The Nature of Animal LightHarvey, E. Newton (Edmund Newton)
Science
The Nature of Animal Light
Harvey, E. Newton (Edmund Newton)
Phosphorescence
.05Å .2Å .8 3.2 12.8 50. 200. 800. 3200. 1.28µ
--------+---------+------------+-------------+---------+-- ...
RADIUM | | | | |
γ | X RAYS | UNEXPLORED | ULTRAVIOLET | VISIBLE |
RAYS | | | | |
--------+---------+------------+-------------+---------+-- ...
1.28µ 5.µ 20. 80. 320. .128cm. .5cm.
... --+------------------+----------+---------
| | | HERTZIAN
| INFRA RED |UNEXPLORED| ELECTRIC
| | | WAVES
... --+------------------+----------+---------
The total radiant energy which a body emits is a function of its
temperature and for a perfect radiator, or what is known as a black body,
the total radiation varies as the fourth power of the absolute
temperature, T. (Stefan-Boltzmann Law). The radiant energy emitted at
different wave-lengths is not the same but more energy is emitted at one
particular wave-length (λ_{max.}) than at longer or shorter ones,
depending also on the temperature. If the various waves are intercepted
in some way, their relative energy can be measured by an appropriate
instrument and spectral energy curves can be drawn, showing the
distribution of energy throughout the spectrum. Fig. 2 gives a few of the
curves, and it will be noted that the maximum shifts toward the shorter
waves the higher the temperature. In fact, for a black body
λ_{max.}×T=2890, and at 5000° C. (about the temperature of the sun)
λ_{max.} lies within the visible spectrum. In gas or electric lights it
lies in the infra-red region. The area enclosed by these spectral energy
curves represents the total energy emitted, and, knowing this and the
area enclosed by the curve of visible radiation, it is easy to determine
how efficient a source of light is as a light-producing body. We shall
inquire more fully into this question in Chapter III, in considering the
efficiency of the firefly as a source of light.
[Illustration: FIG. 2.--Distribution of energy throughout the spectrum
of the sun, electric arc, and gas light (_after Nichols and Franklin_).
Ordinates show the relative intensities of different wave-lengths
emitted. The notches in the curve represent absorption bands and the
dotted line represents what the radiation from the sun would be if no
selective absorption occurred. V=violet and R=red end of visible
spectrum. (_Courtesy Macmillan Co._)]
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