When
I started in the print industry as an apprentice to Gutenberg, I noticed that
the folks in the press room called the inks red, yellow, and blue. This
confused me. Everything I had read in color theory books said that cyan,
magenta, and yellow were the subtractive primaries. These were the primaries
that you use to make a wide range of colors with pigments and filters.
Pigments and filters work by subtracting certain wavelengths of light. On the
other hand, red, green, and blue were the additive primaries, and these were
used to make all the colors when you are mixing light, as in a TV or computer
monitor.
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Polaroid snapshot of
me working at my first job
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Why
were those silly printers using some of the additive and some of the subtractive
primaries? Didn’t they realize that this reduced their gamut? That was the
theory, anyway .
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Just a naming issue?
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Anyone
who knows me, or who loves me can
attest to the fact that I am a firm believer that ignorance is the main
explanation for every cultural and scientific phenomenon. In this case, my
previous blog about counting colors provides a clue as to the sort of
ignorance that might explain why magenta is so curiously called red.
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The
eleven people who read my previous blog learned that there are only eleven
basic one-word color names in our active vocabulary. Neither cyan nor magenta
made that list .
Clearly the folks on press were calling the inks “red” and “blue” because
they have no other words to describe the colors.
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Cyan ink
is blue, and magenta is red
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In
my normal incisive way, it took me a few years to realize that the pressmen
were not quite as ignorant as I thought they were. I guess I spent too much
time running for buckets of halftone dots to actually put my head in a bucket
of ink. When I finally did put my head in a bucket of ink (as part of a
hazing
experiment) I could see that cyan ink is blue, and that magenta ink is red
when you look at them in a bucket.
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Cyan and magenta
inks are blue and red in the can
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Cyan and magenta
inks are cyan and magenta on paper
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So,
this confusion is obviously beyond my original explanation. Just like when a
fellow accidently calls his wife by the name of a former girlfriend, you can
bet there is something deeper going on.
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Beer’s law
revisited
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In
yet another very popular blog
of mine, I provided a charming explanation
of Beer’s law. This blog post is a prerequisite for the following
exciting discussion.
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Let’s
just say that we have a perfect magenta ink. A perfect magenta ink will
reflect all the red light and all the blue light that hits it. As for the
green light, a light shade of magenta might reflect about 10% of the green. A
rich shade of magenta will reflect about 1%.
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Now we bring in Beer’s law. Let’s say we start with
that light magenta and add another layer of the same ink. Beer’s law would
predict that the reflectance would multiply. Since perfect magenta reflects
100% of red and blue light, Beer’s law predicts that the double layer of
magenta will reflect 100% of the red and blue light. Beer’s law would further
predict that the green light would reflect at only 10% X 10%, which is 1%. A
double layer of light magenta becomes a rich magenta.
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Key point here: for this perfect magenta ink, the
hue is still that of magenta. It still reflects most of the red and blue
light, and absorbs most of the green light.
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Let’s
just say that we now switch over to a magenta that is less pure. Let’s just
say that for some inexplicable reason, the publishers of Schlock magazine are unwilling to spend $100,000 per gallon for
their ink. The bargain ink they decide to use does not reflect quite as much
blue light as we would hope; maybe it only reflects 40% of the blue light
when we put a thin film down, and maybe 10% of the green light. Let’s say
that the red light is still reflected at 100%.
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What
happens when we double the amount of ink on the paper? Beer’s law takes over, and we see that blue
light is reflected at 40% X 40% = 16%. Green light? The reflectance goes from 10%
down to 1%. Red light stays at 100%. The table below summarizes the Beer’s
law estimation.
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Blue
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Green
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Red
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Thin
layer
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40%
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10%
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100%
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Thick
layer
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16%
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1%
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100%
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From this table, it would seem that the thick layer of magenta is a lot closer to red. The
plot below shows the actual spectra of two magenta patches, one at a larger
ink film thickness than the other. The plot leads one to the same impression –
that a thick layer of magenta is closer to red in hue than a thin layer.
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Spectrum of a magenta
ink, normal thickness and thick
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The
tentative conclusion is that magenta turns red when it is thick because it is
impure, or more accurately, because there are several different reflectance levels
in the spectrum. When Beer’s law kicks in, the areas of the spectrum where
the reflectance is “mid-level” (i.e. 40% reflectance) are grossly effected by
the ink film thickness.
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The
plots below are the spectra of cyan and yellow inks. If the previous rule
applies, then we would expect that cyan ink will have an appreciable change
in hue as it gets thicker. From the plot of cyan ink, we see that the
reflectance values between 500 nm and 600 nm are “intermediate”, somewhere
between the highest value and the darkest value. This is the green range. As
cyan ink gets thicker, we would expect the amount of green light reflected to
drop.
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Thus,
based on Seymour’s rule of ink hue shift, a quick look at the plot below
would suggest that thick cyan ink will be blue, just like thick magenta ink
will be red. Yellow ink has very little in the way of intermediate values. It
basically has either 75% reflectance or 3%. From that, you would guess that
yellow ink will not change in hue. Note that a bucket of yellow ink does
indeed look yellow.
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Plots of cyan and
yellow ink
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But
spectra can be a bit misleading when trying to discern color. I don’t know
many people who can look at a spectrum and tell what the color is. So, I
offer a little computational experiment to further validate Seymour’s rule of
ink hue shift.
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First,
I will show the results. Then I will explain how I got them. The chart below
shows the a*b* values of a set of ten magenta patches with increasing ink
film thickness. These values are the ten blue diamonds in the plot. There is
clearly a strong hook. The first five are pretty much along a line without
much hue shift. The sixth one goes around the bend, and the last four are changing
a lot more in hue than they are in chroma.
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The magenta hook,
real and estimated
For the other views of this data, I have published an addendum to this blog post.
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The
magenta colored line in the plot is a prediction of what I call the “ink
trajectory”. This is the set of all L*a*b* values that an ink will go though
as you change the ink film thickness. To compute this estimated trajectory, I
started with the spectrum of the sixth patch and that of the paper. (You will
note that the magenta line goes right through that point.) I loaded these
spectra into a spreadsheet, and used Beer’s law to estimate the spectrum over
a range of ink film thickness. You will note that the estimated trajectory
comes reasonable close to predicting actual measured values, and definitely
predicts the hook.
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For
those who want more detail, I have a little more description below. This is
excerpted from a paper I presented at TAGA in 2008.
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This
pretty well settles it in my mind. Magenta ink on paper is magenta. Magenta
ink in a bucket is red. I have explained this with some simple ciphering with
Beer’s law. This led me to define Seymour’s rule of ink hue shift, which
allows you to tell (just by looking at a spectrum), whether an ink will have
an appreciable hook.
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I
then showed some really, really impressive results that show that, armed with
just the spectrum of your paper and that of your ink on that paper, you can
determine the magenta hook. This is clearly a triumph of modern science.
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I
have come a long way since I was ransacking the printing plant to find those
elusive halftone dots!
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