The laws of contrast of colour : $b and their application to the arts of painting, decoration of buildings, mosaic work, tapestry and carpet weaving, calico printing, dress, paper staining, printing, military clothing, illumination, landscape, and flower gardening, &c.Chevreul, M. E. (Michel Eugène)
Science
The laws of contrast of colour : $b and their application to the arts of painting, decoration of buildings, mosaic work, tapestry and carpet weaving, calico printing, dress, paper staining, printing, military clothing, illumination, landscape, and flower gardening, &c.
Chevreul, M. E. (Michel Eugène)
Color
3. When light is reflected by an opaque white body, it is not modified
in proportion to the variously coloured rays which constitute white
light; but, 1. _If the body is not polished_, every point of its
surface is to be considered as dispersing the white light which falls
upon it, in all directions, into the surrounding space; so that the
point becomes visible to an eye placed in the direction of one of its
rays. We may easily conceive that the image of the body, in a given
position, is composed of the sum of the physical points, which send to
the eye so placed, a portion of the light which each point radiates. 2.
_If the body is polished_, as, for example, the surface of a mirror,
a portion of the light is irregularly reflected, as in the preceding
case; while another portion is regularly reflected, giving to the
mirror the property of presenting to an eye, suitably placed, the image
of the body which sends its light to the reflector. One consequence
of this distinction is, that if we regard two plane surfaces which
reflect white light, and differ from each other only in polish, it will
happen that where the unpolished surface is visible, all its parts
will be equally, or almost equally, illuminated; while the eye, when
in a position to receive only the light which it reflects irregularly,
will receive very little light from the polished surface; but it will
receive much more light when in a position to receive that which is
regularly reflected.
4. If the light which falls on a body is completely absorbed by that
body, so that it disappears from sight, as in falling into a perfectly
dark cavity, then the body appears to us black; and it becomes visible
only because it is contiguous to surfaces which reflect or transmit
light. We know of no bodies which are perfectly black, and it is only
because they reflect a little white light that we judge they have
relief, like other material objects.
5. When light is reflected by an opaque coloured body, there is always
a reflection of white light, and a reflection of coloured light; the
latter is owing to the fact that the body absorbs or extinguishes
within itself some of the coloured rays, and reflects the others.
It is evident that the _absorbed_ coloured rays are of a different
colour from the _reflected_ coloured rays; and farther, that if these
be reunited with the former, white light will be reproduced. It is
evident, also, that unpolished opaque bodies reflect irregularly white
light, and the coloured light which makes them appear coloured; and
that those which are polished reflect irregularly a portion only of
these two lights, while they reflect regularly the other portion.
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