a

eae

eee wre

-— we

ohysycians,

who

ad

had

atm

no

.

eet

wee

dtrect way

gE

ae

ee

went

te

determining «nat

tissues were recelving from a give exposure.

he ke ee

che

That is

~~ «

tutor

“3

wee

of nersil

to sav, ome Must use

a “cell phantom” tf one wishes to estimate the dose to a Living cell.
we ust outline
cell phantom.

the requirements ana lecessary charactertstics of
However,

only

the dose

4avptoach

to

tne Ladividual urpan of

the problem from the Ch,

statistics standpoints.
radiation enersy
(L.@., due

to

This

tlisues

Cumuoc of

taterest, ~2 must

1.e., epidentlolugteal and acciceur

is, of course,

tanes plac2

because any

transfer of

only 45 a result of

s7sena

bet.zen 2 ch:ryved

the (fractional) number of cells nit.

Also, because

1.e.,

the “nit slze” or “celi dose”.

magnitude of

the cell cose varies greatly from cell

trom zero to

the maximum amount of kinetic energy carried by

the

dose,

to

be

Thus <e

the TCY in separate, discrete amounts, we need also

the amount of energy deposited,

Thus

regiiced

al

particle and a target-containinsg volume (TCV) within the cell.
energy is deposited tn

unitke

ia an “td* rode amd

to random processes) encounters or collisions

first need, with LLE,

Sucn a

in so dulnhg we cust Be ever mindful that,

the eicly (and peesent) physiclans who operated

Thus

relevant,

must be

registered

The

tuo cell, anc ranges

in

tne particle.

[ndivideals

ace

tre

level of bDfLological organization at which the

initatioa of

interest occurs.

that, while with KLE oniy

The

imporctunc conclusion is

the response cf
the

one physical quantity organ dose is cequired tor risk evaluation, witn LLE
least

The
and

two

fodependent

quantities

First requirement,

cosed

during

electronic.

any given

many hits per cell can
register a

to >

total

of

x

f2

verfod

Te

requires

the shect recovery

be recorded
hits

rcequtrea,
-

a.e

exposure

It can then have

are
wT

iD

at

during

(L.e.,

that

tiie needed in order that

tf a number of phantom cells

au exposure

Cine

t,

then a

cecovering cell will also register x hits during a time
of

the phantom will, with use of

with

the

first

of

at

least

eoidemtological evaluation,
numerically

to

the

tyvo

xt).

Tr

the appropriate scaling factor,

probabilities!

namely,

probability

the

the

that a

needed

nunber

cell

will

of

in

hits

be hit,

provide us

principle
per

cell,

doses,

for
equal

ana

tnrured.

=o
;
The number in a group expected to respond quantally attec a alven exsosuce
provides the numerical probability that such a response will accur.
Thus,
the term probability will be used interchangeably with tne terus “rraction’
or “proportion” of equaily dosed quantal responders and the term “risa”
will be used fLaterchangeably sith the oruportics or inefdence of
stuchastically, and thus unequally-dosed quantal respunders.

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