January 1958 Radio-Electronics
[Table
of Contents]
Wax nostalgic about and learn from the history of early electronics.
See articles from Radio-Electronics,
published 1930-1988. All copyrights hereby acknowledged.
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Like so many things in
life that we take for granted - aspirin, automatic clothes washers, drill motors
and bits, eyeglasses, rifles, bicycles, transistors, to name a few - we rarely think
about the effort that went behind the end product that is now enjoyed. Even relatively
simple devices like scissors are the result of someone saying to himself or herself,
"Self, I need something to make cutting fabric and paper and hair simpler and neater,
so what might that thing look like?" Then, after making a working prototype, improvements
are made based on empirical testing from usage, improvements are made in the form
factor, materials, size, etc., until evolution results in what can be purchased
today. If you have ever been in a product design cycle, either privately or corporately,
then you know the process well. A concept as sophisticated as developing television
is much more involved than developing a pair of scissors, but the fundamentals are
the same. Implementing color TV for commercial broadcast had the dual difficulty
of not just producing affordable and reliable color images, but also being backwards
compatible with black and white (B&W) broadcasts and TV sets already in place.
Adding stereo sound to the original monaural FM radio broadcasts had the same requirement.
This article from a 1958 edition of Radio-Electronics does a superb job of describing
the work that went into implementing color television. You might be as surprised
as I was to learn how much new science was required in the realm of human vision
and color perception in order to design a high quality transmission and presentation.
Prior to color TV, most color perception research went into reflected light (paint,
ink, crayons, etc.) whereas for the first time in human history it was necessary
to determine the peculiarities of emitted light from a light source (cathode ray
tube).
The Strange World of Color Vision
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The Cover
Our cover this month is an abstraction based on a suggestion by Mr. Middleton
to illustrate this article. The two odd-looking discs are used to produce sensations
of color from black and white elements only. (See Fig. 6.) The bar slanting
across the bottom is, of course, the color spectrum as most of us know it, and the
upright panel is the color spectrum of a color-anomalous or "color-blind" person,
whose world of color is based on stimuli from two instead of three primaries. The
floating colored dots or bubbles, chosen to produce a random display of color, are
actually a nighttime color photograph of colored lights on a Ferris Wheel deliberately
shot out of focus. The picture was taken by Jay Maisel.
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Fig. 1 - As wavelength of electromagnetic waves is raised
from 380 to 780 milli-microns, we see in succession all the colors of the rainbow.
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Fig. 2 - The standard color map or chromaticity diagram.
All colors are arranged around white as an optical center.
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By Robert G. Middleton
Television Consultant
Color is by no means simple - it is often incomprehensible and always tricky;
but its apparent inconsistencies make compatible color television possible.
Children and simple folk suppose that the colors they see really exist in nature
and scoff at the idea that colors exist only in the mind.
Physicists explain that the colors we see correspond to waves of electromagnetic
energy from 4 to 8 X 1014 cycles per second. Electromagnetic waves used
in radio and television transmission have longer wavelengths.
Of course, light waves are not color, any more than radio waves are color. Physicists
do not attempt to explain further and physiologists cannot. Psychologists are baffled
and philosophers offer various theories which cannot be proved or disproved.
In spite of the unsatisfactory state of our knowledge concerning color vision,
many interesting laws have been discovered, upon which the technology of color television
rests. Some of these laws are well known while others are familiar only to specialists.
Trichromatic Vision
Of all our body's organs, the eye is most remarkable. Loss of hearing is a personal
tragedy but loss of sight is a calamity - our eyes provide us with more information
concerning the external world than any other organ.
It was once supposed that the eye is a frequency-sensitive organ because we see
various colors when electromagnetic waves of various frequencies enter the eye.
As shown in Fig. 1, a wavelength of 475 mμ (millimicrons, mμ) causes us
to see blue, 520 mμ green, 578 mμ yellow and 700 mμ to see red.
Fig. 1 shows in a limited manner the information given in Fig. 2. The
chromaticity diagram (Fig. 2) shows around its border the wavelengths of light
corresponding to the common colors. Note that there are colors along the base of
the diagram to which no single wavelength of light corresponds. This is a rather
unexpected fact which is discussed later in the article.
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Fig. 3 - Red and green combine to form yellow; red and blue
combine to form magenta; green and blue combine to form cyan.
Fig. 4 - Red, green and blue combine to form white.
Fig. 5. - Each color signal voltage has a phase as well
as an amplitude.
Fig. 6 - Black and white patterns which generate the sensation
of colors when rotated.
Note: I printed the patterns of Fig. 6 and glued a round toothpick through
the center of each. (a) looked sort of bluish and (b) looked sort of reddish, but
there was no clearly discernable color.
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In view of such experimental data, it is reasonable to conclude that each color
we see has a corresponding frequency or wavelength. However, there are difficulties
which make this conclusion unacceptable.
When we mix red light with green light, we do not see either of these two colors.
Instead we see a new color: yellow. On this basis, we must abandon the definition
that yellow corresponds to a wavelength of 578 mμ, since yellow is also produced
by a combination of two other wavelengths.
In fact, investigation has shown that the many thousands of colors which we see
can be obtained by mixing only three colored lights - red, green and blue - in various
proportions. Color television operates upon this law, the law of trichromatic vision.
Fig. 3 illustrates how the primary colors of red, green and blue combine by
pairs to form the complementary colors of yellow, cyan and magenta. Fig. 4
shows how the three primary colors combine to form white.
To obtain compatible operation of black-and-white and color TV receivers, wavelengths
of light are transmitted as various phase angles of a color subcarrier. This is
shown in Fig. 5. Burst is taken as the reference frequency. Red, which has
a wavelength of 700 mμ, is transmitted as a phase angle of 76.5°. Magenta,
which is a combination of 700 mμ and 475 mμ, is transmitted as a phase
angle of 119°.
The colors seen in the spectrum of a prism are 100% saturated. They are pure
colors. Saturated colors are vivid. Desaturated colors are pale - they have a pastel
shade. The wavelength of a desaturated color is the same as the wavelength of the
same saturated color. However, white light is mixed with a saturated color to make
a desaturated color. In Fig. 5, the relative voltages of the saturated colors
are shown by the lengths of the vectors. Now, if we shorten the length of the red
vector to half that shown in Fig. 5, we transmit pink - a desaturated red.
It is no mystery that hues are transmitted in terms of phase, and that saturations
are transmitted in terms of voltage. These values are easily calculated throughout.
We encounter the unknown only when we attempt to understand how a color such as
yellow is seen when the eye is viewing a mixture of red and green lights. Perhaps
we shall never know.
Producing Color
White is a mixture of red, green and blue. Black is the absence of visible electromagnetic
wave energy. As white can be produced from colors, conversely, colors can be produced
by suitable arrangements of black and white. For example, when we mount the disk
shown in Fig. 6-a on the shaft of a variable-speed motor, we see an arc of
color in the rotating pattern. As the speed of the motor is varied, the hue of the
color changes accordingly. A disk which produces red and yellow is shown in Fig.
6-b.
It is thought that there may be three types of color receptors in the retina
of the eye, with peak responses to wavelengths in the regions of red, green and
blue. These color receptors are not sharply tuned but have overlapping responses
or considerable bandwidth. Furthermore, when these color receptors are simultaneously
energized by white light which is then suddenly stopped, the response of the color
receptors does not fall to zero at once, but requires a small time interval to decay
to zero.
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Fig. 7-a - Splitting white light into a color spectrum; b - recombination
of color spectrum produces white light.

Fig. 8 - 0ptical filters use resonant electrical circuits
which are provided by nature in the electronic orbits of the atoms comprising the
filter glass.

Fig. 9 - The brightness of a white bar, like that of a color
bar, is equal to the sum of the brightness of its components.

Fig. 10 - The brightness of a color is equal to the sum of the brightness
of its components.

Fig. 11 - Color is characterized by three quantities: brightness, hue and
saturation. Color brightness is determined only by Y-voltage value and is not affected
by chrominance voltage.

Fig. 12 - The chrominance voltages produced by scanning 25%, 50%, 75% and
100% saturated red. Length of chrominance vector is directly proportional to color
saturation. Its phase does not change with change in saturation.

Fig. 13 - Compatibility of color-TV and black-and-white
TV requires that the Y signal as used in black-and-white transmission be unaltered.
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Because the color receptors have differing decay times, a residual unbalance of
response occurs from the receptors during the decay time so that we see color in
the black-and-white whirling pattern, which attacks the eye with sudden changes
from black to white and vice versa. The disk should be rotated counterclockwise
at a speed on the borderline of persistence of vision, and the level of daylight
or artificial light adjusted to produce the maximum intensity of color in the whirling
pattern. Thin, fairly intense red rings, blue tails and yellow fields will appear
under suitable conditions.
The known facts of "color blindness" also support the theory of three color receptors
in the retina, responding in the regions of red, green and blue.
Test charts are available, which reveal the presence of various types of color
blindness in afflicted persons. Some persons are completely color-blind, but still
get about quite handily, since black-and-white vision remains (provided by the rods
in the retina) although the color receptors (cones) are incapable of response.
All of us are color-blind in dim light. If you walk out of a lighted room into
a dimly lit hall and look at a color chart, you will find that all the colors appear
to be in shades of gray.
We are also color-blind to very small patches of color and semi-color-blind to
somewhat larger patches. All colors seem to drift into orange or cyan hues as a
patch of the color is reduced in size. This is the I axis of color television and
is the basis of wide-band color transmission.
Development of the Eye
In an embryonic infant, the retina develops as an outgrowth of the fore-brain.
However, the function of vision is located in the hind-brain and persons who suffer
injury to the hind-brain are as blind as if their eyes had been put out.
If a person has the hind-brain intact, but his eyes have been injured, he may
still see flashes of light and colors as a result of mechanical stimulation of the
exposed ends of the optic nerves. A somewhat similar response is observed by normal
persons. If the eyelids are closed and pressure is applied to the edge of the eyeball,
rings of yellowish light are seen.
How the sensation of light is produced in the mind when the optic nerves are
energized is not known. As far as color television is concerned, it is essential
only that we know the laws of color mixture whereby any desired color can be synthesized
by a suitable mixture of the three primary colors.
Fig. 7-a shows how a prism can decompose white light into a spectrum of
its color components. Fig. 7-b shows how the color spectrum can be recombined
into white light again. This is not a very striking demonstration. However, we find
that we can remove large regions of the spectrum, leaving only the colors at the
extreme ends and a color at the middle, and still obtain white on re-composition.
This robbed white is quite undistinguishable by the human eye from the first white.
If we were unable to rob the spectrum in this manner, color television as we
know it today would be impossible. It is hard enough to transmit three primary-color
signals in a 6-mc channel containing a black-and-white signal and sound signal without
contending with individual signals for tens of thousands of particular hues.
Robbing the Color Spectrum
A rainbow spectrum of light is conveniently robbed by use of filters, as depicted
in Fig. 8. Optical filters operate like electric or electronic filters, except
that the resonant circuits utilized are contained in the electronic orbits of the
atoms in the filter.
All matter is an arrangement of electrical forces or fields. The electrons comprising
a substance have a certain frequency of rotation about the nucleus of the atom and
are coupled to external space just as an antenna is coupled to space. Incident electromagnetic
energy can be absorbed by electrons in certain orbits, just as a tuned circuit absorbs
electromagnetic energy from an antenna.
Thus, an optical filter is an electronic wavetrap, of atomic dimensions, which
is tuned to the frequency of the electromagnetic energy recognized by us as a given
color. There is no basic difference between an optical filter and a wave trap except
that the wavelengths used in the optical filter are shorter.
Color can be specified on a technical basis in terms of brightness, hue and saturation.
Fig. 9 shows that the brightness of a white bar is equal to the sum of the
brightnesses of its components (red, green and blue). The brightness of red, as
seen on a black-and-white picture tube, is 30%; the brightness of green is 59%;
the brightness of blue is 11 % - hence, the brightness of white is 100%.
Fig. 10 shows that the brightness of a color is equal to the sum of the
brightnesses of its components. Yellow has a brightness, as seen on a black-and-white
picture tube, of 89%. Yellow is comprised of green which has a brightness of 59%
and of red which has a brightness of 30% - hence, the brightness of yellow is the
sum of these brightnesses, or 89%.
The brightness of a color, as transmitted from a color TV station, is given by
the level of the Y (black-and-white) signal component, as shown in Fig. 11.
To this brightness signal level is added a 3.58-mc chroma signal. The chroma signal
specifies hue and saturation. Fig. 12 shows how the voltage of the chroma signal
specifies the saturation (vividness) of the color. We have already seen how the
phase of the chroma signal specifies color (hue).
This particular (NTSC) signal arrangement has been established to provide compatibility
in black-and-white and color TV reception. Fig. 13 shows how a succession of
red, green and blue bars is transmitted as a series of video levels at 30%, 59%
and 11%. This is the only part of the complete color signal which is seen by a black-and-white
TV receiver.
The chroma signal has a relatively high frequency (3.579545 mc) which is largely
filtered out in the if and video amplifier of a black-and-white TV receiver. In
a color TV receiver, however, the chroma signal component is not rejected, but is
processed through the chroma circuits of the color receiver.
The color receiver responds to the phase of the chroma signal by displaying a
corresponding hue; it responds to the voltage of the chroma signal by displaying
a corresponding color saturation. This is how we get compatibility.
Color and Monochrome (B&W) Television
Articles
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