2017
DOI: 10.1002/lom3.10233
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Surface gas exchange determined from an aquatic eddy covariance floating platform

Abstract: We present a new approach to quantifying air-water flux and gas transfer velocity (k 600 ) from underwater eddy covariance (EC) of dissolved oxygen. EC fluxes were measured 35 cm below the air-water interface using an acoustic Doppler velocimeter (ADV) coupled with a fast-responding dissolved oxygen optode probe, integrated on a floating platform. A micro-electro-mechanical system (MEMS)-based inertial motion unit integrated with the ADV enabled compensation of measured velocities for platform motion and chang… Show more

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Cited by 16 publications
(26 citation statements)
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References 68 publications
(121 reference statements)
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“…Although this approach is appropriate for the reef site at the edge of the Bermuda platform that is open to interaction with the wind, it is not appropriate for the Virginia coastal bay that is enclosed by islands, marsh, and banks that limit the influence of wind. Instead, at the Virginia site, we estimated gas exchange rates from the turbulent kinetic energy dissipation rate ( ε ) based on the methods of Zappa et al (, ), as described by Long and Nicholson (). The ε was determined hourly from the fit of the vertical velocity wavenumber spectrum in the inertial subrange (Fairall and Larsen ; Zappa et al ; Long and Nicholson ): S=αε2/3κN5/3 where S is the wavenumber spectrum of the fluctuating components of the vertical velocity, κ N is the radian wavenumber, and α is Kolmogorov's empirical constant (= 0.52; see details in Zappa et al [, ]).…”
Section: Methodsmentioning
confidence: 99%
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“…Although this approach is appropriate for the reef site at the edge of the Bermuda platform that is open to interaction with the wind, it is not appropriate for the Virginia coastal bay that is enclosed by islands, marsh, and banks that limit the influence of wind. Instead, at the Virginia site, we estimated gas exchange rates from the turbulent kinetic energy dissipation rate ( ε ) based on the methods of Zappa et al (, ), as described by Long and Nicholson (). The ε was determined hourly from the fit of the vertical velocity wavenumber spectrum in the inertial subrange (Fairall and Larsen ; Zappa et al ; Long and Nicholson ): S=αε2/3κN5/3 where S is the wavenumber spectrum of the fluctuating components of the vertical velocity, κ N is the radian wavenumber, and α is Kolmogorov's empirical constant (= 0.52; see details in Zappa et al [, ]).…”
Section: Methodsmentioning
confidence: 99%
“…The flux across the benthic-water interface was determined with an eddy covariance system ( Fig. 1a) that consisted of an acoustic Doppler velocimeter (ADV, Nortek) coupled to a Fire-stingO 2 Mini fiber-optic O 2 meter with a temperature-compensated, fast-response (< 0.3 s), 430 μm diameter optode (Pyroscience, GE), similar to previous designs (Long et al 2015a;Long and Nicholson 2018). The mean turbulent O 2 flux was calculated over 0.25 h periods from the product of the instantaneous variations in the vertical velocity and O 2 concentration by:…”
Section: Benthic Fluxesmentioning
confidence: 99%
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