Practical applications of high and low-reflecting films on glass John Strong To cite this version: John Strong. Practical applications of high and low-reflecting films on glass. J. Phys. Radium, 1950, 11 (7), pp.441-443. <10.1051/jphysrad:01950001107044100>. <jpa-00234293> HAL Id: jpa-00234293 https://hal.archives-ouvertes.fr/jpa-00234293 Submitted on 1 Jan 1950 HAL is a multi-disciplinary open access archive for the deposit and dissemination of scientific research documents, whether they are published or not. The documents may come from teaching and research institutions in France or abroad, or from public or private research centers. L’archive ouverte pluridisciplinaire HAL, est destinée au dépôt et à la diffusion de documents scientifiques de niveau recherche, publiés ou non, émanant des établissements d’enseignement et de recherche français ou étrangers, des laboratoires publics ou privés. LE JOURNAL DE PHYSIQUE ET LE RADIUM. TOME 11, JUILLET 19~O, PAGE PRACTICAL APPLICATIONS OF HIGH AND LOW-REFLECTING FILMS ON GLASS Johns Sommaire. - By JOHN STRONG. Hopkins, University, Baltimore, Maryland. Description (accompagnée de projections) des équipements d’évaporation thermique utilisés pour aluminier les grands miroirs de télescope, en particulier le réflecteur Crossley de l’Observatoire Lick, les miroirs de 60 et de 100 pouces du Mont Wilson et, enfin, le miroir de 200 pouces de l’Observatoire Palomar. L’aluminiure des miroirs de célestat et des réseaux est discutée. Discussion d’un procédé pour réduire la réflexion sur le verre, au moyen de couches déposées par évaporation thermique. Ce procédé utilise une première couche à gradient dont l’indice au contact du verre est le même que l’indice N du verre. Cette première couche a une épaisseur indéter- minée (environ 03BB/2) et son indice superficiel est voisin de N2 : elle ne d’épaisseur 03BB/4 est déposée présente pas de couleurs d’inter- première, réduisant ainsi efficacement la réflexion. On utilise, pour former ces couches, des substances qui adhérent fortement au verre et présentent une grande résistance à l’abrasion. Ce procédé a été découvert aussi par Nadau (brevet canadien n° 418.289). férences. Une deuxième couche d’indice N et sur la Introduction. The purpose of this article is supplement my former publications on applications of thin films to astronomical telescopes [1], to enhance their reflectivity. This activity began with my discovery of a practical method to evaporate aluminum films. Owing to the support of the Observatory Council at California Institute of Technology, it was possible for me to coat many mirrors extending from amateurs 6 inch mirrors to the Crossley Reflector of Mt Hamilton, and the 60 inch and 100 inch mirrors of Mt Wilson, and finally to the 200 inch mirror of Mt Palomar. In addition to a report of aluminizing the last I shall report here, briefly, on a novel method of decreasing the reflection of glass which supplements my original publication on that art. - to The 200 inch mirror. Figure I shows the chamber in which the 200 inch mirror was aluminized. It is 1 g feet inside diameter and 7 feet high inside. The walls and ends are made of o.5 inch steel plate, the ends being reinforced with twelve radial 13 inch I-beams. It weighs 3o tons. The gasketed seal between the chamber and its base plate appears in figure I at the third rung down from the top on the ladder. The two Westinghouse 1000 cubic feet per minute pumping units, on the top of the chamber, produced the necessary vacuum (about io-I mm of mercury). - vacuum Fi g. 1 . Article published online by EDP Sciences and available at http://dx.doi.org/10.1051/jphysrad:01950001107044100 ~~I. 442 One of the five platform arcs which surrounded the mirror, and afforded a walk from which workmen could wash the mirror face, is shown standing Fig. between the chamber and the open hatch of the observing floor in the telescope dome. Two of these platforms appear again in figure 2. 2. Fig. 3. Figure shows the mirror after being aluminized. Hendrix, of Mt Wilson Observatory, cooperated with me during the summer and fall of 4~ and future aluminizations are now his respon2 Mr D. 0. sibility. The bottom and top volumes in the chamber are separated by the mirror face, and a rubber gasket between the mirror and the chamber wall. The necessary high vacuum was thus obtainable in the upper volume of the chamber, while only a moderate vacuum was possible in the lower part, because of the many lubricated working parts 443 in the permanently attached mirror support. The use of a silicon monoxide overcoat [2] was considered but this was abandoned when Dr Babcock’s measurements showed only about I per z o0 deterioration of the reflectivity of the 100 inch mirror in seven years. (This mirror was re-aluminized in 1947. Incidentally, the primary mirror of the 48 inch Schmidt telescope was first aluminized at the same time.) The oil cleaning method of Colbert and Weinrich [3] was used. One of the holders of felt pads, used to rub the mirror face, is shown in figure 2 sticking in the elevator-motor cage, and also, in reflection, at the left side of the mirror face. Aluminum was evaporated from 175 tungsten coils, all in a plane 20 inches above the face of the mirror. One half inches of 4o mil aluminum wire The coils were in was evaporated from each coil. circular arrays of 20, 4o, 60, 70 and 100 inches radius with 10, 20, z 4, 36 and 95 coils in each array. I do not use a chromium substrate film either for astronomical mirrors or for our diffraction gratings here at Hopkins. Non-reflecting film. making glass of index 1.5 - " The novel procedure for non-reflecting employs " . This substrate about ?’-ap roximand ates 2 B same its index increases / gradually and N2 at its outer surface. The substrate feeble interference colors and it is only presumed an ideal film would show no color. This affords a surface whose reflection, although much higher than formerly, can now be effectively elimishows nated by a ~‘ film of index N. I succeeded in making such a film at first attempt which reduced the visual reflection of plate glass f rom 4 per 100 to o.5 per 100. The graded film was deposited from two separate sources the first was a quartz source [4] and the last was a titania source. The evaporation periods of these sources were overlapped to effect the necessary gradation in the film~ f rom pure quartz (N) to pure titania (N2). Finally the usual magenta film of quartz was deposited on the titania surface. Although ,I believe this was the first such evaporated film, the principle was subsequently found to have been recognized by Nadeau [5]. REFERENCES. [1] Astroph. J., 1936, 83,1 and references cited therein. U. S. Patent, 2, 456, 899. [2] John STRONG. [3] COLBERT and WEINRICH.2014 U. S. Patent, 2, 383, 469. - film whose index next to the as that of the glass, N. film has an indefinite thickness a graded substrate glass is nearly the [4] [5] U. S. Patent, 2, 386, MORGAN. NADEAU.2014 Canadian Patent, 418, - 875. 289.
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