Abstract. A fast-response (10 Hz) chemiluminescence detector for
ozone (O3) was used to determine O3 fluxes using the eddy covariance
technique at the Penlee Point Atmospheric Observatory (PPAO) on the south
coast of the UK during April and May 2018. The median O3 flux was −0.132 mg m−2 h−1 (0.018 ppbv m s−1),
corresponding to a deposition velocity of 0.037 cm s−1
(interquartile range 0.017–0.065 cm s−1) – similar to the
higher values previously reported for open-ocean flux measurements but not
as high as some other coastal results. We demonstrate that a typical single
flux observation was above the 2σ limit of detection but had
considerable uncertainty. The median 2σ uncertainty of deposition
velocity was 0.031 cm s−1 for each 20 min period, which
reduces with the square root of the sample size. Eddy covariance footprint
analysis of the site indicates that the flux footprint was predominantly
over water (> 96 %), varying with atmospheric stability and, to
a lesser extent, with the tide. At very low wind speeds when the atmosphere
was typically unstable, the observed ozone deposition velocity was elevated,
most likely because the footprint contracted to include a greater land
contribution in these conditions. At moderate to high wind speeds when
atmospheric stability was near-neutral, the ozone deposition velocity
increased with wind speed and showed a linear dependence with friction
velocity. This observed dependence on friction velocity (and therefore also
wind speed) is consistent with the predictions from the one-layer model of
Fairall et al. (2007), which parameterises
the oceanic deposition of ozone from the fundamental conservation equation,
accounting for both ocean turbulence and near-surface chemical destruction,
while assuming that chemical O3 destruction by iodide is distributed over
depth. In contrast to our observations, the deposition velocity predicted by
the recently developed two-layer model of Luhar et al. (2018) (which
considers iodide reactivity in both layers but with molecular diffusivity
dominating over turbulent diffusivity in the first layer) shows no major
dependence of deposition velocity on wind speed and underestimates the
measured deposition velocities. These results call for further investigation
into the mechanisms and control of oceanic O3 deposition.