: or wn eeneet adma aeIaA meOL ee tay CU + eeNPaa 2 cmined digh-Level Exposure je and The above discussion has referred principally to “low-level” Thus severe at exposure, The differences between low- and high- level exposure are shown in Figure 8, for a low-LET radiation only. all. horizontal and then diagonal, is for the specific energy (cell dose), vs. the absorbed dose to the organ. of cells hit, {.e., The heavy solid line, first The upper dotted line Is for the fraction the nunber of hits per cell, as a function of organ absorbed dose. = © 2& 10? 10? 10 10' Pr) 3 16 wo & 10° = ® z Ww Oo c 3oF ~ wy ad ro] 2 @® 10? 310° ~ E 5 o > 10° 6 F103 Cc o Oo ‘ mo, cS = o'r low dose ® ute. Q 5 Gr 9 lot 10-4 te 2 10* 10° high dose a i 104 i 107 L 107 4 i #10' i 10° 10° 10° 10 10° 10 c oO = 8 uw i 10+ Absorbed dose/Gy 28 am the S that an atinuous =_ 3 is Fig. 8 Relationship hetveen the specific energy, 1.e., cell dose, as well as the fraction of affected target-containing volumes within a cell, and the organ absorbed dose in Gy. Note that at large crgan doses, cell and organ dose approach being equal, and the variance becomes small. At low organ doses, the expectation value of the cell Jose becomes constant, although the variance of that mean {a quite large. At these low organ doses, it is only the fraction of cells hit and dosed that can increase with organ absocbed dose. Where the solid line becomes diagonal, the upper large-exposure pact of the curve, each cell has received a large number of hits. If one calls the summation of energy densities from these multiple hits the "cell dose", then it is clear that even though that “dose” vary greatly in size, Snaller and smaller. cell TCV, Cs 22 ght better beey in There risk for each discrete hit. the individual hits constituting the variance of is then no reason It fis adequate, tions * -~221- the mean will become to evaluate separately for practical reasons, the simply