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
The lower edge =O E= of the reflector =B O E= extends about the 15th of
an inch below the axis of the cones, as represented by the dotted line
in Fig. 30; but the lower edge =O E= of the other reflector =A O E=,
which is finely ground to an acute angle, forming a perfectly straight
and smooth line, is placed exactly in the axis of the cones, so as just
to touch a line in the reflector =A O E=, which coincides with the axis
of the cone, and to form a junction with that line in every part of
the two meeting planes. The very nice adjustments which are necessary
to produce so exact a motion are effected by the screws corresponding
to =K= and =L=.
If we now fix the outer ring _r r_ into the ring of a stand =S T=,
so as to be held fast, and turn the cones with the hand, we shall
give motion to the reflector =B O=, so as to place it at any angle
we please, from 0° to 90°; and during its motion through this arch,
the junction of the two reflectors must remain perfect, if the
touching lines are adjusted, as we have described them, to the axis
of motion, which must also be the axis of the cones and rings. If, on
the contrary, we take away the stand, and, holding the instrument in
the hand by either of the cones =M=, =N=, turn the ring =R R= with
the other, we shall give motion to its reflector =A O=, and produce a
variation in the angle in the same manner as before. The same effect
may be produced by an endless screw working in teeth, cut upon the
circumference of the outer ring _r r_.
In order to enable the observer to set the reflectors at once to any
even aliquot part of a circle, or so as to give any number of pairs of
direct and inverted images, the most convenient of the even aliquot
parts of the circle are engraven upon the ring _r r_; so that we have
only to set the index to any of these parts, to the number 12, for
example, and the reflectors will then be placed at an angle of 30° (12
× 30 = 360°), and will form a circular field with _twelve_ luminous
sectors, or a star with _six_ points, and consequently a pattern
composed of _six_ pairs of direct and inverted images.
Public-domain text, read in full here on John Shaqi.
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