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Introduction to Health Physics: Fourth Edition - Ruang Baca FMIPA UB

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496 CHAPTER 9<br />

This result shows that the measured difference is 1.62 standard deviations from zero.<br />

From a table of areas under a normal curve, we find that 1.62 standard deviations<br />

includes 44.74% of the area on each side of the mean, or 89.48% of the area between<br />

±1.62 standard deviations. We interpret this result as saying that we would expect<br />

a difference this great 10 or 11 times out of 100 (100.00 − 89.48 = 10.52) if the<br />

two samples came from the same population. Therefore, the difference between<br />

the two samples is not statistically significant. To be statistically significant at the<br />

95% confidence level, the difference between the two means would have <strong>to</strong> be great<br />

enough <strong>to</strong> be observed only 5 times or less out of 100. When we are using the 95%<br />

confidence level, there is a 5% chance of incorrectly concluding that there is a<br />

difference between the two means when, in fact, the two means are members of the<br />

same population, and the observed difference is due <strong>to</strong> errors of random sampling.<br />

Minimum Detectable Activity<br />

The minimum detectable activity (MDA) is important in low-level counting, when the<br />

count rate of a sample is almost the same as the count rate of the background, Under<br />

these conditions, the background is measured with a blank—that is, with a sample<br />

holder, such as a planchet—and everything else that may be counted with the actual<br />

sample, except that there is no activity in the blank. The MDA is defined as the<br />

smallest quantity of radioactivity that could be distinguished from the blank under<br />

specified conditions. The MDA depends on the lower limit of detection and on the<br />

counting efficiency of a counting system.<br />

In Example 9.14, we wanted <strong>to</strong> know whether the two means differed. In determining<br />

the MDA, we wish <strong>to</strong> know whether the sample activity, M1, is greater than<br />

the blank activity, M2, not merely different from M2. To answer this question we use<br />

a “one-tailed” t test. In the one-tailed test, we resort <strong>to</strong> the cumulative area under<br />

the normal curve. To include 95% of the area under a normal curve, we have 50%<br />

from −∞ <strong>to</strong> the mean, and from the mean <strong>to</strong> the next 45% of the area is 1.645σ .<br />

Therefore, <strong>to</strong> be significant at the 95% confidence level when the one-tailed test is<br />

appropriate, the difference between the means must be ≥1.645σ .<br />

To decide whether or not a given sample has activity in it, we arbitrarily choose<br />

some count rate greater than that of a zero-activity blank that must be exceeded by<br />

the sample. If this decision level LC is chosen so that it will be exceeded only 5 times<br />

out of 100 by a zero-activity blank, then the net count rate of the sample must be<br />

greater than that of the blank by 1.645 standard deviations of the net count rate.<br />

This decision level considers only an alpha or type 1 error—that is, saying that there<br />

is activity in the sample when in fact there is none. Such an error is often called a<br />

false positive. The 95% confidence level means that we will be wrong, or have false<br />

positives 5 times out of 100. A beta, or type 2, error is one where we say that there is<br />

no activity when there really is activity. That is, a type 2 error is a false negative. Itis<br />

possible <strong>to</strong> have a very large type 2 error even if the type 1 error is only 5%. Figure<br />

9-41 illustrates the situation where the sample really contains radioactivity and its<br />

mean count rate is equal <strong>to</strong> the decision level of the background. In this case, the<br />

type 2 error can be 50%. The power of a statistical test, which is defined as<br />

Power = 1 − β, (9.52)

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