Full text: Commissions I and II (Part 3)

nd some Modes 
Record, Vol. II, 
]g Possible Local 
io. 4, September 
in Topographic 
63. 
f Estar Polyester 
ng, Vol. XXVII, 
STEREOSCOPY AND PHOTOGRAMMETRY 
By D. A. Palmer 
ional Archives of 
National Physical Laboratory 
inadiart Surveyor, 
(Invited Paper, Commission I, Xth International Congress of Photogrammetry, 
s of Atmospheric 
XXVI, No. 5, 
Lisbon, 1964) 
and Hypersonic 
Mo. 3, June 1961. 
1 and Terrestrial 
> the IXth Inter- 
Abstract 
Recent developments in stereoscopy are reviewed, and their relevance 
to photogrammetry discussed. 
'es images 
s résultats 
-ogramme 
■■’.SW?:' 
Photogrammetry, like many other highly developed scientific techniques, still 
relies on human beings for an essential part of its operation, namely those whose 
stereoscopic judgement forms the vital link between the photographs and the contour 
maps. There have been several attempts to replace the slightly erratic humans by 
repeatable and predictable machines, but as yet the consequences have been either 
more expensive or less convenient. [1_3] 
Meanwhile, studies of binocular vision are also progressing, and the 
photogrammetrist should keep one eye on such developments to see if they might 
save him time and trouble. Although stereoscopy is a comparatively slow moving 
subject, this is not because everything is already known. On the contrary, the 
process whereby we are able with two eyes to see objects in three dimensions is still 
somewhat obscure. Indeed, at the moment we are able to study only the conse 
quences of that ability rather than the ability itself, because so many of the clues lie 
in that inaccessible organ, the brain, of which the retina is histologically an extension. 
The sine qua non of stereoscopy is that we have two eyes capable of looking 
simultaneously in the same direction. Thus an object under observation will form 
two images, one on each retina. In the normal observer, the impression is never 
theless of a single object; the retinal images have been fused as if according to the 
interesting equation 
A + A = A 
where A represents one image. Incidentally, this curious algebra is valid even 
photometrically, as anyone can see for himself, since a scene viewed with two eyes 
appears no brighter than when viewed with only one. 
In fact, the normal observer (by no means everybody) does obtain something 
extra on the right-hand side of the equation, namely the sensation of depth. The 
objects may appear to be single, but they are also seen standing out at various 
distances within three-dimensional space, a striking experience peculiar to those 
with stereoscopic vision. 
These simple observations suggest the following questions: 
By how much must objects be separated in depth before they become noticeably 
so? 
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