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PCM-2 Manual.pdf - Voss Associates

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I Z -J (R B + RDA x eff)jT<br />

I<br />

,~ RB + RDA x eff<br />

R B -+- R A(mex)<br />

Figure 8<br />

Eq. 42 expresses the computation of RA(MAX)'<br />

JRDA X Eft + R,<br />

RA(MAX) = RDA X Eff - Z ----:r=---­<br />

Eq.42<br />

Optimization<br />

Figure 9 will be used as the basis of discussing how a counting exercise can be set up so as to<br />

maximize its desired performance. Figure 8 illustrates the relationship of RA(MIN) and RA(MAX) on a<br />

single number line whose domain is non-negative count rates. First of all, it is important that RA(MIN)<br />

be kept less than or equal to RA(MAX)' Whereas the spread of the distribution curve is determined by<br />

the standard deviation associated with it, adjusting a will adjust the breadth of its curve and, along<br />

with it, the position of R A relative to the curves peak. Studying the expressions for a B and as (the<br />

radical terms in Eq. 35 and Eq. 42), it should be apparent that the parameter most likely to be<br />

controlled by the operator of a radiation monitor is the length of the counting interval, T. Because T<br />

is in the denominator, larger values of T will reduce a. There can be several interpretations of how a<br />

counting exercise can be optimized. Each is discussed separately.<br />

1J'Vr-7(-R.-+-R-DA-x-e-ff-')/~T<br />

R + R<br />

• o("'n)<br />

LL R. + RDA • .ff<br />

RI + R0(.....)<br />

Figure 9<br />

<strong>PCM</strong>7.MAN

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