Why is the Sky Blue: K-12 Experiments & Demonstrations
Why is the Sky Blue: A simple Explanation
The sky is blue for the same reason that everything that is blue looks blue, like blue ink or a blue shirt. You may think that air, the main sky / atmosphere component, is transparent but thick layers of air - a few kilometers or miles, like the atmosphere's width, are bluish due to small dust perticles. So the sunlight that passes the atmosphere air reaches your eyes blue like a beam of bright like passing some blue glass or filter.
But why are sunsets and sunrises red? Because at sunset times the atmosphere air is red? To understand this you may need some more advanced explanation described in the following chapter.
Why is the Sky Blue
Diffuse sky radiation is solar radiation reaching the earth's surface after having been scattered from the direct solar beam by molecules or suspensoids in the atmosphere. Also called skylight, diffuse skylight, or sky radiation. Of the total light
removed from the direct solar beam by scattering in the atmosphere
(approximately 25 percent of the incident radiation), about two-thirds
ultimately reaches the earth as diffuse sky radiation.
Scattering is the process by which small particles suspended in a medium of a different index of refraction redirect a portion of the incident radiation in all directions. In elastic scattering, no energy transformation results, only a change in the spatial distribution of the radiation. The science of optics usually uses the term to refer to the deflection of photons that occurs when they are absorbed and re-emitted by atoms or molecules.
Why is the sky blue?
The sky is blue partly because air scatters short-wavelength
light in preference to longer wavelengths. Combined, these effects
scatter (bend away in all directions) some short, blue light waves
while allowing almost all longer, red light waves to pass straight
through. When we look toward a part of the sky not near the sun, the
blue color we see is blue light waves scattered down toward us from the
white sunlight passing through the air overhead. Near sunrise and sunset,
most of the light we see comes in nearly tangent to the Earth's
surface, so that the light's path through the atmosphere is so long
that much of the blue and even yellow light is scattered out, leaving
the sun rays and the clouds it illuminates red.
Scattering and absorption are major causes of the attenuation of
radiation by the atmosphere. Scattering varies as a function of the
ratio of the particle diameter to the wavelength of the radiation. When
this ratio is less than about one-tenth, Rayleigh scattering
occurs in which the scattering coefficient varies inversely as the
fourth power of the wavelength. At larger values of the ratio of
particle diameter to wavelength, the scattering varies in a complex
fashion described, for spherical particles, by the Mie theory; at a ratio of the order of 10, the laws of geometric optics begin to apply.
Why is the sky blue instead of violet?
Normalized typical human cone responses (and the rod response) to monochromatic spectral stimuli
Because of the strong wavelength dependence (inverse fourth power) of light scattering according to Raleigh's Law,
one would expect that the sky would appear more violet than blue, the
former having a shorter wavelength than the latter. There is a simple physiological
explanation for this apparent conundrum. Simply put, the human eye
cannot detect violet light in presence of light with longer
wavelengths. There is a reason for this. It turns out that the human
eye's high resolution color-detection system is made of proteins and chromophores (which together make up photoreceptor cells or "Cone" structures in the eye's fovea) that are sensitive to different wavelengths in the visible spectrum
(400 nm–700 nm). In fact, there are three major
protein-chromophore sensors that have peak sensitivities to
yellowish-green (564 nm), bluish-green (534 nm), and
blue-violet (420 nm) light. The brain uses the different responses
of these chromophores to interpret the spectrum of the light that
reaches the retina.
When one experimentally plots the sensitivity curves for the three
color sensors (identified here as long (L), middle (M), and short (S)
wavelength), three roughly "bell-curve"
distributions are seen to overlap one another and cover the visible
spectrum. We depend on this overlap for color sensing to detect the
entire spectrum of visible light. For example, monochromatic violet
light at 400 nm mostly stimulates the S receptors, but also
slightly stimulates the L and M receptors, with the L receptor having
the stronger response. This combination of stimuli is interpreted by
the brain as violet. Monochromatic blue light, on the other hand,
stimulates the M receptor more than the L receptor. Skylight is not
monochromatic; it contains a mixture of light covering much of the
spectrum. The combination of strong violet light with weaker blue and
even weaker green and yellow strongly stimulates the S receptor, and
stimulates the M receptor more than the L receptor. As a result, this
mixture of wavelengths is perceived by the brain as blue rather than
violet.
Neutral points
There are three commonly detectable points of zero polarization of diffuse sky radiation (known as neutral points) lying along the vertical circle through the sun.
- The Arago point, named for its discoverer, is customarily located at about 20° above the antisolar point; but it lies at higher altitudes in turbid air. The latter property makes the Arago distance a useful measure of atmospheric turbidity.
- The Babinet point, discovered by Babinet in 1840, typically
lies only 15° to 20° above the sun, and hence is difficult to observe
because of solar glare.
- The Brewster point, discovered by Brewster in 1840, is
located about 15° to 20° directly below the sun; hence it is difficult
to observe because of the glare of the sun.
Under an overcast sky
There is essentially zero direct sunlight under an overcast sky, so
all light is then diffuse sky radiation. The flux of light is not very
wavelength dependent because the cloud droplets are larger than the
light's wavelength and scatter all colors approximately equally. The
light passes through the translucent clouds in a manner similar to
frosted glass. The intensity ranges (roughly) from 1/6 of direct
sunlight for relatively thin clouds down to 1/1000 of direct sunlight
under the extreme of thickest storm clouds.
See also
External links
Books
This article is licensed under the GNU Free Documentation License. It uses material from Wikipedia Encyclopedia article "Diffuse sky radiation"
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