A_{t} = A₀e^{-λt}

where A_{t} is the radioactivity of an isotope at some time, t, after

the end of the irradiation, and A₀ is the radioactivity at the end of

the irradiation.

[Illustration: Fraction of saturation sodium-24 activity _vs_ Time of

irradiation (hours)]

The activation of sodium-23 to sodium-24, which has a half-life of 15

hours. The horizontal line marked 1.0 represents the “saturation”

activity level for a sample of sodium of a certain size in a constant

neutron flux. Note that after about 120 hours, the activity of the

sample is within 1% of the value at saturation, which is the most

active that sample will ever become at a given φ. Note also that after

the first 15 hours (1 half-life) the sample is exactly half way to its

value at saturation. Thus long irradiations are useful to increase the

sensitivity of the analysis, but only up to a certain point.

The result of all this is that the sensitivity of an analysis depends in

practice on a number of practical as well as theoretical factors:

1. The cross section of the target element.

2. The half-life of the radioactive isotope produced.

3. The time available for irradiation.

4. The flux of neutrons available for irradiation.

5. The promptness with which we can begin measuring radioactivity and

the efficiency of this measurement.

6. Possible interferences due to the presence of elements yielding the

same radioactive elements or those yielding very similar

radiations.

In the next section of this booklet, there are several examples that

will show you how all this works in practice. But to summarize what

these factors mean in terms of sensitivity let us look at the chart in

the figure on page 18. Here all the elements are arranged in a periodic

table. The sensitivities are shaded in coded ranges representing

measurable quantities. They are calculated on the basis that there are

no interferences, that the neutron flux is 10¹⁴ neutrons per square

centimeter per second, and that we can measure 100 gamma rays per minute

without much difficulty assuming a gamma-ray detector efficiency[7] of

10%. The elements labeled β yield radioisotopes that emit few or no

gamma rays and can only be analyzed by neutron activation using

appropriate chemical separation procedures followed by beta

radioactivity measurements. Such chemical separation procedures (to

remove unwanted radioactive isotopes of other elements) are also

sometimes useful to improve the sensitivity of the analysis of gamma-ray

emitters if necessary.

[Illustration: Graph: “Fraction of Sodium-24 remaining” vs. “Time of

decay (hours)”]

The radioactive decay curve of sodium-24. The vertical scale is not

_linear_ but _logarithmic_. Thus, each factor of two in radioactivity

occupies the same distance along the vertical axis. When two samples

are being analyzed for sodium by activation analysis, they must be

compared at the same time after they have been removed from the

neutron flux. If this period of time is different, then a correction

must be applied to one of them, based on the decay curve shown here,

to allow for the difference in decay time for the two. Waiting too

long after the irradiation is completed results in much poorer

sensitivity for the analysis depending on the half-life of the

activation product. In this case, after 2 days it takes approximately

ten times as much sodium to yield the same radioactivity as it would

if the sample were measured when it was fresh out of the reactor.

It is not practical to determine a few elements, shown in black squares,

by activation analysis. Some others, like oxygen and nitrogen (labeled

HE), can be measured by using other projectiles like fast (more

energetic) neutrons, or protons or deuterons[8] produced in a device

called an accelerator. Other elements, those shown in white squares, can

be detected with such great sensitivity, that one can find some in

almost everything. For example, if you had a cube of “pure” aluminum

only 1 millimeter on a side, you could detect gold in it if there were

only one atom of gold for every fifty billion atoms of aluminum.

While it isn’t often that you would want to find a gold needle in an

aluminum haystack, the next section presents some practical

applications. Imagine yourself as the person with the problem in these

situations.

[Illustration: Periodic table of elements, with sensitivity code]

* Th and U are radioactive but with such long half-lives that

neutron activation analysis can be used for their determination.

† µg = Microgram (one-millionth of a gram)

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