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
When the artist represents living objects, or groups of them, and
delineates buildings or landscapes, or when he copies from statues or
models, he produces apparent solidity, and difference of distance from
the eye, by light and shade, by the diminished size of known objects as
regulated by the principles of geometrical perspective, and by those
variations in distinctness and colour which constitute what has been
called aerial perspective. But when all these appliances have been
used in the most skilful manner, and art has exhausted its powers,
we seldom, if ever, mistake the plane picture for the solid which it
represents. The two eyes scan its surface, and by their distance-giving
power indicate to the observer that every point of the picture is
nearly at the same distance from his eye. But if the observer closes
one eye, and thus deprives himself of the power of determining
differences of distance by the convergency of the optical axes, the
relief of the picture is increased. When the pictures are truthful
photographs, in which the variations of light and shade are perfectly
represented, a very considerable degree of relief and solidity is
thus obtained; and when we have practised for a while this species of
monocular vision, the drawing, whether it be of a statue, a living
figure, or a building, will appear to rise in its different parts from
the canvas, though only to a limited extent.
In these observations we refer chiefly to ordinary drawings held in the
hand, or to portraits and landscapes hung in rooms and galleries, where
the proximity of the observer, and lights from various directions,
reveal the surface of the paper or the canvas; for in panoramic and
dioramic representations, where the light, concealed from the observer,
is introduced in an oblique direction, and where the distance of the
picture is such that the convergency of the optic axes loses much of
its distance-giving power, the illusion is very perfect, especially
when aided by correct geometrical and aerial perspective. But when
the panorama is illuminated by light from various directions, and the
slightest motion imparted to the canvas, its surface becomes distinctly
visible, and the illusion instantly disappears.
Public-domain text, read in full here on John Shaqi.
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