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Equilibrium sampling in soil, snow and aquatic ecosystem measurements [Jun 2008]

Soil Exploration Technology

This application note describes the equilibrium sampling method to be used with the Vaisala CARBOCAP® Carbon Dioxide Probe GMP343 for measurements of CO2 concentrations and fluxes in soil, snow or aquatic ecosystems. Some practical hints are provided for the different environments to ensure successful and trouble free measurements. This application note has been prepared in cooperation with Lammi Biological station, Department of Ecological and Environmental Sciences and Department of Forest Ecology at University of Helsinki.

Introduction to methods for measuring CO2 concentrations and CO2 flux in soil, snow and aquatic environments

Equilibrium Sampling
AWE International Issue 15 Jun 2008
© AWE International 2008

In terrestrial ecology, soil CO2 efflux, usually measured with chamber techniques, plays an important role in the CO2 exchange between the land surface and the atmosphere. Recently, the CO2 concentration gradient method has become popular in studying the CO2 transport within the soil and between the soil and the atmosphere.(1,2,3) The CO2 produced in the soil is transported between the soil layers and from the soil to the atmosphere mainly by diffusion. The CO2 efflux can be determined from the concentration gradients in the soil layers and between the soil and the atmosphere. This gradient method is especially suitable for studying the vertical distribution of CO2 production in the soil and for studying the processes affecting the CO2 efflux.

Equilibrium Sampling
AWE International Issue 15 Jun 2008
© AWE International 2008

Continuous chamber measurements of soil CO2 efflux are difficult to carry out in winter, because of the snow cover spanning several months in the arctic and boreal regions. Calculating diffusion of CO2 through the snow pack from CO2 concentration gradient provides an alternative for chamber measurements of CO2 flux in winter.(4,5) The same principles apply in the snow and soil measurements, i.e. the diffusion properties determine the diffusion rate of CO2 through the snow/soil.

Figure 1. Gas collector installation in the soil
AWE International Issue 15 Jun 2008
© AWE International 2008

In aquatic ecology, measurements of dissolved CO2 (e.g. pCO2) have important applications in estimation of CO2 transfer across water–atmosphere interface and in calculations of metabolic rates of aquatic communities. It is possible to calculate the amount of dissolved CO2 in water from alkalinity, pH and dissolved inorganic carbon, see e.g.,(6) but direct measurements of pCO2 are recommended to minimize possible analytical errors. The most common way to directly measure pCO2 is the headspace equilibration technique, where water sample is equilibrated with a headspace gas from which the CO2 concentration is analyzed with infra red gas analyzer or with gas chromatography.(7) When water temperature is measured in connection with pCO2, dissolved CO2 can be calculated by applying Henry’s law, see e.g.(6)

Figure 1. The installation box of GMP343 probes (on the right)
AWE International Issue 15 Jun 2008
© AWE International 2008

Aquatic systems can show quite large temporal variations in CO2 concentrations. Periods of high primary production, i.e. high consumption of CO2, are short and laborious to track with the headspace technique. Conventional measurements of metabolic processes have been done by enclosing the aquatic community into a small bottle and incubating it for several hours before determining the change in gas concentration or amount of incorporated carbon.(8) Conditions in the enclosed bottle differ from those prevailing in nature, thus these methods are prone to give potentially erroneous results.(8,9) Monitoring of metabolic gases in situ in free water gives a more reliable approach to estimate ecologically important processes such as primary production and community respiration.

Figure 2. Daily average of CO2 concentration in soil and snow during a period of January 2006-April 2006 measured using the equilibrium sampling method
AWE International Issue 15 Jun 2008
© AWE International 2008

Here a new system for continuous monitoring of CO2 with a high temporal resolution is introduced. This new equilibrium sampling method is based on circulating air in a closed loop consisting of a CO2 analyzer (the Vaisala CARBOCAP® Carbon Dioxide Probe GMP343 or the Module GMM221), a pump, gas impermeable tubing and a semipermeable tube, which allows gas exchange between the system and the material to be measured. The semipermeable tube is installed in water or in other medium to be measured. The air inside the tubing is circulated by a pump and the gas concentrations inside the loop will reach equilibrium with the gas concentration outside the system. The response time in this diffusion driven system depends on characteristics of the gas permeable membrane and the ratio of equilibrating surface area to total volume of the loop.

Instrument setup for equilibrium sampling

Figure 3. Daily average of CO2 concentration in soil and snow during a period of January 2006-April 2006 measured with probes buried in the soil.
AWE International Issue 15 Jun 2008
© AWE International 2008

A typical measurement setup for equilibrium sampling includes several GMP343 probes (or GMM221 modules) to cover the whole vertical CO2 gradient of interest in soil or water ecosystem. A measurement unit consists of a GMP343, a linear pump (SMG-4, 12VCD, Rietschle Thomas AB with 1.1 L min-1 flow rate) and a stainless steel (RST jointless AISI 316L, 8 x 1.0 mm) and butyl rubber (Saint Germain IR 00022, 6 x 12 mm, VWR International) tubing for gas impermeable part of the loop.

Figure 4. Installations on a floating platform.
AWE International Issue 15 Jun 2008
© AWE International 2008

The semipermeable part of the system consists of 6 x 1.5 mm silicone rubber tube (Rotilabo® Art:9572.1, Roth GmbH) with a stainless steel coil spring enclosed inside the tube (RST 0.5 x 5 x 1 000 mm) to prevent the silicone rubber tube from flattening due to outside pressure (see Figure 2). Gases, including water vapor, diffuse through the silicone rubber, thus it is recommended to add a dead-end stainless steel tube to collect water at the lower end of the upgoing stainless steel tube connected with T-joints (Svagelok, Helsinki Valve & Fitting Oy, Finland). Temperature probes (Philips KTY81-110, Philips Semiconductors) are installed at each measuring depth. Here the analog output option is used with 0 – 5 V output signal and A/D converter (Nokeval Oyj, Finland) converts the analog signal to digital readings and logs it with a computer. The GMP343 probes and pumps were placed in a weather resistant installation box (see Figure 1).

Equilibrium sampling in soil and snow measurements

Equilibrium Sampling
AWE International Issue 15 Jun 2008
© AWE International 2008

The equilibrium sampling method can be used to measure CO2 concentrations in the soil profile. One installation in a vertical face of soil pits at four depths (2, 7, 12, 22 cm) is described here. In addition to CO2 concentration, soil temperature and water content data is needed to calculate the diffusivity in the soil.

Equilibrium Sampling
AWE International Issue 15 Jun 2008
© AWE International 2008

The diffusivity of the soil and its correct determination play a crucial role in the CO2 efflux values obtained with the gradient method. The diffusivity of CO2 in the soil depends on soil total porosity, soil tortuosity, soil water content and transport distance. These variables should be determined for each soil layer to achieve accurate flux calculations. An alternative method for estimating soil diffusivity is to use a tracer gas like radon. Tracer method, however, gives only the average diffusivity of the soil, thus continuous monitoring of soil water content together with the CO2 concentration is recommended.

The CO2 concentrations measured with the equilibrium sampling method in soil and snow show a clear seasonal pattern (Figure 2). The CO2 concentrations increase with increasing soil depth. In addition, CO2 concentrations increase in early spring as snow thaws and soil water content increases. The interruptions in the measurements during thawing are caused by water entering the system.

As a comparison to the equilibrium sampling method, GMP343 probes have been continuously used in soil CO2 profile measurements for three years. The probes buried at 0, 5 and 17 cm depths give comparable results to the equilibrium sampling method between January and March (Figures 2 and 3). Since April the equilibrium sampling method shows higher values, probably due to higher soil water content.

Equilibrium sampling in aquatic ecosystems

In addition to soil and snow studies, equilibrium sampling can be used to study CO2 profiles in aquatic ecosystems. GMP343 probes can be installed on a floating platform in an insulated water resistant box (Figure 4). Gas collector tubings are installed in water at various depths (here 0.1, 0.5, 1.5, 2.0 and 3.0 m).

CO2 measurements can be performed through the whole open water period. Simultaneous measurements of water column photon flux density (PFD, μmol m-2s-1) at 0.5 m depth are carried out to provide information on photosynthesis. Silicone rubber tubing of the gas collectors are replaced once a month to control biofouling and its effects on the CO2 concentration data. At the same time the water collectors are emptied.

The developed measuring system has proved to be reliable. Despite some pump break-ups, continuous measurements of vertical CO2 profiles in water over an open water period can be obtained using the method. The CO2 concentrations show mostly a vertical gradient, where surface water is close to equilibrium with atmosphere and at 3 m depth high CO2 concentration of almost 10 000 ppm exist. At 2 m depth the CO2 concentration exceeded the measurement range of the GMP343 (0 5 000 ppm) during summer months. In October a complete mixing of water column from the surface to the bottom is seen, whereas springtime mixing looks incomplete.

The collected high time resolution data can be used to model the dependence of CO2 consumption and production on environmental parameters and calculate the rates of community metabolism, i.e. primary production and community respiration.(10) The consumed or produced CO2 in the euphotic layer over 30 minutes periods can be computed and a Platt-Jassby – type light-dependence curve can be fitted (so-called P-I curve)(11) to the exchange rate. This is a new method compared to the conventional measurements in laboratory or on ship’s deck, which often result in fairly limited data sets.

Some practical hints for equilibrium sampling experiments

Condensation of water vapor

Condensing water should be taken into consideration when designing an equilibrium sampling system. Air circulation in the gas collector should be secured by avoiding water blockage in the tubing. Suggested solutions are: 1) larger tube diameter 2) larger gas collector equipped with a water collector, which can be emptied from the soil surface or 3) chemical water absorbent in the system. It is good to keep in mind that if the system is in continuous use, the water absorbent needs frequent changing. Alternatively, a water condensing unit colder than the soil can be built, to trap the water. In the GMP343 the heating option should be enabled to avoid water condensation on the probe optics.

Pump reliability

The tested linear pumps (SMG-4, 12VCD, Rietschle Thomas AB) are designed for laboratory use. Pump lifetime might be significantly reduced if operated in cold temperatures (< 5°C), probably due to the plastic membranes of the pump breaking at lower temperatures. Pump lifetime depends also on the DC voltage applied in the system. When operating under the nominal voltage (12V), the rotation of the pumps is lowered and thus the lifetime of the pump is extended.

Power consumption

The described system operates using 12 V DC, thus in principle it could be run with a battery. However, the power consumption is relatively high, thus in long-term use this option is more theoretical. The pumps operate with 6 W wattage and consume 320 mA current. The power consumption of GMP343 (heating option enabled) is about 300 mA. Thus one measurement unit (consisting of one GMP343 and one SMG-4 pump) consumes at least 620 mA current, which in theory can be operated for less than 100 hours using an ordinary 12 V and 60 Ah car battery. In practice this time will be shorter, since the battery cannot be totally discharged. Thus the system should be operated with a mains current or with a solar panel supplying at least 620 mA current for each measurement unit.

Aquatic measurement application

Experience from one year measuring period in lake environment showed the following:

Solid surfaces provide a growing site for aquatic sessile organisms, thus biofouling is often a problem in long-term measurements within natural waters. Growth of periphytic algae can be prevented by covering the gas collector with a light impermeable material, but this does not stop bacterial growth on the surfaces. However, toxic antifouling chemicals are not recommended. To avoid the harmful effect of biofouling on gas exchange, the gas collector must be cleaned or replaced periodically.

Described measurement setup is limited to surface waters of aquatic systems. Handling of long tubings is inconvenient, tricky and somewhat risky. In deepwater measurements the whole instrumentation should be enclosed in a water proof casing and lowered to the measuring depth.

During times of low productivity the measuring system did not show adequate sensitivity due to slow response times. The situation can be improved by reducing the response time by e.g. the sintered PTFE material. A good response time has been achieved by a gas collector by dividing the circulating air into a hundred small silicone rubber tubes.(12,13) However, making such system water tight can be troublesome and its maintenance can be difficult. Thus, keeping the gas collector system simple and improving the response time by optimizing the material is recommended.

Performance of the GMP343 in equilibrium sampling systems

The accuracy and precision of the GMP343 transmitters is adequate for soil profile CO2 measurements, especially with averaging to 1 min. The GMP343 is resistant to moisture and corrosion. Probes have been installed in the forest soil at 0 cm, 5 cm, 17 cm and 27 cm depths since June 2004, where the soil is quite low in pH (pH values 3.5-4 in the surface and 4-5 in deeper layers). The soil has had volumetric water content of 20-30% most of the year and 30-40% in the autumn and during snow thaw. Despite of these relatively harsh conditions, the probes have been working without problems all year round. The buried probes were equipped with sintered PTFE filter and a in-soil adapter. The heating option was enabled to avoid water condensation on probe optics.

The heating option in the GMP343 should be used with caution if they are buried in the soil. The slight heating may affect the soil temperature around the probes. For example, snow melted earlier around the probes probably due to the heating. This 'early spring' may change the soil conditions around the probes. However, this effect is not very significant deeper in the soil, where heat is dissipated. This naturally depends on the heat conductivity of the soil. It is good to monitor the soil temperature near the probes (about 1 cm distance) and at further distance at the same depth to recognize the possible heating effect.

The measurement range of 0…5 000 ppm may be too narrow for soil CO2 profile measurements during the growing season, as CO2 concentration deeper in the soil can easily reach 20 000 ppm. Probe measurement range should be selected according to the highest possible concentration.

References

  1. Tang, J., Baldocchi, D.D., Qi, Y. and Xu, L. 2003. Assessing soil CO2 efflux using continuous measurements of CO2 profiles in soils with small solid-state sensors. Agr. Forest Meteorol. Meteorology 118 (3-4): 207-220.
  2. Jassal, R. S., Black, T. A., Drewitt, M. D., Novak, M. D., Gaumont-Guay, D. and Nesic, Z. 2004. A model of the production and transport of CO2 in soil: predicting soil CO2 concentrations and CO2 efflux from a forest floor. Agr. Forest Meteorol. 124: 219-236.
  3. Pumpanen, J., Ilvesniemi, H., Kulmala, L., Siivola, E., Laakso, H., Kolari, P., Helenelund, C., Laakso, M., Uusimaa, M., Iisakkala, P., Räisänen, J. and Hari, P. Role of recent photosynthate in CO2 efflux from boreal forest soil as determined from soil air CO2 concentration profiles. Submitted to Global Change Biol.
  4. Sommerfield, R. A., Mosier, A. R. and Musselman, R. C. 1993. CO2, CH4 and N2O flux through a Wyoming snowpack and implications for global budgets. Nature 361: 140-142.
  5. Fahnestock, J.T., Jones, M.H., Brooks, P.D., Walker, D.A. and Welker, J.M. 1998. Winter and early spring CO2 efflux from tundra communities of northern Alaska. J. Geophy. Res. 103(D22): 29023-29027.
  6. Stumm, W. and Morgan J. J. 1970. Aquatic Chemistry. Wiley-Interscience.
  7. McAuliffe, C. C. 1971. GC determination of solutes by multiple phase equilibration. Chem. Technol. 1 : 46–51.
  8. Peterson, B. J. 1980. Aquatic primary productivity and the 14C-CO2 method: A history of the productivity problem. Ann. Rev. Ecol. Sys. 1 1: 359-385.
  9. del Giorgio, G. and Williams, P. J. le B. eds. 2006, Respiration in aquatic ecosystems. Oxford University Press.
  10. Hari, P., Pumpanen, Huotari, J., J. Kolari, P., Grace, J., Vesala, T. and Ojala, A. High-frequency measurements of photosynthesis of planktonic algae using rugged nondispersive infrared carbon dioxide probes. Submitted to Limnol. Oceanogr.: Methods.
  11. Platt, T. and Jassby, A. D. 1976. The relationship between photosynthesis and light for natural assemblages of coastal marine phytoplankton. J. Phycol. 1 2: 421-430.
  12. Carignan, R. 1998. Automated determination of carbon dioxide, oxygen and nitrogen partial pressures in surface waters. Limnol. Oceanogr. 4 3: 969-975.
  13. Hanson, P. C., Bade, D. L., Carpenter, S. R. and Kratz, T. K. 2003. Lake metabolism: Relationships with dissolved organic carbon and phosphorus. Limnol. Oceanogr. 4 8: 1112-1119.

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