Abstract

Abstract. Oxygen triple isotope measurements can be used to calculate aquatic gross oxygen production rates. Past studies have emphasised the appropriate definition of the 17O excess and often used an approximation to derive production rates from the 17O excess. Here, I show that the calculation can be phrased more consistently and without any approximations using the relative 17O/16O and 18O/16O isotope ratio differences (delta values) directly. I call this the "dual delta method". The 17O excess is merely a mathematical construct and the derived production rate is independent of its definition, provided all calculations are performed with a consistent definition. I focus on the mixed layer, but also show how time series of triple isotope measurements below the mixed layer can be used to derive gross production. In the calculation of mixed layer productivity, I explicitly include isotopic fractionation during gas invasion and evasion, which requires the oxygen supersaturation s to be measured as well. I also suggest how bubble injection could be considered in the same mathematical framework. I distinguish between concentration steady state and isotopic steady state and show that only the latter needs to be assumed in the calculation. It is even possible to derive an estimate of the net production rate in the mixed layer that is independent of the assumption of concentration steady state. I review measurements of the parameters required for the calculation of gross production rates and show how their systematic uncertainties as well as the use of different published calculation methods can cause large variations in the production rates for the same underlying isotope ratios. In particular, the 17O excess of dissolved O2 in equilibrium with atmospheric O2 and the 17O excess of photosynthetic O2 need to be re-measured. Because of these uncertainties, all calculation parameters should always be fully documented and the measured relative isotope ratio differences as well as the oxygen supersaturation should be permanently archived, so that improved measurements of the calculation parameters can be used to retrospectively improve production rates.

Highlights

  • Luz et al (1999) first suggested that the triple-isotope composition of atmospheric oxygen (O2) could be used as a tracer of biological productivity. They showed that photosynthetic O2 has a small, but measurable excess of the oxygen isotope 17O with respect to atmospheric O2, after normalisation for 18O/16O isotope ratio differences

  • The main goal of the present study is to explore the systematic uncertainty in the calculation of g from triple isotope measurements in dissolved O2

  • 15) ppm reported by Luz and Barkan (2000) for photosynthetic O2, which has been adopted by all subsequent studies of gross oxygen production using the triple isotope technique

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Summary

Introduction

Luz et al (1999) first suggested that the triple-isotope composition of atmospheric oxygen (O2) could be used as a tracer of biological productivity. The relative isotope ratio difference between atmospheric and photosynthetic oxygen can be used to calculate gross oxygen production in the mixed layer, using the gas exchange rate as a “timekeeper”. The advantage of the oxygen triple isotope technique over 18O/16O isotope ratio measurements in determining production is that the calculated rates are independent of the respiratory isotope effect that is not well known and that would otherwise lead to significant uncertainties (Hendricks et al., 2004; Quay et al, 1993; Venkiteswaran et al, 2008). The main goal of the present study is to explore the systematic uncertainty in the calculation of g from triple isotope measurements in dissolved O2. For technical reasons this was not possible for the capital Greek delta designating the triple isotope excess 17

Notation
Quantification of deviations from mass-dependent isotope ratio relationships
Budget calculations
Respiration only
Production only
Production and respiration
Isotopic steady state between production and respiration
Production below the mixed layer
Production within the mixed layer
Iterative calculation of g from 17 and O2 supersaturation s
Non-steady state conditions – calculation of gas exchange coefficients
Input parameters
Respiration
Photosynthesis
Gas exchange
Systematic uncertainty of production within the mixed layer
Calculation method
Practical example: calculation of g values in the Southern Ocean
Findings
Conclusions
Full Text
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