The Nature of Animal LightHarvey, E. Newton (Edmund Newton)
Science
The Nature of Animal Light
Harvey, E. Newton (Edmund Newton)
Phosphorescence
As we know practically nothing of the energy transformations occurring
during the process of light production in organisms, all statements
regarding the efficiency of their light are based on relations between
the visible radiation and total radiation. This involves a measurement
of rays in the infra-red region (heat rays) and ultra-violet region
(actinic rays) as well as the light rays proper, and any other radiant
energy produced. While all spectroscopic investigations show that the
spectrum of luminous animals never extends to the limits of the visible
spectrum in either the red or violet, it is possible that bands occur in
the infra-red or ultra-violet, and special methods must be employed to
detect these. Radiations of all kinds, if converted into heat on
striking the blackened surface of a thermopile, bolometer, or radiometer
can be measured by changes in temperature and the relative amounts of
energy represented be compared in a common unit, the calorie. By proper
screening, all rays except the visible light rays can be cut off from
the measuring instrument and the amounts of energy represented in light
and in total radiation thus be determined.
Dubois (1886) first studied this problem in _Pyrophorus_ by the use of a
thermopile and galvanometer and found a small amount of radiation from
the luminous region in excess of that from a non-luminous region. It
amounted to a galvanometer deflection of 0.95° and was increased 0.3°
during the flash of the insect on electrical stimulation. This increase
of 0.3° is possibly due to heat produced on muscular contraction. In any
case the amount of heat radiated in comparison with that of the candle
is very small indeed. A more careful study has been made by Langley and
Very (1890) with the bolometer. They point out first of all that the
total radiation from the most powerful luminous organ (the abdominal
one) of _Pyrophorus_ which affected their bolometer slightly, would, in
the same time (10 seconds), be sufficient to raise the temperature of an
ordinary mercurial thermometer having a bulb 1 cm. in diameter by rather
less than 2.3 × 10^{-6}° C. We may thus gain some idea of the magnitude
of the measurements to be made. The radiation from _Pyrophorus_ which
affected their bolometer was shown to be due merely to the "body
heat"[2] of the insect, and it is largely cut off by a plate of glass
which is opaque to all wave-lengths of 3µ or more. These waves are given
off by bodies at temperatures below 50° C. and belong "to quite another
spectral region to that in which the invisible heat associated with
light mainly appears." Langley and Very then compared the radiation from
a non-luminous bunsen flame and the _Pyrophorus_ light, interposing a
plate of glass in each case to cut off the waves longer than 3µ, and
found several hundred times more radiation in the case of the bunsen
burner but, nevertheless, perceptible radiation from _Pyrophorus_. The
Public-domain text, read in full here on John Shaqi.
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