EVENT AND 1.2 DESCRIPTION OF EXPOSED GROUPS 3D carried out, nor was its operating condition Whole Body Gamma Doses known to be satisfactory under the emergency condition prevailing at the time of use. For Tur EstimatTep Vauves of external dose given in Table 1.1 were calculated from readings of radiation field survey instruments.* Averages of a numberof dose rate measurements on each island at a given time were used. The readIngs were taken in air, approximately three feet above ground, several days after the inhab- these reasons the later readings, which were higher than the early survey by an average of 50 percent when corrected to the same times, were used in computing the doses listed. The instruments used for the later measurements were calibrated just prior to the surveys. 30 ~secee ORIGINAL SOURCE SPECTRUM ame INFINITE PLANE,3 IN AIR i 1 | 2 20 I ' ' ; LL 8 ' ; ‘ yo § i ° Vs °o \I - 1 ul o ii z I or a 2 ! ' \ 10 | \ i ' ht t ' ' ' i ' 1 ' ‘ k ol! 0 \ 1 14 I ' i | 1 ' ' ji 200 l { ' i ' I t ' { 400 ' ' ' ' | i t ‘ , ;J ' ‘ i 1 | i 1 ' “I 600 ' 1 ' I ! t I ' ' \ ‘ ' ' { 1 j ' ' 3 I ' ' 1 I | ' 1 I ae 8900 is 1000 ' ' ' ENERGY (KEV) Ficure 1.2—-Distribution of inherent energies of gamma radiation from mized fission products, and histogram of degraded energies produced by Compton scattering at level of infinite plane 3 feet in air above uniformly-distributed fission products field, itants were evacuated. Before this time, adequate surveys with well calibrated instruments had not been possible, although readings had been taken with a single survey meter at the time of evacuation. However, preliminary calibration of this instrument had not been Po C3 a *Army Navy catalop AN/PDR-39, 1.21 Characteristics of the Gamma Radiation The fallout material, when deposited on the ground, formed a large planar source of radiation. The energy distribution of the radiation reaching an exposed individual was influenced by its passage throughthe intervening air. A knowledge of the energy spectrum of the ra-