Teaching Earth Sciences - Earth Science Teachers' Association
Teaching Earth Sciences - Earth Science Teachers' Association
Teaching Earth Sciences - Earth Science Teachers' Association
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Figure 1 A simple diagram showing the eruption column and cloud for a super-eruption. A) The eruption involves the evacuation of a magma chamber, causing the rocks above<br />
to subside. This forms a Caldera. B) Part of the upwards flow out of the magma chamber remains negatively buoyant in the atmosphere, spreading out radially as pyroclastic<br />
flows. The deposits from these are called ignimbrites. C) Part of the eruption becomes positively buoyant thanks to the entrainment and heating of surrounding air. This rises<br />
until it reaches neutral buoyancy. D) Once at neutral buoyancy, the ash and gas spread out to form an “umbrella cloud” in the high atmosphere.<br />
and each super-volcano has a unique behaviour. It is<br />
plausible to have two super-eruptions from separate centres<br />
in quick succession.<br />
Atmospheric impact<br />
“I had a dream, which was not all a dream.<br />
The bright sun was extinguished, and the stars<br />
Did wander darkling in the eternal space,<br />
Rayless, and pathless, and the icy earth<br />
Swung blind and blackening in the moonless air;<br />
Morn came and went -and came, and brought no day,<br />
And men forgot their passions in the dread<br />
Of this their desolation; and all hearts<br />
Were chilled into a selfish prayer for light.”<br />
This is an excerpt from a poem entitled “The Darkness” by<br />
Lord Byron in 1816. His poetry was inspired by what has<br />
become known as the “year without summer”, where the<br />
far off Tambora volcano in Indonesia had darkened the sky<br />
and lowered global surface temperatures after erupting in<br />
1815. Lord Byron was not alone in his gloomy outlook, his<br />
guest at his summer house that year was Mary Shelley, who<br />
wrote “Frankenstein” in a morbid literary competition with<br />
Lord Byron.<br />
Sulphuric acid aerosol (H 2<br />
SO 4<br />
) is the main cause of this<br />
atmospheric disturbance, which forms from reactions of<br />
H 2<br />
S and SO 2<br />
with water (Figure 2). Atmospheric lifetimes<br />
of H 2<br />
SO 4<br />
are significantly increased in the stratosphere<br />
compared to the troposphere due to the lack of removal<br />
by precipitation. Therefore, stratospheric residence times<br />
are governed by gravitational sedimentation, which takes<br />
between 1 to 3 years for historic eruptions (Robock, 2000).<br />
For explosive eruptions, the formation of an eruption<br />
column means that volcanic emissions can be transported<br />
into the stratosphere, and therefore lengthen the<br />
atmospheric residence time (Figure 2). The 1991 eruption<br />
of Mt. Pinatubo (Philippines) was the first opportunity to<br />
track a sulphate aerosol cloud in the stratosphere using<br />
satellite imagery. The cloud first spread longitudinally,<br />
encircling the globe within a few weeks (Bluth et al.,<br />
1992). Latitudinal mixing appears to take much longer, the<br />
Pinatubo cloud was initially constrained between 20 o S and<br />
30 o N (Long & Stowe, 1994). Thorough mixing throughout<br />
the stratosphere occurred within 6 months (McCormick et<br />
al., 1995), therefore affecting the whole globe.<br />
The solid particles (termed tephra or ash) have a short<br />
atmospheric residence time, with most of the ash deposited<br />
within a few weeks of eruption. Small quantities of very<br />
fine tephra can remain suspended for a few months<br />
(Robock, 2000), but the impact on scattering incoming<br />
radiation is comparatively brief. Sulphur has a large effect<br />
on the <strong>Earth</strong>’s radiation budget as H 2<br />
SO 4<br />
aerosol particles<br />
have a typical radius of 0.5 µm, comparable to the peak<br />
wavelength in the electromagnetic spectrum from our<br />
Sun. These particles strongly scatter short-wave radiation<br />
and partially absorb in the near infra-red (Andronova et<br />
al., 1999). Incoming light is scattered in all directions, with<br />
back-scattering increasing the net planetary albedo (the<br />
reflectivity of a surface) and forward-scattering increasing<br />
the downwards diffuse radiation (Figure 2). The backscatter<br />
effect is more dominant, causing a net cooling at<br />
the surface during the day as less total radiation reaches<br />
the surface (Harshvardhan, 1979). This phenomenon has<br />
become known as a “Volcanic Winter” (Rampino et al.,<br />
www.esta-uk.net Vol 35 No 1 2010 <strong>Teaching</strong> <strong>Earth</strong> <strong><strong>Science</strong>s</strong> 25