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PCM-2 Manual.pdf - Voss Associates

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Eq. 8<br />

EXAMPLE 2: An alpha CAM equipped with a multi-channel analyzer is set up to monitor for<br />

plutonium contaminated particulates. Background counts (or count rates) are the result of the<br />

presence of radon and thoron which produce a spectral distribution as illustrated in Figure 1 below.<br />

SPECTRUM DISPLAY<br />

10:42 13 Feb 88 10K<br />

Sto.tus: Flow Fa. il 8K<br />

Flow: 0,00 CfM 6k'<br />

Region Counts 4K<br />

Rm1~~Rm3 1~4<br />

I 'I I I<br />

I II I I<br />

'"<br />

I'<br />

I II<br />

"l<br />

I<br />

I<br />

'I<br />

II I I<br />

J/N:) :<br />

0 111285<br />

I II I<br />

2K<br />

I II I<br />

I I I<br />

Cursor Counts oa<br />

160 619 50 100 150 200 250<br />

Figure 1, Alpha CAM Spectrum<br />

Empirical data shows that counts collected in four regions of interest (ROls) have a consistent<br />

relationship in the absence of plutonium. That relationship is expressed by Eq. 9 where the four<br />

ROIs are identified as R, through R 4 and K is a constant.<br />

R I = K R3 Eq. 9<br />

R 2<br />

R 4<br />

Furthermore, when plutonium counts are present, they occur in R j , so that in order to maintain the<br />

equality of Eq. 9, the plutonium counts, Pu, must be subtracted from R I<br />

. This leads to the derivation<br />

of the mean plutonium counts (or mean count rate) as expressed by Eq. 11.<br />

R} - Pu R 3<br />

---=---- = K - Eq. 10<br />

R 2<br />

R 4<br />

Eq.11<br />

Eq. 4 is applied to Eq. 11 by first dissecting it into small, easily managed parts that are illustrated by<br />

Eq. 12 through Eq. 20 for the derivation of the Pu standard deviation. Eq. 21 is the result of<br />

collecting all pertinent terms to solve for (JPt,.<br />

<strong>PCM</strong>2.MAN

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