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
Having fixed upon the proper distance of the sitter, which we shall
suppose to be _six_ feet,—a distance very suitable for examining a
bust or a picture, we have now to take two portraits of him, which,
when placed in the stereoscope, shall have the same relief and the
same appearance as the sitter when viewed from the distance of _six
feet_. This will be best done by a binocular camera, which we shall now
describe.
_The Binocular Camera._
This instrument differs from the common camera in having two lenses
with the same aperture and focal length, for taking at the same instant
the picture of the sitter as seen at the distance of _six_ feet, or any
other distance. As it is impossible to grind and polish two lenses,
whether single or achromatic, of exactly the same focal length, even
when we have the same glass for both, we must bisect a good lens,
and use the two semi-lenses, ground into a circular form, in order
to obtain pictures of exactly the same size and definition. These
lenses should be placed with their diameters of bisection parallel to
one another, and perpendicular to the horizon, at the distance of 2½
inches, as shewn in Fig. 45, where MN is the camera, L, L′ the two
lenses, placed in two short tubes, so that by the usual mechanical
means they can be directed to the sitter, or have their axes converged
upon him, as shewn in the Figure, where AB is the sitter, _ab_ his
image as given by the lens L, and _a′b′_ as given by the lens L′. These
pictures are obviously the very same that would be seen by the artist
with his two eyes at L and L′, and as
ALB = _a_L_b_ = _a′_L′_b′_,
the pictures will have the same apparent magnitude as the original, and
will in no respect differ from it as seen by each eye from E, E′, E_a_
being equal to _a_L, and E′_a′_ to _a_L.
[Illustration: FIG. 46.]
Public-domain text, read in full here on John Shaqi.
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