Tritium Releases and Potential Offsite Exposures
LAWRENCE LIVERMORE NATIONAL LABORATORY (U.S. DOE)
[a/k/a LAWRENCE LIVERMORE NATIONAL LABORATORY (USDOE)]
LIVERMORE, ALAMEDA COUNTY, CALIFORNIA
EPA FACILITY ID: CA2890012584
LAWRENCE LIVERMORE NATIONAL LABORATORY (U.S. DOE)
[a/k/a LAWRENCE LIVERMORE NATIONAL LABORATORY (USDOE)]
LIVERMORE, ALAMEDA AND JOAQUIN COUNTIES, CALIFORNIA
EPA FACILITY ID: CA2890090002
THE SAVANNAH RIVER SITE (U.S. DOE)
[a/k/a SAVANNAH RIVER SITE (USDOE))]
AIKEN, AIKEN, BARNWELL AND ALLENDALE COUNTIES, SOUTH CAROLINA
EPA FACILITY ID: SC1890008989
March 11, 2002
The estimation of radiation dose following conventional models and methods provides anominal measure of radiological impact on health through the so-called "nominal riskcoefficients". These risk coefficients express the probabilities of deleterious impacts onhealth from doses of different types of radiation. There are, though, uncertainties associatedwith such measures that need to be discussed in evaluating any possible impact on publichealth from radiation doses in general and from tritium beta radiation in particular. Suchuncertainties arise in the judged validity of the nominal risk coefficient, the appropriatenessof the weighting accorded the radiation from tritium in comparison with other radiations, andthe possibility of any effects that are peculiar to tritium because of its incorporation in key biological molecules.
Quantitative estimates of the probability of deleterious effects on health in the long termfrom radiation doses less than a few hundred mSv have been the subject of the deliberationsof many expert committees over the years. An example in the USA is the work of theCommittee on the Biological Effects of Ionizing Radiation (NRC 1990), and internationally,the deliberations of the International Commission on Radiological Protection (ICRP 1992),and the United Nations Scientific Committee on the Effects of Atomic Radiation(UNSCEAR 1993). Most quantitative estimates of risk are based on extrapolations from theobservations of the health of the survivors of the atomic bomb detonations in 1945 in Japanat Hiroshima and Nagasaki.
Although the extrapolation models and assumptions made by the various committees havediffered in detail, the best estimates are similar and are believed to be conservative thoughall emphasize the large uncertainties inherent in them, the range of uncertainty including zerorisk when doses are a few millisieverts. There is continuing discussion and re-evaluation bythese committees and by others, with diverse judgements being made about whether the risksfrom these small doses are exaggerated or whether re-evaluation of the data from the atomicbomb survivors in the light of new measurements shows that the current nominal riskcoefficients underestimate actual risk (see below).
Table 5.1 shows estimates of excess cancer mortality from low doses of radiation based ontabulated values in the report of BEIR V (NRC 1990; Table 4-3). The values are lifetimeprobability after exposure to 0.1 Sv (100 mSv) at the age band shown. The values in theBEIR V report have been adjusted here by applying a dose and dose rate reduction factor(DDRRF) of 2 to the tabulated coefficients for solid cancers, following the BEIRCommittee's suggestion (NRC 1990, page 6). The value of 2 is at the low end of the range(2-10) generally observed experimentally so the tabulated values are believed to beconservatively high. The overall average value for a nominal risk coefficient so obtained(4.4% per sievert or 0.044% per rem) is similar to the value recommended by the ICRP of 5% per Sv (ICRP 1992) for cancer mortality in the general population. The values ofprobability in the various age bands in the Table vary by less than a factor of two (except inthe oldest two age groups) from the weighted average. The ICRP also has assigned anadditional 1% per Sv to the recommended risk coefficients to account for hereditary effects.
There are many uncertainties associated with these nominal risk coefficients as the variousbodies have noted and discussed. The challenge has been to extrapolate from theobservations of the consequences of almost instantaneous radiation exposures to twoJapanese populations in 1945 to the potential impacts to current, diverse populations fromradiation doses and dose rates at levels below which any effects have been observed. Oneuncertainty concerns the extent to which the actual physical spectrum of radiations thatexposed the A-bomb survivors has been correctly estimated. For this discussion, we needto introduce the concept of relative biological effectiveness (RBE).
|Age at exposure (years)||Probability of radiation-induced mortality from cancer from 100 mSv (10 rem)|
Table 5.1 Estimates of excess cancer mortality for individuals in 10-year age bands from low doses of radiation based on the estimates of BEIR V (NRC 1990). The values are lifetime probability after exposure to 0.1 Sv (10 rem) at the age band shown. The values in the BEIR V report have been adjusted by applying a dose and dose rate reduction factor (DDRRF) of 2 to the tabulated coefficients for solid cancers, following the BEIR Committee's suggestion (NRC 1990, page 6).
* Averages are weighted for the age distribution in a stationary population having the US mortality rates.
There are many influences on the relationships between the biological consequences of dosesreceived from various kinds of radiations. To represent the aggregate of these influences,the concept of "relative biological effectiveness" or RBE was introduced (ICRP-ICRU1963). The biological effectiveness of a given radiation relative to a reference radiation isdefined as the inverse ratio of the dose of the given radiation that produces the same degreeof a defined biological endpoint as a dose of the reference radiation. A physicalcharacteristic of radiation that has been found to be helpful in defining the RBE has been thedensity of ionization along the path taken in tissue by the ionizing photon or particle - the"linear energy transfer" or LET. Other factors that affect RBE include dose, dose rate, typeof cell or tissue, and the actual biological effect observed. Figure 5.1 illustrates RBE for aradiation of high LET relative to a reference low LET radiation. From figure 5.1, the RBEis either (D4/D3) or (D2/D1) depending on the level of effect at which the comparison ismade. The increased RBE at the lower effect level (and lower doses) here is a result of thecurvilinear nature of the relationship of biological effect with dose of the low LET radiation.
Figure 5.1 Illustration of the relative biological effectiveness (RBE) of a highLET radiation. The reference radiation is low LET. At level of effect E2, the RBEis D4/D3. At level of effect E1, it is D2/D1.
A wide range of RBEs have been obtained from in vivo experiments with biota and in vitroexperiments with cell and tissue cultures. The reference radiation has traditionally beentaken as 250 kVp X-rays although higher energy gamma-ray emitters such as 137Cs and 60Cohave also been used experimentally. For radiation protection purposes, different radiationshave been grouped and the absorbed doses from these groups of radiations, averaged overtissues or organs, are multiplied by "radiation weighting factors" (designated wR (ICRP1992)) to give the quantity "equivalent dose". Absorbed dose and equivalent dose have thesame SI unit of J/kg but to distinguish the quantities their unit has been given the specialnames of gray and sievert respectively. Photons of all energies (i.e., from low energy X-raysto high energy gamma radiation) and electrons (and, hence. tritium beta particles) and muonshave been assigned a weighting factor of unity, neutrons various weighting factors dependingon energy, protons a factor of 5 and alpha particles a factor of 20. The first group areradiations with relatively low LETs but the range within the group is sufficient that RBEsdifferent from unity are observed experimentally, higher energy gamma radiation generallyhaving RBEs less than unity, low energy X-rays and low energy beta particles having RBEsgreater than unity. These observations are consistent with the results of theoretical andexperimental studies of the physics of radiation energy deposition at the microscopic scale(so-called microdosimetry) that have helped to refine the concept of LET. For example, ina spherical target with diameter 1 mm, 60Co radiation deposits 1.5 less energy than do 250kVp x-rays, consistent with the 0.6 RBE typically observed for 60Co radiation.
Nevertheless, for protection purposes, given the variability and imprecision in thequantitative relationships between small radiation doses and biological effects, the ICRP andothers have not seen justification for assigning other than the single weighting factor of unityfor photons and electrons. The ICRP has expressed concern about the impression of spuriousprecision that a finer scale of weighting factors might engender (ICRP 1992). Consistentwith this view, the ICRP, BEIR and UNSCEAR committees (loc. cit.) have taken the gammaradiation associated with the A-bombs to be representative of the low LET band of photonsto which unity weighting factor has been assigned.
Whether this is a reasonable conclusion has been questioned (Straume 1995). The survivorswere actually exposed to unusually high-energy gamma rays. Based on the current dosimetrysystem, survivors of the atomic bombings of Hiroshima and Nagasaki received gamma raysthat were predominantly in the 2 to 5 MeV range. These high energy gamma rays resultedin part from neutron capture as the bomb neutrons penetrated large distances of air.
To estimate the relative biological effectiveness of the A-bomb gamma rays, the biologicaleffectiveness of various low-LET radiations with different mean energies were evaluated(Straume 1995). The radiobiological effects observed were chromosome aberrations(dicentrics) induced in vitro in human lymphocytes. The relative effectiveness of theradiations evaluated spanned a range of ten; 0.5 for 15-MeV electrons (A-bomb gamma rayswere taken as 1), ~2 for 60Co gamma rays, ~4 for 250 kVp x-rays, and ~5 for tritium betaparticles. The implication of these results is that rather than the nominal risk coefficientbeing representative of the middle of the range of low LET radiations grouped with theweighting factor unity, it is more representative of the radiations at the high end of the LETdistribution. A corollary is that those lower in the distribution - 137Cs gamma-rays, tritiumbeta particles etc. - should be formally accorded a higher weighting factor for estimatingequivalent dose or that the nominal risk coefficient assigned to the low LET band ofradiations should be increased.
These are implications that go beyond the mandate of this committee and they are moreproperly addressed by the other expert committees, such as the BEIR VII committee,currently in session, or the ICRP. The discussion above, however, provides a backdrop tothe discussion below on the RBE of tritium and an assessment of relative risk from tritium compared with that estimated on the basis of conventional dosimetry and risk factors.
There have been no direct observations in humans of cancer, hereditary effects, or effects in-utero arising as a result of radiation doses from tritium. Hence, the estimation of any suchrisks in humans has to depend on information from laboratory studies of the effectivenessof tritium relative to other radiations involving animals and in-vitro experiments withvarious biological endpoints or effects, supplemented by theoretical studies of the physicsof energy distribution. An example of the former is the experiment cited above withchromosome aberrations as the endpoint - tritium appeared to be at least twice as effectiveas 60Co gamma rays. An example of the latter is the microdosimetric analysis by Ellett andBraby (1972) who calculated the energy deposited from various radiations in tissue volumesof sizes that reflected cellular and cell nuclear dimensions. For a tissue sphere of 1 mmdiameter the energy deposition from tritium beta particles was 1.5 times that from 250-kVpx-rays, and 3.8 times that from 60Co gamma rays. These values vary with sphere diameter;larger diameters lead to smaller factors. Tritium beta particles, in fact, look very much like65 kVp x-rays from the point of view of pattern of energy deposition such as the distributionof ionization clusters which has been shown by a variety of studies at the micrometer andnanometer scale (most recently Moiseenko et al. 1997). The expectation is, therefore, thattritium beta particles will have an RBE approximately equal to that for 65 kVp x-rays butwith the actual RBE in any particular circumstances reflecting the biological variables.
In reviewing the tritium radiobiological data, Straume and Carsten (1993) identified 12published studies that estimated the RBE for tritium as HTO for a reference radiation of 180-250 kVp x-rays, and 21 studies where the reference radiation was gamma rays from 137Cs or60Co. The mean of the tritium RBEs from the comparisons with x-rays was 1.8; that fromthe comparisons with gamma rays was 2.3. Figure 5.2 shows the RBE values observed inthe published studies that compared tritium as HTO with the x-rays. Although there was anarithmetic mean RBE value of 1.8 with RBE values ranging from about 1 to over 3, in halfthe studies, the values were in the 1 to 1.5 interval.
Figure 5.3 shows the RBE values for HTO observed in published studies in which gammarays were used as the comparison radiation. Again, the RBE values range from about 1 toover 3, but, in this case, the majority of values are in the 2 to 3 interval. Given the relativelysmall sample sizes, the actual distributions (i.e., normal, log normal, etc.) are uncertain. Even so, in both sets, there is a clear consistency between these direct observations andpredictions from the microdosimetric calculations.
Figure 5.3 The number of published studies reporting values in the indicatedintervals for the RBE of tritium as HTO with 137Cs or 60Co gamma rays as the reference radiation (Straume and Carsten, 1993).
The estimates of RBE that have most bearing on the assignment of risk from tritium whencompared with that from the designated reference radiation are those where the biologicalendpoints are relevant to radiological protection - i.e., the so-called stochastic effects; cancerand hereditary effects. Such an example is that of Gragtmans et al. (1984) in which the RBEfor mammary tumor incidence in Sprague-Dawley rats was measured to be 1.18 ± 0.18 when200 kVp x-rays are used as the reference radiation. In the review cited above, the mean RBEfor the studies with x-rays as the reference radiation and with stochastic endpoints was about1.5 with the values for carcinogenesis-related endpoints and chronically-delivered x-rays (tomatch the tritium dose) being close to one.
A further factor to be considered in estimating the relative risk from low doses of a particularradiation is whether the relative effectiveness has been estimated at the appropriate level ofeffect. As can be seen from Figure 5.1, the RBE for the high LET radiation, taking the lowLET radiation as reference, is higher at the lower level of effects (D2/D1 is greater thanD4/D3). Hence a value of RBE obtained at high doses and associated with a high degree ofeffect might be an underestimate of the value appropriate to low doses. Some of the studiescited above (Straume and Carsten, 1993) are in this category. However, the increase in RBEwith decreasing dose and effect is because of the relatively greater curvilinear nature of therelationship between effects and dose for the lower LET (reference) radiation. The nominalrisk coefficient for radiation effects at low doses is based on an extrapolation of observedeffects from high doses of the reference radiation. Hence, the degree of underestimation ofthe RBE for the higher LET radiation depends on the extent to which the non-linearity inrelationship between effect and dose has been taken into account in that extrapolation. In theextrapolation from the A-bomb survivor data, this non-linearity is (partly) taken into accountby applying a dose and dose rate reduction factor (DDRRF) of only a factor of 2 as noted inTable 5.1. It follows that although very large RBEs have been observed in some studies withtritium for extremely sensitive endpoints, these are not indicative that doses from tritiumshould generally be accorded a very high weight for protection purposes; they indicate thegreater curvilinear falling off in relative effectiveness of the lower LET radiation.
In summary, for radiation protection purposes the nominal risk coefficient for cancermortality has conventionally been taken as 5% per sievert (Section 5.1). For the purposesof this report we recognize the derivation of that value from the A-bomb survivor datathrough a DDRRF of 2, is likely to be overestimating (by a maximum of 5 times; morelikely by at least a factor of 2) the risk at low doses compared with high doses. (This isdiscounting there being an actual threshold below which there are no deleterious effects.) Countering this, we recognize that there may be an underestimation because of the very highenergy of the A-bomb gamma rays, possibly by a factor of 2-3 (Section 5.2). Finally, if thereference radiation remains that of 250 kVp x-rays (implicit in the above) then the relativerisk associated with doses from tritium beta particles radiation may be about 1.3 times thatfrom the reference radiation. The combination of these factors leads to no net overalladjustment. The nominal risk coefficient of 5% should therefore be appropriate for dosefrom tritium radiation, at least in the form of HTO which is the form used in the citedstudies. For OBT, an adjustment factor of 10% per sievert would appear to be veryconservative.
As noted in Section 2.4, heterogeneity in the spatial distribution of OBT within cells and cellnuclei complicates dosimetry. A particular level of biological effect observed in a study maybe interpreted to indicate an increased effectiveness of the tritium radiation when the doseis averaged over the irradiated tissue volume. It is difficult to ascertain whether this isbecause of a higher local concentration of tritium in cells or cell nuclei or is because of agreater effectiveness per disintegration that occurs in an organically bound location.
There is a further conceptual difficulty in that the quantity "equivalent dose" as defined isa "macro" quantity; that is, its derivation from absorbed dose with particular weightingfactors is only valid for absorbed doses averaged over tissues and organs. The nominal riskcoefficient relates to doses obtained in this manner. Since dose is energy absorbed per unitmass (i.e., J/kg), it can be estimated for any small volume of tissue - such as that of a cellnucleus. Because of the concentration of energy deposition along ionizing particle tracks,estimation of the dose in a volume that is close to the extent of the track can give high valuesof dose. For example, a single track from a low LET radiation delivers a dose of a few mGyto a cell nucleus.
For tritium, the absorbed dose in a cell nucleus, diameter 8 mm, 270 pg mass, would be about2.7 mGy per tritium decay (270 mrad). A consequence of this is that at annual doses of theorder of 1 mGy/a (100 mrem/a) there is less than one event in each cell each year. Theradiobiological consequences of this kind of temporal and spatial distribution of absorbedenergy at the microscale, and possible implications for protection, need to be treated asfactors that may affect risk explicitly rather than attempting to fold them into somemacroscale quantity similar to equivalent dose. Below, we therefore estimate theimplications of any radiological effects peculiar to OBT in terms of the nominal risk fromtissue-averaged doses of tritium as HTO.
Straume (Straume 1993) concluded that the risks from tritium that decays from anorganically-bound position appear to range from similar to those from tritium as HTO (forexample for amino acids and proteins) up to a factor of two greater for tritium decaying froma nucleotide such as thymidine. The uncertainty in these estimates arising from thedosimetry difficulties was noted.
Tritium can certainly be concentrated in mammalian cell nuclei if particular tritium-labeledorganic compounds such as the nucleotide, tritiated thymidine (a DNA precursor) areinjected into the body (see NCRP 1979b for example). However, a large fraction of thebroad mixture of labeled organic compounds ingested in food is broken down into basicbiological building blocks before being re-synthesized back into organic material in the body. Hence, ingestion of OBT and its subsequent catabolism and metabolism will lead to a broaddistribution of tritium in organic material in the body, only some of which will be innucleotides. The ratio of the risk coefficient for doses from OBT in general to that for doses from tritium as HTO would therefore appear to be less than two and likely within the range from one to two.
When the tritium in an organic molecule disintegrates, the molecule is, in effect, losing ahydrogen atom - which has changed to helium - and the molecule will be changed. TheNCRP (NCRP 1979b) in its review of OBT in genetic material noted that mutations had beenobserved if specific positions in particular nucleotides had been labeled with tritium (e.g.,the 5-position of cytosine). It concluded that such labeling would, in practice constitute sucha small fraction of organic labeling that the effects would be negligible compared with any from the radiation dose from the tritium beta particles.
Estimates of tritium incorporation, dose, and risk become more complicated when exposure totritium occurs in utero or during early neonatal life. Although fetal cells divide rapidly duringcertain stages of development, they also differentiate to form organs and tissues that in certain casesundergo very little or no subsequent cell division. Thus, the incorporation of tritium intobiomolecules of long-lived cells (e.g., neurons and oocytes) could result in larger integrated dosesover the lifetime of the cells. In women, the entire oocyte pool is produced by rapid cell divisionduring in utero development. The oocytes thus produced do not divide again until after ovulationand fertilization in adulthood. Therefore, a pregnancy at the age of, say, 30 years is the result offertilization of a 30-year-old oocyte. If that particular oocyte had incorporated non-exchangeabletritium into its DNA some 30 years previously in utero, the oocyte would have been absorbing aradiation dose from the incorporated tritium throughout this time. The effective half-life would bethe 12.3 year physical half-life of the tritium
One way of estimating the dose from incorporated tritium that is ingested with food (the main sourceof incorporated tritium) is to conservatively assume that the OBT taken in with food is all in theform of tritiated thymidine, an important component of DNA, and that the DNA in oocytes aresubsequently labeled with this compound and that there is no loss of the tritium. The extent oflabeling can be estimated from the results of studies with mice into which tritiated thymidine hadbeen injected (Baker and McLaren 1973), from an estimate (NCRP 1979b) that labeling is five timesless when tritiated thymidine is ingested rather than injected, and by scaling body size from mouseto human. If the food intake (at 1.6 kg/d) over the 5 months during which the oocytes are formed(from 2 months after fertilization to 7 months; Baker 1963) has the activity concentration of 10Bq/kg, (0.27 pCi/kg) the value typical for the current LLNL environment, there would be an averageconcentration of 30 pBq per oocyte nucleus (8 x 10-22 Ci). At this concentration, the probability of even one tritium decay in any oocyte before it is fertilized is very small (See Table 5.2).
|Number of tritium decays||Number (%) of oocytes experiencing tritium decays by given age|
|15 years||30 years|
Table 5.2. The number of oocytes that will have experienced zero, one, or more tritium decays in a 15 year-old and a 30 year-old woman. The assumptions are as given in the text. A Poisson distribution is assumed for the probability of decays. The number of oocytes remaining after 15 years is taken as 390,000 and after 30 years, 15,000 (from Peters and McNatty 1980).
It follows that most oocytes will have received no dose from tritium and that those in which therehave been one or more tritium decays will have received, on average, a dose of 2.7 mGy, 5.4mGy, or 8.1 mGy (270, 540 or 810 mrad), depending on whether there was one, two or threedecays (See Section 5.3.1). The actual doses in the oocytes that experience at least one decaywill be distributed according to the beta spectrum of tritium; i.e., from zero to approximatelythree times the average. The dose averaged over all oocytes remaining at 30 years (a measure ofthe overall risk), based on these very conservative assumptions, is approximately 40 Sv (4mrem) (from 2.7 mGy x 1.4%).
It is important to note that the predominant forms of OBT expected in the vicinity of LLNL andSRS are not tritiated thymidine nor other tritium-labeled nuclear bases. Rather, there areexpected to be a broad range of tritiated organic molecules such as proteins, carbohydrates,sugars, etc., that have incorporated tritium in plants and animals. Tritium from thesebiomolecules would not be incorporated to the same extent as tritiated thymidine and, hence,there would fewer oocytes with tritium disintegrations in the nucleus than estimated here fortritiated thymidine.
A less extreme approach to estimating the dose to oocytes from incorporated is to assumethat the organic material of the oocyte is labeled to the same extent as the rest of the bodytissues and that the dose to oocytes varies with the relative retention times of the oocyte-bound tritium and OBT in other tissues ; i.e., 12.3 years relative to 40 days. In 30 years,approximately 80% of the tritium will have decayed and the dose absorbed in that timewould be about 90 times the dose that would have been absorbed if the long-retained OBThad been retained only with the ~40 day half life. Since there is post-natal synthesis of RNAin oocytes (NCRP 1979b), some of the oocyte-bound tritium will be eliminated (i.e., theeffective half-life will be less than 12.3 years), reducing this factor of 90 times accordingly. If we take, conservatively, that the tritium intake giving rise to the estimated current annualdose around LLNL from OBT (approximately 0.04 µSv; see Section 4.3.2,) all occursduring the 5 months in which the oocytes are formed, then the dose from incorporated tritiumto oocytes over 30 years would be less than 90 x 0.04 µSv » 4 µSv. On the basis of theseassumptions, approximately 0.1% of the oocytes would have experienced a tritium decay (4µSv/2.7 mSv), compared with approximately 1% as estimated above with more conservativeassumptions.
For comparison, if the same environmental levels of tritium were to be present during the 30years during which the dose from incorporated tritium has been estimated, then the dose tothe oocytes from HTO ingested in drinking water and food through that period would be in30 x [0.1 µSv + 0.07 µSv] » 5 µSv (0.5 mrem; from Section 4.3.1). Accordingly, theincorporated tritium (based on the latter set of assumptions) would about double the numberof oocytes experiencing a tritium decay through this period.
The conclusion is that certainly less than 1% (and, more likely, less than 0.1%) ofpregnancies occurring in women who are exposed to food contaminated with tritium at thecurrent levels observed around LLNL and SRL will have arisen in an oocyte that hasexperienced a dose from the beta decay of tritium that was incorporated in oocytes duringoogenesis. A fertilized oocyte (a zygote) divides resulting in a rapidly developing embryoand the large number of divisions will quickly eliminate the remaining tritium in the nuclearDNA. Hence, the risk of interest is that associated with one or two tritium decays in theoocyte nucleus before fertilization.
The nominal value for probability of severe hereditary effects (which includes autosomaldominant and X-linked diseases plus multi-factorial diseases) chosen by the ICRP is 5 x 10-6per mGy (ICRP 1992). A recent ICRP publication (ICRP 1999) concluded that this valuewas likely to be an overestimate but that there was sufficient uncertainty that a change in the nominal value was not warranted. Hence, if we conservatively allow for an enhancedeffectiveness of tritium radiation relative to gamma radiation of 1.3 and of the effectivenessof tritium as OBT relative to tritium as HTO of 2, for a dose of 2.7 mGy from a singledisintegration on average, then the probability of a severe hereditary effect if a tritiumdisintegration does occur in a oocyte nucleus is 5 x 10-6 x 1.3 x 2 x 2.7 = 3.5 x 10-5. Hencethe probability of a severe hereditary effect attributable to oocyte labeling at oogenesis in anoocyte in which a decay actually occurs would be in the range 1.3 x 10-5 (with no enhancedeffectiveness assumed for tritium) to 3.5 x 10-5 (with an overall enhanced effectiveness of 1.3x 2 = 2.6 for OBT relative to gamma radiation).
The overall probability for an individual must also include the probability that a fertilizedoocyte is one that has actually experienced a tritium decay. From above, at current levelsof tritium contamination, this proportion is less that 1% and likely less than 0.1%. Hencethe overall probability of a severe hereditary effect attributable to oocyte labeling atoogenesis is in the range (0.1% x 1.3 x 10-5 ) to (1% x 3.5 x 10-5 ); that is, a range of1.3 x 10-8 to 3.5 x 10-7.
For exposures to higher levels of tritium in foods, such as might have been experienced inthe past, the effect for increases by one or two orders of magnitude is to increaseapproximately proportionately, the fraction of oocytes that actually experience a decayfrom incorporated tritium. (Yearly exposures around LLNL were estimated to have beenan order of magnitude greater than those of recent years - see Section 4.2.3. Hence, onecan conclude that the overall probabilities as estimated in the previous paragraph wouldbe an order of magnitude higher.)
An estimate can be made of the oocyte labeling that may have occurred after a releasesuch as that from LLNL in 1970 (see Section 4.2.1) when 11 PBq (289 kCi) were releasedin the form of HT. Currently, airborne annual releases from LLNL are approximately 8TBq (200 Ci; assumed to be HTO) and the dose is estimated to be less than 1 mSv. If weassume a 1% conversion of HT to HTO for the 1970 release (which is dosimetricallyconservative) then scaling by the estimate for current values gives an estimated dose fromthat release of (11 PBq x 1% x 1 mSv) / (8 TBq ) » 15 mSv (1.5 mrem). Thecorresponding value for dose from OBT in current conditions was deduced to be 0.04mSv (see above and Section 4.3.2). Scaling this value for the 1970 release gives 15 x0.04 mSv = 0.6 mSv (60 mrem) from OBT in general. If we take this factor of 15 asapplying also to the dose from oocyte-incorporated tritium, then certainly less than 15%(and likely less than 1.5% ) of the oocytes would be labeled and the range of overallprobability of a severe hereditary effect attributable to oocyte labeling at oogenesis wouldthen be approximately is in the range 2 x 10-7 to 5 x 10-6.
All the values of probability of any severe effect from oocyte labeling are low, even with themost conservative of the assumptions made here. It is important to recognize that, at theconcentrations of tritium in environmental media that are considered in this review, theextent of oocyte labeling that can occur is such that only a very small fraction of oocytesexperience even one decay and that the dose associated with such a decay averagesapproximately 2.7 mGy (270 mrem).
There are uncertainties in each step of an estimation of risk (release, transport, exposure, dose and biological effect), , as discussed in Sections 2, Sections 3 and 4 and Section 5. An assessment of risk is most informative if the knowledge of these uncertainties is propagated through the estimation and the estimated doses, or risks, characterized by a mean and an overall uncertainty. Examination of the relative contributions of the various individual uncertainties to the overall value can be helpful in indicating the major "drivers" of uncertainty - and possibly indicating where efforts to reduce uncertainty might be most efficacious. It is also much easier to explain doses and risk estimates to a concerned public group if such information is made available. Examples of such dose distributions are seen in the report of the recent dose assessment for SRS (Till et al. 1999). . A series of papers by Hamby (1993, 1994, 1995, 1998, 1999) and Kock and Hamby (1998) discussed uncertainties specifically in estimations of doses from tritium.
In the above discussion of risk from tritium, an attempt has been made to avoid undulyconservative assumptions. We recognize though, that there are broad bands of uncertainty- in both directions - about the parameters that we have suggested. Hence, it is difficult tobe sure a priori that risk estimates considered "conservative" are in fact conservative withouta closer look at the distribution of uncertainties. If the uncertainties on the individualparameters are estimated correctly and the parameters are correctly identified and dealt withstatistically, then the resultant distribution should be a realistic estimate of the overalluncertainty. An example for cancer risk from tritium is illustrated in Figure 5.4 (Straume1993). This shows the range of uncertainty in the risk coefficient that arises when theindependent distributions of the parameter values are statistically combined. Theassumptions in that analysis differ in detail from some made here but the differences tend tobe offsetting so the central value for the risk coefficient is not substantially different fromthat in Table 5.3 for tritium as HTO.
The adjustments that might be appropriate to apply to the nominal risk coefficient as defined for radiation protection purposes that have been discussed above are summarized in Table 5.3.
|Nominal risk coefficient for population average||5% per Sv-adult |
8% per Sv - child
|Multiplying factor for DDRRF (dose and dose rate reduction factor)||0.4 |
0.1 to 1 range
|Multiplying factor for A-bomb gamma-ray energy adjustment||2 |
1 to 5 range
|Multiplying factor for RBE for tritium as HTO||1.3 |
1 to 2 range
|Multiplying factor for RBE for OBT relative to HTO||2 |
1 to 3 range
|Adjusted risk coefficient for tritium as HTO (population average)||5% per Sv|
|Adjusted risk coefficient for tritium as OBT (population average)||10% per Sv|
Table 5.3. Adjustments to the nominal risk coefficient that account for uncertainties in the nominal risk coefficient for application to exposures to tritium in the forms of HTO and OBT. These adjustments are based on a reference radiation of 250 kVp X-rays. Uncertainty ranges are included for some factors with single values representing consensus opinions of the panel.
Figure 5.4 Calculated frequency distribution of excess cancer mortality risk induced by HTO in a population like that of the U.S. (or the excess cancer deaths permillion people per mGray radiation dose; Straume, 1993).
A further caveat that needs to be placed on the above nominal risk coefficients isquestionable validity of applying them quantitatively to predicting the probability ofincreases in cancer mortality from incremental annual doses of the order of, or less than,those received from natural background (a few mSv or a few thousand mSv). There is thecertainty that any impacts on health will be small and possibly effectively zero. TheBEIR V committee (NRC 1990) was quite explicit on this topic: ". . . epidemiologicaldata cannot rigorously exclude the existence of a threshold in the millisievert dose range. Thus the possibility that there may be no risks from exposures comparable to externalnatural background radiation cannot be ruled out." The complexity and variability ofbiological processes that can be stimulated as well as harmed by physical stressors (suchas ionizing radiation) at the dose levels such that cells in tissues are receiving only a fewionizing events during a year rules out any realistic precise quantitative application of a"one rule fits all" risk coefficient obtained by extrapolation from observations of effects at much higher doses.
The levels of tritium contamination in the environments around both the Savannah River Siteand the Lawrence Livermore National Laboratory are low and the radiation doses to membersof the public from tritium in drinking water and food are correspondingly low. Individualannual doses are only the order of 1 mSv (see Table 6.1 below), even taking into accountpossible contributions from organically bound tritium in foodstuffs. Although theorganically-bound component has not generally been explicitly measured in vegetation orfood samples there is sufficient information on the behavior of tritium in the environmentto provide the assurance that, at the current concentrations of tritium in environmentalmoisture, tritium that may have become organically-bound will not result in substantiallylarger values of dose than currently estimated.
The nominal risk of cancer from annual doses around the two sites is also shown on Table6.1. The values shown are population averaged, or averaged over the mix of individuals ina population (males, females, and all age groups). From the discussions in Sections 2.4 and5.1, it follows that the nominal risk to infants will not be more than three times greater thanthis averaged value. The conclusion is that for the annual doses of the order estimated, thenominal risk is less than one in ten million. This is a hypothetical value that is defined byATSDR to represent "no increased risk" (ATSDR 1991) . Any impact on health must bevery small and certainly not detectable compared with any impact there might be from thenatural background radiation of everyday living.
Table 6.1 Estimates of current annual doses and risks from tritium ingested in drinking water and foods in the vicinity of the Savannah River Site and the Lawrence Livermore National Laboratory. Modeling assumptions and data are as described in the previous sections. The estimates are based on conservatively estimated concentrations in drinking water and in food moisture in the environment around the SRS of 40 Bq/L and 10 Bq/L respectively (see Table 3.3), and in the drinking water and food moisture in the environment around LLNL of 10 Bq/L (see Section 4.2.1).
The dose from tritium that is ingested as OBT in foods obtained from environments widelycontaminated with tritium will add to the dose received from tritium ingested in the form ofwater in food and in drinking water. Enough is known about the behavior of tritium in theenvironment that reasonable bounds can be placed on likely levels, given the observed levelsof HTO. For an environment where water is generally contaminated with tritium, theadditional dose from tritium ingested as OBT is unlikely to result in a total dose from tritiumthat is more than twice that from tritiated water alone.
The technologies currently employed in the monitoring and measurement of tritium at LLNLappear to be consistent with practices described in the literature and widely practiced innuclear establishments elsewhere.
For the current levels of contamination around the SRS and the LLNL site, even if ultra-conservative estimates were to be made of the organically-bound tritium in foodstuffs, theincrease in the dose so estimated using current dosimetric models would still be very smallcompared with any that would have any appreciable impact on the health of the localcommunities.
Ideally, this conclusion concerning the current significance would be supported by directmeasurements of OBT in representative samples of foods in the Livermore area. However,measurements of OBT are expensive and the magnitude of current doses from tritium ingeneral does not warrant there being precise knowledge of the amounts of tritium as OBTcompared to that as HTO in each food - a more general set of upper bounds suffices. Itmight be worthwhile providing some assurance of the validity of the conclusion about theupper bounds to current levels of OBT by undertaking some sampling of foodstuffs along thelines of studies described in the text, for measurement of the OBT by 3He mass spectrometry. Such results would also help to validate the applicability of generic values that can beassembled from detailed review of the published data from locations elsewhere.
One of the issues that could be resolved by 3He mass spectrometric measurement of OBT,is how much past releases from LLNL may have contributed to OBT in the Livermore valley. To obtain such information would require selection of the samples in which the OBTturnover is sufficiently slow to provide a detectable residual from past releases - tree ringsare a possibility. Interestingly, scientists at LLNL have recently used accelerator massspectrometry (AMS) to measure tritium in tree rings (taken from a tree on the Nevada TestSite (NTS), near a groundwater sampling site for which sampling data go back to themid-1970s). At the expected OBT activities around LLNL it appears that AMS analyticalprocedures would require much larger sample volumes. Larger samples could in principlebe used for tree rings with much lower tritium levels. The results from NTS demonstratedvery good correlation between groundwater tritium (HTO) and the tree ring measurementsfor the same sampling date. Perhaps this novel method could be helpful in particularlocations at both LLNL and SRS; it would be worthwhile evaluating whether it would besuitable for the validation of historical tritium releases at LLNL and SRS
The relative biological effectiveness (RBE) of tritium in its various chemical forms is thesubject of on-going studies, both experimental and theoretical, as are the biokinetics andmetabolism of tritium by humans in various organic forms. There are different interpretationsof the published results. The levels of tritium that appear to be present around the facilitiesdiscussed in this report are low. Far more conservative assumptions or interpretations intritium dosimetry and radiobiological effectiveness could have been made in this reportwithout affecting the overall conclusion that the tritium levels as reported do not appear tobe sufficient to be having an effect on local communities. Efforts to resolve both themetabolic and RBE questions for tritium and OBT in particular need to be continued toprovide the needed quantification should instances arise with higher levels of contaminationin the environment.
Releases in the past may not have been as well measured and reported as is the current case. If the conclusions about past routine releases from LLNL made in this review are correct,then the doses from those releases, although more than an order of magnitude higher onaverage over the past years than the current annual releases, are still below levels that shouldprompt public health concerns. A broader review of documentation that is available mightclarify some of the uncertainties noted.
Although LLNL reports identify uncertainties for many of their individual tritiummeasurements, they do not appear to provide uncertainties on their dose estimates. Giventhe information available to them, it seems that the uncertainties could be identified andpropagated so that realistic best-estimate uncertainties would be provided for the doseestimates. It would be preferable to have best-estimate doses with uncertainties, rather thanthe "conservative" doses listed in the LLNL annual reports. It is understood that the dosesto the public are low and that the use of "conservative" single-value estimates is a commonpractice, partly driven by the regulatory need to demonstrate compliance with limits. However, such an approach is not very transparent. This makes it difficult for a reviewer ora community group to understand the uncertainties.
We recognize that national laboratories must be consistent with the radiation protectionrequirements and guidelines established by the Department of Energy in demonstratingcompliance. A parallel realistic assessment, taking into account OBT as well as HTO andincluding uncertainties in the various parameters and using more realistic models would behelpful. We note that in the most recent annual report from LLNL (Larson et al. 2000) thereis a short assessment of OBT. Such an approach would allow national laboratories to reflectany evolving consensus on such matters as the appropriate radiation weighting factors ornominal risk coefficients before such evolutions are cast into regulations.
It would be helpful if LLNL could provide inter-comparisons between CAP88-PC and measured HTO at additional off-site locations and distances (Simpkins and Hamby, 1997). The comparisons that have been made at short distances indicate an increasing overestimation of ambient air concentrations by CAP88-PC relative to measured HTO values. It would be helpful to verify that similar health protective overestimates of dose occur under all relevant conditions and locations.
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