On account of the small depth of penetration of 1-3 MeV electrons, a technique is used for the radiation of large objects--or, rather, large surfaces--whereby the electron beam is moved back and forth, or scanned, over a certain width, at the same time as the surface to be radiated is moved, at a uniform rate, at right angles to the scanning direction. Besides the radiation of a large surface,
... [Show full abstract] the scanning and the moving of the table have still another important function, viz., keeping the total energy absorbed locally per time unit low enough to avoid the development of too high temperatures, which would lead to damage to exit window of accelerator and the radiated object.