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1 November 2007 Numerical Simulation of the Carbon Cycle Over The Tibetan Plateau, China
Guangzhou Fan, Tingjun Zhang, Jinjun Ji, Kerang Li, Jiyuan Liu
Author Affiliations +
Abstract

Significant interaction occurs between ecosystem physiological processes and climate. Studying this interaction is beneficial for understanding dynamics of climate change as well as forecasting future climate change. On the Qinghai-Xizang Plateau, the highest plateau in the world, interaction between ecosystem physiological processes and climate affect mid-levels of the atmosphere, so the study of this interaction has a special significance. We use two models, a carbon cycle model (CCM3) and a land surface model (LSM), to simulate ecosystem carbon cycle characteristics over the Tibetan Plateau and its influence on climate. The CO2 flux varies seasonally with ecosystem physiology processes on the Plateau: fluxes are highest in summer and lowest in winter. The seasonal variation of vegetation net CO2 flux shows that vegetation is an atmospheric carbon sink during most of the year, except in winter. This means that vegetation could weaken the greenhouse effect, which is important in terms of global warming. The land ecosystem is a weak carbon source from October to April, and it is a carbon sink from May to September (especially between June and August). The Tibetan Plateau CO2 fluxes vary spatially. The fluxes are highest over the southwest and southeast boundary areas and the northeast region of the Plateau in summer, and are lowest in the middle and northwest regions in winter. The interaction of CO2 flux and temperature shows that higher temperatures increase vegetation photosynthesis and all respiration. The abrupt increase in land ecosystem physiological processes with increasing temperature indicates that any warming due to increased atmospheric CO2 caused by human activity will be weakened by the land ecosystem over the Tibetan Plateau.

Introduction

Vegetation affects the Earth's hydrologic cycle, atmospheric circulation, the thermal characteristics of the Earth's surface, and heat exchange between the surface and the atmosphere. Vegetation interacts with rain and groundwater, affects surface winds and surface albedo, and absorbs and releases atmospheric gases. These interactions affect local, regional, and even global climate.

Vegetation is also significantly affected by climate change. Most historical studies of the interaction of the ecosystem and climate focus on the physical processes that plants are part of (Charney, 1975; Xue et al., 1990; Carlos et al., 1991; Fan et al., 1998; Claussen, et al., 1999). In one study of biogeophysical feedback, Fan et al. (1998) found that if northwestern China were deforested, the annual mean surface temperature would rise and the annual mean sea-level pressure would decrease in eastern and southern Asia. Precipitation would increase in China and the Indochina peninsula, and would decrease in the Indian peninsula. Ground surface heat sources in northwestern China would be clearly strengthened after the deforestation, which would weaken the winter monsoon and strengthen the summer monsoon in eastern and southern Asia. Fan et al. (1998) indicate that vegetation in temperate, arid, semiarid, and tropical rain forest areas affects physical processes differently.

Recently, the interaction between ecosystem physiological processes and climate change has been studied in more depth. For example, vegetation clearly plays an important role in the “greenhouse effect” of increased concentrations of atmospheric CO2 and this discovery is significant for understanding climate change (Kabat et al., 1998). By measuring and analyzing changes in the concentration of atmospheric oxygen and the 13C/12C ratio, we have gained a new understanding of current global carbon circulation. Studies have found that mid-latitude ecosystems are important carbon sinks, which can absorb about 2 Gt a−1 of human-generated CO2 (Zhang and Sun, 1999). Bonan (1991) used an ecosystem model to study the CO2 fluxes of 23 forests in Alaska and found that only one forest is a source of CO2; the other 22 were all CO2 sinks. Mora et al. (1996) discovered that during the last half of the Paleozoic, atmospheric CO2 concentration decreased about 10%, due to an increase in vegetation and the start of the Carboniferous glacier age, caused by climate change. Sellers et al. (1996) simulated the physiological response of vegetation when exposed to an increase in atmospheric CO2 and found that the CO2 increase could result in continental warming in addition to the conventional “greenhouse effect,” but this relationship was found to be inverse during the growing season. Shi and Guo (1997) indicated that the Earth's ecosystem has a dual action in the global carbon cycle. A halt of human activity would make the Earth a source of atmospheric CO2, but the response to the increased CO2 would be to initiate changes that would create a CO2 sink. Oechel et al. (2000) showed that the Alaskan tundra reverted to being a carbon sink during the last decade of the 20th century, with decreased carbon release. But during the 1980s, the tundra was a source of carbon. Cox et al. (2000) hypothesized that the Earth's land biosphere will be a carbon sink until 2050, and then become a carbon source. Hu et al. (2001) investigated the effects of elevated CO2 on grasslands and found that the carbon reserves of the soil increased about 11% after increased CO2, despite no clear increase in the net primary production. The increased CO2 concentrations reduced the microbial nitrogen in the soil, resulting in a net accumulation of carbon. Additionally, Schlesinger and Lichter (2001) and Oren et al. (2001) showed that soil and fallen leaves in North Carolina under the trees contain only small amounts of carbon, and this nutrient shortage affects the carbon reserving ability of the trees for the long-term.

These studies have shown that vegetation can effect regional or (and) global climate. Climate change can also clearly affect the distribution of vegetation and the ability of vegetation to absorb atmospheric CO2. Christensen et al. (1999) examined the carbon cycle and CH4 exchange in a vertical section of tundra in Eurasia, and found that the long-term carbon accumulation ratio (net absorption of atmospheric CO2) is influenced by climate parameters (such as the average temperature in July, and annual precipitation). With higher temperatures and/or greater precipitation, the carbon absorbing velocity was increased.

Fan and Cheng (2002) used a land surface model to simulate the interaction between the physiological processes of Tibetan Plateau vegetation and climate during the summer monsoon. They showed that the Plateau vegetation physiological processes are clearly affected by climate and the CO2 concentration of the atmosphere. Higher temperatures, greater soil moisture, and higher CO2 concentrations benefit photosynthesis and respiration. Vegetation absorbs CO2, weakening any warming due to the CO2 “greenhouse effect.” Fan and Cheng (2002) then created a simple conceptual model of the interaction between vegetation physiological processes and climate (Fig. 1). Vegetation increases when climate is warm and moist. Increased vegetation absorbs more CO2 reducing the CO2 concentration and weakening the greenhouse effect. This cools the climate, decreasing evaporation. This can then decrease atmospheric moisture and precipitation, which can create a cold, dry climate. The cold and the drought conditions decrease vegetation, which decreases CO2 absorption. The CO2 concentrations then cause climate warming. Evaporation is increased, along with atmospheric moisture precipitation. The climate then changes to warm and rainy climate, and the cycle is complete. This feedback can be called “biogeochemical feedback” as the “biogeophysical feedback” advanced by Charney (1975).

Figure 1.

A simple conceptual model of the interaction between vegetation physiology and climate (Fan and Cheng, 2002).

i1523-0430-39-4-723-f01.gif

There have been various studies on the interaction between land ecosystems and climate change, but each of these studies was in a different area, at different times, and used different methods. The Qinghai-Xizang Plateau (the highest plateau in the world) is located in this mid-latitude area. Its ecosystem influences climate change and directly affects the upper atmosphere. The modeling study of Fan and Cheng (2002) used a one-grid land surface model, and only modeled the summer monsoon. That study only simulated the interaction between the vegetation physiology processes and climate, and did not consider the influence of microorganism respiration. Therefore, it did not present the entire interaction between the ecosystem and climate over the Plateau. Researchers have also not studied the spatial and temporal distribution and variation of carbon cycle over the Tibetan Plateau. Our study used a land surface model (LSM mainly used to test the simulation ability of CCM3—Community Climate Model Version 3) and CCM3 to simulate the spatial and temporal distribution and variation of carbon circulation over the Tibetan Plateau and its possible influence on climate.

Models and Experiments

Lsm Model and Experiment Design

Lsm Introduction

The land surface model (LSM1.0) was developed by Bonan (1996). It is a one-dimensional model that includes dynamic ecosystem processes such as biophysical processes, hydrological processes, and biochemical processes. It can be used to model the exchanges of energy, momentum, moisture, and CO2 between the land and the atmosphere. The CO2 exchange in the model includes vegetation photosynthesis, vegetation respiration, and microorganism respiration. The CO2 absorbing rate of photosynthesis is related as (µmol s−1 m−2)

i1523-0430-39-4-723-e01.gif
where Cs is the CO2 concentration at the leaf surface (Pa), Ci is the internal leaf CO2 concentration (Pa), rs is leaf stomatal resistance (s m2 µmol−1), and patm is atmospheric pressure (Pa).

CO2 loss during plant respiration is broken into maintenance respiration and growth respiration. The maintenance respiration Rm (µmol s−1 m−2) is

i1523-0430-39-4-723-e02.gif
where L is the leaf area index (m2 m−2), Rf25 is the foliage respiration at 25°C (µmol s−1 m−2), Vsb is the stem biomass (kg m−2), Rs25 is the stem respiration at 25°C (µmol s−1 kg−1), Vrb is the root biomass (kg m−2), Rr25 is the root respiration at 25°C (µmol s−1 kg−1), Tv is the vegetation temperature (°C), and arm is a temperature sensitivity parameter. f(N) is the foliage nitrogen factor, and βt is the soil water factor. The growth respiration Rg (µmol s−1 m−2) is
i1523-0430-39-4-723-e03.gif
where Asun and Asha are the sunlit and shaded leaf photosynthesis, respectively, and Lsun and Lsha are the sunlit and shaded leaf area indices.

Microbial respiration Rs (µmol s−1 m−2) is

i1523-0430-39-4-723-e04.gif
where θ ¯ is the volumetric soil water content to a depth of 1 m , a1 is one-half field capacity, a2 is one-half saturation, Sc is soil carbon (kg m−2), a3 is the respiration rate (µmol CO2 kgC−1 s−1) at 10°C, a4 is a temperature sensitivity parameter, and Ts is the temperature (°C) of the first soil layer.

Lsm Input Data

The atmospheric boundary conditions required by the LSM include

  1. atmospheric reference height (zatm)

  2. pressure at zatm

  3. temperature at zatm

  4. zonal wind at zatm

  5. meridional wind at zatm

  6. specific humidity at wind at zatm

  7. surface pressure

  8. large-scale precipitation

  9. convective precipitation

  10. partial pressure CO2 at zatm (355 × 10−6 mol mol−1)

  11. partial pressure O2 at zatm (0.209 mol mol−1)

  12. incident direct beam solar radiation (<0.7 µm)

  13. incident direct beam solar radiation (≥0.7 µm)

  14. incident diffuse solar radiation (<0.7 µm)

  15. incident diffuse solar radiation (≥0.7 µm)

  16. incident longwave radiation.

The physical variables from (1) to (9) and (16) are given by the GAME (GEWEX Asia Monsoon Experiment)/Tibet experiment, which was a 3-mo enhanced observation from 16 June to 16 September 1998 over the Ando area (32°14′30″N, 91°37′30″E). Quality analysis and error information are given by Ishikawa et al. (1999).

The four radiation variables are calculated by experiential formula:

  • Incident direct beam solar radiation Fs,b = λd (1 − λb)Fsw

  • Incident diffuse solar radiation Fs,d = λdλbFsw

  • Incident direct beam solar radiation Fn,b = (1 − λd)(1 − λb)Fsw

  • Incident diffuse solar radiation Fn,b = (1 − λdbFsw

where

λb = β + (1 − β)Ct,

i1523-0430-39-4-723-e05.gif
i1523-0430-39-4-723-e06.gif

Fsw is the total shortwave radiation of the land surface, cosθ is the solar zenith angle, and Ct is cloud cover.

The land surface parameters of LSM1.0 include the longitude and latitude of the center of the grid cell, the surface type, the soil color type, etc. The longitude and latitude are used to calculate the solar zenith angle. The surface type is used to confirm the vegetation type and its fractional cover. The model includes 29 land surface types and 14 vegetation types. Every land surface type includes three vegetation types and the fractional cover. The soil color is used to confirm the drought and wet soil albedo. These parameters are presented by Bonan (1996).

Lsm Experiment Design

The LSM experiment uses the GAME/Tibet observed data and calculated radiation data in addition to measured land surface data. The experiment ran from 0000 h on 16 June to 2400 h on 16 September 1998, with a time interval of 5 min.

Because the temporal coverage of directly observed carbon cycle data is very short, the CCM3 simulated carbon cycle fluxes over the Tibetan Plateau cannot be tested with observed data. But the LSM experiment driven data are mainly the observed data discussed as in LSM Input Data (above). The modeling results might be quite reasonable, so the LSM results can be compared to the CCM3 results to test the CCM3 modeling energy.

Ccm3 Introduction and Experiment Design

CCM3 (Community Climate Model Version 3) was developed by the National Center for Atmospheric Research (NCAR). It has been well tested and is broadly used to simulate global atmospheric circulation, precipitation, and temperature. This study tested CCM3's simulation of the carbon cycle.

The vertical coordinate used in CCM3 is a hybrid sigma-pressure system that includes 18 levels. The horizontal coordinate used triangular truncation 42 waves (T42). The models spatial coverage is about 2.5° longitude by 2.5° latitude. The integral time step is 20 min. The terrain, land surface character, sea temperature, and land-sea distribution data are observed data. The model is coupled one time for every month. The land surface model coupled in CCM3 is LSM. The model is initialized on 15 April 1986 and ends on 28 February 1993 about seven integral years. The first 2 yr of data are released. Only the last 5 yr of data (from 1 March 1988 to 28 February 1993) are used for analysis. The experiment includes five growing seasons.

Ability of Ccm3 to Simulate the Carbon Cycle

Simulation of the Global Carbon Cycle

Bonan (1998) used CCM3/LSM1.0 to simulate the carbon cycle for the Tibetan Plateau region. The results showed that the model could simulate CO2 fluxes quite well. So in this paper, we will simply test the ability of CCM3 to simulate the carbon cycle.

Figure 2 shows a time/longitude cross-section of mean net CO2 flux (the vegetation photosynthesis absorption of CO2 minus the vegetation respiration release of CO2), simulated by CCM3/LSM1.0. Net CO2 flux is lowest at about 60°S and near the North Pole. This is because these areas are mainly composed of ocean. Photosynthesis and respiration are at their highest levels in the summer (from April to September) over the middle latitudes of the Northern Hemisphere (40°N to 65°N), and the net CO2 flux is correspondingly high. Thus, the mid-latitude vegetation ecosystem may be the most important atmospheric carbon sink in the global land ecosystem. It can weaken the global climate warming. Northern Hemisphere mid-latitude CO2 flux is negative during the winter (from December to January). The vegetation net CO2 flux at the equator area is greater than at other sites, except the northern mid-latitudes.

Figure 2.

Time/longitude cross-section of monthly grids mean net CO2 flux, simulated by CCM3. The abscissa is latitude, the ordinate is month. The units are µmol s−1 m−2.

i1523-0430-39-4-723-f02.gif

In the Southern Hemisphere, CO2 flux (including vegetation photosynthesis, vegetation respiration, vegetation net flux, microorganism respiration, and land ecosystem net flux) is highest in January. The land ecosystem net flux over most of the Southern Hemisphere is positive, with the largest fluxes over the tropical rain forest areas. The fluxes of the Northern Hemisphere are lower in January, especially in the area to the north of 30°N, where the land ecosystem net flux is negative during January. This means that the land ecosystem is a carbon sink. As the year progresses, the areas of highest flux gradually move north, reaching their northernmost position in July. At the same time, the fluxes in the Southern Hemisphere diminish, becoming negative over the entire Southern Hemisphere except for the area near the equator. In July, most areas of the Northern Hemisphere CO2 have positive fluxes. After July, the areas of highest CO2 flux gradually move south. These flux distribution characteristics generally agree with previous studies, confirming that CCM3 simulation of the land ecosystem carbon cycle is credible.

The mean annual vegetation photosynthesis over the global grids (ocean and land grids) is about 0.55 µmol s−1 m−2 and the mean annual respiration is about 0.32 µmol s−1 m−2. Thus the global mean absorbing net CO2 flux for surface plants is about 0.23 µmol s−1 m−2 every year. This shows that vegetation can absorb about 10 Gt of atmospheric CO2 every year, excluding microorganism respiration. The simulated microorganism respiration is about 0.17 µmol s−1 m−2. Therefore, taking into consideration the microorganism respiration, the land ecosystem can absorb about 2.6 Gt CO2 every year. This is approximately 30% higher than the CO2 amounts found by Zhang and Sun (1999), but they only measured carbon absorption in the middle latitudes of the Northern Hemisphere. The CCM3 simulation results presented here are consistent with the other study results.

Comparison Of Tibetan Plateau Carbon Cycle Fluxes of Lsm and Ccm3

As previously asserted, the reliability of using CCM3 to simulate the carbon cycle over the Tibetan Plateau cannot be tested because of the lack of observational data. Therefore, we used LSM and the GAME/Tibet data and compared them to the CCM3 results to test the reliability of CCM3. The results of the LSM experiment may be more reliable because it is driven by the observed data. Because the simulation period of LSM is from 16 June to 16 September 1998, and the simulated area is one point (Ando area), only the July and August results from the area nearest to Ando can be compared. The Ando land surface type is cool grassland. It means that the vegetation type include cool grass (plant cover is about 60%), warm grass (plant cover is about 20%) and bare (plant cover is about 20%).

Table 1 shows the comparison of the LSM and CCM3 simulations of CO2 fluxes over the Ando area in July and August. The simulated fluxes from each model show little deviation from one another. The greatest variation is in vegetation respiration in August, with an error of about 33.3%. We conclude that the CCM3 simulated CO2 fluxes over the Tibetan Plateau are credible, and that CCM3 could be used to simulate the land ecosystem physiological carbon cycle over the Tibetan Plateau and its influence on climate.

Table 1

LSM and CCM3 simulations of CO2 fluxes near Ando (units are μmol s−1 m−2).

i1523-0430-39-4-723-t01.gif

Characteristics of the Land Ecosystem Carbon Cycle over the Tibetan Plateau

Seasonal Characteristics of the Carbon Cycle

This study only analyzed the seasonal variation of CCM3-simulated land ecosystem carbon fluxes over the Tibetan Plateau (those areas higher than 3000 m).

Vegetation photosynthesis, vegetation respiration, and vegetation net CO2 flux are highest in summer (from June to August), with maximum values of 2.72 µmol s−1 m−2, 1.17 µmol s−1 m−2, and 1.57 µmol s−1 m−2, respectively (Fig. 3). These maximums are the 75.6%, 67.8%, and 83.7% of their respective annual means. In winter (December to February), vegetation photosynthesis and vegetation respiration are only 0.03 µmol s−1 m−2 and 0.05 µmol s−1 m−2, respectively, and vegetation net CO2 flux becomes negative (about −0.02 µmol s−1 m−2). Therefore, the vegetation system over the Tibetan Plateau is an atmospheric carbon source in winter.

Figure 3.

CCM3-simulated seasonal variation of CO2 fluxes over the Tibetan Plateau. (a) Vegetation photosynthesis. (b) Vegetation respiration. (c) Vegetation net CO2 flux. (d) Microorganism respiration. (e) Land ecosystem net CO2 flux. All plots have units of in μmol s−1 m−2. Positive photosynthesis values indicate a flux from the atmosphere to vegetation. Positive respiration values indicate a flux to the atmosphere from vegetation. Positive net fluxes indicate a flux to the atmosphere.

i1523-0430-39-4-723-f03.gif

During the spring (March to May), vegetation photosynthesis, vegetation respiration, and vegetation net CO2 flux are 0.43 µmol s−1 m−2, 0.27 µmol s−1 m−2, and 0.17 µmol s−1 m−2, respectively. In autumn (September to November), these parameters are 0.42 µmol s−1 m−2, 0.26 µmol s−1 m−2, and 0.16 µmol s−1 m−2. The spring values are 12%, 15.6%, and 9% of their annual mean values, and the autumn values are 11.7%, 15%, and 8% of the annual means. The carbon sink effect from vegetation is greatest in summer over the Tibetan Plateau, with a milder effect in spring and autumn.

The microorganism respiration over the Tibetan Plateau is highest in summer and lowest in winter, but it has less seasonal variation than vegetation photosynthesis and respiration (Fig. 3). The CCM3-simulated microorganism respiration was 0.23 µmol s−1 m−2 (39.5% of the annual mean) in summer, 0.07 µmol s−1 m−2 (11.6% of the annual mean) in winter, 0.15 µmol s−1 m−2 (25.6% of the annual mean) in spring, and 0.14 µmol s−1 m−2 (24.4% of the annual mean) in autumn.

The land ecosystem net flux is negative from October to April, during which the land ecosystem releases CO2 to the atmosphere as a weak carbon source (Fig. 3). From May to September, the land ecosystem becomes an atmospheric carbon sink, with the greatest carbon sink effect occurring between June and August (1.35 µmol s−1 m−2).

Temporal/spatial Characteristics of the Carbon Cycle

Using the 5-yr averaged monthly mean data, we study the temporal/spatial characteristics of the carbon cycle for the Tibetan Plateau (Fig. 4).

Figure 4.

Spatial distribution of annual mean CO2 fluxes over the Tibetan Plateau. (a) Vegetation photosynthesis. (b) Vegetation respiration. (c) Vegetation net CO2 flux. (d) Microorganism respiration. (e) Land ecosystem net CO2 flux. All plots show fluxes contoured in units of μmol s−1 m−2.

i1523-0430-39-4-723-f401.gif

Figure 4.

Continued.

i1523-0430-39-4-723-f402.gif

Vegetation photosynthesis displays notable spatial variation over the Tibetan Plateau (Fig. 4a) as well as temporal variation. Vegetation photosynthesis is about 0 µmol s−1 m−2 in January over most areas of the Tibetan Plateau (not shown), but is slightly above zero over the southeast boundary area. After January, photosynthesis over the Plateau gradually increases, especially in the east and the northeast, remaining at zero only in the west and northwest before April. Thereafter, photosynthesis increases over the entire Plateau until July. Photosynthesis along the southwest boundary, the east boundary and in northeast areas are highest, with values of 10 µmol s−1 m−2, 6 µmol s−1 m−2, and 5 µmol s−1 m−2, respectively. After July, photosynthesis gradually weakens, with reduced center values and ranges, until it again is zero in November in most areas. Spatial variation of photosynthesis is greatest on the south boundary of the Plateau due to the variability in vegetation over the terrain.

The temporal/spatial variation of vegetation respiration over the Tibetan Plateau is similar to the variation of photosynthesis (Fig. 4b). In January, vegetation respiration is greatest in the southern and eastern boundary areas, with low respiration in all other areas (not shown). Vegetation respiration gradually increases between January and July, with mean values of 4 µmol s−1 m−2, 3 µmol s−1 m−2, and 2 µmol s−1 m−2 at the southwest boundary, southeast boundary, and in the northeast, respectively. The difference between respiration and photosynthesis is that respiration increases earlier than photosynthesis in the spring.

The vegetation net CO2 flux (Fig. 4c) is equal to vegetation photosynthesis minus vegetation respiration. During January and February, the vegetation net flux is negative over most of the Tibetan Plateau, except its southeast boundary (more photosynthesis than respiration) (not shown). Thus, the vegetation system is a carbon source. From February to March, the vegetation net CO2 flux becomes positive over the southwest, south, southeast, and east boundaries, and over a part of the northeast Plateau. These areas then become a carbon sink. Net CO2 flux continues to increase and spread until July, when the net flux is positive across most of the Plateau except in a small northwest area. After July, the vegetation net CO2 flux decreases and contracts from the western and central areas, and the vegetation becomes a carbon source until November, except in the southwest boundary area of the Plateau.

The soil microorganism respiration varies spatially across the Tibetan Plateau (Fig. 4d), as well as temporally (not shown). Microorganism respiration gradually increases from January to July and then gradually decreases, similar to the temporal variation of vegetation respiration. Spatially, the distribution of annual mean microorganism respiration is similar to that of the vegetation CO2 fluxes (Fig. 4d). Microorganism respiration is highest in the southwest, along the southern boundary, and in the northeast of the Plateau.

Figure 4e shows that most areas of the Tibetan Plateau are carbon sinks, except for a small area in the northwest Plateau. During January and February, the land ecosystem net CO2 flux (equal to the vegetation net CO2 flux minus microorganism respiration) is negative across the Tibetan Plateau (photosynthesis is less than respiration). Thus, the land ecosystem is a carbon source to the atmosphere. Between March and May, the net CO2 flux becomes positive in the southwest, south, and eastern boundary areas are carbon sinks. Net CO2 flux is highest in July, across the Plateau. After September, CO2 flux decreases, and the carbon sink effect of the land ecosystem gradually weakens. By October, most areas of the Plateau become a carbon source, except the southwest, south, and eastern boundary areas, and a small area in the northeast. Net CO2 fluxes in November and December are similar to those of January.

Co2 Flux Changes with Temperature

Some preliminary simulations with CCM3/LSM0.0 showed that simple physiological and ecological assumptions can result in reasonable simulation of land-atmosphere CO2 exchange, as compared to observed estimates of annual net primary production and annual microbial respiration (Bonan, 1995). In this paper, we used CCM3/LSM1.0 to study the CO2-temperature relationship.

There is a definite intra-annual temporal and spatial distribution of CO2 fluxes over the Tibetan Plateau, caused by seasonal changes. These seasonal changes are caused by solar radiation and accompanying temperature variations. Analyzing the relationship between temperature change and land ecosystem CO2 flux will aid in the understanding of the interactions between the ecosystem carbon cycle and climate. Our CCM3 simulation spanned 60 mo (about five growing seasons), giving us 60 monthly mean temperatures over the Tibetan Plateau. Figure 5 shows CO2 flux variations with temperature.

Figure 5.

Monthly mean CO2 flux and temperature. (a) Vegetation photosynthesis. (b) Vegetation respiration. (c) Vegetation net CO2 flux. (d) Microorganism respiration. (e) Land ecosystem net CO2 flux. All fluxes are in μmol s−1 m−2, and temperatures are in °C. Smooth curves show 6th order polynomial fits.

i1523-0430-39-4-723-f05.gif

Vegetation photosynthesis increases with increasing temperature (Fig. 5a). There are three abrupt change periods. At low temperatures, photosynthesis over the Tibetan Plateau is low (about 0 µmol s−1 m−2), but an abrupt change happens when the temperature reaches about 4°C and photosynthesis rises to 0.9 µmol s−1 m−2. The second abrupt change occurs at about 7.3°C when photosynthesis increases to about 2.25 µmol s−1 m−2. The third change occurs when the temperature reaches about 9.7°C and photosynthesis is 3.5 µmol s−1 m−2.

Vegetation respiration changes with temperature, in a manner similar to that of the photosynthesis change (Fig. 5b). As temperature rises, vegetation respiration increases nonlinearly, with three abrupt changes when the temperature is about 4°C, 7.3°C, and 9.7°C.

Vegetation net CO2 flux is less than 0 when the temperature is lower than −8°C (Fig. 5c), and the vegetation is thus a carbon source. With rising temperatures, the vegetation net CO2 flux increases nonlinearly, with three abrupt changes occurring when the temperature is 4°C, 7.3°C, and 9.7°C. Vegetation thus absorbs more atmospheric CO2 over the Tibetan Plateau with rising temperatures, and the vegetation physiological processes could weaken the greenhouse effect caused by human activity on the Plateau.

Microorganism respiration increases in a quasi-linear fashion with increasing temperatures (Fig. 5d). Land ecosystem net CO2 flux is less than 0 when the temperature is lower than 4°C (Fig. 5e), and the land ecosystem is thus a carbon source. With rising temperatures, the vegetation net CO2 flux increases nonlinearly, with three abrupt changes occurring when the temperature is 4°C, 7.3°C, and 9.7°C.

Because the land ecosystem net CO2 flux increases with rising temperature, the ability of the land ecosystem to absorb atmospheric CO2 over the Tibetan Plateau also increases with temperature, which means that the land ecosystem could weaken the greenhouse effect caused by human activity on the Plateau.

The flux jumps at discrete temperatures may be an important result, but the reasons are not included in the simulation. An improved study on the vegetation physiological process is needed.

Discussion and Conclusions

This study used CCM3 to simulate the ecosystem carbon cycle over the Tibetan Plateau, and its interaction with the climate. The results show that CO2 flux varies seasonally with the ecosystem physiology processes on the Plateau. The CO2 fluxes are highest in summer and lowest in winter. The seasonal variation of vegetation net CO2 flux shows that vegetation is an atmospheric carbon sink during most of the year, except in winter. This means that the vegetation could weaken the greenhouse effect, which is important in terms of global warming. The land ecosystem net CO2 flux shows that the land ecosystem is a weak carbon source from October to April, and is a carbon sink from May to September (especially between June and August).

The Tibetan Plateau CO2 fluxes vary spatially. The fluxes are highest over the southwest and southeast boundary areas and the northeast region of the Plateau in summer, and are lowest in the middle and northwest regions in winter.

The interaction of CO2 flux and temperature shows that higher temperatures increase vegetation photosynthesis, vegetation respiration, and microorganism respiration. The abrupt increase in the land ecosystem physiological processes with increasing temperature indicates that any greenhouse effect due to increased atmospheric CO2 caused by human activity will be weakened by the land ecosystem over the Tibetan Plateau. Thus the ecosystem over the Tibetan Plateau has the ability to adjust or moderate the greenhouse effect.

This study was conducted using two simple numerical experiments, and the results were not tested with observed data. This is a shortcoming. In addition, the models used in this study have some restrictions. For example, the ecosystem parameters are set and cannot be changed with climate, and the model's atmospheric CO2 concentration is also set and cannot be changed with ecosystem physiological processes. These shortcomings, and the short simulation runtime, will be addressed in future studies.

Acknowledgments

This work was supported by: (1) Program of National Natural Science Foundation (40675037), (2) The Key Program of SiChuan Province Youth Science and Technology Fund (05ZQ026-023), and (3) Opening Project of Chengdu Institute of Plateau Meteorology (IPM).

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Guangzhou Fan, Tingjun Zhang, Jinjun Ji, Kerang Li, and Jiyuan Liu "Numerical Simulation of the Carbon Cycle Over The Tibetan Plateau, China," Arctic, Antarctic, and Alpine Research 39(4), 723-731, (1 November 2007). https://doi.org/10.1657/1523-0430(07-502)[FAN]2.0.CO;2
Accepted: 1 June 2007; Published: 1 November 2007
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