Colour Measurement and MixtureAbney, William de Wiveleslie, Sir
Science
Colour Measurement and Mixture
Abney, William de Wiveleslie, Sir
Color
We will now proceed to demonstrate how we can measure the amount of
spectral light reflected by different pigments. Let us take a strip of
card painted with a paste of vermilion, leaving half the breadth white;
and similarly one with emerald green. If we place the first in the
spectrum so that half its breadth falls on the red, and the other half
on the white card, we shall see that apparently the red and orange rays
are undiminished in intensity by reflection from the vermilion, but that
in the green and beyond but very little of the spectrum is reflected.
With the emerald green placed similarly in the spectrum, the red rays
will be found to be absorbed, but in the green rays the full intensity
of colour is found, fading off in the blue. What we now have to do is
to find a method of comparing the intensities of the different rays
reflected from the pigments, with those from the white surface. We will
commence with the second of the two methods which the writer devised
with this object, and then describe the first, which is more complex.
Suppose we have, say a card disc three inches in diameter, painted with
the pigment whose reflective power has to be measured, and place it on a
rotating apparatus with black and white sectors of say five inches
diameter, and capable of overlapping so as to show different proportions
of black to white (see Fig. 42). If we throw a colour patch (shown in
Fig. 14 as the area inside the dotted square) on the combination of
black and white, and at the same time on the pigmented disc, it is
probable that either one or other will be the brighter. By moving the
slit along the spectrum it is evident, however, that a colour can be
found which is equally reflected from them both whilst rotating. Take as
an example the sectors as set at two parts white, to one part black, the
centre disc being vermilion, the slit is moved along the spectrum until
such a point is reached that the colour reflected from the ring and the
disc appears of the same brightness, for it must be recollected that
they cannot differ in hue, as the light is monochromatic. It will be
found that the place where they match in brightness is in the red, the
exact position being fixed by the scale at the back of the slide. Taking
the proportion of black to white as three to one, the match will be
found to take place in the orange. Increasing the proportion of black
more and more, a point will be reached where the reflection takes place
uniformly along the blue end of the spectrum, this will be from the
green to the end of the violet. By sufficiently increasing the number of
matches made, a curve of reflection can be made showing the exact
proportion of each ray of the spectrum that is reflected. The uniform
reflection along the blue end of the spectrum shows that a certain
amount of white light is reflected from the pigment.
Public-domain text, read in full here on John Shaqi.
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