Colorado State University
General Circulation Model
Latitudinal Gradient of Atmospheric CO2 Due to Seasonal Exchange
with Land Biota.
A. Scott Denning*, Inez Y. Fung**, and David A. Randall*
NATURE, 376, 240-243.
*Department of Atmospheric Science, Colorado State University, Fort Collins, Colorado 80521, USA
**National Aeronautics and Space Administration, Goddard Space Flight Center, Institute for Space Studies,
2880 Broadway, New York, New York 10025, USA, and
School of Earth and Ocean Sciences, University of Victoria, Victoria BC V8W2Y2, Canada
The mixing ratio of atmospheric carbon dioxide (CO2) is increasing due to fossil
fuel combustion, but the rate of increase (about 3e12 kg/yr , GtC/yr) is only
about half of the rate of emissions (6 GtC/yr). A complete accounting of the
remaining 3 GtC/yr is not possible at this time. It is clear that some of the
global sink is in the oceans and some is in the terrestrial biosphere, but the
relative importance of each, as well as the geographic distribution of the sink
and the mechanisms involved are still a matter of debate. The observed record of
spatial and temporal variability of CO2 concentration at remote marine sites
around the world contains information that has been used in conjunction with
numerical models of atmospheric transport to deduce the location and nature of
the carbon sinks. One of the most important constraints on such estimates is the
observed gradient in CO2 concentration between the high latitudes of the
Northern and Southern Hemispheres. Simulation models of tracer transport suggest
that a significant north-south gradient is due to fossil fuel emissions, with
small contributions arising from natural carbon exchanges. Using a full
atmospheric general circulation model with a special representation of turbulent
mixing near the ground, we investigated the transport of CO2, and found that the
meridional gradient imposed by the seasonal terrestrial biota is nearly half as
strong as that imposed by fossil fuel emissions. Such a strong gradient implies
that the sinks of atmospheric CO2 in the Northern Hemisphere must be stronger
than previously suggested.
Annual mean mixing ratio of CO2 (ppmv) in the PBL as simulated by the
CSU GCM using surface fluxes representing the purely seasonal exchange with the
terrestrial biosphere as calculated in ref. 15 and used in ref. 4. The value at
the South Pole has been subtracted at every grid point. The concentration was
initialized to be globally uniform, and the model was run on a coarse 7.2 x 9
grid with 9 levels for 10 years. The end of this *spin up: run was then used as
the initial condition for a further 4 year integration on a 4 x 5 grid with 17
levels. All results presented here are for the final three years of the 4 x 5
run.
Annual mean mixing ratio (ppmv) of simulated CO2 (a) using the seasonal
biotic fluxes of ref. 4, and (b) using the fossil fuel emission estimates of
ref. 4. Values are annual means in the PBL at the grid cells containing the 21
flask sampling stations used in ref. 4. Where the grid cell was defined as land,
we chose the adjacent cell off-shore because flask sampling protocol selects
marine air only. Filled squares indicate values simulated by the CSU GCM, and
open circles indicate values simulated by the GISS tracer model. The curves are
cubic polynomials fit by least-squares to the station values (the solid curves
were fit to the GISS results and the dashed curves were fit to the CSU GCM
results). The value at the South Pole has been subtracted.
Seasonal variations of (a) prescribed surface flux of CO2 from the
terrestrial biosphere to the atmosphere, (b) simulated mass flux due to cumulus
convection at the top of the atmospheric PBL, and (c) simulated depth of the
atmospheric PBL. Values are area-weighted means for land points north of 28 N,
averaged for each calendar month.
Correlation coefficients of the relationship between prescribed monthly mean
terrestrial surface CO2 flux and (a) simulated cumulus mass flux at the top of
the PBL, and (b) simulated depth of the PBL. The correlation was calculated
separately at each land grid cell in the model, and the resulting values were
contoured to produce the maps in the figure. Note that the color scheme has been
reversed (reds indicate negative values and blues indicate positive values) for
easier comparison to Fig. 1.
A. Scott Denning
School of Environmental Science and Management
University of California - Santa Barbara
Santa Barbara, CA 93106-5131
(805)893-7363
denning@esm.ucsb.edu