Solarization (photography): Difference between revisions
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{{Short description|Photographic tone reversal due to overexposure}} |
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{{about||the photographic effect involving exposure during development in the darkroom|Sabattier effect||Solarization (disambiguation)}} |
{{about||the photographic effect involving exposure during development in the darkroom|Sabattier effect||Solarization (disambiguation)}} |
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[[File:Hydroelectric power plant with solarisation.jpg|upright=1.5|alt=Solarized photography|thumb|Photography exhibiting solarization effect: the sun appears black.]] |
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{{Alternative photography}} |
{{Alternative photography}} |
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In photography, '''solarization''' is the effect of ''tone reversal'' observed in cases of extreme [[Exposure (photography)|overexposure]] of the [[photographic film]] in the camera. Most likely, the effect was first observed in scenery photographs including the sun. The sun, instead of being the whitest spot in the image, turned black or grey. For instance, [[Minor White]]'s photograph of a winter scene, ''The Black Sun 1955'',<ref>[https://www.moma.org/collection/works/47096 ''The Black Sun 1955'']</ref> was a result of the shutter of his camera freezing in the open position, producing severe overexposure.<ref>{{cite book |title=Große Photographen |chapter=1940 bis 1960 |work=Life Die Photographie |publisher=Time-Life International (Nederland) B.V.. |year=1973 |page=216|quote=in German }}</ref><ref name="Jolly1">{{cite web |url=https://www.wljollysolarizationchemistryphotography.org/book-solarization-demystified |archive-url=https://web.archive.org/web/20190110235054/https://www.wljollysolarizationchemistryphotography.org/book-solarization-demystified |url-status=dead |archive-date=January 10, 2019 |title=SOLARIZATION DEMYSTIFIED |last=Jolly |first=William L. |access-date=2019-01-13 |quote=Chapter 1 }}</ref><ref name=Warren>{{cite book |last1=Warren |first1=Lynne |url=https://books.google.com/books?id=FLTyvuWX6MMC&pg=PA85 |title=Encyclopedia of twentieth-century photography |date=2005|publisher=Routledge|location=New York|isbn=978-1-57958-393-4|pages=1459–1460}}</ref> Ansel Adams had also earlier created a solarized sun image, titled ''Black Sun, Owens Valley, California, 1939'', by overexposure.<ref>{{Cite web |url=http://www.harlanerskine.com/blog/2008/04/the-black-sun-by-ansel-adams-and-minor-white.html |title=''Black Sun, Owens Valley, California, 1939'' |date=15 April 2008 |access-date=2019-01-13 }}</ref> |
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==Definition== |
==Definition== |
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When a photographic layer, suitable for solarization (see below), is exposed to actinic radiation, the resulting darkening after development will not increase steadily, but reaches a maximum which decreases under more intense exposure. In general is the phenomenon only then called solarization if the exposure has been produced in one "shot", meaning no pauses or double-exposures. The exposure to achieve solarization can be increased by exposure time or by increasing the light intensity<ref name="Frieser">{{cite book |last1=Tomamichel |first1=Franz |title=Die photographische Empfindlichkeit |chapter=8.6. Photographische Effekte durch den Abbau eines vorgelegten latenten Bildes |volume=3 |editor-last=Frieser |editor-first=H. |editor2-last=Haase |editor2-first=G. |editor3-last=Klein |editor3-first=E. |work=Die Grundlagen der photographischen Prozesse mit Silberhalogeniden |location=Frankfurt am Main |publisher=Akademische Verlagsgesellschaft |year=1968 |pages=1217–1232 |oclc=310490074 |language=de }}</ref> |
When a photographic layer, suitable for solarization (see below), is exposed to [[Actinism|actinic radiation]], the resulting darkening after development will not increase steadily, but reaches a maximum which decreases under more intense exposure. In general is the phenomenon only then called solarization if the exposure has been produced in one "shot", meaning no pauses or double-exposures. The exposure to achieve solarization can be increased by exposure time or by increasing the light intensity<ref name="Frieser">{{cite book |last1=Tomamichel |first1=Franz |title=Die photographische Empfindlichkeit |chapter=8.6. Photographische Effekte durch den Abbau eines vorgelegten latenten Bildes |volume=3 |editor-last=Frieser |editor-first=H. |editor2-last=Haase |editor2-first=G. |editor3-last=Klein |editor3-first=E. |work=Die Grundlagen der photographischen Prozesse mit Silberhalogeniden |location=Frankfurt am Main |publisher=[[Akademische Verlagsgesellschaft]] |year=1968 |pages=1217–1232 |oclc=310490074 |language=de }}</ref> |
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==History== |
==History== |
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The solarization effect was already known to |
The solarization effect was already known to [[Daguerre]] and is one of the earliest known effects in photography. [[John William Draper]] was the first to call the overexposure effect solarisation. [[John Herschel|J.W.F. Herschel]] already observed the reversal of the image from negative to positive by extreme overexposure in 1840.<ref name="Frieser" /> Also [[Noël Paymal Lerebours|N.M.P. Lerebours]] observed the phenomenon in 1842 (without him recognizing what it was) when he made a [[daguerreotype]] of an [[image]] of the [[sun]]. The result was seen as unsatisfactory because the solar disk (image of the sun on the daguerreotype plate) was [[Overexposure|overexposed]] and solarized.<ref>{{cite book |last1=Barger |first1=M. Susan |last2=White |first2=William B. |url=https://books.google.com/books?id=FLTyvuWX6MMC&pg=PA85 |location=Baltimore and London |title=The Daguerreotype: Nineteenth-Century Technology and Modern Science |publisher=Johns Hopkins University Press |date=12 May 2000 |page=85 |isbn=9780801864582 }}</ref> Ludwig Moser reported in 1843: "...that the light in the camera obscura produces at first the well known negative image; with continued action of the light the image turns into a positive image.... and recently I have obtained in fact on occasion a third image which is negative".<ref name="Frieser" /> In 1880 [[Pierre Janssen|Janssen]] had obtained in the strongest sunlight a repetition of the solarization phenomena.<ref>{{cite book |last1=Eder |first1=Josef Maria |title=History of Photography |chapter=LXIX. Photographic Analysis of Movement by Janssen and Marey |location=New York |publisher=Dover Publications, Inc. |year=1972 |page=506 |isbn=978-0-486-23586-8 }}</ref><ref>{{cite book |last1=Launay |first1=François |title=The Astronomer Jules Janssen |chapter=The Method of Stellar Circles |chapter-url=https://books.google.com/books?id=3YaAup49nqoC&q=janssen+solarization&pg=PA116 |location=New York Dordrecht Heidelberg London |publisher=Springer |year=2012 |page=116 |isbn=978-146140-697-6 |access-date=2019-01-08 }}</ref> |
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==Explanation<ref name="Frieser" /> |
==Explanation== |
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'''Source:'''<ref name="Frieser" /> |
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Not every photographic layer exhibits solarization. Pure [[Chloride]] and [[Iodine]] based silver [[photographic emulsion|emulsions]] are difficult or unable to solarize. In general, it can be stated that solarisation can only be observed if the photographic layer is capable to create a latent image inside the halide grain underexposure by actinic radiation.<ref name="Frieser" /> |
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Many explanations have been given but until further notice, the solarization was until 1929 generally understood as a combination of two main processes: the coagulation (clotting) and the regression process. |
Not every photographic layer exhibits solarization. Pure [[chloride]] and [[iodine]] based silver [[photographic emulsion|emulsions]] are difficult or impossible to solarize. In general, it can be stated that solarisation can only be observed if the photographic layer is capable of creating a latent image inside the halide grain underexposure by actinic radiation.<ref name="Frieser" /> Many explanations have been given but until further notice, the solarization was until 1929 generally understood as a combination of two main processes: the coagulation (clotting) and the regression process. |
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=== Regression theory === |
=== Regression theory === |
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The regression process theory was formulated by H. Luppo-Cramer in 1911, based on research by [[Ferdinand Hurter|F. Hurter]], [[Vero Charles Driffield|V.C. Driffield]] and H. Luggin. |
The regression process theory was formulated by H. Luppo-Cramer in 1911, based on research by [[Ferdinand Hurter|F. Hurter]], [[Vero Charles Driffield|V.C. Driffield]] and H. Luggin. |
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By exposure the surface and the interior of a silver-bromide sphere will disintegrate by the expulsion of bromide. Whereas the bromide on the surface can permeate away, the bromide can not so easily permeate away from the interior. The overexposure generates now a bromide pressure that escapes from the internal sphere and permeates to the surface where it oxidizes the latent image situated there, constituting the regular latent image under normal exposures. This destroys the latent image, because only silver on the surface can be developed. |
By exposure the surface and the interior of a silver-bromide sphere will disintegrate by the expulsion of bromide. Whereas the bromide on the surface can permeate away, the bromide can not so easily permeate away from the interior. The overexposure generates now a bromide pressure that escapes from the internal sphere and permeates to the surface where it oxidizes the latent image situated there, constituting the regular latent image under normal exposures. This destroys the latent image, because only silver on the surface can be developed. |
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=== Coagulation theory === |
=== Coagulation theory === |
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H. Arens published in 1925 a paper about reversal effects in which he concluded that solarization is based upon the finding that under increasing exposure the latent image successively coagulates and thus increases the size of each particular |
H. Arens published in 1925 a paper about reversal effects in which he concluded that solarization is based upon the finding that under increasing exposure the latent image successively coagulates and thus increases the size of each particular silver speck. This again causes the silver speck to lose its catalytic effect for the development. |
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=== Bromide migration theory === |
=== Bromide migration theory === |
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H. Kieser published in 1929 a paper in which he speculated about the possibility of bromide migration by [[Electron deficiency|defect electrons]] ([[Silver bromide#Photosensitivity| |
H. Kieser published in 1929 a paper in which he speculated about the possibility of bromide migration by [[Electron deficiency|defect electrons]] (see: [[Silver bromide#Photosensitivity|Photosensitivity]]). |
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In recent years an understanding has been agreed upon in which this bromide migration to the surface by overexposure forms a bromine condensation, resulting in bromine molecules or bromine atoms diffusing to the |
In recent years an understanding has been agreed upon in which this bromide migration to the surface by overexposure forms a bromine condensation, resulting in bromine molecules or bromine atoms diffusing to the silver specks of the latent image. Thus the latent image at the crystal surface can be re-[[Halogenation|halogenated]] by chemical reaction, notwithstanding an increase of the amount of latent image in the interior of the crystal. Still, the regression and coagulation theories are believed to contribute up to a certain level to the solarization effect. |
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==Pseudo-solarization== |
==Pseudo-solarization== |
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{{Main|Sabattier effect}} |
{{Main|Sabattier effect}} |
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'''Pseudo-solarisation''' (or '''pseudo-solarization''') is a phenomenon in |
'''Pseudo-solarisation''' (or '''pseudo-solarization''') is a phenomenon in photography in which the image recorded on a [[Negative (photography)|negative]] or on a photographic print is wholly or partially reversed in tone. Dark areas appear light or light areas appear dark. The term is synonymous with the '''Sabattier-effect''' when referring to negatives. Solarisation and pseudo-solarisation are quite distinct effects. |
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In short, the mechanism is due to halogen ions released within the halide grain by exposure diffusing to the grain surface in amounts sufficient to destroy the latent image.<ref>{{cite book |title=The Focal Dictionary of Photographic Technologies |last= Spencer|first=D A |authorlink= |year=1973 |publisher=Focal Press |location= |isbn=0-240-50747-9 |page=574 |
In short, the mechanism is due to halogen ions released within the halide grain by exposure diffusing to the grain surface in amounts sufficient to destroy the latent image.<ref>{{cite book |title=The Focal Dictionary of Photographic Technologies |last= Spencer|first=D A |authorlink= |year=1973 |publisher=Focal Press |location= |isbn=0-240-50747-9 |page=574 |url= |accessdate=}}</ref> |
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==References== |
==References== |
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Latest revision as of 12:52, 29 November 2024
| Alternative photography |
|---|
 |
In photography, solarization is the effect of tone reversal observed in cases of extreme overexposure of the photographic film in the camera. Most likely, the effect was first observed in scenery photographs including the sun. The sun, instead of being the whitest spot in the image, turned black or grey. For instance, Minor White's photograph of a winter scene, The Black Sun 1955,[1] was a result of the shutter of his camera freezing in the open position, producing severe overexposure.[2][3][4] Ansel Adams had also earlier created a solarized sun image, titled Black Sun, Owens Valley, California, 1939, by overexposure.[5]
Definition
[edit]When a photographic layer, suitable for solarization (see below), is exposed to actinic radiation, the resulting darkening after development will not increase steadily, but reaches a maximum which decreases under more intense exposure. In general is the phenomenon only then called solarization if the exposure has been produced in one "shot", meaning no pauses or double-exposures. The exposure to achieve solarization can be increased by exposure time or by increasing the light intensity[6]
History
[edit]The solarization effect was already known to Daguerre and is one of the earliest known effects in photography. John William Draper was the first to call the overexposure effect solarisation. J.W.F. Herschel already observed the reversal of the image from negative to positive by extreme overexposure in 1840.[6] Also N.M.P. Lerebours observed the phenomenon in 1842 (without him recognizing what it was) when he made a daguerreotype of an image of the sun. The result was seen as unsatisfactory because the solar disk (image of the sun on the daguerreotype plate) was overexposed and solarized.[7] Ludwig Moser reported in 1843: "...that the light in the camera obscura produces at first the well known negative image; with continued action of the light the image turns into a positive image.... and recently I have obtained in fact on occasion a third image which is negative".[6] In 1880 Janssen had obtained in the strongest sunlight a repetition of the solarization phenomena.[8][9]
Explanation
[edit]Source:[6]
Not every photographic layer exhibits solarization. Pure chloride and iodine based silver emulsions are difficult or impossible to solarize. In general, it can be stated that solarisation can only be observed if the photographic layer is capable of creating a latent image inside the halide grain underexposure by actinic radiation.[6] Many explanations have been given but until further notice, the solarization was until 1929 generally understood as a combination of two main processes: the coagulation (clotting) and the regression process.
Regression theory
[edit]The regression process theory was formulated by H. Luppo-Cramer in 1911, based on research by F. Hurter, V.C. Driffield and H. Luggin.
By exposure the surface and the interior of a silver-bromide sphere will disintegrate by the expulsion of bromide. Whereas the bromide on the surface can permeate away, the bromide can not so easily permeate away from the interior. The overexposure generates now a bromide pressure that escapes from the internal sphere and permeates to the surface where it oxidizes the latent image situated there, constituting the regular latent image under normal exposures. This destroys the latent image, because only silver on the surface can be developed.
Coagulation theory
[edit]H. Arens published in 1925 a paper about reversal effects in which he concluded that solarization is based upon the finding that under increasing exposure the latent image successively coagulates and thus increases the size of each particular silver speck. This again causes the silver speck to lose its catalytic effect for the development.
Bromide migration theory
[edit]H. Kieser published in 1929 a paper in which he speculated about the possibility of bromide migration by defect electrons (see: Photosensitivity).
In recent years an understanding has been agreed upon in which this bromide migration to the surface by overexposure forms a bromine condensation, resulting in bromine molecules or bromine atoms diffusing to the silver specks of the latent image. Thus the latent image at the crystal surface can be re-halogenated by chemical reaction, notwithstanding an increase of the amount of latent image in the interior of the crystal. Still, the regression and coagulation theories are believed to contribute up to a certain level to the solarization effect.
Pseudo-solarization
[edit]Pseudo-solarisation (or pseudo-solarization) is a phenomenon in photography in which the image recorded on a negative or on a photographic print is wholly or partially reversed in tone. Dark areas appear light or light areas appear dark. The term is synonymous with the Sabattier-effect when referring to negatives. Solarisation and pseudo-solarisation are quite distinct effects.
In short, the mechanism is due to halogen ions released within the halide grain by exposure diffusing to the grain surface in amounts sufficient to destroy the latent image.[10]
References
[edit]- ^ The Black Sun 1955
- ^ "1940 bis 1960". Große Photographen. Time-Life International (Nederland) B.V.. 1973. p. 216.
in German
{{cite book}}:|work=ignored (help) - ^ Jolly, William L. "SOLARIZATION DEMYSTIFIED". Archived from the original on January 10, 2019. Retrieved 2019-01-13.
Chapter 1
- ^ Warren, Lynne (2005). Encyclopedia of twentieth-century photography. New York: Routledge. pp. 1459–1460. ISBN 978-1-57958-393-4.
- ^ "Black Sun, Owens Valley, California, 1939". 15 April 2008. Retrieved 2019-01-13.
- ^ a b c d e Tomamichel, Franz (1968). "8.6. Photographische Effekte durch den Abbau eines vorgelegten latenten Bildes". In Frieser, H.; Haase, G.; Klein, E. (eds.). Die photographische Empfindlichkeit (in German). Vol. 3. Frankfurt am Main: Akademische Verlagsgesellschaft. pp. 1217–1232. OCLC 310490074.
{{cite book}}:|work=ignored (help) - ^ Barger, M. Susan; White, William B. (12 May 2000). The Daguerreotype: Nineteenth-Century Technology and Modern Science. Baltimore and London: Johns Hopkins University Press. p. 85. ISBN 9780801864582.
- ^ Eder, Josef Maria (1972). "LXIX. Photographic Analysis of Movement by Janssen and Marey". History of Photography. New York: Dover Publications, Inc. p. 506. ISBN 978-0-486-23586-8.
- ^ Launay, François (2012). "The Method of Stellar Circles". The Astronomer Jules Janssen. New York Dordrecht Heidelberg London: Springer. p. 116. ISBN 978-146140-697-6. Retrieved 2019-01-08.
- ^ Spencer, D A (1973). The Focal Dictionary of Photographic Technologies. Focal Press. p. 574. ISBN 0-240-50747-9.
