The kaleidoscope : $b its history, theory and construction. With its application to the fine and useful artsBrewster, David
Science
The kaleidoscope : $b its history, theory and construction. With its application to the fine and useful arts
Brewster, David
Kaleidoscopes
In the various forms of the Kaleidoscope which have been described
in the preceding chapters, the pictures which it creates are visible
only to one person at a time; but it is by no means difficult to fit
it up in such a manner as to exhibit them upon a wall to any number of
spectators. The necessary limitation of the aperture at the eye-end
of the instrument, however, is hostile to this species of exhibition,
as it requires a very intense light for the purpose of illuminating
the objects. The general principle of the apparatus requisite for this
purpose is shown in Fig. 50, where =C D G F= is the tube containing
the reflectors =A O E=, etc. The objects from which the pictures are
to be created are placed in the cell =C D=, which may be made either
to have a rotatory movement round the axis of the tube, or to slide
through a groove, like the sliders of a magic lantern. These objects
are powerfully illuminated by a lens =B=, which concentrates upon them
the direct light of the lamp or candle =H=, and also the part of the
light which is reflected from the mirror =M N=. At the eye-end =E=
of the Kaleidoscope, is placed a lens =L L=, close to the end of the
reflectors, and having its centre coincident with the centre of the
aperture at =E=. In order that this lens may form behind it an image =P
P= of the objects placed in the object-plate =C D=, its focal length
must be less than the length =A E= of the plates. If the focal length
of =L L= is so small as one-half of =A E=, then it follows, from the
principles of optics, that the distance =L P= at which the image is
formed behind the lens, will be precisely equal to the distance =A E=
of the object; but this is obviously too small a distance, for the
diameter of =P P= would be equal only to the apparent diameter of the
circular aperture of the Kaleidoscope, or to twice =A O=. Hence it is
necessary, that the focal length of the lens =L L= be less than =A E=,
and greater than half of =A E=. Two-thirds, or three-fourths of =A E=
will be found to be a suitable focal length; for if it is larger than
this, the image will be formed upon the wall or screen at too great a
distance from the instrument.
When the instrument is thus fitted up, an enlarged image of the pattern
will be thrown upon the wall, which must be covered with white paper,
or some white ground, in order to exhibit the colours to advantage. By
turning the object-plate round its centre, or, if it is a rectilineal
one, by pushing it through the groove, and at the same time giving it
a rotatory motion, the pattern on the wall will undergo every possible
transformation, and exhibit to the spectators, in a magnified form,
all those variations which have been observed by applying the eye to
the Kaleidoscope.
Public-domain text, read in full here on John Shaqi.
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