WHY IS THE SKY BLUE?
by Miles Mathis
for the world is hollow and I have touched the sky
Abstract: I will show that the current explanation is upside down.
In researching this topic, I was surprised to find two different answers from two of the top
mouthpieces of current physics. The top answer on a Yahoo search is by Philip Gibbs at the
University of California, Riverside1. It is that blue light is bent more than other colors. Gibbs
shows us this illustration:
Problem there is that we can move the Sun a few degrees and switch that effect. Just take the
Sun above the first guy and he sees an unbent blue ray. The other guy sees a bent red ray. Light
must be coming from all directions, not just the direction of the Sun, so this illustration is more
than useless, it is misleading.
Gibbs then shows it is air molecules, not dust, that do the bending, and he tells us that Einstein
calculated in 1911 the scattering by molecules. These equations of Einstein are said to be “in
agreement with experiment.” We are told, “the electromagnetic field of the light waves induces
electric dipole moments in the molecules.”
Gibbs then asks the million dollar question: “Why not violet?” If short wavelengths are bent
more than long, then violet should be bent even more than blue, and the sky should be violet.
He says it is due to the cones in our eyes. He shows the figure here
and says that violet light stimulates red as well, making us see blue.
The second top answer is from NASA, and is for kids. I would leave it be for that reason, except
that the third2 and fifth and sixth top answers are strictly the same as this one. All these answers
are glosses of the only slightly longer and fuller answer at Wikipedia, which is fourth only
because it is titled “Diffuse Sky Radiation.” That answer is that the blue sky is caused by
Rayleigh scattering from molecules. Molecules scatter short wavelengths more than long
wavelengths.
The Wiki answer is the fullest I found on the web, but even it is short, without the usual
attempts to misdirect with large amounts of math or complex theory. We are sent to the page for
Rayleigh scattering, but we get one equation and then the whole theory: “the shorter wavelength
of blue light will scatter more than the longer wavelengths of green and especially red light,
giving the sky a blue appearance.” Wiki doesn't even bother to spin some yarn to explain “why
not violet.”
So let's look at this theory, such as it is. We already have two theories, although they seem to be
similar or equivalent at a first glance. Gibbs' theory is that since red light is bent less, it never
reaches the ground except near sunset. We get this impression from his illustration, although he
never states it explicitly. It is slightly preferable to the scattering hypothesis and the scattering
illustration, since it begins to address a smart kid's question: “If red is scattered less, wouldn't it
just reach the ground directly, with more intensity?” So Gibbs draws bending instead of
scattering. You see Gibbs has a few dormant scruples left, which makes him try to tweek the
horrible answer he has been given from above. He also tries to answer the “why not violet?”
question, although he clearly isn't up to it. His own figure, from eyeball physiology, shows in
technicolor detail that the green receptors are also stimulated at violet wavelengths, so why talk
about the red and ignore the green? He isn't making any sense. Even if the red were stimulated
while the green were not, you still can't build blue from violet plus red, at least not according to
the current model. Since the retina is not white, you can't stack these red and violet responses to
get blue. That would require red canceling the red in violet. But if the eye is seeing both red and
violet, that will make the violet more red, not less red. You can't make violet into blue by adding
red in paint mixing, CMY, or RGB. The current model is an RGB model, and when crossing
violet light and red light on a white background, you don't get blue. In RGB, you cross red and
blue to get magenta. Just the opposite of his implication.
But all this is moot, since his figure shows a green response, too. We need to mix red, green, and
violet, to address his logic. In RGB, that should give us something quite near white. In CMY, it
would give us something nearer black. His whole explanation of “why not violet” is a wash, and
he would have been better to come up with a different dodge.
Gibbs' semi-honesty also comes through in his ability to admit that violet is not lacking in the
sky. Some have tried to answer “why not violet?” by claiming that our eyes are not as sensitive
to it, or that it is absorbed by the high atmosphere, but Gibbs admits that it must be there, and
that we must be sensitive to it, since we see it very well in rainbows.
But back to the main question. Forget violet. Can bending or scattering explain “why not red?”
Suppose that atmospheric molecules do scatter blue more or more often than red: does that
explain the lack of red in the sky? No. To explain the lack of red, you need to keep red from
hitting the ground, so you need to propose that it is bent so much it goes back up, or it is
absorbed so much that it never comes down. Neither scattering nor bending does that or can do
that, at least not with the current model of light. No smart schoolkid will be fooled by Gibbs
replacing scattering with bending, since his question remains: “If red is either scattered or bent
less or less often, shouldn't it just have a more direct path to the ground?”
The answer Gibbs is trying to shield or prop up is the scattering answer, which uses Rayleigh
scattering as the whole explanation of the blue sky. This is what we get from Wiki:
The strong wavelength dependence of the scattering (~λ-4) means that blue light is scattered
much more readily than red light. In the atmosphere, this results in blue wavelengths being
scattered to a greater extent than longer (red) wavelengths, and so one sees blue light coming
from all regions of the sky.
Notice that Wiki has just interpreted the Rayleigh molecule equation in two different ways. In
the first sentence, we are told that the wavelength dependence means that short wavelength light
is scattered “more readily.” In the second sentence, we are told that short wavelengths are
scattered “to a greater extent.” This leads us to ask, “Are the short wavelengths supposed to be
scattered more often, or at a greater angle?” If we study the Rayleigh equation carefully, we find
the answer is the angle, not the probability of being scattered.
I = I08π4α2(1 + cos2θ)/λ4R2
As you see, we have a representation of the angle, but no representation of the probability of
being scattered. The constant α is the polarizability of the molecule, so it cannot vary with the
wavelength of the light. The Rayleigh equation gives us an intensity of the scattered light, given
an incoming wavelength. In other words, the Rayleigh equation requires the incoming light to be
of one wavelength. We can only insert one wavelength into that equation at a time, as you see.
We let red light hit a molecule, for example, and the equation tells us how intense the scattered
white light will be. This is because the scattering turns the red incoming light into all colors (or,
rather, no colors), depending on the angle of scattering. That is what scattering means. That is
why the sky is bright instead of dark. If we subtracted out the color problem, we would explain
the whiteness of the sky as due to scattering. That is why space is dark: no molecules are
scattering, creating the whiteness.
We can see this from Wiki, on the page for scattering.
Scattering changes or destroys the original wave, as you see. You cannot scatter a wave and keep
the wave at the same time. That is having your blue and eating it, too. Despite this, current
theory assumes that a wavelength that is blue is scattered, remaining the same blue wavelength;
that if anything it gains intensity from the Rayleigh equation; and that it is then reflected down
(but not rescattered) by other molecules. Question: why do the first molecules scatter it and the
second molecules just reflect it down? How do molecules know when to scatter and when to
reflect? Amazing, really, that air molecules can redirect blue so many times without affecting it,
but that air molecules cannot do that with red (except at sunset, of course).
To see how dishonest all this is, we can study this figure at Wikipedia:
Figure showing the more intense scattering of
blue light by the atmosphere relative to red light
They have created a figure to show what they want to show, although the Rayleigh equation
doesn't show it. The figure shows more scattering of blue as a percentage of incoming light, and
just in case you missed it, they make the upper part of the figure sky-blue and tell you one more
time the conclusion: “Rayleigh scattering gives the sky its blue color.” They just need a
manipulative soundtrack and a nude woman waving a magic wand and the propaganda would be
complete. But even the figure contradicts itself, since they feel obligated to cover themselves by
giving us a bit of subtext: “figure showing more intense scattering of blue light....” Wait, they just
said in the figure's sidebar that the figure showed more scattering as percentage, and now they
are saying the figure shows more intense scattering. But, as I just showed you, the two claims
are not the same. The equation does indeed show more intense light scattered from incoming
blue, but it doesn't show more scattering of blue as a percentage of all incoming light. Our brain
is being massaged here.
If we apply the Rayleigh equation to all the different wavelengths, it is just telling us that our
scattered white light will be more intense if we start with short wavelength light instead of long
wavelength light. And that is just because short wavelength light has more energy to start with.
It has a greater frequency, and therefore, according to the Planck relation, it has more energy.
More energy supplies more intensity in scattering.
So, you see, the Rayleigh equation doesn't tell us a damn thing about color. It doesn't tell us
that blue light is scattered more often, or even more. It isn't scattered more, it is scattered at a
greater angle, and that just tells us that scattered blue light will cause more intense white light.
Current theory assumes that Rayleigh scattering is elastic, since it needs to keep the blue light
blue. But there is no proof of that other than the color blue we see. They have no mechanics to
explain it or prove it, and since all the math is pushed to fit the data, the math cannot be proof
of anything.
You see, Rayleigh scattering is even less understood than Compton scattering7 or Thomson
scattering. At least in these two theories of scattering, we have some mention of photons. We
have particles acting on eachother: if not colliding, then at least exchanging energies. Beyond
that, we have emission and emission fields. But with Rayleigh scattering, we have none of that
partial rigor. We just have an equation, derived by slippery means, and then an illogical theory
tacked onto it. We are shown a wavelength dependence in the equation, but then the theory and
explanation stops. We aren't told how this explains blue reaching the eye but not red. We are
told the blue is scattered more than the red; but then what? If the red isn't scattered so much or
so often, wouldn't it just continue on down to the ground? And if so, why is it invisible?
Current theory has a huge hole in it, and it becomes very conspicuous in this problem of
scattering. We are given an equation for scattering but no explanation of it. Nowhere on the web
or in any book could I find a definition of this sort of scattering. What is happening
mechanically? No one knows, because they will not define the light as either a wave or a
particle. We aren't told if the wave is being scattered or if photons are being scattered. All the
math and sentences imply it is the wave, but none of the specifics are ever addressed. The
quantum mechanical explanation of scattering is currently the Feynman explanation, using
sum-overs. In this explanation, Feynman, like non-quantum explainers, mainly avoids any
mechanics. Feynman tells us it is photons that are scattered, but he likes to use his little clocks
and vectors8 to solve these problems, and he will not admit that these clocks and vectors track
the waves. Clocks are waves. At any rate, this is the nearest we get to a mechanical explanation
of photon mechanics, but it is a purposeful misdirection. Feynman and other quantum physicists
have told us not to ask mechanical questions, which is convenient for them.
Feynman came closest to being able to solve these problems because he allowed himself a math
that represented the photon as both wave and particle at the same time. Before that, we have to
go all the way back to Maxwell to find someone giving the photons themselves waves (or spins),
and Maxwell only tried that for a couple of years before it gave it up. Before Maxwell, we go
back to Newton, who tried to give his corpuscles spins (and spins are waves). Both Newton and
Maxwell were shouted down or ignored, and since Feynman died quantum physics has ditched
his clock method as too visual and mechanical. But treating the photon as both particle and
wave is the only way to solve this problem. I have no use for sum-overs or photons with clocks,
but we can solve this problem by giving the photon spin.
We can solve without throwing out Rayleigh's equation; or Einstein's 1911 calculations, either.
We just need a bit more theory. Contemporary theory didn't have quite enough physics to
explain it, so they had to fill the gap with bluster and fudge. The truth is, red is actually
scattered more than blue, but Rayleigh's equation can't show that by itself. Rayleigh's equation
doesn't contain the theory or the variables to tell us what wavelength is scattered the most often,
and nothing in current light theory does either. But it turns out that red is scattered more simply
because its wavelength is larger. I have shown in other papers6 that the wavelength of light is
not caused or carried or expressed by the wave front or by a group of photons or by any
medium. It is caused by each individual photon. Each photon has a tiny local wavelength,
caused by spin about an axis, and this local wavelength is stretched out by the speed of the
photon. The orbital velocity of the photon is 1/c, and the linear velocity is obviously c, so the
local wavelength is stretched out by c2. That is where the c2 in Einstein's famous equation
comes from.
Given that, we see that the individual red photon is bigger than the individual violet photon, at
the quantum level. Because it is bigger, it has a slightly larger cross section. So it is more likely
to collide with anything, electron or proton or molecule or other particle. Conversely, violet
photons are more likely to dodge collision. Yes, violet photons, because they have a smaller
wavelength, actually avoid scattering better than red photons. What we see in sky color are
photons that haven't been scattered, not photons that have been scattered. As a first rule, the
scattered photons make the white, and the unscattered photons make the color.
This is also the explanation for how light can arrive with many different wavelengths. The
current model cannot show how incoming white light from the Sun can carry all the
wavelengths at once. If a wave hits an air molecule in being scattered, how can the wave be red
and yellow and green and blue all at once? A wave must have some structure, by definition, and
a wave that was green in one place and red in the next wouldn't have any structure. Light is still
drawn as a field wave in modern illustrations (in the rare case that these phenomena are
illustrated), and a field wave cannot vary its wavelength all over the place. But if each photon
can carry the wave, then it is easy to show how white light can carry various colors. If light is
not a field wave, then this question answers itself, by simply evaporating. Photons may sort
themselves by wavelength, but the energy of the “wave” is not determined by particle alignment
or rowing or fronts or anything else. A single photon can express the wave by itself.
Why not violet? Because, to see a violet sky, it would require that violet is never scattered and
all other colors are always scattered. That is not logical. We have found that violet is less likely
to be scattered, but not that it is never scattered. So the sky color we see is an average of all the
unscattered light that reaches us. Some small part is red, a bit more is yellow, a bit more is
green, a bit more is blue, and a bit more is violet. We add them all up, and what do we get? We
get blue. We get a spectrum weighted by probability toward violet, but not all the way to violet.
You will say, “But if we are seeing all these colors in the sky, shouldn't the sky be white? All
the colors together are white.” Well, the sky is a fairly pale blue. So we have a lot of white
there, yes. But the sky color we see is unscattered light, not scattered light. So even though it
has some components across the spectrum, it is fairly coherent, relative to the scattered light
also entering the eye. By coherent, I just mean that it is coming to us in a relatively orderly
fashion. It has not been scattered, so it is more orderly than scattered light. The eye reads
scattered light as white, but it does not read two (or more) unscattered colors arriving together
as white. It is known that the eye reads color relative to other color, and it treats unscattered
light like that. We already know that if one source is sending the eye several colors, the eye
weighs the colors and averages. That is how it creates blue-grey and brown and so on. Because
the sky is heaviest at the violet end and lightest at the red end, the eye averages at blue, then
greys it out. The blue part of that is the average wavelength, and the grey part of that is the
overlaying of the colors.
You will say that the current explanation could steal that last part from me and ditch all the
hoodoo about red being bigger than violet. Yes, they could and they probably will. But the truth
is they have the mechanics upside down. The blue is not scattered more often, the red is. If the
blue were scattered more, the sky would be red.
I passed this theory by a mainstream physicist, and his first comment was that if we are seeing
unscattered blue, then we should see it only in the direction of the Sun. I found that comment a
bit shocking, since to make it you have to assume that light is arriving on the Earth only in a
narrow band the width of the visible Sun. I am not aware that anyone thinks that, physicist,
artist, or shoe salesman. We all know that the Sun is emitting light spherically, and that the
Earth intercepts this light across its whole diameter. Perhaps this physicist meant that light
coming from other directions than the visible Sun had to be focused a bit to reach any one eye,
but that isn't hard to explain. The Earth's upper atmosphere simply focuses the incoming light,
due to its own spherical shape, like a big eyeball. This focusing is very imperfect, simply pulling
the light generally toward the surface, but it is enough to account for the light coming from all
directions. Yes, the light from the direction of the Sun itself will be the most intense by far, but
it is not difficult to explain light coming from all directions.
He then said, “In that case, I don't see that we need scattering at all. You just explained
scattering without scattering.” No, I didn't. I explained light being spread across the diameter of
the Earth, but that does not negate scattering, or give scattering nothing to do. My mechanism of
imperfect focusing is not meant to be a replacement for scattering, and it couldn't possibly create
the brightness that scattering creates. Nonetheless, I don't see how it can be denied. Why would
the spherical shape of the atmosphere NOT create this focusing of incoming light? The current
theory uses this theory of focusing by a sphere to explain rainbows, as when the spherical
raindrop deflects light toward its rear center. If the raindrop does it, why wouldn't the Earth's
atmosphere? The physicist admitted my point.
If that point is admitted, then we only have to show that this focusing does not destroy all
possibility of blue light. It doesn't, of course, since we all know that blue light can be reflected
or deflected. We then have blue light coming from all directions in the sky (but the least near
the horizon). Some of it will be scattered, increasing the brightness of the sky, and some will
not. The blue we see is the unscattered blue.
We see clear proof I am right if we then ask the standard model why clouds are white. We are
told that clouds scatter all the light the same amount via Mie scattering, creating white light. So
Mie scattering creates white clouds and Rayleigh scattering creates a blue sky. This despite the
fact that the math is basically the same for the two. Both Rayleigh and Mie applied Maxwell's
equations to similar problems, only Mie's particles were bigger. In fact, Rayleigh's equations
were first applied to spherical particles, same as Mie's. They were then tweeked to account for
the fact that air molecules are not spherical or otherwise isotropic. However, this tweeking is not
where the wavelength enters the equations. Rayleigh included the wavelength variation even
before the equations were tweeked for the anisotropy. Why? Because Rayleigh developed his
scattering equations specifically to explain why the sky was blue! He needed a wavelength
variation and Mie didn't. The equations were pushed to match data.
You can't have large particles that scatter all light the same and small particles that scatter blue
more, unless you show some mechanical reason for that difference. Rayleigh couldn't show that
reason and neither has anyone else. No one has claimed it is the anisotropy of air molecules that
is the cause, although that is the only apparent difference, other than size. They can't do that
because, as I said, the Rayleigh equations show wavelength variation even with isotropic
molecules.3 If it is not the anisotropy that causes the wavelength variation, is it the size? We
don't know, since the mathematicians won't tell us, but Wiki will admit that, “In contrast to
Rayleigh scattering, the Mie solution to the scattering problem is valid for all possible ratios of
diameter to wavelength.” This must mean that the Rayleigh solution is a subset of the Mie
solution; and that means that one cannot work in a fundamentally different way than the other.
And that means that we have no explanation for why Rayleigh scattering is wavelength
dependent and Mie scattering isn't. The explanation is that the sky is blue and clouds are white,
which is of course circular.
As usual, the theorists try to misdirect us from this realization with a lot of fancy math. We are
told that, “Quantum mechanical perturbation theory for two-photon elastic processes provides
both a powerful and elegant means (e.g.: Craig and Thirunamachandran, 1984)”3 for deriving
the Rayleigh equation. But if you honestly believe that a QM perturbation solution will be
elegant, you are not paying attention. I suggest you study some QM perturbation solutions and
get back to me. What would be truly elegant would be a simple mechanical solution, but QM
was forbidden from giving you that by the Copenhagen interpretation, back in the 1920's.
Instead, they pile more math on your head to try to keep you from asking for sense. Nowhere in
this perturbation solution do they address my question here, as to what is causing the
wavelength dependence. The perturbation solution is not more mechanical, it is very much less
mechanical. More math is always used to cover less mechanics.
We also get sentences like this: “The polarizability of a molecule will depend on its orientation
relative to the direction of the incident light and, in general, is a tensor of rank 2.”3 Yes, but that
is just misdirection. I don't give a flying squirrel what rank the tensor is, I want to know what the
polarizability of the molecule has to do with its ability to sort wavelengths. Keep your math in
your hat, but tell me how a small sphere or non-sphere can sort wavelengths while a large
sphere cannot. Until you can do that, I am going to assume all your math is just used to create
the answer you need.
To show this pushing of math to force a solution, we may look closer at this page I have been
quoting from the University of California at Irving. This author, Chris McLinden, develops the
Rayleigh equation as “a limiting case of Mie scattering.”4 But since Mie scattering creates white
light, he cannot do this without cheating. He imports equations from his Mie page to develop a
Rayleigh matrix, and then says, “and from equation (2.39), the Rayleigh scattering cross-section
is...” And we get the Rayleigh equation, complete with the wavelength in the denominator.
Unfortunately, there is no equation 2.39 on his website. We assume it is a typo for 3.39, but
neither equation 3.39 nor any of the equations around it have any wavelength variables in them.
How could they, since equation 3.39 is on his Mie scattering page: Mie scattering is not
wavelength dependent! Where did the wavelength come from? We cannot dismiss this as just an
unimportant oversight or recent typo, since this is a university website that has been up for over
a decade, and that scores number five on a websearch for “Mie scattering.”
At number five on a search for “Rayleigh scattering”, we pull up a website by Philip Laven5 that
clarifies this a bit. There we find that the scattering angle is proportional to x3, and that x =
2πr/λ. But r here is the radius of the scattering sphere. So, again, we have to ask by what
mechanics a small sphere shows a dependence between r and λ, and a larger sphere does not.
And, again, Mr. Laven has nothing to say about it. He has more fancy graphs than Wikipedia
itself, but no more mechanics. Like Wiki, he has zero mechanics.
Notice that I can explain white clouds without contradicting myself. I have said that all
scattering creates white light, and clouds simply scatter more. Therefore they are whiter.
Because the particles in clouds are much larger than molecules, neither the blue light nor the
red light can dodge them. All the wavelengths are scattered, destroying the blue. If clouds have
any color, it tends to be a light violet. This also confirms my theory, since violet is the smallest
visible photon. If any photons can dodge the scattering, it is violet. If any color gets through, it
will be violet, not blue.
I will be told that clouds tend to go to grey, but those are shadows. The greys are always on the
dark sides of clouds, when clouds are dense enough to scatter most light up or sideways. The
grey is not color, it is relative darkness.
Current theory is also contradictory in its explanation of why the Sun appears yellow. Wiki tells
us:
Conversely, glancing toward the sun, the colors that were not scattered away—the longer
wavelengths such as red and yellow light—are visible, giving the sun itself a slightly yellowish
hue.
So we see yellow because it is not scattered, and blue because it is? That doesn't make any sense
at all. Current theory tells us that the blue is coming to us indirectly, and the yellow is coming
directly, but we already know that isn't how light works. Scattered light coming
indirectly—from all directions—is seen as white light. This is because as light is scattered, its
energy is affected by the angle of scattering. Molecules scatter photons at any number of
different angles, and blue photons that are scattered are no longer seen as blue. You can't scatter
light in all directions and then claim it is still blue. I have already shown why we see blue, and it
isn't because blue light is scattered, staying blue.
Just think of it this way: assume current theory is correct, and work back from your eye. Say you
are receiving blue from all parts of the sky, except from the direction of the Sun. That means
you are receiving blue from all different angles. Go up into the sky, to one molecule that is
scattering the light to you. There is an angle at that molecule between you and the Sun. The
molecule supposedly deflected the blue photon from the Sun to you, at that angle. Now go to
all the other molecules that are doing the same thing. The angle is different for each one. How
can the angle be any possible angle, and the light stay blue? According to this theory, any angle
of scattering is blue, and no angle of scattering is red. Impossible.
We can see other big problems with current theory. Current theory tells us that yellow light
from the Sun is not scattered, and that is why we see a yellow Sun. But in the next sentence, the
same theory tells us that in space, the Sun is white. Well, if the light from the Sun is actually
white, and the light we see in the line of the Sun is unscattered, then we should see the Sun as
white here on Earth, too. They just told us the light was coming directly to our eye, and was not
scattered. If it isn't scattered, why is it changed? Why isn't it white? They would have to answer
that the violet, blue, green, and red is scattered, leaving only the yellow unscattered. But in that
case they have contradicted themselves. In the line of the Sun, we don't see blue because it is
scattered away. But everywhere else, we do see blue because it is scattered away. In that case,
we have to ask again, “Do we see color because it scattered, or because it is unscattered? You
have to make up your mind. You can't have it both ways.” According to current theory, if we see
blue because it is scattered, then we should see yellow in the direction of the Sun because it is
also scattered. But if that were true, we would have to ask why molecules in line with the Sun
act differently. Why do molecules in the line of the Sun scatter yellow? Or, going back to the
previous theory, why would molecules in the line of the Sun scatter everything except yellow?
It has to be one or the other, but both are illogical. Molecules in the line of the Sun cannot act
differently than molecules in other parts of the sky.
The current answer is that molecules in the line of the Sun scatter shorter wavelengths, just like
everywhere else, but that is a fudge, since the Sun only looks yellow: it does not look green or
red. If the sky scatters blue, then the Sun should look red, green, and yellow. Current theory
tries to average these three into yellow, but according to current theory, neither light nor the eye
works that way. If we are seeing red, green, and yellow from a source, we will not average that
into yellow, we will combine it into brown or grey. Yes, if we are receiving much more yellow
than green and red, we will see a greyed out yellow, but that is not the situation with the Sun.
The Sun we see is supposed to be white minus violet, and white minus violet is not yellow.
In other words, my average worked above, since I was not averaging three equal parts. I was
averaging large amounts of blue and violet with much smaller amounts of green, yellow, and
red. This gave me an average of a slightly greyed out blue. But the current model is trying to
average equal parts of red, yellow and green to get yellow. Even if they steal my averaging
method, they still can't get yellow from that. They get brown or grey. And, besides, they can't
use my averaging method, because their theory is not a color averaging theory. Their theory is a
physiological RGB theory, where you would cross red and green to get yellow. If you add
yellow to that, you get a double saturated yellow. They should predict a very yellow Sun, not a
pale yellow Sun.
The reason we see a Sun that appears slightly yellow is mainly because it is next to a blue sky. It
is an optical illusion. It is related to this optical illusion called “moth eggs”.
The “eggs” are actually white, but appear yellow against this background of blue and green. You
will say that the sky is not green, but I have shown that it contains some unscattered green, just
as this illusion does. This is why the Sun looks yellower in the summer: the green of the trees
and landscape reflects off the sky, adding green to the background the eye sees. On a
background of green and blue, white will appear pale yellow.
Another reason we think the Sun is yellower than it is concerns the afterimage. We can only
glance at the Sun for a split second. If you try it you will see that the yellow is in the afterimage,
burned in the retina around the Sun. You don't really see a yellow Sun, you see a yellow
afterimage. If you block the circle of the Sun and just look at the sky around the Sun, you will
see that the yellow is mostly a myth. We are mistaking bright warm white for yellow. The white
looks warm because it is surrounded by cool blue. Even the yellow in the afterimage is false,
since it is also caused by the original blue response. It is the retina's response to very white light
on a blue background. The retina always tries to supply the contrary color, for reasons still
unknown; and the brighter the light, the more the retina supplies the contrary. The yellow circle
is just this response to blue: that is why it is only on the edge of the Sun, where the blue meets
the white.
Then why is the sky red at sunset? If the current model is upside down, then they must be wrong
about that, too. Yes, they are. They say that the blue is scattered less then, but it is actually
scattered more. The dust particles that do the scattering at sunset are bigger than atmospheric
molecules, so the violet and blue light can't dodge it as well. The violet light is therefore
scattered almost as much as the red.
The current explanation is that red at sunset is caused by particles at low altitudes, from dust,
pollution, or other causes. Unfortunately, Rayleigh scattering (and Tyndall scattering, which
Gibbs mentions on his page) is not different for larger particles. The Rayleigh equation for
particles larger than molecules also has the wavelength variable in the denominator, which
means dust particles would not scatter red preferentially over blue, according to current theory.
Given current theory, dust should also scatter blue more or more often, because λ4 is in the
denominator. These people do not seem to be able to read an equation: they think they can push
it any way they like, scattering blue in one case and red in another.
But they are correct that the angle to the Sun is important. At sunrise and sunset, we see red due
to reflection from clouds and dust, not scattering. That is, we see a single bounce, at a specific
angle. To see red, our eye has to be at a very specific angle to the cloud or dust. Even some
editors at Wiki seem to understand this, since at the Tyndall Effect page, we find
The term "Tyndall effect" is sometimes applied to light scattering by macroscopic particles such
as dust in the air. However, this phenomenon is more like reflection, not scattering, as the
macroscopic particles become clearly visible in the process.
There it is, Wiki contradicts Gibbs, and actually gets something right. We know that the red
must be caused by reflection, because we get red in the area of sky opposite the Sun as well as
the area toward the Sun. Clouds at the right angle can reflect red back to us.
You will say, “If red is scattered more by the Rayleigh equation, then it should be scattered a lot
by dust and the dense atmosphere at low altitudes. So it should be scattered massively in this
situation.” Yes, and it is. I didn't say that red wasn't scattered at sunset. I said that the red we see
isn't caused by this scattering. The phenomenon of red sunsets is not caused by scattering. The
red we don't see is caused by scattering. The red we do see is unscattered light (of any original
wavelength) that is reflected to us at the right angle.
1http://math.ucr.edu/home/baez/physics/General/BlueSky/blue_sky.html
2http://www.sciencemadesimple.com/sky_blue.html
3
http://www.ess.uci.edu/~cmclinden/link/xx/node21.html
4http://www.ess.uci.edu/~cmclinden/link/xx/node20.html
5http://www.philiplaven.com/p8b.html
6
Mathis, Miles. Planck's Constant and Quantization. 2008.
7 Mathis, Miles. The Compton Effect, Duality, and the Klein-Nishina formula. 2010.
8
Mathis, Miles. Three Problems Solved Mechanically. 2008.