A Different Approach to Evaluating Health Effects from Radiation Exposure
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V. P. Bond! , C. A. Sondhaus?, and L. E. Feinendegen>

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ABSTRACT

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Absorbed dose D is shown to be a composite variable,

the product of

the fraction of cells hit (F) and the mean “dose" (hit size) Z to the hit
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cells. D is suitable for use with high level exposure (HLE) to radiation

NS,

and its resulting acute organ effects because F = 1.0,

and

approximates closely enough the mean energy density in both the cell and

ral a
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the organ.

However, with low-level exposure (LLE) to radiation and its

consequent probability of cancer induction from a single cell, F is <<1.0
and stochastic delivery of energy to cells results

acellular

of single hit sizes.

d

with exposure,

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and

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so that only F can vary with D.

46,

none
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the fraction of cells transformed, obtained with LLE,

misleading.

It does not mean that any (cell) dose, no matter how small,

on the
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diat.

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cells.

Rather,

it means

is

that an exposure of a population of the

constituent relevant cells of an organ results in a Linear increase in the
number of cells dosed, but not in cell dose.

The probability of such a

dosed cell transforming and initiating a cancer can only be greater than
Otherwise stated,

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Ra

the apparent proportionality between this

zero if the hit size ("dose of energy”) to the cell is large enough.

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However, because D is the

quantity and

can be lethal,

ancer

in a wide distribution

As a result the expectation value of z is constant

mean organ= and not cell dose,

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so that D

if the “dose” is defined at the proper level of

biological organization, namely,

the cell and not

the organ, only a large

dose to that cell is effective.

The above precepts are utilized to develop

a drastically different approach to evaluation of the risk from LLE, that
holds promise of obviating any requirement for use in this region of the

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principal components of the present system: absorbed organ dose, LET, a

standard radiation, RBE, Q, dose equivalent and rem.
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rookhaven National Laboratory

This research was supported in part by the U.S. Department of Energy
under Contract DE-ACO2-76CHO0016. Accordingly, the U.S. Government
retains a nonexclusive, royalty-free license to publish or reproduce the

published form of this contribution, or allow others to do so, for U.S.
Government purposes.
Army Chemical School, Radiation Laboratory, Fort McClellan, Alabama

3 Laboratory for Nuclear Research (KFA), Juelich, FRG
-203-

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