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Intensity-Modulated Illumination of Paintings and an Unexpected 3-Dimensional Effect

Bibliographic Data

ID10283150
AuthorsA A Mills (0000-0003-3056-7764, corresponding author)
Year1978
Volume11
Issue3
Pages213
Publication date1978-01-01
Peer ReviewedYes
Open AccessNo
TypeARTICLE
VenueLeonardo (JOURNAL)
Journal identifiersISSN: 0024-094X • E-ISSN: 1530-9282
PublisherJSTOR (PUBLISHER)
DOI10.2307/1574147
OpenAlexW2326951098
LanguageEN
Citations received1
References cited1

The whitest paints used by artists reflect about 90% of the light incident upon them, while black surfaces still reflect as much as 4 or 5%, so the maximum luminance scale that can normally be realised upon an opaque base is of the order of 20:1. Most older paintings would be expected to show a shorter range than this, due to such factors as sulphide darkening, fading of pigments and the yellowing of oily media and varnish. In a real 3-dimensional scene, objects seldom receive the same illumination. Objects in shadow receive much less radiation than those in direct sunlight, so that still less light is reflected if they are inherently highly absorbing. The result is a much longer luminance scale. L. A. Jones and H. R. Condit gathered quantitative photometric data for a wide selection of scenes and found that an average range was 160:1, with values going up to 760:1 for scenes containing brightly sunlit white clouds and deep foreground shadows[1]. It is therefore apparent that the luminance range of a painting will rarely match that of the scene depicted, particularly for an outdoor or sunlit subject [2]. Some compression of the scale is inevitable, and no amount of 'flat' illumination directed upon it will correct this. This argument does not apply to pictures painted in transparent colours on a transparent support such as glass, which (like photographic colour slides) may be illuminated and viewed by transmitted light. However, only a few painters have worked with this medium, for example Gainsborough [3]. In order to extend the luminance scale of a painting upon an opaque support, light must be directed preferentially upon the lighter areas of the work with progressively lesser amounts upon the darker portions. Around 1908 R. W. Wood realised that intensity modulation could be obtained by illuminating a painting through a photographic diapositive (slide) of itself [4], but the techniques and apparatus available at that time rendered the procedure clumsy and impracticable, and his scheme was not published. I have investigated the effects of illuminationg high quality reproductions of works by Vermeer and by other artists in this manner,using modern 35-mm monochrome transparencies and associated equipment. I found that precise registration between the projected image and the original was most important. This was facilitated by adding a zoom lens plus vertical and horizontal screw adjustments to the slide projector. When exact alignment was achieved, it was observed that Vermeer's works, in particular, were dramatically transformed: one appeared to be viewing the actual scene through an open window rather than a flat representation

Art · Computer graphics (images) · Intensity (physics) · Optics · Painting · Physics · Visual arts · Aesthetic Perception and Analysis · Architecture and Art History Studies · Color perception and design · Computer Science · Materials Science

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    John M Kennedy, M H Pirenne•Leonardo•1971

Unique citing works1
Citations per year0.02
Citation span1981 - 1981 (1)
Citation velocityhistorical
Highly citedNo

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