Table 8-3: Biosphere <strong>and</strong> Exposure FEPs <strong>for</strong> Rn-222 <strong>Assessment</strong>FEP ID FEP Name Included inthe<strong>Assessment</strong>Model?CommentGAS_Rn_B_RBEM_01 Release to open air No Exposure to radon inoutdoor air is notconsidered due to therelatively lowconcentrations, <strong>and</strong>negligible doses,anticipated (e.g. Sumerling,2008).GAS_Rn_B_RBEM_02Entry <strong>and</strong> accumulationin buildingsYesGAS_Rn_B_RBEM_03 Empirical relationships YesGAS_Rn_B_RBEM_04GAS_Rn_B_RBEM_05Occupancy <strong>and</strong> humanhabitsDose factors <strong>for</strong> radon<strong>and</strong> radon daughterexposureYesNoGAS_Rn_B_RBEM_06 Other sources of radon NoOccupancy treated as adeterministic parameterImplicit in Rn-222 dosefactorReferencesLean C <strong>and</strong> Willans M (2010). A Features, Events <strong>and</strong> Processes <strong>and</strong> UncertaintyTracking System to support the 2011 ESC. National Nuclear Laboratory Reportprepared <strong>for</strong> LLW Repository Ltd, NNL (09) 10762, Issue 1.1, March 2010.72
QRS-1443ZG-1, Version 3.0Appendix B: Comparison with Previous LLWR<strong>Assessment</strong> ResultsThere are a range of differences between the assumptions made in the 2011 ESC <strong>and</strong>those made <strong>for</strong> previous LLWR assessment calculations (McGarry, 2003; Ball et al.,2008; Sumerling, 2008). Differences include, <strong>for</strong> example, the inventory <strong>and</strong> itsdistribution, the volume of the regions of the facility, the diffusion coefficient of radon,the path length from the waste to the surface.In the 2002 ESC gas pathway assessment (McGarry, 2003), the diffusion path lengthsassociated with the trenches <strong>and</strong> vaults were 6.5 <strong>and</strong> 4.9 m respectively. In all casesconsidered in the 2002 ESC, the highest calculated peak exposure from the indoorinhalation of Rn-222 13 was associated with Vault 8. For the best estimate calculation,using an Rn-222 diffusion coefficient of 5.0E-7 m 2 s -1 (Lee, 2002), the peak exposurearising from indoor inhalation of Rn-222 over Vault 8 was calculated to be 8.33E-3 mSv.Increasing the diffusion coefficient to 1.0E-6 m 2 s -1 resulted in the calculated peakexposure over Vault 8 increasing to 8.00E-2 mSv. Decreasing the path length to 1 m,but keeping the diffusion coefficient as the best estimate case, lead to the calculatedpeak exposure over Vault 8 increasing to 1.23E-1 mSv. That this calculated exposure islower than that calculated in the 2011 ESC can be explained by the difference ininventory assumed <strong>for</strong> Vault 8 (2.3E-1 TBq was assumed <strong>for</strong> Vault 8 in 2002) <strong>and</strong> thediffusion coefficients assumed (1E-5 m 2 s -1 in the 2011 ESC, as compared to 5.0E-7 m 2 s -1in 2002).In the 2008 R2S9 Submission, <strong>for</strong> the situation of the engineered cap remaining intact,the level of release of radon gas from the LLWR was expected to be very low, such thatdoses would be imperceptible above the natural levels of radon in outdoor air locally(Ball et al., 2008; Sumerling, 2008). This has also been demonstrated in the 2011 ESCcalculations.For human intrusion, three possible cases were assumed whereby a building wasconstructed on the cap, which varied in their assumptions as to the potential source ofRn-222 entering the building. Exposure from the inhalation of both Rn-222 <strong>and</strong> Rn-220were considered; the calculated annual exposures are given in Error! Reference sourcenot found.. These results agree within a factor of five with the 2011 ESC reference caseresults. As with the 2011 ESC, their most cautious case leads to the calculated dosefrom Rn-222 being greater than 3 mSv also.13 This exposure pathway was considered <strong>for</strong> the local resource dominated PEG.73