Popular lectures on scientific subjects : $b Second series, with an autobiography of the authorHelmholtz, Hermann von
Science
Popular lectures on scientific subjects : $b Second series, with an autobiography of the author
Helmholtz, Hermann von
Science; Universities and colleges -- Germany
To the series of subjective phenomena, which artists are compelled to
represent objectively in their pictures, must be associated certain
phenomena of _irradiation_. By this is understood cases in which
any bright object in the field spreads its light or colour over the
neighbourhood. The phenomena are the more marked the brighter is
the radiating object, and the halo is brightest in the immediate
neighbourhood of the bright object, but diminishes at a greater
distance. These phenomena of irradiation are most striking around a
very bright light on a dark ground. If the view of the flame itself
is closed by a narrow dark object such as the finger, a bright misty
halo disappears, which covers the whole neighbourhood, and, at the same
time, any objects there may be in the dark part of the field of view
are seen more distinctly. If the flame is partly screened by a ruler,
this appears jagged where the flame projects beyond it. The luminosity
in the neighbourhood of the flame is so intense, that its brightness
can scarcely be distinguished from that of the flame itself; as is the
case with all bright objects, the flame appears magnified, and as if
spreading over towards the adjacent dark objects.
The cause of this phenomenon is quite similar to that of aërial
perspective. It is due to a diffusion of light which arises from the
passage of light through dull media, excepting that for the phenomena
of aërial perspective the turbidity is to be sought in the air in front
of the eye, while for true phenomena of irradiation it is to be sought
in the transparent media of the eye. When even the healthiest human
eye is examined by powerful light, the best being a pencil of sunlight
concentrated on the side by a condensing lens, it is seen that the
sclerotica and crystalline lens are not perfectly clear. If strongly
illuminated, they both appear whitish and as if rendered turbid by a
fine mist. Both are, in fact, tissues of fibrous structure, and are
not therefore so homogeneous as a pure liquid or a pure crystal. Every
inequality, however small, in the structure of a transparent body can,
however, reflect some of the incident light--that is, can diffuse it in
all directions.[21]
[Footnote 21: I disregard here the view that irradiation in the eye
depends on a diffusion of the excitation in the substance of the
nerves, as this appears to me too hypothetical. Moreover, we are here
concerned with the phenomena and not with their cause.]
The phenomena of irradiation also occur with moderate degrees of
brightness. A dark aperture in a sheet of paper illuminated by the sun,
or a small dark object on a coloured glass plate which is held against
the clear sky, appear as if the colour of the adjacent surface were
diffused over them.
Public-domain text, read in full here on John Shaqi.
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