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Regional Basic Professional Training Course in Korea

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<strong>Regional</strong> <strong>Basic</strong> <strong>Professional</strong> <strong>Tra<strong>in</strong><strong>in</strong>g</strong> <strong>Course</strong> (BPTC) on Nuclear Safety<br />

layer(HVL) is used. This concept applies only <strong>in</strong> the case of photons.<br />

If a beam of photons consists of only a s<strong>in</strong>gle energy, the beam is referred to as<br />

monoenergetic. A beam of photons may be composed of many energies, generally the<br />

case with X‐ray. As a result, it is common to speak of quality and quality and quantity of<br />

a beam of photons.<br />

Quality refers to the energy of particular photons, and quantity refers to the number of<br />

photons of each specific energy. Quality and quantity are described together <strong>in</strong> a concept<br />

known as <strong>in</strong>tensity, def<strong>in</strong>ed as the total energy conta<strong>in</strong>ed <strong>in</strong> the beam quality x quantity<br />

per unit area per unit time. Hence:<br />

I(<strong>in</strong>tensity)<br />

ETotal<br />

=<br />

Area • Time<br />

The area referred to is the cross‐sectional area of the beam at a particular po<strong>in</strong>t <strong>in</strong> space.<br />

S<strong>in</strong>ce most beams of photons spread out as they move away from the source, it is<br />

important to specify where the <strong>in</strong>tensity is be<strong>in</strong>g calculated.<br />

In the follow<strong>in</strong>g discussion of HVL, a monoenergetic beam of photons has been assumed.<br />

The application to a non‐monoenergetic (polyenergetic) beam is described afterward.<br />

Consider a beam of photons approach<strong>in</strong>g a barrier, e.g., a simple wall, as shown <strong>in</strong> Fig.<br />

(2.15). Some of the photons penetrate to the far side of the wall, and some are attenuated<br />

by the wall material. The number of photons attenuated by the wall is a function of both<br />

the energy of the photons and the atomic number and density of the material compos<strong>in</strong>g<br />

the wall. In general, two pr<strong>in</strong>ciples apply:<br />

1. The more energetic the photons, up to a certa<strong>in</strong> energy, the less likely they are to be<br />

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