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Radiography in Modern Industry - Kodak

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A filter reduces excessive subject contrast (and hence radiographic contrast) by harden<strong>in</strong>g theradiation. The longer wavelengths do not penetrate the filter to as great an extent as do theshorter wavelengths. Therefore, the beam emerg<strong>in</strong>g from the filter conta<strong>in</strong>s a higher proportion ofthe more penetrat<strong>in</strong>g wavelengths. Figure 39 illustrates this graphically. In the sense that a morepenetrat<strong>in</strong>g beam is produced, filter<strong>in</strong>g is analogous to <strong>in</strong>creas<strong>in</strong>g the kilovoltage. However, itrequires a comparatively large change <strong>in</strong> kilovoltage to change the hardness of an x-ray beam tothe same extent as will result from add<strong>in</strong>g a small amount of filtration.Figure 39: Curves illustrat<strong>in</strong>g the effect of a filter on the composition and <strong>in</strong>tensity of an x-ray beam.Although filter<strong>in</strong>g reduces the total quantity of radiation, most of the wavelengths removed arethose that would not penetrate the thicker portions of the specimen <strong>in</strong> any case. The radiationremoved would only result <strong>in</strong> a high <strong>in</strong>tensity <strong>in</strong> the regions around the specimen and under itsth<strong>in</strong>ner sections, with the attendant scatter<strong>in</strong>g undercut and overexposure. The harder radiationobta<strong>in</strong>ed by filter<strong>in</strong>g the x-ray beam produces a radiograph of lower contrast, thus permitt<strong>in</strong>g awider range of specimen thicknesses to be recorded on a s<strong>in</strong>gle film than would otherwise bepossible.Thus, a filter can act either to <strong>in</strong>crease or to decrease the net contrast. The contrast andpenetrameter visibility (See "Film Gra<strong>in</strong><strong>in</strong>ess, Screen Mottle") are <strong>in</strong>creased by the removal of thescatter that undercuts the specimen (See Figure 40) and decreased by the harden<strong>in</strong>g of theorig<strong>in</strong>al beam. The nature of the <strong>in</strong>dividual specimen will determ<strong>in</strong>e which of these effects willpredom<strong>in</strong>ate or whether both will occur <strong>in</strong> different parts of the same specimen.<strong>Radiography</strong> <strong>in</strong> <strong>Modern</strong> <strong>Industry</strong> 55

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