An illustrative comparison of the event-size distributions for gamma-rays and alpha-particles in the whole mammalian cell nucleus.
- PubMed: 9881727
Abstract
PURPOSE: Recent laboratory studies of endpoints designated as due to radiation-induced genomic instability have cast doubt on the validity of the current theoretical framework. Under this framework extrapolations are made from directly determined risks of radiation-induced cancer to those circumstances for which no direct information exists, namely at low doses and dose rates at low LET and at low dose exposures to high LET radiations. Based upon an approach in which the 'state' of the genome, as exemplified by the pattern of gene expression, rather than the base sequence of the genomic DNA, is taken to be the origin of genomic stability, it is hypothesized that the critical factor determining the likelihood of destabilization by ionizing radiation is the dose to the whole cell nucleus. CALCULATIONS: The frequency distributions of event sizes from two qualities of radiation, low LET y-rays and 5 MeV alpha-particles, are compared with 60Co gamma-rays being taken to be a low LET reference radiation in determining the RBE of other radiation qualities. In the absence of measured event-size distributions for 60Co gamma-rays in spheres of similar size to the human cell nucleus, the 4.5 microm sphere has been chosen as illustrative. Frequency distributions for 5 MeV alpha-particles are derived, based on the idealized situation of a parallel beam of constant LET, with all particles traversing the sphere. RESULTS: When compared for a dose of 1 mGy the event-size (dose) distributions of the two qualities do not intersect. It is estimated that only 0.4% of the energy from the alpha-particles falls in the range of event sizes that can be produced by 60Co gamma-rays. CONCLUSIONS: Contrary to belief over the past 50 years, there is, in this low dose range, no 'continuum' based upon quantities such as LET or lineal energy that would provide a basis for extrapolation from measured RBE values. RBE is thus seen to be purely empirical. In addition, the potential to induce effects in bystander cells is not considered when deriving weighting factors for alpha-particles of the type that contribute significantly to public exposure to environmental radiation.
An illustrative comparison of the event-size distributions for gamma-rays and alpha-particles in the whole mammalian cell nucleus.
An illustrative comparison of the event-size distributions for c-raysand a-particles in the whole mammalian cell nucleusK. BAVERSTOCK†* and M. THORNE‡(R eceived 21 M ay 1998; accepted 17 J uly 1998)
Abstract. agents) by relating the probability of developing aPurpose: Recent laboratory studies of endpoints designated as due cancer to the exposure of the target tissue to radi-to radiation-induced genomic instability have cast doubt on the ation, expressed in terms of absorbed tissue dose.validity of the current theoretical framework. Under this frame- This applies for certain qualities of radiation, mainlywork extrapolations are made from directly determined risks of low LET, within a limited range of mainly ‘high’radiation-induced cancer to those circumstances for which nodirect information exists, namely at low doses and dose rates at doses and dose rates. Radiation is most commonlylow LET and at low dose exposures to high LET radiations. understood to lead to cancer through the accumula-Based upon an approach in which the ‘state’ of the genome, as tion of mutations to speci c genes, many of whichexempli ed by the pattern of gene expression, rather than the are supposed to be responsible for growth controlbase sequence of the genomic DNA, is taken to be the origin of and ‘genomic housekeeping’. The absorption of radi-genomic stability, it is hypothesized that the critical factordetermining the likelihood of destabilization by ionizing radiation ation leads to ionization, either directly in the DNAis the dose to the whole cell nucleus. of these genes, or resulting in the generation ofCalculations: The frequency distributions of event sizes from two reactive free radicals from other components of thequalities of radiation, low LET c-rays and 5MeV a-particles, nucleus, including water, which chemically attackare compared with 60Co c-rays being taken to be a low LET the DNA. The resultant chemical damage leads toreference radiation in determining the RBE of other radiationqualities. In the absence of measured event-size distributions for changes in the genomic sequence, either disabling,60Co c-rays in spheres of similar size to the human cell nucleus, activating or over-expressing speci c genes. Thesethe 4.5mm sphere has been chosen as illustrative. Frequency changes are assumed to be inherited in a stabledistributions for 5MeV a-particles are derived, based on the manner in progeny of the irradiated cells, so creatingidealized situation of a parallel beam of constant LET, with all a clone of cells, which through further accretion ofparticles traversing the sphere.R esults: When compared for a dose of 1mGy the event-size (dose) mutations will, after a latent period of up to severaldistributions of the two qualities do not intersect. It is estimated tens of years, express the malignant phenotype.that only 0.4% of the energy from the a-particles falls in the The probability of cancer induction is often lin-range of event sizes that can be produced by 60Co c-rays. early related to absorbed tissue dose, or more-or-lessConclusions: Contrary to belief over the past 50 years, there is, in so, in an irradiated tissue or organ, and very rarelythis low dose range, no ‘continuum’ based upon quantities suchas LET or lineal energy that would provide a basis for extrapola- according to a power of dose greater than two. Thistion from measured RBE values. RBE is thus seen to be purely can be interpreted as indicating that the initialempirical. In addition, the potential to induce e å ects in bystander change, leading to malignancy, takes place in a singlecells is not considered when deriving weighting factors for a- cell from which the malignant clone is derived, i.e.particles of the type that contribute signi cantly to public cancer is ‘monoclonal’ in origin. It is clear that cellsexposure to environmental radiation. receive signals from their neighbours that in uencetheir growth control, but if it were necessary to1. Introduction induce relevant changes in several cells at the sametime, the e å ects would be related to higher powersRadiation is a reproducible, if somewhat weak of dose.carcinogen, which through epidemiological studies The long latency for radiation-induced cancerson exposed populations has been relatively well and the fact that malignant cells exhibit degrees ofquanti ed (compared with many other carcinogenic malignancy, both point to cancer being a progressiverather than an ‘on/o å ’ process. Conventional radio-*Author for correspondence: e-mail: 106305.2424@compuserve.com biology sees the latent period as one in which a†WHO REMPAN Project Oæ ce, WHO Collaborating ‘transformed’ or ‘initiated’ cell acquires the additionalCentre, Authority for Radiation and Nuclear Safety, PL/PO speci c mutations that ultimately result in the malig-Box 14, FIN–00881, Helsinki, Finland. nant karyotype and phenotype. Under most models‡Hollybrook, 38 Pondtail Road, Horsham, West Sussex RH125HR, UK. these mutations are considered independent of one0955–3002/98 $12.00 © 1998 Taylor & Francis Ltd
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