Atmospheric CO
concentrations are increasing by about 1.5 ppm
every year. This 1.5 ppm increase integrated over the volume of
the atmosphere accounts for about 50% of the CO
released to
the atmosphere from fossil fuel burning and deforestation (henceforth
``anthropogenic'' CO
). The rest of the anthropogenic release
(the part that does not remain in the atmosphere) goes mainly into
the oceans and the terrestrial biosphere and soils. Knowing how
CO
is partitioned between oceanic and terrestrial CO
sinks is critical for making CO
forecasts into the future.
This paper provides a brief review concerning the oceanic uptake
of anthropogenic CO
. (A more detailed review is provided
by Siengenthaler and Sarmiento, 1993.)
Thermodynamic considerations suggest that a 1.5 ppm per year rise
in atmospheric CO
levels should lead to a CO
increase
in ocean surface water of about 1
mole/l. Until the late
1980s, dissolved inorganic carbon (DIC) measurements in seawater
could not resolve CO
differences less than 15-20
moles/l. Thus direct measurements of the anthropogenic
CO
increase were out of the question. Measurement
capabilities have now improved to the point where DIC measurements
can be made to an accuracy of 2-3
moles/l. Under the auspices
of the World Ocean Circulation Experiment (WOCE) and the Joint
Global Ocean Flux Study (JGOFS), ocean chemists are accumulating an
ocean-wide data set from which the ocean's current CO
distribution can be mapped. Unfortunately, it may still be
10 or 20 years before the ocean's CO
levels will be mapped
well enough a second time to document the CO
increase by difference.
In the meantime, our primary methods for estimating oceanic
CO
uptake will have to be based on models which help us
evaluate indirect or proxy constraints on CO
uptake. Before
1990, most modelling efforts employed simple box models which
attempted to predict the oceanic penetration using some kind of
upper ocean mixing parameterization. In these models, ocean mixing
rates were determined by adjusting or `tuning' mixing parameters
until the model could reproduce the transient penetration of
bomb-produced tracers like tritium (
H) and bomb
C.
If one assumes that the mixing coefficients appropriate for bomb
tracers are also appropriate for anthropogenic CO
, the tuned
model can be used to simulate the increase in oceanic CO
using
the observed atmospheric CO
time history as a boundary condition.
Recently, two attempts have been made to calculate anthropogenic
CO
uptake using ocean general circulation models (GCMs) in
which CO
uptake is driven by a fully resolved ocean
circulation field (Maier-Reimer and Hasselmann, 1987; Sarmiento et
al., 1992). The GCMs and the tracer-calibrated box models are in
basic agreement that the oceanic uptake of anthropogenic CO
during the 1980s was about 2 GtC/yr (2 x 10
g C per year).
This is about 30% of total anthropogenic emissions, or about 60%
of the portion attributed to the ocean/terrestrial sink.
It is important to point out that ocean models generally treat the
entry of anthropogenic CO
into the ocean as if it is a simple
perturbation of the ocean's natural carbon cycle. ``Anthropogenic
CO
'' is treated as a separate tracer from the background or
natural DIC in the ocean. Of course, anthropogenic CO
and
natural CO
are not separable. CO
only goes into the
ocean when the atmospheric partial pressure of CO
(pCO
)
exceeds the CO
partial pressure in the ocean. Maps of
pCO
, the pCO
difference between ocean and
atmosphere, document large CO
influxes and outfluxes which
were presumably in balance in pre-industrial times. The
anthropogenic perturbation skews the influx-outflux balance to
favor influx overall.
The oceanographic perspective on CO
uptake was dealt a big
blow at the outset of the 1991-1994 review period. Keeling et al.
(1989) and Tans et al. (1990) made estimates of the ocean's
CO
uptake by trying to fit the observed latitudinal variation
of atmospheric CO
concentrations using atmospheric transport
models. The atmospheric models in these exercises are given known
source distributions (anthropogenic CO
enters the atmosphere
mainly in the northern hemisphere) and different ocean CO
sink scenarios. The atmospheric models then predict latitudinal
CO
distributions for each source-sink scenario. These can
then be evaluated against the observed latitudinal distribution as
derived from the network of CO
sampling stations (Conway et
al., 1988).
During the 1980s, atmospheric CO
levels in the high latitudes
of the northern hemisphere were only 3 ppm higher than CO
levels in the high latitudes of the southern hemisphere. The
atmospheric transport calculations of Keeling et al. and Tans et
al. suggest that this gradient is too small to allow much transport
between the hemispheres. Thus the main sink for atmospheric
CO
would appear to be in the northern hemisphere.
According to Tans et al., the terrestrial biosphere and soils must
be the main CO
sink because the ocean sink in the northern
hemisphere is fairly small. Tans et al. conclude that there must
be a substantial net increase in carbon storage in northern
hemisphere terrestrial vegetation and soils every year. They
partition roughly 80% of the global ocean/terrestrial sink into
the terrestrial biosphere and soils, and give the oceans only about
20%. They estimate that the oceans are currently taking up only
0.3-0.8 GtC/yr.
Tans et al.'s increased terrestrial carbon storage in temperate
northern latitudes may be evidence for massive amounts of CO
fertilization, the direct stimulation of vegetative growth by
enhanced CO
concentrations in the atmosphere. In their
favored scenario, the annual carbon storage in northern terrestrial
biomass and soils exceeds carbon losses due to tropical
deforestation by about 1.0-1.5 GtC/yr. If the oceanic uptake is
larger, the level of CO
fertilization is still substantial,
but northern terrestrial carbon storage is reduced to a level which
more-or-less balances the release of CO
by tropical
deforestation.
The Tans et al. conclusion presents oceanographers with a major
problem. Given the huge area of ocean in the southern hemisphere,
the ocean's capacity to absorb CO
should be skewed toward the
south (Sarmiento et al., 1992). Bomb tracers are observed to
penetrate vertically throughout much of the ocean's upper kilometer
in both hemispheres. How could the southern hemisphere ocean be
such a small sink for anthropogenic CO
?
The problem here, in one important aspect, is mainly a problem of
definition. The atmosphere's north-south CO
gradient is
influenced by ocean-atmosphere CO
fluxes which include both
natural and anthropogenic components. The ocean models used to
estimate oceanic uptake of anthropogenic CO
explicitly ignore
the natural cycle. Natural fluxes of CO
between the ocean
and atmosphere can be quite large with respect to the anthropogenic
perturbation. The region between 5
N and 5
S in the
equatorial Pacific by itself outgasses
1 GtC/yr which must be
balanced by CO
uptake elsewhere.
Of particular interest here is the possibility that the ocean is
naturally transporting carbon across latitude circles or between
the hemispheres. Meridional transports within the ocean imply that
there are natural CO
fluxes between the ocean and atmosphere
which influence atmospheric CO
gradient. The ocean and land
also exchange carbon (via rivers). These aspects of the natural
cycle are not taken into account in the Tans et al. analysis. The
question then becomes: are there characteristics of the natural
carbon cycle which can reconcile
2 GtC/yr of ocean uptake
with a small interhemispheric transport in the atmosphere? The
answer, as will be reviewed below, would seem to be ``yes,'' although
our knowledge of the natural carbon cycle is still not adequate to
close the carbon budget completely.