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Radiography in Modern Industry - Kodak

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Chapter 18: The Photographic Latent ImageAs shown <strong>in</strong> Figures 67 and 68, a photographic emulsion consists of a myriad of t<strong>in</strong>y crystals ofsilver halide--usually the bromide with a small quantity of iodide--dispersed <strong>in</strong> gelat<strong>in</strong> and coatedon a support. The crystals--or photographic gra<strong>in</strong>s--respond as <strong>in</strong>dividual units to the successiveactions of radiation and the photographic developer.The photographic latent image may be def<strong>in</strong>ed as that radiation-<strong>in</strong>duced change <strong>in</strong> a gra<strong>in</strong> orcrystal that renders the gra<strong>in</strong> readily susceptible to the chemical action of a developer.To discuss the latent image <strong>in</strong> the conf<strong>in</strong>es of this site requires that only the basic concept beoutl<strong>in</strong>ed. A discussion of the historical development of the subject and a consideration of most ofthe experimental evidence support<strong>in</strong>g these theories must be omitted because of lack of space.It is <strong>in</strong>terest<strong>in</strong>g to note that throughout the greater part of the history of photography, the nature ofthe latent image was unknown or <strong>in</strong> considerable doubt. The first public announcement ofDaguerre's process was made <strong>in</strong> 1839, but it was not until 1938 that a reasonably satisfactoryand coherent theory of the formation of the photographic latent image was proposed. That theoryhas been undergo<strong>in</strong>g ref<strong>in</strong>ement and modification ever s<strong>in</strong>ce.Some of the <strong>in</strong>vestigational difficulties arose because the formation of the latent image is a verysubtle change <strong>in</strong> the silver halide gra<strong>in</strong>. It <strong>in</strong>volves the absorption of only one or a few photons ofradiation and can therefore affect only a few atoms, out of some 10 9 or 10 10 atoms <strong>in</strong> a typicalphotographic gra<strong>in</strong>. The latent image cannot be detected by direct physical or analytical chemicalmeans.However, even dur<strong>in</strong>g the time that the mechanism of formation of the latent image was a subjectfor speculation, a good deal was known about its physical nature. It was known, for example, thatthe latent image was localized at certa<strong>in</strong> discrete sites on the silver halide gra<strong>in</strong>. If a photographicemulsion is exposed to light, developed briefly, fixed, and then exam<strong>in</strong>ed under a microscope(See Figure 126), it can be seen that development (the reduction of silver halide to metallic silver)has begun at only one or a few places on the crystal. S<strong>in</strong>ce small amounts of silver sulfide on thesurface of the gra<strong>in</strong> were known to be necessary for a photographic material to have a highsensitivity, it seemed likely that the spots at which the latent image was localized were localconcentrations of silver sulfide.

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