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Issue 5, February 2002
Exploring the Ozone Hole: Mechanisms of Stratospheric Denitrification
Sadhna Vora
Chemistry, Harvard University
vora@jyi.org
Imagine…checking
the weather forecast to find out whether it is safe to go outside.
Imagine…learning to deal with the growing and inescapable threat
of cancer. Imagine…living in a world whose ozone layer has been
torn and ravaged…
The ozone layer is a blanket of ozone that exists six to 30 miles
above the earth's surface in the stratosphere (EPA 2001). Crucial
to life on earth, it protects against the sun's harmful ultraviolet
radiation. However, chemicals used in refrigerants, pesticides,
and industrial solvents pose a grave threat to the earth's ozone
layer. Chlorine radicals that form from chlorofluorocarbons (CFCs)
react with ozone to convert it into simple diatomic oxygen, rendering
it incapable of absorbing harmful UV light. High levels of CFCs,
which are used in numerous industrial and household contexts, have
combined with blustery weather to create a gaping hole in the layer
of ozone over Antarctica. This ozone ‘hole' is a reduction of ozone
of up to 70% that occurs seasonally in the stratosphere over Antarctica.
This hole reached its record size in September 2000, when it claimed
more than 15 million square miles, an area as large as the continent
of North America.
CFC concentrations are normally held in check by nitrogen oxides,
also called NOx. Molecules of NOx deactivate
the chlorine radicals that destroy ozone. Any process that depletes
the stratosphere of NOx reservoirs contributes to higher
levels of chlorine radicals and therefore enhances ozone depletion.
While the chemistry driving ozone depletion itself is understood,
the process of denitrification still remains a mystery, with two
prominent theories competing for viability.
Possible Mechanisms of Denitrification
The current denitrification theories rely on Polar Stratospheric
Clouds (PSCs) as the denitrification agents. It is thought that
PSC particles containing nitric acid settle out of the stratosphere,
thus forming a permanent sink for nitrogen-containing species. However,
there are two types of PSCs, each forming under different conditions
and composed of different particles-which gives rise to two theories,
each one dependent upon a single type of PSC.
Type I PSCs form at a few degrees below 196 K (-77ºC)
and are composed of nitric acid hydrate droplets. They are relatively
small, typically having a radius less than 10-10
m (Dessler 1999), and therefore fall very slowly from the stratosphere.
Because of their small size, they also are at a higher risk of evaporation
and therefore have a relatively short lifetime. Type 2 PSCs are
composed of ice particles. They are less abundant than Type 1 PSCs
because they form only at or below the frost point, 188K (-85ºC).
These particles tend to be larger, with average radii of five to
20 micrometers (10-6
m) (Dessler 1999), and therefore have more rapid sedimentation velocities
and longer lifetimes (Table 1).
Table 1 - Summary
of Type 1 and Type 2 PFCs
Any denitrification mechanism must take into account two empirical
facts: First, denitrification has been observed to occur without accompanying
dehydration of the atmosphere (Fahey 1990). However, if appreciable
sedimentation of either type of PSC occurred, dehydration would also
be observed. A viable mechanism therefore must allow for nitrogen
oxides to descend from the atmosphere without causing water to leave
as well. Second, denitrification has been observed during middle to
late June, a relatively warm period in the Antarctic (Tabazadeh 2001).
However, Type 2 PSCs do not normally exist above the frost point.
A denitrification mechanism must then either rely only on Type 1 PSCs
or must somehow account for the existence of Type 2 PSCs above the
frost point.
Type 1 PSC-Mediated Denitrification
The small size of
Type 1 PSC particles causes them to fall very slowly through the
atmosphere (Dessler 1999). They are therefore at high risk of evaporating
before having fallen a significant distance. Because of this probability
of evaporation, it is unlikely that these particles will be able,
in their natural state, to carry NOx down from the atmosphere.
Therefore, if Type 1 PSCs were to denitrify the atmosphere, a few
particles must somehow grow into larger particles. The process by
which the small Type 1 PSC particles might attain the size necessary
for stratospheric denitrification has invited attention from the
scientific community.
One group of scientists, headed by R.J. Salawitch, described the
composition of these larger particles as well as the conditions
necessary to create them. They proposed that in areas where the
temperature drops slowly with descent through the stratosphere,
ice could selectively deposit on PSC particles, allowing them to
grow to sizes reaching up to a micrometer. In the presence of slow
cooling rates, the first ice/PSC particles to form are energetically
favored to have more ice deposited on them, while the others do
not grow appreciably. Eventually, the ice/PSC particles reach a
size that is favorable for sedimentation out of the atmosphere.
When this occurs, denitrification results. Because ice deposition
occurs on only a fraction of the PSC particles, little dehydration
accompanies the denitrification.
The important feature of the Salawitch mechanism is the presence
of slow cooling rates. If the cooling rates through the stratospheric
column were rapid, the atmosphere would quickly become supersaturated
with respect to HNOx, causing condensate to be deposited
indiscriminately on all PSC particles. None of the particles would
reach the size necessary for sedimentation. If slow cooling rates
are empirically observed, this theory is a plausible explanation
for denitrification without accompanying dehydration. Furthermore,
because Type 1 PSCs form above the frost point, the observation
that denitrification occurs at relatively warm temperatures is explained.
Other studies of Type 1 PSCs employ a similar line of reasoning
(Fahey 1990; Dessler 1999).
Type 2 PSC-Mediated Denitrification
While the studies
discussed above explain denitrification through Type 1 PSC sedimentation,
it has been argued that the slow cooling rates necessary for selective
nucleation are not present in the atmosphere (Gary 1989). Thus, the
questions of how denitrification can occur above the frost point and
with little dehydration still stand. A mechanism that addresses these
questions using Type 2 PSCs has been presented by S.E. Wofsy and his
colleagues (1990).
The fundamental concept involving this second mechanism is the idea
of a coating around the Type 2 PSC particles. Wofsy and his colleagues
reasoned that a coating would protect Type 2 PSC particles from relatively
warm temperatures, allowing them to denitrify the atmosphere even
at temperatures above the frost point. These scientists observed that
a Type 2 PSC loses 80% of its initial mass upon descending 100m through
the stratosphere. However, after this initial descent, its size remains
roughly constant.
Wofsy hypothesized that the coating involved in this process is composed
of a hydrate of nitric acid. As the surrounding atmosphere cools,
the partial pressure of nitric acid exceeds its equilibrium value
and it begins to condense on ice particles. In doing so, it lowers
the vapor pressure of the ice, preventing its evaporation even at
temperatures several degrees above the frost point.
The Wofsy mechanism meets another criterion as well: it allows for
denitrification to occur without dehydration. Because only a select
few the ice particles are preserved long enough to attain a sufficient
size for sedimentation, the vast majority of particles remain in the
stratosphere. Thus, water is not removed from the stratosphere in
any significant amount. It seems possible that coated Type 2 PSC particles
could denitrify the atmosphere at temperatures above the frost point
and without dehydration, in accordance with observations.
More recent experiments have supported Wofsy's hypothesis. Goodman
et. al. (1997) proved that nitrate exists on ice crystals found in
the stratosphere. Furthermore, Tolbert and Middlebrook showed that
ice particles coated with an artificially induced thin layer of nitric
acid hydrate survived to temperatures four degrees higher than particles
lacking the coat (1990). However, questions remain about the exact
method by which the nitrate coating forms. Some have criticized Wofsy's
mechanism, arguing that it results in the creation of a highly porous
nitric acid coating, one that does not succeed in prolonging the particle's
lifetime (Biermann et al. 1998).
Conlcusion
While the last decade
has yielded important theoretical insights into atmospheric denitrification,
questions still remain. The slow stratospheric cooling rates necessary
for Type 1 PSC denitrification are not always observed, and there
are still questions about how a coating that effectively prolongs
the lifetime of Type 2 PSCs can form (Table 2).
Table 2 - Type 1 and Type 2 PSCs as potential denitrifiers
The danger is that a rise in CFC concentrations would cool the stratosphere
such that PSCs would routinely persist for this time period, not only
over the Antarctic, but over the Arctic as well. Denitrification would
consequently occur extensively over both poles, allowing for the existence
of high concentrations of chlorine radicals and subsequent ozone depletion.
The growing hole over the Antarctic would then be joined by an Arctic
ozone hole.
Fortunately, CFC emissions have decreased in recent years. Because
the issue of ozone depletion is such a pressing one for public health
and safety, we must strive toward heightened public awareness of the
dangers of ozone depletion and continue in the trend of decreased
CFC emissions. On an individual level, this means repairing leaky
air conditioners and reducing use of aerosol sprays. Industry must
also take on the challenge of reducing CFC emissions by using alternatives
to ozone-depleting substances. The Environmental Protection Agency
has listed alternatives to commonly used industrial CFCs (EPA
2001) as a means of encouraging the public to use alternative
products. More broadly, international cooperation and heightened awareness
of environmental health hazards are necessary to address this global
problem.
Suggested Reading
Biermann,
U.M., J.N. Crowley, T. Huthwelker et al. "FTIR studies
on lifetime prolongation of stratospheric ice particles due to NAT
coating." Geophys. Res. Lett. 25 (1998): 3939-3942.
Dessler, A.E., J. Wu, M.L. Santee et al. "Satellite observations
of temporary and irreversible denitrification." J. Geophys.
Res. 104.D11 (1999): 13,993-14002.
Environmental Protection Agency. Ozone Protection Regulations:
Substitutes for Ozone-Depleting Substances Washington: GPO, 2001.
EPA SunWise Ozone Layer. Environmental Protection Agency, Global
Programs Division. 2002. http://www.epa.gov/sunwise/ozonelayer.html
Fahey, D.W. et al. "Observations of denitrification and
dehydration in the winter polar stratospheres." Nature
344 (1990): 321-4.
Gary, B.L. "Observational results using the microwave temperature
profiler during the Airborne Antarctic Ozone Experiment." J.
Geophys. Res. 11 (1989) 223-32.
Goodman, J. et al. "New Evidence of size and composition
of polar stratospheric cloud particles." Geophys. Res. Lett.,
24.5 (1997) 615-18.
Koop, T., U.M. Biermann, W. Raber et al. "Do Stratospheric
Aerosol Droplets Freeze above the Ice Frost Point?" Geophys.
Res. Lett. 22.8 (1995) 917-20.
Salawitch, R.J., G.P. Gobbi, S.C. Wofsy, et al. "Denitrification
in the Antarctic stratosphere." Nature, 339 (1989): 525-7.
Tabazadeh, A. et al. "Quantifying Denitrification and
Its Effect on Ozone Recovery." Science, 288.5480 (2000)
1407-11.
Tolbert, M.A. and A.M Middlebrook. "FTIR studies of model polar
stratospheric cloud surfaces." J. Geophys. Res. 95.22
(1990) 423-31.
Wofsy, S.C., R.J. Salawitch, J.H.Yatteau et al. "Condensation
of HNO3 on Falling Ice Particles: Mechanism for Denitrification of
the Polar Stratosphere." Geophys. Res. Lett., 17.4 (1990)
449-52.
Journal
of Young Investigators. 2002. Volume Five.
Copyright © 2002 by Sadhna Vora and JYI. All rights reserved.
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