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Varian Linatron High-Energy X-ray Applications 2007

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Introduction<br />

X-<strong>ray</strong>s are a type of electromagnetic energy that occupies a<br />

particular place in the electromagnetic spectrum. What we<br />

refer to as X-<strong>ray</strong>s is a type of energy that can be understood<br />

as both particles and waves because they have characteristics<br />

of both. Photons are the particle aspect of X-<strong>ray</strong>s, which<br />

are mass-less and travel at the speed of light. These are<br />

produced by <strong>Linatron</strong>s when high energy electrons are<br />

accelerated and strike a high density metal target. This<br />

releases photons in the X-<strong>ray</strong> frequency band as shown in<br />

Fig. 1-1.<br />

FIGURE 1-1. Spectrum<br />

Nondestructive testing using high energy (greater than 1<br />

MeV) radiographic techniques has been in use for more<br />

than 60 years. During this period, a number of highenergy<br />

X-<strong>ray</strong> sources have been developed for the detection<br />

of flaws in heavy metal sections. More recently, these x-<strong>ray</strong><br />

sources have found important uses in cargo screening and<br />

related security inspections applications. Please consult<br />

other <strong>Varian</strong> documentation for information on cargo<br />

screening applications.<br />

The first commercial high-energy X-<strong>ray</strong> source was the 1<br />

MeV resonant transformer, introduced by General Electric<br />

in 1939. A few years later there appeared 2 MeV versions<br />

of the resonant transformer, Van de Graaff generators with<br />

energies of 1 MeV and 2 MeV, and Betatrons with electron<br />

beam energies ranging from 15 MeV to 25 MeV.<br />

page 3<br />

The maximum X-<strong>ray</strong> output of these early machines was<br />

limited. Electron linear accelerators, which became available<br />

commercially about 1956, offered a way to substantially<br />

increase the X-<strong>ray</strong> output and made practical the<br />

radiography of steel sections greater than 2 feet thick. This<br />

met the need of modern nuclear technology which required<br />

radiographic examination of assemblies containing relatively<br />

thick sections of very dense material, such as uranium and<br />

tungsten alloys. Linear accelerators proved capable of<br />

penetrating and recording flaws or other anomalies on x-<strong>ray</strong><br />

film through many inches of such materials.<br />

<strong>Varian</strong> SIP (Security and Inspection Products) first<br />

extended its linear accelerator technology into the highenergy<br />

radiography field in December 1959 with the<br />

delivery to the U.S. Navy of a 10 MeV machine designed<br />

to produce high-quality radiographs of the Polaris missile<br />

and other solid rocket motors. In the years that followed,<br />

<strong>Varian</strong> SIP continued to supply similar machines to<br />

government and industrial customers.<br />

In 1968, <strong>Varian</strong> SIP introduced the <strong>Linatron</strong>®, a line of<br />

industrial linear accelerators with energy ranges from 1 to<br />

15 MeV. The <strong>Linatron</strong> represented a significant advance<br />

in reliability and ease of operation and handling. A typical<br />

<strong>Linatron</strong> installation includes an X-<strong>ray</strong> head (Figs. 1-2 and<br />

FIGURE 1-2. <strong>Linatron</strong> M9 X-<strong>ray</strong> head.<br />

<strong>Varian</strong> <strong>Linatron</strong> applications

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