The actual proportion of a revolution during which current is supplied
the motor is therefore rigorously determined by the clock pendulum,
and the motor is selected so that its revolutions are exactly timed
to this clock pendulum which has no work to do other than the circuit
closing, and can hence be regulated to keep accurate time. The small
fly-wheel (9), the weight of which is carefully adjusted with respect
to the general amount of work to be done, attached to the motor shaft,
effectively steadies its action during the process of government.
This Gerrish type has been variously modified in detail to suit the
instruments to which it has been applied, always following however the
same fundamental principles.
[Illustration: FIG. 139.—Gerrish Drive on 24 inch Reflector.]
An admirable example of the application of this drive is shown in Fig.
139, the 24 inch reflector at the Harvard Observatory. The mount is
a massive open fork, and the motor drive is seen on the right of the
mount. There are here two motors, ordinary fan motors in size. The
right hand motor carries the fly-wheel and runs steadily on under the
pendulum control. The other, connected to the same differential gear as
the driving motor, serves merely for independent regulation and can be
run in either direction by the observer to speed or slow the motion in
R. A. These examples of clock drive are merely typical of those which
have proved to be successful in use for various service, light and
heavy. There are almost innumerable variations on clocks constructed on
one or another of the general lines here indicated, so many variations
in fact that one almost might say there are few driving clocks which
are not in some degree special.
The tendency at present is for large instruments very distinctly toward
a motor-driven mechanism operating on the right ascension axis, and
governed in one of a considerable variety of ways by an actual clock
pendulum. For smaller instruments the old mechanical clock, often
fitted with electric brake gear and now and then pendulum regulated, is
capable of very excellent work.
The principle of the spectroscope is rudimentarily simple, in the
familiar decomposition of white light into rainbow colors by a prism.
One gets the phenomena neatly by holding a narrow slit in a large piece
of cardboard at arms length and looking at it through a prism held with
its edge parallel to the slit. If the light were not white but of a
mixture of definite colors each color present would be represented by
a separate image of the slit instead of the images being merged into a
continuous colored band.
With the sun as source the continuous spectrum is crossed by the dark
lines first mapped by Fraunhofer, each representing the absorption by
a relatively cool exterior layer of some substance that at a higher
temperature below gives a bright line in exactly the same position.
Public-domain text, read in full here on John Shaqi.
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