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Atlantic fCO2 Crossovers

System Information

The purpose of this analysis was to determine if any significant systematic offset existed between the various legs of the WOCE/NOAA/JGOFS Atlantic Ocean measurements of fugacity of CO2 (fCO2). Three different types of instruments were used to measure discrete fCO2 samples. With each an aliquot of seawater was equilibrated at a constant temperature of either 4° or 20°C with a headspace of known initial CO2 content. Subsequently, the headspace CO2 concentration was determined by non-dispersive infrared analyzer (NDIR) or by quantitatively converting the CO2 to CH4 and then analyzing it using a gas chromatograph (GC) with a flame ionization detector. The initial fCO2 in the water was determined after correcting for the loss or gain of CO2 during the equilibration process. This correction can be significant for large initial fCO2 differences between the headspace and the water, and for systems with a large headspace-to-water volume ratio (Chen et al. 1995).

The system used by Takahashi and co-workers on A21/A12 (Chipman et al. 1993; DOE 1994) involved equilibration of a ~50-mL headspace with a ~500-mL sample at either 4°C or 20°C depending on ambient surface water temperatures. The Takahashi values, reported as partial pressure of CO2 (pCO2), were converted to fCO2 using the correction factor (~ 0.996) given by Weiss (1974). Wanninkhof and co-workers utilized two systems during the Atlantic survey cruises. An NDIR-based system with ~500-mL samples was used for analyses during A16S and A16N (Wanninkhof and Thoning 1993). A GC-based system with samples collected in a closed, septum sealed bottle having a volume of ~120-mL of seawater and a headspace of ~10-mL was used for A05R (Neill et al. 1997). Wallace and co-workers used the setup described in Neill et al. on A08 but with bottles having a volume of ~50-mL of seawater and a headspace of ~5-mL.

Detectors were calibrated after every 4-12 samples with gas standards traceable to manometrically determined values of C. D. Keeling at SIO. An assessment of fCO2 accuracy is difficult to determine because of the lack of aqueous standards. Estimates of precision based on duplicate samples range from 0.1 to 1% depending on fCO2 and measurement procedure, with higher fCO2 levels on the infrared based system (>700 µatm) giving worse reproducibility (Chen et al. 1995).

Crossover Analysis

The stations selected for each crossover were those with carbon data that were within roughly 100 km (˜1° latitude) of the crossover point. Data from deep water (>1500 m) at each of the crossover locations were plotted against the density anomaly referenced to 4000 dB (σ-4) and fit with a second-order polynomial. For the crossover compari

son all samples run at 4°C were normalized to 20°C by calculating the TALK from fCO2 (4°C) and TCO2, and subsequently calculating fCO2 (20°C) from the TCO2 and calculated TALK. The carbonate dissociation constants of Mehrbach et al., (1973) as refit by Dickson and Millero (1987) and ancillary constants listed in DOE (1994) are used for these calculations using the program of Lewis and Wallace (1998). Crossover information is given in the summary table bellow.

Upon examination, it became clear that there may a problem for the crossovers that required a temperature conversion. For example, temperature conversion from 4° to 20°C using the Mehrbach constants yield fCO2 values in the deep Pacific that are about 50 µatm higher than those derived from use of Roy constants of the conversion. Since the discrepancy in dissociation constants has not been fully resolved, the crossover comparison for fCO2 data analyzed at different temperatures and for comparisons of measured versus calculated values is problematic.

Data from deep water (>1500 m) at each of the 12 crossovers analyses at five locations, were plotted against the density anomaly referenced to 4000 dB (σ-4) and fit with a second-order polynomial. The difference and standard deviation between the two curves was then calculated from 10 evenly spaced intervals over the density range common to both sets of crossovers. The standard deviation for the 12 fCO2 crossover comparisons was 13.4 µatm. The average of the absolute value of the differences was 9.8±8.4 µatm.

Summary

Summary Table of Crossover Results (opens a new window)

References

Last modified: 2021-03-17T18:30:24Z