
False
Alarm or Public Health Hazard?: | ||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||||
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Figure 1. The evolution of health protection standards for nuclear workers is shown. It can be seen that international and national radiation protection commissions have had to revise their recommendations repeatedly in the past.Source: U.S. Department of Energy, Office of Environmental Management [7]. |
Defining Safe Dose
Such a tradition has led some scientists to suggest the existence of a practical dose threshold for low-LET radiation [3,4,5,8,9]. Others have expressed the opinion that the data have been inconclusive on the question of whether a safe dose threshold exists or not [2,10].
A safe dose and safe dose rate of ionizing radiation (i.e., zero radiogenic risk) means that all exposed persons remain unharmed during and after the exposure. In other words, no one will suffer from a radiation induced cancer or die prematurely from other radiogenic disease. A non-zero risk at any dose or dose rate, on the other hand, means that no one is safe during exposure and afterward; a certain fraction of exposed persons will suffer from radiation induced cancer and die prematurely, whereas the rest will remain unharmed.
Much is at stake in considering the existence of a harmless dose threshold. If this notion is a fallacy, as is asserted here, then raising the present radiation safety standards--as advocated by the Health Physics Society [11]--would lead to an even larger increase of cancers and genetic defects worldwide over those already initiated by past radioactive releases. Such an action would be indefensible.
In contrast, the present authors conclude that the proposition of a safe dose range, a safe dose rate, or a reduced biological effectiveness at protracted low-dose exposures has been shown to be false. This firm conclusion is based on an aggregate of independent and diverse findings, such as studies of excess cancers (including leukemias and thyroid cancers) in nuclear workers exposed to accumulated occupational doses comparable to natural background or in children who had been x-rayed in utero at acute doses of a few tenths of cGy (rem) [12,13].
From a worldwide perspective, genetic effects are of even greater potential consequence for public health than the induction of somatic malignancies discussed above. Ample evidence is accumulating of chromosome aberrations induced by low doses without threshold that carry a high probability for transmitting detriment to future generations [12,13,14,15]. Recent studies found evidence for generationally delayed detriment as a consequence of radiogenically induced genomic instability [16]. Radiobiological studies on human cell models in vitro, at low doses and at varying dose rates, have also been consistent with epidemiological studies in contradicting both a conjectured reduced biological effectiveness at low doses and low dose rates and a safe dose threshold [17,18].
The conclusion reached here is that any increase in radiation exposure above unavoidable background leads to significant added risks for somatic and/or genetic health detriment whether for populations at large (e.g., from venting or fallout from weapons tests and from releases from nuclear production sites or waste repositories) or for individuals (e.g., from occupational or medical exposures). Comprehensive and independent assessment of risks versus expected benefits will pose enormous ethical, economic, and political challenges to present national and international institutions, both public and private, which constitutionally or by international agreements have been entrusted with serving the peoples well being.
A Microdosimetric Argument
By combining microdosimetric considerations for the induction of mutations in the cell nucleus with low-dose epidemiological findings, an even more compelling argument against the existence of a safe dose threshold can be made as follows [19].
Tracking Imperfections of Cell Repair
In order to consider the meaning of dose at the cellular level we must relate the number of primary ionization tracks traversing a cell nucleus to a given dose. The smallest possible dose is not a fraction of a Gray but a single traversal of an ionizing track through the cell nucleus.
As we know, the energy of x-rays and gamma-rays is deposited in biological material via Compton-electrons and photo-electrons. One can, therefore, use the calculations of Paretzke and a recursion method [20] to convert the energy of an x-ray or gamma-ray into a number of electrons and their energy distribution. Thus, it is possible to convert the original photon energy to electrons and to calculate their summarized range [21,22].
With help of the relation 1cGy = 6.24 x 1010 keV/g one can now determine how many photons of a given energy are required to deposit a dose of 1 cGy. With this information the corresponding number of electron tracks is obtained.
Since the average dimensions of a mammalian cell and its nucleus are known [23], we can calculate the number of nuclear traversals per dose unit for X- and gamma-radiation of different origin [Table 1].
Gaps in the Repair Process
We know from numerous experiments with model systems that enzymatic repair processes are seen to work without impairment even at doses of a few Grays [24,25,26,27,28]. Furthermore, it has been confirmed repeatedly in studies with human cells in vitro that repair is achieved within six hours or less even after doses of several Grays [29,30,31,32]. There is also confirmed information on the number and type of DNA lesions.
There are, however, numerous references in the literature supporting the assertion that certain DNA lesions are not repaired or are misrepaired1. For example:
With the information discussed so far, we can examine whether there is or is not any safe dose.
Challenging the Notion of a Safe Threshold
Imagine the following scenario, in which the repair processes are presumed to work flawlessly up to a certain dose of a few cSv (100 cSv = 1 Sv).
In this scenario the individuals could accumulate rather high doses in many small dose fractions. No increased cancer risk should be detectable, however, in a long term follow up. Since it is acknowledged that the accumulated high dose, given all at once, will increase the cancer risk, we would have to conclude that each of the small dose fractions is harmless and that a dose threshold and a safe dose rate would indeed be real.
If, however, the long term followup studies were to reveal increased cancer incidence in the population exposed only to small dose fractions over a long time period, then the presumption of an error-free repair system, even at low doses, would be untenable. Also, the idea of a safe dose threshold would be wrong.
Dose fractions or doses, respectively, and the derived number of tracks per cell nucleus per exposure, drawn from a number of epidemiological studies of exposed persons that have been accepted in the scientific literature, are compiled in Table 2. In all nine studies a statistically significant increase in cancer incidence was observed in the exposed population.
These studies show that the following doses cannot be regarded as safe with respect to cancer induction:
9 cSv, 7.5 cSv, 4.6 cSv, 1.6 cSv, 1 cSv, 0.9 cSv, 0.5 and 0.1 cSv
We can conclude, therefore, that whenever an ionizing track traverses a nucleus of a mammalian cell there is always a non-zero chance that it will cause a carcinogenic lesion and that the lesion will remain unrepaired, will be inherently unrepairable, or will be misrepaired. In short, there is an intrinsic failure rate in the repair system even at the lowest conceivable doses and rates.
The Flawed Case for a Safe Dose
In summary, for the essential stochastic end points of radiation damage (cancer induction and mutation) the idea of a safe dose threshold and of a safe dose range must be given up. According to present epidemiological data, only the linear (curve 3) or the supralinear (curve 4) dose-effect relationships shown in Figure 2 are consistent with scientific evidence from human data. Recently, radiobiologists have also come to the conclusion that cancer can be initiated as a result of a single radiation track through a single cell nucleus [44].
![]() |
Figure 2: Various models for the shape of dose effect curves have been proposed, mainly to allow extrapolation from effects found at higher doses to effects in the low dose range relevant to occupational exposure and radiation protection. The model represented by the J-shaped curve (1) presumes that at low doses detrimental effects are even lower as compared to those occuring in the unexposed population. This so-called hormetic effect has, however, no scientifically credible foundation for stochastic effects such as radiogenic mutation and cancer induction. Model 2 (curve 2) assumes no detrimental effect up to a dose threshold T, followed by a linear increase at higher doses. No supporting data can be found for this model as long as stochastic effects of radiation are considered. Model 3 (curve 3), the most widely accepted, assumes a linear relationship between absorbed dose and detrimental effect without threshold. Numerous supporting data can be found in the relevant literature. In the linear-quadratic relation (curve 5) the assumption is made that a linear extrapolation from high to low doses would overestimate the detrimental effects and that dose rate effectiveness factors (DREF) between 2 and 5 have to be employed to describe the detrimental effects at the low dose region. In the BEIR V Report [2] the committee states: There are scant human data that allow an estimate of the dose rate effectiveness factor and for most other cancers in the life span study (LSS) the quadratic contribution is nearly zero, and the estimated DREFs are near unity. The supralinear model (curve 4) describes the observation made by several investigations in the low dose range in model systems as well as epidemiological research. There is evidence that the supralinear curve correctly describes the excess cancer risk of the A-bomb survivors exposed to doses below 20 cGy [48]. |
The proponents of dose thresholds and even of hormetic effects will argue that there are many studies in which no statistically significant radiation effect was found by the authors. These studies are, however, unsuited for deciding whether there is a dose threshold or not. Inability to find a significant effect can never be an argument for a safe dose. In many of these studies the followup periods were too short, the size of the cohorts was too small, or important confounding factors were not properly taken into account.
A group of independent scientists (physicians and epidemiologists), assembled and sponsored by Physicians for Social Responsibility, have critically reviewed 124 epidemiological studies supported or financed by the U.S. Department of Energy and/or by the British Government and have found that they are decisively flawed and tend to produce false negative results[45].
It is no surprise, therefore, that a large number of government-sponsored epidemiological mortality studies show no significant association between cancer induction and low dose radiation exposure.
Conclusions
Combining the known mechanism of low-LET interactions in human cells with findings from several independent epidemiological studies clearly shows that the repair system of the mammalian cell is imperfect and that there is no harmless dose threshold.
This conclusion, drawn from the aggregate of scientific evidence, has complex ethical, economic, and political implications for continuing radioactive contamination of our soil, water, and atmosphere. The following two facts have to be faced:
From this perspective, the authors deem continued application of nuclear technology for energy production, whether in the U.S. or as an export to developing nations, a violation of the fundamental spirit of the Universal Declaration of Human Rights.
How should the application of nuclear technology be managed and are there viable alternatives?
As radiologists and physicians in general become better informed about the lack of any risk-free threshold and about the magnitude of radiogenic risks, they will and should opt to minimize the use of radiation in diagnostic and therapeutic procedures. The saga of the early embrace of x-raying pregnant women and the ultimate warnings against such a procedure can serve as an object lesson [12,13]. It is essential, however, that physicians include better informed patients in meaningful risk-benefit assessments.
The argument is now being made by the nuclear energy industry and its government and corporate supporters that nuclear energy generation is the only solution to forestall global warming. Studies by respected scientists, however, have shown that energy conservation, using state-of-the-art improvements in the efficiency of energy-driven devices, combined with the development of community-based alternative energy technologies including solar power, wind, biomass, and fuel cells, can meet the energy needs of both developed and developing nations [46,47]. In addition, these technologies can also provide employment in both small and large enterprises, including jobs for those with advanced technical skills who presently work in the nuclear industries.
What is needed is a well-integrated policy that must include a reordering of national priorities. Such redirection of the enormous public and private resources presently invested in industries responsible for polluting the earth with chemicals and radiation can only be brought about by the effective commitment of informed citizens.
Footnote
1. There are many repair pathways in a normal and transformed mammalian cell. The enzymes responsible for detecting and eliminating lesions like strand breaks, base loss and so on depend on the correct information in the complementary DNA strand. If, however, radiation damage affects both strands at the same place and at the same time, enzymes no longer can repair such lesions although the enzymes molecules themselves are completely intact. These so-called sites of multiple damage are frequently induced by ionizing radiation. Repair of those sites is either impossible or occurs at rather low fidelity.
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Table
1: Tissue Dose in Centi-Gray when the Average Track-Rate per Cell Nucleus is One | ||
Origin of Electron Packets | Average
Nuclear Traversals per Nucleus in Delivery of 1 cGy | Dose
in cGy when Average Track-Rate per Nucleus is one |
| 30 keV X-rays | 1.34 | 0.75 cGy |
| 250 keV X-rays | 2.30 | 0.43 cGy |
| 596
keV gammas Radium-226 | 2.94 | 0.34 cGy |
| 662 keV gammas Cesium-137 | 3.16 | 0.32 cGy |
| 1608 keV gammas A-Bomb | 5.41 | 0.19 cGy |
Table 2: Average
Tracks per Cell Nucleus from each Exposure in Nine Human studies | ||||
| Nr. | Study | Organdose [cSv]/Exposure | Tracks
per Cell Nucleus at 1 cSv | Average Number of
Tracks per Cell Nucleus from each Exposure |
| 1 | Nova Scotia Fluoroscopy [31] | 7.5 | 1.34 | 10.03 Rounded : 10 |
| 2 | Israeli Scalp-Irradiation [32] (Authors revised estimate) | 7.5 9.0 | 1.34 | 10.03 Rounded : 10 12.04 Rounded : 12 |
| 3 | Massachusetts Fluoroscopy [33] | 4.6 | 1.34 | 6.15 Rounded : 6 |
| 4 | Canadian Fluoroscopy [34] | 4.6 | 1.34 | 6.15 Rounded : 6 |
| 5 | Stewart In-Utero Series [35-37] | 0.5 | 1.34 | 0.67 less than one ; 51% with one track |
| 6 | MacMahon In-Utero Series [38] | 0.9 | 1.34 | 1.20 ~ one |
| 7 | British Luminizers [39] | 0.1 | 2.94 | 0.29 less than one; 75% with no track |
| 8 | Harvey Twins In-Utero Series [40] | 1.0 | 1.34 | 1.34 ~one |
| 9 | Israeli Breast-Cancer in Scalp-Irradiation Study [32] | 1.6 | 1.34 | 2.1 ~ 2 |
* WK is Professor and Director, Institute for Radiation Biology, University of Münster, Germany.
** RHN is Professor Emeritus of Physics and Environmental Sciences, Portland State University, Portland, OR USA.
Address correspondence to: Wolfgang Köhnlein, Robert-Koch-Strasse 43, 48129 Muenster, Germany; e-mail: kohnlei@uni-muenster.de; or Rudi H. Nussbaum, Portland State University, Portland OR 97205-0751 USA; e-mail: d4rn@odin.cc.pdx.edu.
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