CHAPTER II.

Evolution of the Method.

The writer was formerly a brewer, and this work had its origin in an

observation that the finest flavour in beer was always associated

with a colour technically called “golden amber,” and that, as the

flavour deteriorated, so the colour assumed a reddish hue. It was these

variations in tint that suggested the idea of colour standards as a

reliable means of reference.

The first experiments were made with coloured liquids in test tubes

of equal diameter, and by these means some useful information was

obtained; but as the liquids soon changed colour, frequent renewals

were necessary, and there was always a difficulty and uncertainty in

their exact reproduction.

To obviate this, glass in different colours was tried, and long

rectangular wedges with regularly graded tapers were ground and

polished for standards, whilst correspondingly tapered glass vessels

were made for the beers. These were arranged to work side by side,

and perpendicularly, before two apertures of an optical instrument,

which gave a simultaneous view of both. The apertures were provided

with a fixed centre line, to facilitate the reading off of comparisons

of thickness. There was no difficulty in obtaining glass which

approximated to the required colour when used in one thickness only.

But as thickness varied, the test no longer held good for both

standards, their rates of colour change being different, making the

method unreliable.[1]

[1] It was afterwards found that these colour changes through

variations of intensities were due to a natural law to be described

under the heading of “Specific colour.” (_See_ page 32.)

The system about to be described is one of analytical absorption, and

has been published from time to time in the form of papers, read before

Societies interested in the question of colour standardization; as also

in two descriptive works by the present writer. The earlier works were

necessarily fragmentary, but gathered system as the subject progressed.

At an early stage in the investigations it was realized that the

handbooks of the period dealt largely with theoretical differences

which were of little service to the technical worker. Under these

circumstances the writer applied for advice to the late Mr. Browning

of the Strand, who gave it as his opinion that no work existed which

could be of service to the writer. All that could be done was to go on

until something should be arrived at. On this, all theoretical reading

was put aside, and the work proceeded on the simple lines of observing,

recording, and classifying experimental facts.

In working with glass of different colours it was found that some

combinations developed colour, whilst other combinations destroyed

it. This suggested the probability of a governing natural law; and

experimental work was undertaken in the hope of discovering it. The

result was the construction of a mechanical scale of colour standards,

which are now in use in over one thousand laboratories, and no

question of their practical accuracy arises. The principal conditions

for ensuring accuracy and constancy of results are embodied in the

following code of nine precautions, which have been published for

nearly twenty years without being disputed. They may therefore be

considered as governing laws, at least for the present. The colour

theory adopted for these Governing Laws has grown out of a series of

experimental facts capable of demonstration, and is summed up in the

following code of nine Laws.

Laws 1, 2, and 3 relate to White and Coloured Light, and are as

follows:--

1. Normal white light is made up of the six colour rays, Red, Orange,

Yellow, Green, Blue and Violet in equal proportions. When these rays

are in unequal proportions the light is abnormal and coloured.

2. The particular colour of an abnormal beam is that of the

one preponderating ray, if the colour be simple, or of the two

preponderating rays if the colour be complex. The depth of colour is in

proportion to the preponderance.

3. The rays of a direct light are in a different condition to the

same rays after diffusion, and give rise to a different set of colour

phenomena.

Laws 4, 5, 6, and 7 deal with The Limitations of the Vision to

appreciate Colour.

4. The vision is not simultaneously sensitive to more than two colours

in the same beam of light. The colour of any other abnormal ray is

merged in the luminosity of the beam.

5. The two colours to which the vision is simultaneously sensitive

are always adjacent in their spectrum order, Red and Violet being

considered adjacent for this purpose.

6. The vision is unable to appreciate colour in an abnormal beam

outside certain limits, from two causes:

(_a_) The colour of an abnormal beam may be masked to the vision from

excess of luminosity.

(_b_) The luminous intensity of the abnormal beam may be too low to

excite definite colour sensations.

7. The vision has a varying rate of appreciation for different colours

by time, the lowest being for red. The rate increases in rapidity

through the spectrum, until the maximum rate is reached with violet.

And since this varying rate necessitates a time limit for critical

observations, five seconds has been adopted as the limit, no variations

being perceptible in that time.

Laws 8 and 9 relate to Colour Constants.

8. The colour of a given substance of a given thickness is constant so

long as the substance itself, and the conditions of observation, remain

unaltered.

9. Every definite substance has its own specific rate of colour

development for regularly increasing thicknesses.

Light and Colour Theories, and their relation to light and colour standardization · 第 2 / 12 章