T.O. 33B-1-16-42linear attenuation coefficient (m) can be changed by changing radiation energy. This in turn will change the ratio IT/I0or the percent radiation transmitted through a part of thickness, x. In industrial radiographic applications, thedifference in thickness (often due to discontinuities) is the actual parameter from which interpretation is made.Therefore, the greater the change in the radiation transmitted due to a particular change in material thickness, the moreobvious is the thickness change revealed in the final image. This radiation difference due to material thickness changeis called the material contrast. The material contrast is a function of the absorption characteristics of the part beinginspected and the radiation energy level. When measurements have been made and a numerical value has beenestablished, it is called the material contrast factor.6.5.5.2 PercentRadiationTransmission.When monochromatic radiation is used, the percentage of radiation transmission can be calculated from the formallaws of attenuation. Since this condition seldom exists in actual practice, the percent of radiation transmitted must beempirically measured. When the proper recorder is used, the actual measurements will include the scattered radiationas well as the transmitted primary beam, both of which can be expected to expose a film or interact with any otherrecorder in a typical industrial radiographic set-up.SECTION VISPECIAL RADIOGRAPHIC TECHNIQUES6.6 SPECIALRADIOGRAPHICTECHNIQUES.6.6.1 Introduction.The previous sections of this chapter have been primarily concerned with conventional film radiography. While filmradiography offers a very versatile tool for the detection and identification of material discontinuities, there are a varietyof special techniques that may be employed to extend the capabilities of conventional radiography. Special techniquesmay be placed into two broad categories. The first relates to radiographic techniques with a specific objective ofextending the capabilities of the inspection method in general. This first category would include such techniques asmulti-thickness, multiple film, triangulation, thickness measurement and stereo (three-dimensional techniques). Thesecond category relates to special imaging methods, such as radioscopy with techniques such as image intensifiers, orX-ray vidicon, photoradiography, Polaroid radiography, photothermographic film and radiographic paper. Specialradiographic methods that are not included in authorized inspection manuals SHALL NOT be used without writtenapproval of the appropriate depot engineering activity.6.6.2 SpecialPurposeTechniques.6.6.2.1 MultiThicknessTechniques.Most real life situations involve the radiography of parts of widely varying thicknesses and sometimes of two or morematerials. If it is possible to concentrate on one area with a nearly constant thickness, optimization of image density isstraightforward. Often, however, it is necessary to obtain an acceptable exposure for two or more difference thicknesseson the same image. Small thickness variations, for example, of 0.8 to 0.6 inches, can lead to large variation in density,from 1.2 to 1.7 respectively. The aim is to insure that all areas of interest have densities that are not so low so as to losefilm contrast and not so high that they cannot be evaluated. An acceptable range of densities is 1.0 to 3.5. Theprocedure recommended during technique development is to identify the thickest area of interest, and then fromexposure charts and trial-and-error, determine the exposure and kilovoltage that gives a density of 1.0. A trial shot willthen show the density of the image of the thinnest area of interest. There are three possible courses of action:a. If the density of the image of the thinnest section is approximately 3.5 and the image can besatisfactorily interpreted, the technique is optimized.b. If this density is too low, the exposure should be increased to raise the average density of thick and thinareas.
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