The stereoscope : $b its history, theory, and construction, with its application to the fine and useful arts and to educationBrewster, David
History
The stereoscope : $b its history, theory, and construction, with its application to the fine and useful arts and to education
Brewster, David
Stereoscope
If we wish to have a greater degree of relief than we have with our
two eyes, either in viewing colossal statues, or buildings, or
landscapes, where the deviation from nature does not, as in the human
face, affect the expression, or injure the effect, we must increase
the distance of the lenses in the binocular camera, or the angle of
direction of the common camera. Let us take the case of a colossal
statue 10 feet wide, and suppose that dissimilar drawings of it about
_three_ inches wide are required for the stereoscope. These drawings
are _forty_ times narrower than the statue, and must be taken at such
a distance, that with the binocular camera the relief would be almost
evanescent. We must therefore suppose the statue to be reduced _n_
times, and place the semi-lenses at the distance _n_ × 2½ inches. If
_n_ = 10, the statue 10 feet wide will be reduced to ¹⁰/₁₀, or to 1
foot, and _n_ × 2½, or the distance of the semi-lenses will be 25
inches. With the lenses at this distance, the dissimilar pictures of
the statue will reproduce, when combined, a statue one foot wide, which
will have exactly the same appearance and relief as if we had viewed
the colossal statue with eyes 25 inches distant. But the reproduced
statue will have also the same appearance and relief as a statue a foot
wide reduced from the colossal one with mathematical precision, and it
will therefore be a better or more relieved representation of the work
of art than if we had viewed the colossal original with our own eyes,
either under a greater, an equal, or a less angle of apparent magnitude.
We have supposed that a statue a foot broad will be seen in proper
relief by binocular vision; but it remains to be decided whether or
not it would be more advantageously seen if reduced with mathematical
precision to a breadth of 2½ inches, the width of the eyes, which
gives the vision of a hemisphere 2½ inches in diameter with the most
perfect relief.[55] If we adopt this principle, and call B the breadth
of the statue of which we require dissimilar pictures, we must make
_n_ = B/2½, and _n_ × 2½ = B, that is, the distance of the semi-lenses
in the binocular camera, or of the lenses in two cameras, must be made
equal to the breadth of the statue.
In concluding this chapter, it may be proper to remark, that unless
we require an increased relief for some special purpose, landscapes
and buildings should be taken with the normal binocular camera, that
is, with its lenses 2½ inches distant. Scenery of every kind, whether
of the picturesque, or of the sublime, cannot be made more beautiful
or grand than it is when seen by the traveller himself. To add an
artificial relief is but a trick which may startle the vulgar, but
cannot gratify the lover of what is true in nature and in art.
_The Single Lens Binocular Camera._
Public-domain text, read in full here on John Shaqi.
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