Surfactant control of gas transfer velocity along an offshore coastal transect: results from a laboratory gas exchange tank
Understanding the physical and biogeochemical controls of air–sea gas exchange is necessary for establishing biogeochemical models for predicting regional- and global-scale trace gas fluxes and feedbacks. To this end we report the results of experiments designed to constrain the effect of surfactant...
Main Authors: | , , |
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Format: | Article |
Language: | English |
Published: |
Copernicus Publications
2016-07-01
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Series: | Biogeosciences |
Online Access: | http://www.biogeosciences.net/13/3981/2016/bg-13-3981-2016.pdf |
Summary: | Understanding the physical and biogeochemical controls of air–sea gas
exchange is necessary for establishing biogeochemical models for predicting
regional- and global-scale trace gas fluxes and feedbacks. To this end we
report the results of experiments designed to constrain the effect of
surfactants in the sea surface microlayer (SML) on the gas transfer velocity
(<i>k</i><sub>w</sub>; cm h<sup>−1</sup>), seasonally (2012–2013) along a 20 km
coastal transect (North East UK). We measured total surfactant activity (SA),
chromophoric dissolved organic matter (CDOM) and chlorophyll <i>a</i> (Chl <i>a</i>) in
the SML and in sub-surface water (SSW) and we evaluated corresponding
<i>k</i><sub>w</sub> values using a custom-designed air–sea gas exchange tank.
Temporal SA variability exceeded its spatial variability. Overall, SA varied
5-fold between all samples (0.08 to 0.38 mg L<sup>−1</sup> T-X-100), being
highest in the SML during summer. SML SA enrichment factors (EFs) relative to
SSW were ∼ 1.0 to 1.9, except for two values (0.75; 0.89: February
2013). The range in corresponding <i>k</i><sub>660</sub> (<i>k</i><sub>w</sub> for CO<sub>2</sub> in
seawater at 20 °C) was 6.8 to 22.0 cm h<sup>−1</sup>. The film factor
<i>R</i><sub>660</sub> (the ratio of <i>k</i><sub>660</sub> for seawater to <i>k</i><sub>660</sub> for “clean”,
i.e. surfactant-free, laboratory water) was strongly correlated with SML SA
(<i>r</i> ≥ 0.70, <i>p</i> ≤ 0.002, each <i>n</i> = 16). High SML SA typically
corresponded to <i>k</i><sub>660</sub> suppressions ∼ 14 to 51 % relative to
clean laboratory water, highlighting strong spatiotemporal gradients in gas
exchange due to varying surfactant in these coastal waters. Such variability
should be taken account of when evaluating marine trace gas sources and
sinks. Total CDOM absorbance (250 to 450 nm), the CDOM spectral slope ratio
(<i>S</i><sub>R</sub> = <i>S</i><sub>275 − 295</sub>∕<i>S</i><sub>350 − 400</sub>), the 250 : 365 nm CDOM
absorption ratio (<i>E</i><sub>2</sub> : <i>E</i><sub>3</sub>), and Chl <i>a</i> all indicated spatial
and temporal signals in the quantity and composition of organic matter in the
SML and SSW. This prompts us to hypothesise that spatiotemporal variation in
<i>R</i><sub>660</sub> and its relationship with SA is a consequence of compositional
differences in the surfactant fraction of the SML DOM pool that warrants
further investigation. |
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ISSN: | 1726-4170 1726-4189 |