About New Kinds of Telescopes, Especially for Handheld Use. Ueber neue Arten von Fernrohren, insbesondere fuer den Hangebrauch. Lecture held at the session of the Society for Advancement of Industrial Activity on January 7, 1895 by Dr. S. Czapski, Scientific Colleague of the Optical Laboratory of Carl Zeiss in Jena Continuation, Number 5; from the 'Central-Zeitung fuer Optik und Mechanik' (Journal for Optics and Mechanics), Berlin, 01 Mar., 1896 Translation by Ilse Roberts and Peter Abrahams The purpose of such a field glass is twofold. It allows the observer to remain behind cover, viewing ‘around a corner’ with only the objective unprotected and visible to the object or vulnerable to a bullet. If the offset of the objective from the ocular is sufficiently large, the head and body of the observer can be completly hidden without limiting the observation. For simple telescopes, this is the only advantage, but it alone should make these instruments useful for military purposes, and there are many other circumstances in which they could be useful. Fig. 16 shows a simple telescope of this type in three views. The sequence of prisms, derived from the first principle of the prism system (fig. 6), is similar to fig. 13. There are 4 prisms, P is an isosceles right angle reflecting prism, just behind the objective O. The remaining three prisms are shown as a larger reflecting prism q with two reflecting surfaces, and another smaller prism p attached to it. They are installed in the housing G that holds the ocular o of the telescope. The second purpose of such a telescope is more important, and concerns its function when joined with another for binocular use. Such binoculars are desirable for esthetics alone, especially for instruments with erecting prisms, which have an asymmetrical appearance as monoculars, with an accentuated offset between the objective axis and the ocular axis. There have been attempts to cover up this asymmetry with a symmetrical housing that does not resemble its interior, but in our opinion these have been less attractive than a tightly fitting housing. If two of these asymmetrical bodies are connected in a symmetric way, the transformed instrument does not offend the eye, and even gives the opportunity for pleasing forms of execution. By connecting two telescopes into a binocular, the opportunity arises to increase or decrease the distance between the objectives without adding any additional optical elements to the system. The distance can be larger or smaller than the distance between the oculars, the minimum being determined by the dimensions of the prisms, or it can be enlarged almost any amount. To accomplish this, the user need only adjust the connection between the telescopes [separate the objectives by opening the hinge between the oculars]. If this connection is designed so that when the oculars (oo in fig. 17) are adjusted to the user’s interpupillary distance, the tubes form an acute angle towards the objectives, as in 17a, the objectives become closer to each other than the oculars are, until they touch. With small objectives, this can give nearly completely unplastic, 2 dimensional images, although this is not usually advantageous. In fig. 17, the axes of the telescope tubes EE contain both the ocular axis and the objective axis. If the connection between the telescopes is designed so that the axes EE diverge to the outside, when adjusted to interpupillary distance (fig. 17b), the distance between the objectives becomes larger than the interpupillary distance. This can give the user an enhanced perception of depth or space, an increased plasticity of the images in comparison to a binocular of similar specifications with objectives spaced the same distance as the oculars. This increase can be measured in comparison to a common binocular, and is exactly equal to the ratio of the objective distance to the ocular distance. The increased plasticity in comparison to a naked eye view equals the linear magnification times the increase in objective distance. This phenomenon, and its qualitative and quantitative relations, is not a new discovery. Helmholz, the recently deceased leader in physics and physiology, recognized all this long ago, pursued all the theoretical and practical consequences, and described it in his famously clear and precise manner. Any explanation here would be only a repetition of his research in Physiologic Optics (1st edition, especially pp. 647 and 681), and in another paper (Pogg. Ann. Bd. 102, pp.16a--175, 1857). These papers are recommended to anyone interested, for they are an opportunity for instruction and much enjoyment, to those who read them. Helmholtz called the instrument which he constructed the “Telestereoscope”. We prefer “Relieffernrohr” [relief telescope], for common use. These use reflections of the image by arranging the (already required) optical elements of the telescope along its longitudinal axis. The Helmholtz invention was little used in the years since its publication, which astonishes anyone who has experienced the charm of these instruments. I believe that inadequate execution, especially the adjustment of the axes of each telescope by the mechanics and opticians entrusted with it, is to blame. If this is so, that these instruments cannot provide fusable images to the eyes, then the eyes are forced to adjust to the optics, which soon causes disgust with such instruments. However, with correct adjustment, the highly plastic images produced by a Telestereoscope of any variety, give a special charm to the landscape from the increased relief they provide. It is often observed, that a first time user of these instruments is unaware of their pecularity and hardly feels their charm. With increased use of these optics, an increase in receptive feeling for their images occurs, which increases the enjoyment and also the capacity for (or the consciousness of) plastic seeing, even with the naked eye. Perhaps the capacity to see stereoscopically has atrophied for many people from lack of exercise, so that it is slowly strengthened and awakened by practice. Perhaps the sense of depth, like the sense of color, varies with the population and with attention and practice. If this is so, the present era could be the entry to an age of better development of that sense. At the least, the inclination to use the stereoscope for photographic images, and the efforts to give these instruments a functional design, is quite noticeable to those who follow photographical literature. The binocular telescope here described will make its contribution by granting an increased enjoyment of viewing colorful, moving, and real nature; like the stereoscope gives for photographs. (*Esthetic enjoyment requires less magnification (larger f.o.v.) and increased distance between objectives. Increased plasticity does not give distant objects an appearance of greater magnification, but the observer seems to see smaller plastic details in them, as described in Helmholtz.) This ‘sense of depth’ is as worthy of attention and development as any. Nature has given us equipment to view our world with two eyes, from two different viewpoints at one time. The ability to unify these two distinct images and to infer the spatial arrangement of the objects in the images, is a source of much esthetic pleasure and also a valuable skill for orientation. The differences between the two images from the two eyes are seen as characteristics of the various distances of the objects in view, and are seen with a sensitivity of perception that is unrivalled. Binoculars with increased distance between the objectives can heighten this sense, as compared to binoculars of the same power, and of normal configuration. This is obvious to any attentive observer using these instruments. Landscapes, that appear as a uniformly extending plane through a telescope or even a common binocular; when observed through a relief telescope reveal at first glance diverse stratifications, waves, slopes, precipices, and cracks. The user can almost see the air which separates the features of the terrain, that are projected onto each other in a simple telescope. The study of a terrain according to its depth formation is possible, adding to the information on width and height seen with common telescopes. To obtain these advantages, it is necessary to adjust these telescopes to provide images that are magnified to exactly the same size, with exactly parallel optical axes with no divergence. An adjustment to individual interpupillary distances is required of the connection between the telescopes, and a focusing mechanism for each side is needed. The degree of plasitcity of the fused image depends to a great degree upon the resolution with which the two individual images are seen. Since one eye of a person often has small differences from the other eye, the focusing requirement is indispensible. These requirements have been met in the Zeiss instruments. Other than meeting the required stability, the type of mechanical connection between the telescopes is immaterial. They can be joined by a hinge or another joint which permits adjustment to interpupillary distance without losing parallelism of the optical axes. They can also be set in a rigid connection, without adjustment for interocular distance; or with other forms of adjustment. Required is a mechanical connection that maintains the large distance between the objectives when interocular distance is adjusted. 3