SCOPE 13 - The Global Carbon Cycle

12

Carbon in the Freshwater Cycle 

S. KEMPE
 
ABSTRACT
12.1 INTRODUCTION
12.2 THE WATER CYCLE
12.3 CARBON IN PRECIPITATION
12.4 VOLCANIC CO2
12.5 SOIL AIR
12.6 TYPES OF RUNOFF
12.7 GROUNDWATER IN KARST ROCKS
12.8 DEEP GROUNDWATER
12.9 RIVERS
12.10 REVISION OF LIVINGSTONE'S (1963) RIVER LOADS
12.11 POSSIBLE SINKS OF CARBON IN THE FRESHWATER CYCLE 
REFERENCES

ABSTRACT

Annually 1.08 x 1020 g of water precipitates on to the continents, of which 0.376 x 1020 g runs off in rivers. This water is the motor of erosion and terrigenous biological activity alike. The amount of CO2 in rain is small (0.065 x 1015 g C/year) compared with the amount which enters the-water in the soil (net flux reaching the oceans: 0.23 x 1015 g C/year). Some 0.8 % of all CO2 produced by root respiration and microbial activity reaches the ocean by water transport. The gross flux from soil to groundwater, however, is larger, because much of the CO2 is given off when groundwater reappears in springs. CO2 pressures are 100 times larger in soil air, and 10 times larger in shallow groundwater and in rivers, than in the atmosphere. Both ground and river waters show pronounced seasonal variability of CO2 pressure and alkalinity. An estimated 20% of carbonate rocks occurs in the crust, but only 4% of the continental area shows karst features. These areas play a distinct role in the carbonate dissolution rate; Europe, the continent with the highest karst percentage, has the largest carbonate concentrations in its rivers.

12.1 INTRODUCTION

The continental fresh waters contain the most diversified carbon pool on earth. Not only does fresh water act as a storage for various inorganic and organic compounds, but it is also a chief transport medium between some of the sizewise more important carbon storages in the biota, lithosphere, and oceans. Furthermore, water is a necessary reaction partner of carbon dioxide, both in the carbonate system and in the biological formation of organic matter. To carry out photosynthesis, land biota is totally dependent on the availability of water (see Chapter 8, this volume, Figure 8.2).

This chapter provides an introduction to the global water cycle, and a discussion of the different water compartments and their respective carbon contents.

12.2 THE WATER CYCLE

Fresh water is available as precipitation (rain, snow, or dew), ice, rivers, lakes, and ground water. The best values of the global water cycle currently available have been calculated by Baumgartner and Reichel (1975). Figure 12.1 illustrates the global water cycle: annually 4.25 x 1020 g of water evaporates from the oceans; this is equivalent to a water layer, 117.8 cm thick, spread over the total ocean surface. A total of 0.397 x 1020 g is transferred from the oceans to the continents (11 cm). The continents receive a precipitation of 1.081 x 1020 g annually, equivalent to a layer of 74.6 cm covering the total land area. Of this amount, two-thirds re-evaporate and one-third returns in rivers and glaciers to the sea. The global ratio between evaporation and runoff is 0.357.

 Figure 12.1 The global water cycle (drawn after data by Baumgartner and Reichel, 1975). P = precipitation, E = evaporation, r.t. = residence time

Table 12.1a lists some estimates of the sizes of various water reservoirs. It must be noted that there is no accepted value for the total volume of rivers and lakes available; estimates deviate by as much as a factor of 10. But it is this relatively tiny fraction of water which man most urgently needs, and which he most criminally misuses. Even less information is available for groundwater volumes. Estimates depend on assumptions of mean porosity, mean sediment depth, and mean depth of groundwater table.

Table 12.1b compiles the data for continental runoff and its carbon load. The most recent attempt to make a global calculation of the amount of river loads was made by Livingstone (1963). In Section 12.10 some corrections are made to the Livingstone calculations: these corrections include updated values for river discharge. Corrections on mean dissolved matter concentrations of the major rivers also seem to be necessary. For many rivers, long-term weighted means are available today, while Livingstone used only data from random sampling.

As rivers provide the bulk transportation from land to ocean (Table 12.2), their average loads are of primary interest for the carbon cycle. The second largest discharge rate of eroded material is due to glaciers, while minor amounts are transported by ground water, atmospheric dust, volcanic events, and shore erosion.

Table 12.1a Water volumes of the earth in solid, liquid, and gaseous forms. (Table 1, Baumgartner and Reichel, 1975. Reproduced by permission of the R. Oldenbourg-Verlag GmbH, München)


1015 g

%

Oceans
1 348000 000

97.39

Polar ice caps, icebergs, glaciers

27 820 000

2.01

Groundwater, soil moisture

8062000

0.58

Lakes and rivers

225 000

0.02

Atmosphere

13 000

0.001

Total
1 384 120 000

100.00

Fresh water

36 020 000

= 2.60

Fresh water as a percentage of total
Polar ice caps, icebergs, glaciers

77.23

Ground water to 800 m depth

9.86

Ground water from 800 to 4000 m depth

12.35

Soil moisture

0.17

Lakes (fresh water)

0.35

Rivers

0.003

Hydrated earth minerals

0.001

Plants, animals, humans

0.04

Total

100.00


Various estimates of masses of the hydrosphere (Units in 1015 g H2O)
 
Lvovich Flohn Garrels et al. %
(1970) (1973) (1975)

Oceans 1 370 000 000 1 370 000 000 1 370 000 000 80
Pore water in 60 000 000 320 000 000 18.8
rocks
Soil water 21 000
Groundwater 4 00 0000
(750 m)
Ice  24 400 000 27 000 000 16 500 000 1.2
Lakes and rivers 231 000 116 000 34 000 0.002
Atmosphere  12 400 10 500 0.0006

12.3 CARBON IN PRECIPITATION

The freshwater cycle starts with 1020 g of water falling annually as precipation on the continents (Fig. 12.1). The precipitation should chemically assume equilibrium with the atmosphere.

Table 12.1b Annual river discharge and carbon content


Livingstone (1963) (see Section 12.10)
Baumgartner and
Reichel (1975)

Discharge
Salinity  HCO3
C
Discharge
Continent
1015 g H2O
 ppm
ppm
ppm    1015 g H2 O

Europe
2 498.5
182
95
18.7
2 800
Asia
11 108.5
142
79
15.5
12 200
N. America
4 557.3
142
68
13.3
5 900
S. America
8008.4
69
31
6.1
11 100
Africa
5 901.3
121
43
8.5
3 400
Australia
316.3
59
31.6
6.2
2 400
(Antarctica as ice
2000)
Recalculated sums and
32 390.1
122.4
59.8
11.8
37 700
weighted means
Dissolved Organic Carbon (DOC):
3.28
(Garrels et al., 1975)
Particulate Organic Carbon (POC):
1.76
Discharge of carbon (in 1015 g/year) as
HCO3
DOC
POC
from Livingstone:
0.382
Baumgartner and Reichel:
0.445
0.123
0.066
Including new data from Amazon River:
0.454

With an atmospheric CO2 pressure (PCO2) of 0.0003 parts CO2 in 1 part of air, we can, according to Henry's law, expect the CO2 content of rainwater to be between I ppm at 0 °C and 0.5 ppm at 20 °C. Because continents and precipitation are unevenly distributed over the climatic zones of the globe (Figure 12.2 a, b), it is difficult to assess a global mean precipitation temperature. At 15 °C (0.6 ppm CO2), the annual flux with precipitation to the continent surface should amount to

0.6 x 10-6 CO2 x 1.08 x 1020 g H2 O = 0.065 x 1015 g CO2 (0.018 x 1015 g C/year or 0.0014 x 1015 moles CO2 )

Part of the CO2 is instantaneously lost again into the atmosphere, when the precipitation evaporates from rocks, soil, or vegetation. In this context, the ratio between physical evaporation and biological evapotranspiration should be of interest.

In the more densely populated humic zones of the earth, industrial fossil-fuel burning increases the CO2 content of air locally and rain may contain larger CO2 concentrations as compared with the global average.

Actual measurements of CO2 in rainwater (Table 12.3) show, in fact, a much larger content than expected from the equilibrium argument. The real flux of CO2 from atmosphere to land with precipitation may, therefore, be several times larger than previously anticipated. No global data are available on rain concentrations of organic carbon.

Table 12.2 Agents of material transport to oceans (After Garrels et al., 1975, Table 10. Reproduced by permission from Chemical Cycles and the Global Environment, by Garrels, Mackenzie and Hunt. Copyright © 1975 by William Kaufman, Inc., Los Altos, California. All rights reserved)


% of total 
Agent transport Remarks

Streams  89 Present dissolved load 17%, suspended 72%;
during geologic past more nearly equal.
 
Groundwater  2 Estimate poor, dissolved materials like those
of streams. Major area of ignorance with 
respect to possible contamination.
 
Dust  0 .2 Dust to ocean related to deserts and wind
patterns. Sahara major source for tropical
Atlantic. Composition similar to average
sedimentary rock; many dusts have high
(30%) organic content.
 
Shore erosion  1 Silts, muds, and sands eroded from shore-
lines by waves, tides, and currents. Composition
 like suspended load of streams.
Ice 7 Ground-up rock debris as well as material up
to sizes of boulders. Chiefly from Antarctica
and Greenland. Distributed in northern and
southern seas by icebergs. Composition
similar to average sediments.
Volcanic 0 .3 (?) Lavas and gases transported from earth's
interior. Amounts and compositions of
gases poorly known, but include CO2, CH4,
H2S, SO2, NH3, H2. Dusts from explosive
volcanoes may be important in climatic
control. No one knows how much material
from volcanoes is new to exogenic cycle.

CO2 in rain alone cannot account for the HCO3 found in rivers. According to 

H2O + CO2 + CaCO3 Ca(HCO3)2 Ca 2+ + 2HCO3

at least half of the stream HCO3 must originally be derived from the atmosphere, i.e. 0.23 x 1015  g C (Table 12.1b).

Figure 12.2 (a) Areas of oceans and continents versus latitude in 5° intervals. (b) Precipitation, evaporation, and runoff from continents versus latitude in 5 ° intervals (drawn after data by Baumgartner and Reichel, 1975)

Table 12.3 CO2 content of precipitation (Miotke 1968. Reproduced by permission of the author)


1. Rainwater
Mg CO2 /1
McLeod (1869)
2.7
Frankland (1874)
2.5
Baumert (1877) in Paul, B. H.
0.7
Peligot (1877) in Paul, B. H.
1.0
H. Lehmann (1956) Cuba
2.53.5
Bögli (1961) Switzerland
2.22.6
Miotke (1965) Picos, Spain
2.2
 
2. Meltwater from snow
Bögli (1951) fresh meltwater
0.851.76
Bögli (1961) from vegetated soil
2.643.63
Miotke (1965) Picos, fresh meltwater
0.4

12.4 VOLCANIC CO2

Whether or not volcanic CO2 or CO2 from hydrothermal sources play a quantitatively important role is not yet known. Recycled CO2, emitted by volcanic vents or moffettes, directly adds to the atmophere. The estimates of this process differ widely. In certain areas, however, there exists a diffuse CO2 flow through the crust. These areas are marked by rivers and lakes which carry more bicarbonate than alkaline earth metals. Soda lakes have developed by this process in Ethiopia, Kenya, Tanzania, and in Eastern Turkey (Lake Van; Kempe, 1977). Crater lakes often have sub-lacustrine CO2 sources, adding volcanic carbon (e.g. Laacher See, Federal Republic of Germany; Lake Kivu, East Africa).

12.5 SOIL AIR

Additional atmospheric CO2 dissolves in rainwater, only if rain comes into direct contact with alkaline earth metal carbonate rocks. Rain running down bare limestone creates karren by gradual dissolution of CaCO3 and slow uptake of atmospheric CO2 Bögli, 1975). The final carbonate concentration, however, which these runoff films reach, is far below that of ground or river water.

The major part of CO2 responsible for weathering of carbonates and silicates (see Chapter 13, this volume) enters precipitation water when it percolates through soil. Due to the immense total surface of soil particles, soil water is in equilibrium with soil air. At this point a substantial amount of CO2 enters the freshwater cycle.

In soils, bacterial oxidation decomposes the photosynthetically produced organic matter to CO2. Root respiration is an equally important source of CO2 in soil. CO2 is generated in the. upper few metres of soil, and diffuses upward to the atmosphere and downwards to groundwater. Concentrations and diffusion rates vary with seasons, climate, type of soil, and type of'vegetation cover. CO2 partial pressures (PCO2) of up to 0.2 have been measured in soils, and an average PCO2 of 0.03 is often quoted (Miotke, 1974). To monitor CO2 emission from soils, two methods have been followed: (i) the CO.2 increase in a plastic dome covering the soil surface is measured, and (ii) the apparent diffusion constants of the respective soil profile is determined in the laboratory, together with CO2 profiles under regular field conditions. Albertsen (1977) has obtained annual averages of CO2 emissions by this second method for four sites with different vegetation types in Northern Germany: coniferous forest 31 g C/m2 year; deciduous forest 86 g C/m2 year; forest clearing 196 g C/m2 year; and agricultural land 404 g C/m2 year. The bulk CO2 emission is directed towards the atmosphere; only in spring and early autumn was a concentration gradient towards the groundwater noticed.

The total CO2 content of soil air may be estimated by assuming an average groundwater table depth of 6 m (Garrels et al., 1975), an average PCO2 of 0.003 (which is certainly on the low side), an average gas effective porosity of 0.2, and a vegetation-covered total continental area of 100 x 106 km2 (see Chapter 5, this volume, Table 5.2, total continental area minus deserts, semideserts and ice). This calculation yields 36 x 109 m3 of CO2 of 9.7 x 1012 g C. As the annual net primary productivity amounts to about 60 x 1015 g C/year (Chapter 5, this volume), the residence time of CO2 in soil is approximately one hour. This result is obtained on the assumption that the total primary production is degraded in the soil. This is obviously not the case, as a residence time of one hour is in contradiction with the slow diffusion rate through soil. Therefore, large quantities of litter must degrade under direct contact with the free atmosphere.

The annual net flux of CO2 from soil to groundwater must at least equal the difference between half the HCO3 load of the streams and the CO2 in rain: 0.23 x 1015 g C 0.018 x 1015 g C = 0.21 x 1015 g C. Garrels et al. (1975) assume that this amount of CO2 used in the weathering of rocks is derived directly from the atmosphere. As discussed above, this does not seem to be the case. The CO2 in the process of weathering is derived from 26.5 x 1015 g C of CO2 in the model by Garrels et al. (1975) produced by respiration and decay, which then diminishes to about 26.3 x 1015 g C returning directly to the atmosphere. Consequently the flux of CO2 used in weathering from the atmosphere to land also diminishes.

The fractionation of degradation CO2 between atmosphere and groundwater is 122/1; 0.77% of the CO2 produced by degradation of terrestrial organic matter is transferred to groundwater.

With respect to the interaction of water and soil, one other aspect should be noted. If, indeed, most of the CO2 in groundwater is soil-derived, then this CO2 must be much older than that furnished by rain. The turnover of humus lapses over a long period, often several hundred years. Reiners (1973) has presented a good review of detritus sizes and turnover masses. Sinter chronology by 14C is limited by the inability to define the time of humus turnover. Double analyses of wood and its sinter cover show the flowstone cover to be much older than the wood, even after adjusting for the dead CO2 derived from the country rock of the cave roof. It should be possible, by this method, to estimate the fractionation of soil CO2 between percolated water and air.

12.6 TYPES OF RUNOFF

Three types of runoff have to be discerned: overland flow, interflow, and subsurface runoff by groundwater.

Surface runoff is mostly low in dissolved matter, but carries almost all of the suspended particles of the runoff. At times of maximal runoff, the concentration of dissolved substance decreases while suspended load increases.

Interflow occurs through the very upper part of the soil cover, through cracks in the soil, and small surface voids. Interflow behaves hydrologically much like surface runoff, but has geochemical similarities to groundwater.

Groundwater passes totally through the soil and can be clearly discerned geochemically from surface runoff. Its discharge peak after thunderstorms is much delayed or cannot be identified at all. Hydrologists have developed several methods to divide river stage curves into surface and groundwater runoff. These methods, however, are not widely used, and global estimates on the ratio of surface to groundwater discharge have not, as yet, become available.

Three types of groundwater aquifers can be discerned: cleft, porous, and conduit aquifers. The first two have diffuse flow patterns and occur in igneous rocks and shales (cleft), and in sandstones and unconsolidated alluvial rocks (porous). Conduit flow occurs mostly within carbonate karst rocks. Some 80% of the continental surface is covered by sediments, of which 60% are shales, 20% carbonate rocks, 15% sandstones, and 5% evaporite deposits. The average composition of the sediment cover is slightly different, with 65% shale and 15% carbonates (Garrels and Mackenzie, 1971; Garrels et al., 1975).

12.7 GROUNDWATER IN KARST ROCKS

The area governed by conduit flow is probably less than 20% of the continental surface, as many calcareous sandstones and shales do not develop conduits. Northern Germany, for example, is underlain by calcareous glacial till, and rivers show high alkalinity and alkaline earth contents similar to karst areas, though hydrologically and morphologically no criteria of karst have been developed.

Balázs (1977a) estimated the total area with morphological karst features to be 4% of the continents (Table 12.4). The bulk of the karst occurs in Europe and Asia between 60° N and 20° N latitude, with smaller areas in North America and even less in the southern hemisphere (Figure 12.3). Carbonates occur either in the orogenic belts, or as epicontinental sediments deposited from shallow seas. These areas can form vast karst plateaus once they are uplifted, as in the case of Southern China where the largest single karst area exists. The most pronounced karstification occurs where limestone and humid climate coincide. Figure 12.4 is a map which shows the main areas of karst: the AppalachianCaribbean, the European, the South-East Asian and Pacific Karst Provinces (Balázs, 1977b).

Table 12.4 Distribution of karst areas (Balázs, 1977a. Reproduced by permission of the 7th International Speleological Congress and by permission of the author)


Area of Area of karst/1000 km2 Percentage of karst/
continent continent =100%
Continent 106 km2 orogenic epeirogenic Total orogenic epeirogenic Total

Europe
10.5
528
890
1418
5.0
8.5
13.5
Asia
43.9
808
793
1601
1.8
1.8
3.6
Africa
30.3
67
923
990
0.2
3.0
3.2
North and Central 24.2
760
100
860
3.1
0.4
3.5
America
South America
17.9
90
90
0.5
0.5
Australia and the
8.5
132
250
382
1.6
2.9
4.5
Pacific
Total without
135.3
2385
2956
5341
1.8
2.2
4.0
Antarctica

Figure 12.3 Karst areas in comparison to orogen and platform areas in western and eastern hemispheres (top figure). Latitudinal distribution of karst areas in 5° intervals both for total and individual continents (Balász, 1977a. Reproduced by permission of the 7th International Speleological Congress and by permission of the author.)

Figure 12.4 Regions of largest geoclimatic potential for karstification (Balázs, 1977b. Reproduced by permission of the 7th International Speleological Congress and by permission of the author.)

These karst areas play an important role in the bicarbonate budget. Subsurface runoff is the main mode of discharge in karst. Here, high soil PCO2 (Miotke, 1974) can be neutralized to saturation with calcite (CaCO3) or dolomite (CaMg(CO3)2 ), binding large amounts of CO2. As limestone areas are more common in the humid areas of North America, Europe, and Asia than in the southern continents, we find a very low mean alkalinity in Australian and South American rivers (see Table 12.1) where hardly any limestone exists. In fact, Europe (with a karst area of 13.5%) has the largest average total dissolved solid (TDS) concentration (182 ppm) of all the continents. Half of this load is HCO3 (95 ppm).

The complex flow patterns within a carbonate conduit aquifer are illustrated by Figure 12.5. Very often, air-filled caves intersect the path of seepage water. Most caves exchange their air quite rapidly with the atmosphere. Cave air has, therefore, a lower PCO2 than soil water percolating from above. The water loses CO2, thus increasing the PCO2 of cave air. Air currents transport the CO2 back to the surface, where cave mouths are sources of CO2 . When the water loses CO2, sinter is formed. Where there is no soil above the cave, sinter cannot precipitate, a fact which is best illustrated by 14C flowstone analyses, which show an interruption of sintering in glacial times (Franke and Geyh, 1972).

Figure 12.5 Water types encountered in a carbonate aquifer and their interconnecting flowpatterns (Harmon et al., 1972. Reproduced by permission of the British Cave Assocation and by permission of the authors.)

Table 12.5 Karst water analyses (Harmon et al., 1972. Reproduced by permission of the British Cave Research Association and by permission of the authors)


Temp. Ca2+ Mg2+ HCO3- pH Hardness* Hardness† SIc PCO2 Number
log of
samples

GRAND AVERAGES OF KARST WATER TYPES
Surface
Soil water
15.5
14
6
100
5.91
60
83
-2.61 -0.98
11
 
Vadose Zone
Dripstones
13.5
58
23
300
7.64
239
246
+0.11 -2.31
18
Vertical shafts
11.4
31.3
4
91 7.47
94
75
-0.79 -2.62
31
 
Zones of fluctuation and phreatic storage
Cave streams
10.7
43
7
144
7.38
136
119
-0.60 -2.36
23
Standing cave pools
12.9
37
25
214
7.77
194
176
-0.08 -2.60
18
Wells
19.1
63
15