The Boy's Playbook of Science: Including the Various Manipulations and Arrangements of Chemical and Philosophical Apparatus Required for the Successful Performance of Scientific Experiments in Illustration of the Elementary Branches of Chemistry and Natural PhilosophyPepper, John Henry
Science
The Boy's Playbook of Science: Including the Various Manipulations and Arrangements of Chemical and Philosophical Apparatus Required for the Successful Performance of Scientific Experiments in Illustration of the Elementary Branches of Chemistry and Natural Philosophy
Pepper, John Henry
Science -- Juvenile literature
The fan is held in one hand, and the first finger of the other can be
made to touch all the sticks if placed sufficiently near to A; and
supposing the sticks are called rays of light, the intensity must be
great at that point, because all the rays fall upon it; but if the
finger is removed towards the outer edge--viz., to B, it now only
touches some three or four sticks; and pursuing the analogy, a very few
rays fall upon that point--hence the light has decreased in intensity,
or to speak correctly, "Light decreases inversely as the squares of the
distance." This law has already been illustrated at page 13; and as an
experiment, the rays from the oxy-hydrogen lantern may be permitted to
pass out of a square hole (say two inches square), and should be thrown
on to a transparent screen divided into squares by dark lines, so that
the light at a certain distance illuminates one of them; then it will be
found that at twice the distance, four may be illuminated, at three
times nine, and so on. (Fig. 254.)
[Illustration: Fig. 254. Lantern at the three distances from the
transparent screen, which is divided into nine equal squares.]
Upon this law is based the use of photometers, or instruments for
measuring light, and supposing it was required to estimate roughly the
illuminating power of any lamp, as compared with the light of a wax
candle six to the pound, the experiment should be conducted in a dark
room, from which every other light but that from the lamp and candle
under examination must be excluded.
The lamp, with the chimney only, is now placed say twelve feet from the
wall, and a stick or rod is placed upright and about two inches from the
latter, so that a shadow is cast on the wall; if the candle is now
lighted and allowed to burn up properly, two shadows of the stick will
be apparent, the one from the lamp being black and distinct, and the
other from the candle extremely faint, until it is approached nearer
the [Page 267] wall--say to within three feet--when the two shadows may
be now equal in blackness. (Fig. 255.) After this is apparent to one or
more persons, the distances of the lamp and candle from the wall are
carefully measured, and being squared, and the greater divided by the
lesser number, the quotient gives the illuminating power. For example:
The lamp was 12 feet from the wall 12 × 12 = 144.
The candle was 3 feet " 3 × 3 = 9.
9) 144
----
16
Therefore the illuminating power of the lamp is equal to 16 wax candles
six to the pound.
[Illustration: Fig. 255. A. The lamp. B. The candle. C. The rod throwing
the two shadows, marked D and E, on a white wall or a sheet of paper.]
There are other and more refined means of working out the same fact, but
for a rough approximation to the truth, the plan already described will
answer very fairly.
Public-domain text, read in full here on John Shaqi.
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