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Although the expression of radiation-induced biological effects and responses may be at either the cell, organ or organism level, induction of some of these phenomena (e.g. cancer of clastogenic and genetic effects) can have their origin in the interaction of a single charged particle with the target-containing volume (TCV) of the cell, e.g. the cell nucleus. However, the independent variable now used in both organ and cell population studies, the absorbed dose to the organ, provides no information directly on particle-TCV interactions. Even if calculated as a mean to an organized population of cells, the absorbed dose becomes a composite and confounded quantity, (FzN), in which F is the fraction of TCVs 'hit' by a particle during a given exposure, z is the mean value of z1, the energy absorbed in the TCV in a single hit, and N is the mean number of hits per affected TCV. Scientific precepts demand the avoidance of such confounded variables by achieving their isolation. The needed separation can be effected by the use of microdosimetric techniques, which make it possible to hold one component quantity constant while the others are varied. As an example, low-level radiation exposure (LLE) can be used to hold F at a constant value of 0.2 where, on average, there is but one hit per TCV. The probability of a cellular quantal response, as a function of z1 only, can then be determined by use of LLE to radiations covering a wide span of LETs. Conversely, the effect of varying only the fraction of cells hit can be studied by holding z constant. This can be accomplished by working within a narrow band of LET, but only in the LLE range. The effectiveness of preirradiation altering cell sensitivity as a function of the number of hits per TCV can be determined by working within, and somewhat above, the LLE range. In either risk assessment or the application of radiation as a pretreatment, minimal consequences can be assured only if very low-level exposure is employed in order that F will be small, and if the exposure is in a field of radiation of very low LET so that z1 will be as small as possible. That is to say, exposure conditions with low consequences cannot be specified in terms of any single quantity.

Low-dose irradiation is usually considered to be rather ineffective in producing biologically relevant effects. Yet, individual radiation absorption events within cell nuclei or whole cells interact stochastically with subcellular structures due to the multiple ionizations along primary or secondary particle tracks, depending on ionization density. Whereas radiation effects are usually seen in the context of structure and function of DNA, other cellular effects, perhaps influencing DNA by secondary biochemical mechanisms, also warrant attention. Thus, previous work from this laboratory with bone marrow that was obtained from whole-body exposed mice, has shown that single or few instantaneous radiation absorption events per cell from gamma-rays produce an acute and temporary partial inhibition of the enzyme thymidine kinase; the effect appears within about 1 h after the event, reaches its maximum at approximately 4 h and disappears completely within another 6 h. This pattern of enzyme inhibition is fully concordant with the pattern of inhibition of uptake of tritiated thymidine or 125I-labelled deoxyuridine into the DNA; also concordant is a temporary increase in the concentration of free thymidine in the blood serum of the exposed mice. The particular response of thymidine kinase was considered to relate to some, thus far unknown, repair systems and/or to a defence mechanism of the hit cells. In order to further elucidate the role of the acute and temporary partial inhibition of thymidine kinase in cellular metabolism, experiments were carried out in which mice were acutely exposed to 0.01 or 0.1 Gy and again exposed to the same dose at different times up to 12 h after the first exposure. At regular time intervals after the second exposure bone marrow cells were obtained and thymidine kinase activity was studied by various assays. The results indicate that the first acute irradiation conditioned the cells in such a way that the second acute irradiation produced either an enhanced inhibition and recovery of thymidine kinase activity, or no effect at all was seen, when the second irradiation was given between about 3 and 8 h after the first irradiation. From 8 to 12 h after the first irradiation the cells apparently resumed their original state, so that the second irradiation produced effects quite similar to those seen after a single irradiation in unconditioned cells.(ABSTRACT TRUNCATED AT 400 WORDS)

This paper presents a microdosimetric approach to the problem of radiation response by which effects produced at low doses and dose rates can be understood as the consequences of radiation absorption events in the nucleus of a single relevant cell and in its DNA. Radiation absorption at the cellular level, i.e. in the cell nucleus as a whole, is believed to act through radicals. This kind of action is called 'non-specific' and leads to the definition of an 'elemental dose' and the 'integral response probability' of a cell population. Radiation absorption at the molecular level, i.e. in sensitive parts of the DNA, is thought to act through double-strand breaks. This kind of action is called 'specific' and leads to a 'relative local efficiency'. In general, both mechanisms occur for all types of radiation; however, it is the dose contribution of both specific and non-specific effects that determines the radiation quality of a given radiation. The implications of this approach for the specification of low-dose and low dose-rate regions are discussed.

The spectral energy deposition in small volumes by 60Co gamma-rays and by 200 kV X-rays was measured with a walled spherical counter, a walled cylindrical counter and a wall-less cylindrical counter. The simulated volumes had dimensions of 0.1--3 mum. By comparing the spectra of the spherical and cylindrical walled counters the influence of the counter shape is derived. The wall effect is discussed by comparing the spectra and the mean lineal energy measured with the walled and the wall-less cylindrical counters. The influence of the counter size and of radiation quality on the energy deposition spectra is also analysed.