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After every sunset, once the sun is gone, I always enjoy seen the belt of venus rising in the other side, followed by the Earth's shadow.

This is a picture I took (you will find better ones online). The Pinkish-purple band on top is the Belt of Venus, and the blue band on the bottom is the Earth's shadow.

enter image description here

This figure from Sky & Telescope explains it well:

enter image description here

While contemplating these beauties, I've had hard time understanding why we see the colors we do. To my eyes, the belt of Venus looks purple, which didn't makes sense to me, as the very short wavelength of purple light should have been scattered long before arriving back there. Then all made sense when I realized that if you mix blue and red light you get purple. So the color comes from the blue mixed with the red light backscattered by the high atmosphere that is still illuminated by the Sun.

However, I can't still figure out why the Earth's shadow looks blue, and I haven't been able to find an answer (here some links about the Earth's shadow but without an explanation of the color: 1, 2, 3).

We know the sky is blue and the sunset red to due the preferential scattering of blue light by the air. But: How can the air in the Earth's shadow scatter blue light if it doesn't get any direct illumination, and any indirect illumination getting back there should be VERY depleted in blue (i.e. mostly red light)?

I thought the fact that the belt of Venus scatters red instead of blue as the rest of the atmosphere, is precisely because back there there is no more blue light left, so the weaker scattering of red light becomes noticeable (please let me know if I'm wrong there).

Or is the air actually emitting blue light in some sort of fluorescence/glowing?

PS: As this is a purely atmospheric phenomena I though it would be better suited here than in the Astronomy SE.

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2 Answers 2

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To my eyes, the belt of Venus looks purple, which didn't makes sense to me, as the very short wavelength of purple light should have been scattered long before arriving back there. Then all made sense when I realized that if you mix blue and red light you get purple.

You got that part right. Purple is not violet. Violet is a spectral color at the high frequency end of the visible portion of the spectrum, while purple is a non-spectral color on the line of purples that spans from nearly ultraviolet to nearly infrared. We see color as a wheel rather than as a line. One possible explanation is that the long wavelength ("red") cones have a secondary response in the violet end of the spectrum. Spectral violet light excites both the short wavelength and long wavelength cones, but so does a non-spectral mix of red and blue light.

And that's what you're seeing in the Belt of Venus -- a muted mix of red and blue, or a purple (or perhaps magenta, or a rosy pink).

So the color comes from the blue mixed with the red light backscattered by the high atmosphere that is still illuminated by the Sun. However, I can't still figure out why the Earth's shadow looks blue.

The backscattered red light doesn't come from the high atmosphere. It comes from the troposphere. The high atmosphere (the stratosphere and above) contains very few particulates. The upper atmosphere is the only part of the atmosphere that remains sunlit above the eastern horizon after sunset. The sunlight hitting the upper atmosphere is Rayleigh scattered, so you see that very faint blue scattered light. You don't see the backscattered reddish light from the particulate-containing lower atmosphere at the eastern horizon because that part of the atmosphere is fully in the Earth's shadow above the eastern horizon.

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  • $\begingroup$ Taught me a lot in that, great stuff $\endgroup$ Feb 2, 2018 at 5:09
  • $\begingroup$ @DavidHammen I didn't meant anything specific by "high atmosphere" I didn't mean anything specific, sorry, I just mean the "upper part" that is still illuminated, I've edited the question accordingly. But going back to your answer, you mean that there is two different scattering processes? So Raleigh happen in air molecules and scatter blue light and another process involving particulate material scatter the red light? In that case how the air in the shadow can re-scatter blue light and the particulates in the shadow do not re-scatter red light? Is it just a intensity difference thing? $\endgroup$ Feb 6, 2018 at 0:34
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    $\begingroup$ "One possible explanation is that the long wavelength ("red") cones have a secondary response in the violet end of the spectrum" — this is completely irrelevant, even if it's so. The usual chromaticity diagram can be reproduced from the unimodal spectral responses of the L,M,S cones, and the line of purples is still there. $\endgroup$
    – Ruslan
    Jan 28, 2021 at 9:09
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How can the air in the Earth's shadow scatter blue light if it doesn't get any direct illumination, and any indirect illumination getting back there should be VERY depleted in blue (i.e. mostly red light)?

You're completely right. If you simulate light scattering only, you'll get exactly this result: a sandy-colored sky, with a bit redder belt of Venus, and a gray shadow of the Earth:

enter image description here

But our stratosphere contains a small amount of ozone, which absorbs in the orange region of the spectrum in what is known as Chappuis band:

Chappuis band spectrum

At daytime the solar light propagates at a small angle to the atmosphere, crossing a low amount of ozone, so the color of the sky is not affected (see also the question at Chemistry.SE: What exact color does ozone gas have?). But at twilight the sunlight goes through a large layer of atmosphere horizontally, thus the Chappuis absorption is very prominent.

The same simulation as above, but with ozone included (and with a bit higher exposure), will look like this:

enter image description here

Why is the shadow more blue (less orange) than the other parts of the sky? It's because in the shadow, there's no light from the single scattering: a ray from the Sun must be scattered at least twice to get to the earthly observer. This makes the Rayleigh scattering multiplier $\propto\lambda^{-4}$ apply twice, thus increasing the blue component of the inscattered light relatively to the red component. OTOH, the other atmosphere parts being not in the shadow, means that they do have contribution from the light scattered once, which has only a first power of this multiplier.

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    $\begingroup$ Great answer, can you add some information of what model/software did you use for the modelled atmospheres? And also a reference for Chappius absortion profile? Thanks, this is very interesting. $\endgroup$ Jan 29, 2021 at 13:52
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    $\begingroup$ @CamiloRada the reference to Chappuis profile is given in the answer at the link to Chemistry.SE, and the software is my own project CalcMySky. $\endgroup$
    – Ruslan
    Jan 29, 2021 at 13:55
  • $\begingroup$ @Ruslan eso.org/sci/publications/messenger/archive/no.143-mar11/… $\endgroup$
    – user1066
    Apr 25, 2021 at 11:52
  • $\begingroup$ @gansub what exactly did you want to say by this link? I seem to have seen this paper, and the part I remember it for is the statement under Figure 5 that doesn't make sense to me (actual color of ozone is blue, but they identify the dirty-yellow band of the atmosphere with the ozone layer). $\endgroup$
    – Ruslan
    Apr 25, 2021 at 12:01
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    $\begingroup$ @gansub belt of Venus is very poorly visible when the sunset is obscured by clouds. In this case the Earth's shadow just smoothly blends into the upper part of the sky. $\endgroup$
    – Ruslan
    Apr 25, 2021 at 17:35

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