9 EVENT AND DESCRIPTION OF EXPORED GROUTS relationship to the surface dese and depth dose as dees the air dese mansnred in 0 “yest? esr” beam in the chmic or laboratory. source” beam air dems with comparable besliga eReri are contained: It would Rongelap, (irewp I... __.- yor Rongenk, (iroup II]... -- iw er appear wader these circumstances aad in most Ailinginae, Group IT... rather than dose measured in air, would be the Utink, Groep IV. 22-2 -_- experimental conditions that the midline dow, baer wr 160 to. date ° -- ani en eee Bale AA tL rie ‘ag, tt “. e 3 5 49 EXPOSURE, ’ MANY SOURCES ee : 7 € 2 5 $ Rano L986 « x . r + OILATERM. EXPOSURE, OFVERGING SOURCE et__ 0 5 Le) eo 1s + 2 CM MASONITE 2 3% y 3% DEPTH DOSE DISTRIBUTION IN CYLINDRICAL PHANTOM, CO" FACILITY, (NMR!) Fietas |.4—Comperison of drpta dose curves in maamite phantoms from bilateral exposure to a single point source, and aimultancuns erposure to malitiple sources with a ephcricel dietndution eround the phantom. better common parameter in terms of which to predict biological effect. On this assumption, the wir dose values stated in Table 1.1 should be multiphed by approximately 1.5 in order to compare their etfects to those of a given air dow from a “point source” beam geometry delivered bilaterally. If this is done, awsuming a fallout of 12 houry, the following “point 381712 0-56 2 The geometry of radiation from a fallout field is not identical either to the geometry of bilateral point sources or spherically distributed sources since the plane source delivers the radiation largely at a yrazing angle. However, the total field situation is better approximated by solid than by plane geometry. Exponure geosetry in a radioactive cloud would be sphenvcal.

Select target paragraph3