Does this sound familiar? You have just had a full day of diving;
you're sitting with some new friends on the hotel terrace, having a drink and watching the
sun sink into the Caribbean, when one of them says, 'Wonder if we'll see the green flash
tonight?' You don't know what he's talking about, but you play along and like everyone
else you stare at the sun until it's gone. There was no flash, and you think you've been
had. Well, you haven't. There is a green flash, but you have to be very
lucky to see it.
The green flash was apparently first documented by Captain Back of the
H. M. S. Terror while in the arctic during its expedition of 1836-1837. Referring to a
January 17 event he wrote:
'In the morning however, at a quarter before ten o'clock while standing
on an ice hummock about seventeen feet high, and looking toward the east,
I had observed the upper limb of the sun, as it filled a triangular cleft
on the ridge of the headland, of the most brilliant emerald colour, a
phenomenon which I had not witnessed before in these regions.' (Murray 1838).
At first glimpse of a rising sun or final glimpse of a setting sun is
when you might see a momentary burst of dazzling green light. It is not, as some have
suggested, simply a product of retina fatigue whereby the removal of the brilliant orange
of a sunset induces its complementary color to be seen. The green light is physically
there, and has been photographed (Meinel 1983).
To understand this phenomenon one must begin with the fact that air is
a refractive medium --- it bends light. Although the bending produced by
a given layer of air is very weak (index of refraction at sea level is ~ 1.0003), it
becomes progressively stronger as light approaches the earth's surface and the air density
increases. At sunset the cumulative effect is to 'elevate' the sun's image by about half a
degree above its true position. Moreover, like most optically transparent media, air is
also dispersive --- it bends light of different frequencies by different
amounts. This is easily demonstrated with a telescope at sunset by viewing the sun
alternately through blue and red filters and seeing the sun's blue disk about 20 seconds
of arc higher than the red disk (see the figure below). The naked eye's resolution limit
is only about 120 seconds of arc, which explains why we don't normally see a blue fringe
at the top of the sun and a red fringe at the bottom.
Suppose now that you are viewing the setting sun through an 'ideal'
atmosphere: clear air, sharp horizon, air density monotonically decreasing with increasing
altitude. The top of the sun's 'red disk' is tangent to the horizon and is setting normal
to it. In 1.4 seconds the sun's 'blue disk' will sweep towards the horizon and vanish.
During that time you will see light that has progressively more colours subtracted from
it, first red, then orange, then yellow, etc., until in the last split second before the
sun totally disappears there should only be blue. So why don't we see a blue flash? Some
people do. Lord Kelvin, in 1899, referred to exactly that when he described the sun rising
over Mont Blanc, Switzerland. But there are good reasons why the flash should usually be
green, and not blue.
The light sensitivity of the human eye is a function of wavelength.
Under normal daylight ('photopic') conditions the peak stimulus is light in the
yellow-green portion of the spectrum, as shown below.
At sunrise and sunset, when the oblique rays from the sun travel a longer distance
through the atmosphere, the light reaching the earth has had a considerable portion of its
blue content removed by Rayleigh scattering (that's why the sun looks red). The scarcity
of blue light causes the peak stimulus to shift slightly towards the yellow, making a blue
flash less likely and a greenish-yellow one more likely. But it is well known (Wilson and
Brocklebank 1961) that when the eye sees a small patch of light adjacent to a large one,
the small patch will be perceived as being slightly shifted in colour in the direction of
the colour that is complementary to that of the large patch. With a large expanse of red
sky and a wisp of greenish-yellow at the sun's rim, the wisp of greenish-yellow therefore
appears to be biased towards the blue-green, and the flash appears to be emerald green. A
blue flash can occur only if the atmosphere is unusually clear, and scattering does not
deplete the sunlight of too much of its blue component.
Why is the green flash so elusive? A necessary condition for seeing it
seems to be a well-layered atmosphere, where the index of refraction increases without
interruption towards the surface of the earth. In fact, the gradient of the index of
refraction should be greater than usual, to accentuate the dispersion of colours. This is
not at all a common atmospheric condition. Usually the atmosphere has some turbulence,
with anomalies in temperature and humidity from layer to layer. Such inhomogeneities cause
abnormal refraction, which can produce a confused separation of colors. At the extreme,
the required ordering of colours (blue above red) could be reversed, which would make it
impossible to see a green flash.
Click here for a Green
Flash photo!
This article has been translated into Romanian by Alexander Ovsov.
REFERENCES:
Glenn E. Shaw, "Observations and Theoretical Reconstruction of the Green
Flash", Pure and Appl. Geophysics, 102, 223-235, 1973.
Aden and Marjorie Meinel, "Sunsets, twilights, and evenihg
skies" (Cambridge University Press, New York, 1983), Chapter 3.
Sir George Back "Narrative of an expedition in H. M. S.
Terror, undertaken with a view to geographical discovery on the Arctic shores, in the
years 1836-7" (J. Murray, London, 1838), p. 191.
M. H. Wilson and R. W. Brocklebank, "Color and Perception:
The Work of Edwin Land in the Light of Current Concepts", Contemporary Physics,
December 1961, p. 101.