA. The high proportion of complex exchanges may be due to the increased efficiency of double-strand break induction and to the high density of tracks per unit absorbed dose targeting pre-existing sites, some of which may be close to the incident nuclear membrane.

Dose- and time-response relationships for lethal mutations and chromosomal instability induced by ionizing radiation in an immortalized human keratinocyte cell line.

PURPOSE: To investigate the relationship between two well-established delayed effects of ionizing radiation, experiments were conducted to determine the induction and expression of lethal mutations (delayed reproductive death) and chromosomal instability with respect to dose and time in a human immortalized keratinocyte cell line. METHODS: HPV-G cells were gamma- or alpha-irradiated and maintained in culture for up to 72 population doublings. At intervals, measurements were made of cloning efficiency and the cells examined for apoptosis and cytogenetic aberrations. RESULTS: The descendants of cells surviving 1 or 3 Gy gamma-irradiation, but not 0.5 Gy gamma-irradiation, exhibited a reduced colony-forming efficiency. The reduction persisted at a constant rate of 15-20% clonogenic cell loss per population doubling for up to 72 population doublings. Apoptosis was demonstrated in all colonies in the 1 and 3 Gy groups at 30 and 72 population doublings post-irradiation but not in the 0.5 Gy group. A significant persistent reduction in colony-forming ability (approximately 80%) was demonstrated in the progeny of cells irradiated with 0.5 Gy alpha-particles. After 30 population doublings, the proportion of chromosomally aberrant cells was significantly greater than control values for all doses of both high- and low-LET radiations. The major cytogenetic aberrations (chromatid breaks, chromosome fragments and minutes) were consistent with the transmission of chromosomal instability. The expression of instability declined between 30 and 72 population doublings in the 0.5 Gy and 3 Gy gamma-irradiation groups, but persisted up to 72 population doublings in the 1 Gy group. The expression of chromosomal instability was greater in the descendants of alpha-irradiated cells and showed little evidence of reduction with time. CONCLUSIONS: Unstable aberrations characteristic of radiation-induced chromosomal instability may commonly result in apoptosis and account for a component of the delayed reproductive death/lethal mutation phenotype in HPV-G cells. However, the absence of lethal mutations in the descendants of 0.5 Gy gamma-irradiated cells indicates a low-LET threshold effect for this particular endpoint. Overall, and particularly at low doses, there is no direct correlation between the two endpoints, indicating the absence of a simple relationship between these manifestations of radiation-induced genomic instability.

The uptake and turnover of 90Sr in the human skeleton.

In the United Kingdom, measurements have been made of the concentration of 90Sr in human bone from 1955 to 1970, and in human diet since 1958. A correlation of these two series of observations has enabled estimates to be made of (i) the fraction of the dietary intake of 90Sr that reaches the skeleton, (ii) the rate of turnover of 90Sr in the skeleton, and (iii) the way in which both these parameters vary with age. The results may be used to predict future levels of 90Sr in human bone from measurements of the radionuclide in diet, and also to calculate the radiation doses received by tissues in bone from intakes of 90Sr and 89Sr.

Influence of macrophages on microdistribution of inhaled UO2 aerosol in rat lung.

Following the inhalation of an aerosol of UO2 (mass median aerodynamic diameter = 3 microns and geometric standard deviation = 1.6) the lungs of male albino rats were populated by foci containing UO2 particles. A method of neutron-induced autoradiography on Lexan plastic was used to reveal these foci in thin sections cut from the lung. For masses of UO2 in the lung that differed by more than a factor of 10 (39 to 450 micrograms) the number of foci per g of lung increased, but not in proportion to the mass of UO2 deposited. This limited increase in the number of foci was considered to result from physiological limitations on the number of alveolar macrophages available for engulfing the UO2 particles.

Frequency and distribution studies of asymmetrical versus symmetrical chromosome aberrations.

Two aspects of the relationship between Asymmetrical (A) and Symmetrical (S) radiation-induced chromosomal aberrations are considered in this paper. (1) Are A and S truly alternative modes of lesion interactions? Relative frequencies for chromatid-type and chromosome-type are examined, and new lymphocyte data using banding is used to look at this, and also for parallelism in chromosome participation of the two forms for various aberration categories. All the tests applied suggest that A and S are alternative interaction modes. (2) The long-term survival characteristics of A and S are discussed, and the differences in expected frequencies of derived S per surviving cell from chromosome-type and chromatid-types are stressed. Since many in vivo tissues have varying mixtures of potential chromatid and chromosome aberration-bearing target cells, ultimate cell survival and derived S frequencies may differ between tissues for the same absorbed dose. An Appendix gives Relative Corrected Lengths (RCL) for chromosomes of the human karyotype which should be used when testing the various exchange aberration categories for random chromosome participation.

Retinoblastoma: a model for deriving the mutation rate without using any estimate of the size of the population at risk.

Paediatric cancer of the retinae arises from a transient population of stem cells whose growth and decay are responsible for the development of the fully differentiated photo-receptors and nerve cells. A model is described which fits the data on the incidence of bilateral retinoblastoma and gives the somatic mutation rate without using an estimate of the size of the population at risk. It also gives the shape of the retinoblast growth/decay curve. The model has been tested on two independent sets of data from the USA, and given that both sets are representative of the USA as a whole, there seems to have been little change in the somatic mutation rate over the last 30 or so years. For a total retinoblast formation of 4 x 10(6) cells, the average mutation rate is 2.94 x 10(-7) per cell per year.