Competition between Baroclinic Instability and Ekman Transport under Varying Buoyancy Forcings in Upwelling Systems: An Idealized Analog to the Southern Ocean
Open accessAbstract
Coastal upwelling rates are classically determined by the intensity of the upper-ocean offshore Ekman transport. But (sub)mesoscale turbulence modulates offshore transport, hence the net upwelling rate. Eddy effects generally oppose the Ekman circulation, resulting in so-called ‘‘eddy cancellation,” a process well studied in the Southern Ocean. Here we investigate how air–sea heat/buoyancy fluxes modulate eddy cancellation in an idealized upwelling model. We run CROCO simulations with constant winds but varying heat fluxes with and without submesoscale-rich turbulence. Eddy cancellation is consistently evaluated with three different methods that all account for the quasi-isopycnal nature of ocean circulation away from the surface. For zero heat fluxes the release of available potential energy by baroclinic instabilities is strongest and leads, near the coast, to nearly full cancellation of the Ekman cross-shore circulation by eddy effects, i.e., zero net mean upwelling flow. With increasing heat fluxes eddy cancellation is reduced and the transverse flow progressively approaches the classical Ekman circulation. Sensitivity of the eddy circulation to synoptic changes in air–sea heat fluxes is felt down to 125-m depth despite short experiments of tens of days. Mesoscale dynamics dominate the cancellation effect in our simulations which might also hold for the real ocean as the relevant processes act below the surface boundary layer. Although the idealized setting overemphasizes the role of eddies and thus studies with more realistic settings should follow, our findings have important implications for the overall understanding of upwelling system dynamics.
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Written from the paper’s full text.
TL;DR
In idealized CROCO upwelling simulations with constant winds, eddy cancellation of the Ekman cell is strongest when air–sea heat fluxes are zero and weakens as heat flux increases, so the residual cross-shore flow approaches the classical Ekman circulation. The cancellation is dominated by mesoscale turbulence and is sensitive to heat-flux changes down to ~125 m, though the idealized periodic channel overemphasizes eddy effects relative to real EBUS.
Key findings
- For zero heat flux (NF), available potential energy release by baroclinic instability is strongest; near the coast, eddy effects nearly fully cancel the Ekman cross-shore circulation, i.e., zero net mean upwelling flow. With increasing heat flux, eddy cancellation is reduced and the transverse flow progressively approaches the classical Ekman circulation.
- At 70-m depth and 64 km offshore, eddies cancel 72%–87% of the Ekman transport in NF, 46%–60% in MF, and around 40% in HF across three streamfunction methods. The eddy streamfunction reaches −2.8 m² s⁻¹ in NF, stronger in opposing direction than the mean Eulerian streamfunction (2.3 m² s⁻¹).
- The APE release term \(w'b'\) averaged between 16 and 112 km offshore decreases from 1.44 × 10⁻⁷ m² s⁻³ in NF to 1.06 × 10⁻⁷ m² s⁻³ in HF, a decrease of about 25%; at 75-m depth it is reduced by about 50% in HF compared with NF. Sensitivity to heat flux reaches down to 125-m depth, while below 125 m the domain-averaged \(w'b'\) curves show almost no difference and vanish around 200 m.
- Mesoscale dynamics dominate the cancellation: a factor-of-10 resolution change (800 m vs. 8 km) does not dramatically alter \(w'b'\) below 50 m, though mixed-layer values differ by about 25%. The paper’s EKE exceeds real EBUS values by a factor of 2–10; rescaling suggests real EBUS cancellation of roughly 3%–6% in the northern Benguela to 10%–30% in the California Current System.
Methods
- CROCO is used in an idealized upwelling configuration: 400 km alongshore × 600 km cross-shore, periodic alongshore, closed coast and offshore boundaries, shelf/slope/flat bottom, 100 sigma levels, constant \(f\) corresponding to ~14.5°S, constant wind stress of 0.075 N m⁻² after a ramp, and a prescribed alongshore pressure gradient driving an onshore return flow.
- Heat-flux sensitivity experiments use restoring with \(dQ/dT = 0\) (NF), 225 (MF), and 250 W m⁻² K⁻¹ (HF); MF receives on average about 200 W m⁻² near the coast and 50 W m⁻² 200 km offshore. Each experiment has 12 ensemble runs at 800-m and 8-km horizontal resolution; runs last 120 days including 80-day spinup, with analysis over days 81–120.
- Eddy and residual circulations are quantified with three streamfunction formulations: transformed Eulerian mean (TEM), isopycnal averaging at constant cross-shore distance, and isopycnal averaging at constant depth. Baroclinic instability strength is evaluated as APE release via the covariance \(w'b'\).
Limitations
- Paper-stated: the idealized periodic channel lacks a beta effect, so EKE is 2–10 times higher than in the real EBUS; the rescaling to real EBUS assumes eddy overturning scales linearly with EKE. Experiments are only 40 days and not in statistical equilibrium, and wind variability and alongshore pressure-gradient variability are ignored.
- Paper-stated: the idealized setting overemphasizes the role of eddies, and more realistic EBUS studies are needed; negative buoyancy-flux cases and biogeochemical tracers were not investigated. The choice of pure flux versus restoring surface buoyancy boundary condition may also matter.
- Evident from the text: constant wind forcing, no seasonal cycle, simplified bathymetry/coastline, a closed offshore boundary with a sponge layer, and short ensemble duration may further limit realism and statistical robustness.
Model-written summary. Check it against the paper before relying on it.
Integrity signals
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Cites
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Claims the paper makes
11 of 66 cited sources checked · 3 supported · 0 flagged · accuracy not yet measured
- Premisecitation
(Sub)mesoscale turbulence modulates offshore transport and hence the net upwelling rate.
“But (sub)mesoscale turbulence modulates offshore transport, hence the net upwelling rate.”
Quote in the paperSubstantial claim1 of 3 sources checked- cites Lathuilière et al. 2010 source
The Summary (§5, paragraph 51; page unavailable) says mesoscale filaments export nitrate and phytoplankton offshore, supporting the transport part. But it also says the eddying and non-eddying simulations have the same upwelling mass flux, so the paper does not support the claimed change in net upwelling rate. (LLM, conf=0.91)
Experimental — accuracy not yet measured - cites Gruber et al. 2011 source
- cites Colas et al. 2013 source
- Interpretationcitation
Feeding the surface Ekman flow would involve bottom Ekman transport, thereby limiting the realism of the model for most upwelling sectors.
“Feeding the surface Ekman flow would therefore involve bottom Ekman transport, thereby limiting the realism of the model for most upwelling sectors (Lentz and Chapman 2004).”
Quote in the paperSubstantial claim1 of 1 sources checked- cites Lentz and Chapman 2004 source
The Estimation of the nonlinear cross-shelf momentum flux section describes a model in which onshore transport in the bottom boundary layer and interior balances offshore surface Ekman transport. But the Numerical model results section says return flow can occur predominantly in the interior, with essentially none in the bottom boundary layer. The paper therefore does not establish that feeding the surface flow necessarily involves bottom Ekman transport or that this limits a model’s realism for most upwelling sectors. (LLM, conf=0.84)
Experimental — accuracy not yet measured
- Premisecitation
Air-sea buoyancy fluxes constrain rates of fluid transfer across isopycnals in the mixed layer, hence also subduction and obduction rates at the base of the mixed layer in steady state.
“Indeed, they constrain rates of fluid transfer across isopycnals in the mixed layer, hence also subduction and obduction rates at the base of the mixed layer in steady state [subduction (obduction) being related to a convergence (divergence) of diapycnal flux of fluid, Fig. 1].”
Quote in the paperSubstantial claim1 of 2 sources checked- cites Marshall 1997 source
- cites Gent 2016 source
The Introduction discusses how surface boundary conditions affect eddy compensation of the overturning circulation, and the Discussion’s Figure 1 caption identifies atmospheric forcing and fluxes. Neither passage states that air–sea buoyancy fluxes constrain fluid transfer across isopycnals or steady-state subduction and obduction at the mixed-layer base. Searches for those relationships, including “mixed layer,” “subduction,” and “obduction,” found no supporting passage in our copy. (LLM, conf=0.72)
Experimental — accuracy not yet measured
- Premisecitation
Neglecting mixing in the ocean interior, the time-averaged residual meridional transport is entirely determined by the knowledge of air-sea buoyancy fluxes.
“Neglecting mixing in the ocean interior the time-averaged residual meridional transport is thus entirely determined by the knowledge of airsea buoyancy fluxes (Walin 1982;Marshall 1997).”
Quote in the paperSubstantial claim1 of 2 sources checked- cites Walin 1982 source
Section 4 says that surface heat flux can directly estimate the poleward surface drift and associated circulation when the mixing term is negligible, particularly at low and medium temperatures. It does not establish that air–sea buoyancy fluxes entirely determine the time-averaged residual meridional transport; for high temperatures, it says the mixing term is vital. (LLM, conf=0.84)
Experimental — accuracy not yet measured - cites Marshall 1997 source
- Interpretationcitation
The recirculation confined in the mixed layer revealed by C_TEM Eddy, and to a lesser extent C_iso2y Eddy, is the signature of submesoscale-driven mixed layer restratification.
“The recirculation confined in the mixed layer revealed by C TEM Eddy (and to a lesser extent C iso2y Eddy ) is the signature of submesoscaledriven mixed layer restratification (Fox-Kemper et al. 2008).”
Quote in the paperSubstantial claim1 of 1 sources checked- cites Fox-Kemper et al. 2008 source
- Findingown data
Mesoscale dynamics dominate the cancellation effect in the simulations.
“Mesoscale dynamics dominate the cancellation effect in our simulations”
Quote in the paperSubstantial claim - Findingown data
MF experiments receive on average a heat input of about 200 W m^-2 near the coast and 50 W m^-2 200 km offshore.
“MF experiments receive on average a heat input of about 200 W m 22 near the coast and 50 W m 22 200 km offshore (Fig. 5a).”
Quote in the paperNot a substantial claim - Findingown data
Sensitivity of the eddy circulation to synoptic changes in air-sea heat fluxes is felt down to 125-m depth despite short experiments of tens of days.
“Sensitivity of the eddy circulation to synoptic changes in air-sea heat fluxes is felt down to 125-m depth despite short experiments of tens of days.”
Quote in the paperSubstantial claim - Findingown data
The behaviors of C_TEM Eddy and C_iso2y Eddy as the heat flux forcing changes are very similar.
“The behaviors of C TEM Eddy and C iso2y Eddy as the heat flux forcing changes are very similar.”
Quote in the paperNot a substantial claim - Findingown data
At 75-m depth, w'b' is reduced by about 50% in HF compared to NF.
“at 75-m depth w 0 b 0 is reduced by about 50% in the HF compared to NF”
Quote in the paperNot a substantial claim - Findingown data
In the present idealized EBUS regime, a factor of 10 difference in resolution does not dramatically alter the magnitude of w'b' in the mixed layer: for NF maximum values reach 1.44 m2 s-3 at dx=800 m and 1.15 m2 s-3 at dx=8 km, a decrease of about 25%.
“Notably, in the present idealized EBUS regime, the factor of 10 difference in resolution does not dramatically alter the magnitude of w 0 b 0 in the mixed layer: for NF maximum values reach 1.44 (resp.1.15) m 2 s 23 at Dx 5 800 m (resp.Dx 5 8 km), which corresponds to a decrease of about 25%.”
Quote in the paperNot a substantial claim - Findingcitation
The residual circulation below the surface layer is not particularly better aligned with the isopycnals than the mean Eulerian circulation, contrary to what is typically found in the Southern Ocean.
“Note that the residual circulation below the surface layer is not particularly better aligned with the isopycnals than the mean Eulerian circulation, contrary to what is typically found in the SO (Karsten and Marshall 2002).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Karsten and Marshall 2002 source
- Findingnone given
In the ocean subsurface at 50-100-m depth, all three formulations agree on patterns and intensity, even close to 8i and 9i.
“In the ocean subsurface (at 50-100-m depth) where we seek to understand the eddy effect on buoyancy advection, all three formulations agree on patterns and intensity, even close to 8i and 9i.”
Quote in the paperNot a substantial claim - Findingown data
A subsurface undercurrent in opposite direction hugs the continental slope with maximal velocities of 0.15 m s^-1 in 150-200-m depth.
“A subsurface undercurrent in opposite direction hugs the continental slope with maximal velocities of 0.15 m s 21 in 150-200-m depth (Fig. 5c).”
Quote in the paperNot a substantial claim - Findingown data
Submesoscale processes, poorly represented in mesoscale runs, matter in the mixed layer and immediately below it.
“Inspecting Figs.7a, 7c, and 7d confirms that submesoscale processes (poorly represented in mesoscale runs) matter in the mixed layer and immediately below it.”
Quote in the paperSubstantial claim - Findingown data
Typically an anticyclonic mesoscale warm core eddy forms at some point near the shelf break with diameter of roughly 150 km and a sea level anomaly of about 10 cm.
“Typically an anticyclonic mesoscale warm core eddy forms at some point near the shelf break with diameter of roughly 150 km and a sea level anomaly of about 10 cm (Figs.6a,b).”
Quote in the paperNot a substantial claim - Findingown data
Although w'b' declines with depth below the mixed layer, it remains enhanced down to about 100-m depth within about 100 km from shore, where the tilt of the isopycnals is most pronounced.
“Although w 0 b 0 exhibits a marked decline with depth below the mixed layer, it remains enhanced down to about 100-m depth within about 100 km from the shore, i.e., where the tilt of the isopycnals is most pronounced (Fig. 7a).”
Quote in the paperNot a substantial claim - Findingown data
The wind forcing results in an offshore Ekman transport in the upper 30-40 m of the water column.
“The wind forcing results in an offshore Ekman transport in the upper 30-40 m of the water column (Fig. 5d).”
Quote in the paperNot a substantial claim - Findingown data
The lower part of the eddy cell weakens by over 50%, from -1.3 m2 s-1 in NF to -0.55 m2 s-1 in HF, at 70 km offshore and 75-m depth.
“For instance, the lower part of the eddy cell weakens by over 50% (from 21.3 m 2 s 21 in NF to 20.55 m 2 s 21 in HF) at 70 km offshore and 75-m depth.”
Quote in the paperSubstantial claim - Findingown data
Further offshore, 200 km from the coast, maximum w'b' values decrease to 0.6-0.9e-7 m2 s-3 at 20-m depth.
“Further offshore 200 km from the coast the maximum values decrease to values from 0.6 to 0.9 3 10 27 m 2 s 23 in 20-m depth (Fig. 7a).”
Quote in the paperNot a substantial claim - Findingown data
Averaged between 16 and 112 km offshore, w'b' decreases from maximum 1.44e-7 m2 s-3 in NF to 1.06e-7 m2 s-3 in HF, about a 25% decrease.
“With increasing air-sea flux w 0 b 0 decreases (Fig. 7c) from maximum values 1.44 3 10 27 m 2 s 23 in the NF case to 1.06 3 10 27 m 2 s 23 in the HF case, when averaged between 16 and 112 km offshore.This represents a decrease of about 25%.”
Quote in the paperSubstantial claim - Findingown data
The general thermal structures and circulation features of the idealized upwelling configuration resemble those typical of real upwelling systems.
“The general thermal structures and circulation features of the idealized upwelling configuration resemble those typical of real upwelling systems (Figs. 5 and 6).”
Quote in the paperSubstantial claim - Findingown data
In the upper 50 m at 200 km and down to 100 m closer to the shelf break, the intensity of the residual circulation is smaller than that of the mean Eulerian circulation by a factor of 4 or more.
“In the upper 50 m at 200 km and even down to 100 m closer to the shelf break the intensity of the residual circulation is smaller than that of the mean Eulerian circulation by a factor of 4 or more.”
Quote in the paperSubstantial claim - Findingown data
Mean surface temperatures as low as 14°C are simulated at the shelf break.
“Mean surface temperatures as low as 148C are simulated at the shelf break (Figs.5c,d).”
Quote in the paperNot a substantial claim - Findingown data
The shoaling of maximum w'b' from 19 m in NF to 15 m in HF is associated with thinning of the mixed layer from 27 m in NF to 23 m in HF with increasing air-sea flux.
“The shoaling of the maximum w 0 b 0 (19 m in NF and 15 m in HF, Fig. 7c) is associated with a thinning of the mixed layer (27 m in NF and 23 m in HF, Fig. 7c) with increasing air-sea flux.”
Quote in the paperNot a substantial claim - Findingown data
An alongshore surface jet of about 0.4 m s^-1 in same direction as wind forcing develops over the shelf and upper slope.
“An alongshore surface jet of about 0.4 m s 21 in same direction as wind forcing develops over the shelf and upper slope (Fig. 5c).”
Quote in the paperNot a substantial claim - Findingown data
Mixed layer depths between 60 and 100 m are reached in 5% of the time.
“More specifically, mixed layer depths between 60 and 100 m are reached in 5% of the time.”
Quote in the paperSubstantial claim - Findingown data
Similar decreases are found between simulations with medium and high heat fluxes.
“Similar decreases are found between simulations with medium and high heat fluxes.”
Quote in the paperNot a substantial claim - Findingown data
Downward velocities of up to 100 m day^-1 are found at the cold side of these fronts.
“Downward velocities of up to 100 m day 21 are found at the cold side of these fronts (e.g., at x 5 150-200 km and y 5 150 km in Fig. 6c).”
Quote in the paperSubstantial claim - Findingown data
In the HF case, all three methods show cancellation levels of around 40%.
“In the HF case all three methods show cancellation levels of around 40%.”
Quote in the paperNot a substantial claim - Findingown data
Below 50-m depth, release of available potential energy in mesoscale and submesoscale runs is indistinguishable.
“Below 50-m depth release of available potential energy in mesoscale and submesoscale runs are indistinguishable.”
Quote in the paperNot a substantial claim - Findingnone given
Advective feeding of the surface layer with upwelling water vanishes.
“Most importantly, advective feeding of the surface layer with upwelling water vanishes.”
Quote in the paperSubstantial claim - Findingown data
A frontal zone separates the upwelling waters from the open ocean where surface temperatures increase to 20°C at 200 km offshore.
“A frontal zone separates the upwelling waters from the open ocean where surface temperatures increase to 208C at 200 km offshore (Figs.5c,d).”
Quote in the paperNot a substantial claim - Findingown data
Below the mixed layer, eddy streamfunction differences between mesoscale and submesoscale simulations are small and presumably not significant given the dispersion within the ensemble runs.
“Below the mixed layer eddy streamfunction differences between mesoscale and submesoscale simulations are small and presumably not significant given the dispersion within the ensemble runs.”
Quote in the paperNot a substantial claim - Findingown data
The mean cross-shore distribution of w'b' shows maximum values above 1.8e-7 m2 s-3 at 20-m depth around 30 km offshore during the NF case at submesoscale resolution.
“The mean crossshore distribution of w 0 b 0 shows maximum values above 1.8 3 10 27 m 2 s 23 at 20-m depth at around 30 km offshore during the NF case at submesoscale resolution (Fig. 7a).”
Quote in the paperNot a substantial claim - Findingown data
The Eulerian circulation is broadly consistent with isopycnal doming in the upper 150 m of the water column especially within 80 km from shore.
“The Eulerian circulation is broadly consistent with isopycnal doming in the upper 150 m of the water column especially within 80 km from shore (Figs.5c,d).”
Quote in the paperNot a substantial claim - Findingown data
In contrast to C_Mean, the sensitivity of the eddy-induced and residual circulation to air-sea heat forcing is noticeable well below the mixed layer base.
“In contrast to C Mean , the sensitivity of the eddy-induced and residual circulation to air-sea heat forcing is noticeable well below the mixed layer base (Figs.9h,l).”
Quote in the paperSubstantial claim - Findingown data
The idealized upwelling solution produces turbulent structures as found in upwelling systems: mesoscale eddies, filaments and sharp submesoscale temperature fronts, particularly at the finest resolution.
“The idealized upwelling solution also produces turbulent structures as found in upwelling systems: mesoscale eddies, filaments and sharp submesoscale temperature fronts particularly at the finest resolution (Fig. 6a).”
Quote in the paperNot a substantial claim - Findingown data
At 125 m depth, residual streamfunction values above 1 m2 s-1 are found away from the coast where the tilt of the isopycnals and BCI strength is reduced.
“At greater depth (125 m) residual streamfunction values above 1 m 2 s 21 are found away from the coast (Fig. 8i) where the tilt of the isopycnals and BCI strength (Fig. 7a) is reduced.”
Quote in the paperNot a substantial claim - Findingown data
The simulations fall in between the intermediate case and the total cancellation case.
“Our simulations fall in between the intermediate case and the total cancellation case.”
Quote in the paperSubstantial claim - Findingown data
Comparison between w'b' evolutions after day 80 for the three heat flux forcings reveals a fast adjustment process over about 3-5 days.
“Comparison between the w 0 b 0 x,e,S (t) evolutions after day 80 for the three heat flux forcings reveals a fast adjustment process that takes place over about 3-5 days (not shown).”
Quote in the paperSubstantial claim - Findingown data
Following the initial adjustment, APE release remains approximately stable until day 120.
“Following this initial adjustment, APE release remains approximately stable until day 120 (not shown).”
Quote in the paperSubstantial claim - Findingown data
The absolute change in mixed layer w0b0 when going from mesoscale to submesoscale resolution is similar in Colas et al. (2012) and the present work (2.8e-8 in the NF case versus 4.5e-8 for the winter season off Peru in Colas et al. 2012).
“In reality, note that the absolute change in mixed layer w 0 b 0 when going from mesoscale to submesoscale rich model resolution is quite similar inColas et al. (2012) and our work (2.8 3 10 28 in our NF case in Fig.7cversus 4.5 3 10 28 for the winter season off Peru in Fig.10ofColas et al. 2012).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Colas et al. (2012)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Premisereasoning
Without an alongshore pressure gradient, no interior geostrophic onshore flow can be established.
“Without an alongshore pressure gradient no interior geostrophic onshore flow can be established.”
Quote in the paperSubstantial claim - Interpretationreasoning
The dominance of mesoscale dynamics in the cancellation effect might also hold for the real ocean as the relevant processes act below the surface boundary layer.
“which might also hold for the real ocean as the relevant processes act below the surface boundary layer.”
Quote in the paperNot a substantial claim - Premisereasoning
Due to the absence of any beta effect, there is no westward propagation of Rossby waves.
“Due to the absence of any b effect, there is no westward propagation of Rossby waves.”
Quote in the paperNot a substantial claim - Premisereasoning
In the reentrant upwelling channel, no alongshore pressure gradient can a priori exist at the system scale due to periodic boundary conditions.
“In our reentrant upwelling channel no alongshore pressure gradient can a priori exist at the system scale due to the periodic boundary conditions.”
Quote in the paperSubstantial claim - Study design and conductreasoning
The reduced bottom depth of 1960 m in combination with the high number of vertical levels results in relatively high vertical resolution especially near the surface.
“Here we use a reduced bottom depth of 1960 m in combination with the high number of vertical levels results in a relatively high vertical resolution especially near the surface.”
Quote in the paperSubstantial claim - Study design and conductreasoning
The duration of each experiment is only 40 days, which is insufficient to get statistically reliable averages.
“The duration of each experiment is only 40 days, which is insufficient to get statistically reliable averages.”
Quote in the paperSubstantial claim - Premisecitation
The remapping from temperature to depth space becomes problematic wherever the water column becomes well mixed or nearly so.
“Specifically, the remapping from temperature to depth space becomes problematic wherever the water column becomes well mixed or nearly so.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Nurser and Lee 2004a
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationnone given
These vertical velocities are a crucial part of the eddy flow that counteracts the Ekman transport of buoyancy.
“These vertical velocities are a crucial part of the eddy flow that counteracts the Ekman transport of buoyancy as we investigate in detail in the following chapter through three different approaches.”
Quote in the paperSubstantial claim - Interpretationreasoning
The eddy cancellation mechanism and its sensitivity to air-sea buoyancy forcing highlighted for submesoscale-permitting simulations result mainly from mesoscale turbulence effects.
“In short, the eddy cancellation mechanism and its sensitivity to air-sea buoyancy forcing highlighted in the previous section for submesoscale-permitting simulations results mainly from mesoscale turbulence effects.”
Quote in the paperSubstantial claim - Study design and conductown data
The elevated degree of cancellation obtained is for an upwelling configuration in which EKE is well above typical EBUS values.
“Pending discussion in section 4, note though that the elevated degree of cancellation we obtain is for an upwelling configuration in which EKE is well above typical EBUS values.”
Quote in the paperNot a substantial claim - Interpretationreasoning
The transition layer provides the required diabatic forcing to accommodate a slow but nonzero residual circulation consistent with upwelling to about 80-120-m depth that bifurcates offshore above this depth range.
“This provides the required diabatic forcing to accommodate a slow but nonzero residual circulation consistent with upwelling to about 80-120-m depth which bifurcates offshore above this depth range (Figs.8i and 9i).”
Quote in the paperSubstantial claim - Premisecitation
A transition layer with relatively elevated mixing levels is found below the mixed layer.
“Although our simulations do not resolve all relevant processes, a transition layer with relatively elevated mixing levels is found below the mixed layer (Large et al. 1994;Johnston and Rudnick 2009).”
Quote in the paperSubstantial claim0 of 2 sources checked - Interpretationcitation
This signature is improperly captured by isopycnal averaging at constant cross-shore distance.
“As expected, this signature is improperly captured by isopycnal averaging at constant cross-shore distance (Held and Schneider 1999).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Held and Schneider 1999 source
- Interpretationreasoning
Elevated EKE is an inherent consequence of the periodic channel simplification with which the beta effect is not compatible.
“Elevated EKE is an inherent consequence of our periodic channel simplification with which the b effect is not compatible.”
Quote in the paperSubstantial claim - Study design and conductreasoning
The simulations analyzed have EKE levels that significantly exceed those found in the real ocean, by a factor of 2-10 depending on the EBUS sector.
“First and foremost, the simulations we analyze have EKE levels that significantly exceed those found in the real ocean, by a factor of 2-10 depending on which EBUS sector is considered.”
Quote in the paperSubstantial claim - Interpretationown data
The eddy-induced circulation can counteract, or cancel, mean advection by the Ekman circulation to a large degree.
“The results suggest that (i) the eddy-induced circulation can counteract (or cancel in the SO terminology) mean advection by the Ekman circulation to a large degree”
Quote in the paperSubstantial claim - Interpretationown data
Mean buoyancy advection by the Ekman indirect overturning circulation is strongly counteracted by eddies when air-sea heat fluxes are such that no or limited diapycnal flow occurs in the surface layer, as Walin theory would predict in steady state.
“Beyond modest quantitative differences the main robust conclusion concerns the sensitivity of the eddy and residual circulation to air-sea heat fluxes: just as the Walin theory would predict in a steady state situation, mean buoyancy advection by the Ekman indirect overturning circulation is strongly counteracted by the eddies when the air-sea heat fluxes are such that no or limited diapycnal flow”
Quote in the paperSubstantial claim - Interpretationown data
The fact that simulations for different air-sea flux cases exhibit similar residual circulations indicates that the transient-adjustment reason is secondary.
“The fact that our simulations for the different air-sea flux cases exhibit similar residual circulations indicates that this reason is secondary.”
Quote in the paperSubstantial claim - Premisereasoning
The present result is seemingly at odds with previous studies including Colas et al. (2012), where a 15-fold increase in horizontal resolution strongly increases APE to EKE conversion near the surface.
“This result is seemingly at odds with previous studies includingColas et al. (2012, their Fig.10) where a 15-fold increase in horizontal resolution strongly increases APE to EKE conversion near the surface.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Colas et al. (2012)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
The real ocean behavior is expected to differ, with much smaller eddy effects in terms of Ekman flow cancellation than those reported.
“As thoroughly discussed in the previous section, the real ocean behavior is expected to differ, with much smaller eddy effects in terms of Ekman flow cancellation than the ones we reported.”
Quote in the paperSubstantial claim - Interpretationown data
The California Current System is the system where eddy cancellation is expected to be strongest and possibly cancel a large fraction of the Ekman circulation in some circumstances (up to 30%-40%).
“The CCS is the system where eddy cancellation is expected to be strongest and possibly cancel a large fraction of the Ekman circulation in some circumstances (up to 30%-40%, Fig. 11).”
Quote in the paperSubstantial claim - Premisecitation
Two estimations of the eddy cancellation strength in the California Current System can be drawn from Nagai et al. (2015) and Colas et al. (2013).
“Two estimations of the eddy cancellation strength in the California current system can be drawn from Nagai et al. (2015) and Colas et al. (2013).”
Quote in the paperNot a substantial claim0 of 2 sources checked - Interpretationown data
These results are consistent with the well-accepted view that the role of eddies in EBUS is not of leading order, as it is in the Southern Ocean.
“These results are consistent with the wellaccepted view that the role of eddies in EBUS is not of leading order (as it is in the SO).”
Quote in the paperNot a substantial claim - Premisecitation
The absence of beta precludes the westward radiation of energy, for instance through Rossby wave propagation or beta drift of vortices.
“The absence of beta precludes the westward radiation of energy, for instance through Rossby wave propagation or beta drift of vortices (Carton 2010).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Carton 2010
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- Interpretationreasoning
The eddy contribution to buoyancy advection tends to counteract advection by the Ekman transport, so as to limit the slope of the isopycnals.
“The eddy contribution to buoyancy advection tends to counteract the advection by the Ekman transport, so as to limit the slope of the isopycnals.”
Quote in the paperSubstantial claim - Interpretationcitation
Diagnostics of the eddy-induced circulation in realistic simulations for this upwelling sector tend to confirm our estimates.
“Diagnostics of the eddy-induced circulation in realistic simulations for this upwelling sector tend to confirm our estimates.”
Quote in the paperSubstantial claim0 of 2 sources checked - Interpretationown data
Figure 11 provides estimates for the amount of cancellation in the four EBUS, going from 3% to 6% in the northern Benguela to 10%-30% in the California Current System.
“It provides estimates for the amount of cancellation in the four EBUS, going from 3% to 6% in the northern Benguela, to 10%-30% in the California Current System.”
Quote in the paperSubstantial claim- The authors state this as an assumption: The intensity of the eddy overturning streamfunctions scales linearly with EKE.
- Interpretationcitation
Both prior estimates of eddy cancellation strength are within the range of values inferred from the present study.
“Both estimates are within the range of values inferred from the present study.”
Quote in the paperNot a substantial claim - Premisecitation
Slightly weaker but comparable values of 10%-15% are obtained in Colas et al. (2013) for summer, when upwelling winds and air-sea heat fluxes are most positive.
“Slightly weaker but comparable values of 10%-15% are obtained in Colas et al. (2013) for summer, when upwelling winds and air-sea heat fluxes are most positive.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Colas et al. (2013) source
- Study design and conductnone given
Drifts in the thermohaline structure of the simulations remain small.
“However, drifts in the thermohaline structure of our simulations remain small”
Quote in the paperSubstantial claim - Interpretationreasoning
The efficiency of eddy cancellation varies with the strength of air-sea buoyancy flux forcing: eddies are most effective at impeding transport of buoyancy by Ekman currents when air-sea buoyancy fluxes provide no or limited warming of upwelled surface waters drifting offshore, allowing more intense and deeper-reaching frontal conditions.
“The efficiency of this eddy cancellation process varies with the strength of the air-sea buoyancy flux forcing: eddies are most effective at impeding the transport of buoyancy by Ekman currents in situations where air-sea buoyancy fluxes provide no or limited warming of upwelled surface waters drifting offshore, which allows more intense and deeperreaching frontal conditions to be produced.”
Quote in the paperSubstantial claim - Interpretationreasoning
The alongshore periodicity also limits the time-averaging and/or ensemble run size requirements in a context where stochastic variability is important and can blur the role of eddies and its sensitivity to forcings.
“It also limits the time-averaging and/or ensemble run size requirements in a context where stochastic variability is important and can blur the role of eddies and its sensitivity to forcings.”
Quote in the paperSubstantial claim - Premisecitation
Maximum eddy-induced streamfunction values for summer reported in Colas et al. (2013) reach about 0.2 m2 s-1, i.e., about 15% of the Ekman transport for that season.
“Maximum eddy-induced streamfunction values for summer reported in Colas et al. (2013, see their Fig.8) reach about 0.2 m 2 s 21 , i.e., about 15% of the Ekman transport for that season.”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Colas et al. (2013) source
- Premisecitation
Counting streamfunction contours in Nagai et al. (2015) gives an annual mean eddy cancellation intensity of about 25% of the Ekman flow at 50-m depth and 100 km from shore for central California.
“Counting streamfunction contours in Figs.5a and 5b of Nagai et al. (2015) gives an annual mean eddy cancellation intensity ;2/8 5 25% of the Ekman flow at 50-m depth and 100 km from shore for central California.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Nagai et al. (2015) source
- Interpretationreasoning
The apparent conflict between the present result and Colas et al. (2012) is misleading because of the great difference in subsurface mesoscale w0b0 between the idealized simulations and a real upwelling system like the Humboldt system.
“The reason why the comparison is misleading at first sight is the great difference in subsurface mesoscale w 0 b 0 between our idealized simulations and a real upwelling system like the Humboldt system (see section 4).”
Quote in the paperSubstantial claim - Interpretationreasoning
The relationship V_ek (b_y)_ml = B_ml(y) may exert a strong constraint on the mean upper-ocean thermohaline structure of upwelling systems, because given the wind and buoyancy forcings (b_y)_ml would need to adjust so that the left- and right-hand sides match.
“This relationship may seem to exert a strong constraint on the mean upper-ocean thermohaline structure of upwelling systems because given the wind and buoyancy forcings (b y ) ml would need to adjust so that the leftand right-hand side can match.”
Quote in the paperNot a substantial claim- The authors state this as an assumption: The upwelling channel is alongshore periodic, making the alongshore eddy flux component u0b0 irrelevant.
- The authors state this as an assumption: The flow is 2D laminar and steady-state, with Ekman circulation as the only flow component.
- The authors state this as an assumption: The buoyancy gradient in the mixed layer is horizontal (no vertical stratification) and independent of depth.
- The authors state this as an assumption: Heat is neglected in the mixed layer integration.
- Interpretationreasoning
Under the assumptions of a 2D laminar steady-state upwelling with only Ekman circulation, a horizontal and depth-independent mixed-layer buoyancy gradient, and neglected heat, the vertical integral of the buoyancy equation yields V_ek (b_y)_ml = B_ml(y).
“Integrating vertically over the mixed layer in which the buoyancy gradient is supposed to be horizontal (no vertical stratification) and independent of depth, and neglecting heat, we find”
Quote in the paperSubstantial claim- The authors state this as an assumption: The upwelling channel is alongshore periodic, making the alongshore eddy flux component u0b0 irrelevant.
- The authors state this as an assumption: The flow is 2D laminar and steady-state, with Ekman circulation as the only flow component.
- The authors state this as an assumption: The buoyancy gradient in the mixed layer is horizontal (no vertical stratification) and independent of depth.
- The authors state this as an assumption: Heat is neglected in the mixed layer integration.
- May combine two claims. 38
- Classified as probably not a substantial claim. 40
May combine two claims.
PremisecitationEddy effects generally oppose the Ekman circulation, resulting in eddy cancellation, a process well studied in the Southern Ocean.
“Eddy effects generally oppose the Ekman circulation, resulting in so-called ''eddy cancellation,'' a process well studied in the Southern Ocean.”
Quote in the paperSubstantial claim2 of 3 sources checkedMay combine two claims.
PremisecitationQuasi-balanced mesoscale and submesoscale turbulence is responsible for rectified eddy transport which also tends to counteract the Ekman upwelling cell.
“quasi-balanced mesoscale and submesoscale turbulence is responsible for rectified eddy transport which also tends to counteract the Ekman upwelling cell.”
Quote in the paperSubstantial claim1 of 3 sources checked- cites Lathuilière et al. 2010 source
The Summary (§5; page unavailable) reports that mesoscale circulation and filaments transport nitrate and phytoplankton offshore. But the Discussion (§4; page unavailable) explicitly says that rectification of the mean flow by mesoscale dynamics was not addressed. The paper does not establish that eddy transport counteracts the Ekman upwelling cell; its Physical Model (§2.1; page unavailable) attributes compensating onshore transport to an imposed alongshore pressure gradient. (LLM, conf=0.84)
Experimental — accuracy not yet measured - cites Gruber et al. 2011 source
- cites Colas et al. 2013 source
Probably not a substantial claim: may not pass S3 (load-bearing).
Study design and conductreasoningSpurious diapycnal mixing associated with the WENO scheme has negligible effects in this study.
“Spurious diapycnal mixing associated with this scheme cannot be entirely avoided but shall have negligible effects in our study”
Quote in the paperNot a substantial claim1 of 2 sources checked- cites Marchesiello et al. (2009)
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Lemarié et al. (2012) source
Section 2, “Active Tracer Advection,” says numerical schemes must respect small levels of diapycnal mixing, and Section 2.1 says spurious mixing should be kept as small as possible. But the paper describes a modified RSUP3 scheme, not WENO, and does not establish that WENO-associated mixing has negligible effects in the citing authors’ study. Section 6.1 instead reports significant mixing for diffusion along σ-surfaces in long-term simulations. (LLM, conf=0.78)
Experimental — accuracy not yet measured
Classified as probably not a substantial claim.
PremisecitationIn the Southern Ocean, air-sea buoyancy fluxes are much more informative than the wind forcing with respect to the meridional tracer transport.
“There air-sea buoyancy fluxes are, somewhat counterintuitively, much more informative than the wind forcing with respect to the meridional tracer transport (Marshall 1997;Gent 2016).”
Quote in the paperSubstantial claim1 of 2 sources checked- cites Marshall 1997 source
- cites Gent 2016 source
The Introduction says the Southern Ocean overturning circulation affects uptake of heat, carbon dioxide, and other tracers. The Discussion reports that buoyancy-driven variability produced a much larger change than Southern Hemisphere winds in the North Atlantic overturning circulation. Neither passage establishes that air–sea buoyancy fluxes are more informative than winds for meridional tracer transport in the Southern Ocean; the comparison concerns a different region and quantity. (LLM, conf=0.78)
Experimental — accuracy not yet measured
Probably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
PremisecitationIn many upwelling sectors, alongshore pressure gradients can yield onshore velocities that counteract, or more infrequently reinforce, the Ekman flow.
“In many upwelling sectors they can yield onshore velocities that counteract, or more infrequently reinforce, the Ekman flow (Colas et al. 2008;Marchesiello et al. 2010;Ndoye et al. 2017;Jacox et al. 2018).”
Quote in the paperNot a substantial claim1 of 3 sources checked- cites Colas et al. 2008 source
- cites Marchesiello et al. 2010 source
- cites Ndoye et al. 2017 source
Section 3.3 reports that alongshore gradients produce onshore geostrophic flow over the southern Senegal shelf, reducing or reversing the offshore flow expected from Ekman transport. The paper does not establish that this happens in many upwelling sectors, or that reinforcement of Ekman flow occurs less frequently. Page numbers are not available in our copy. (LLM, conf=0.86)
Experimental — accuracy not yet measured
May combine two claims.
Findingown dataFor zero heat fluxes, the release of available potential energy by baroclinic instabilities is strongest and leads, near the coast, to nearly full cancellation of the Ekman cross-shore circulation by eddy effects, i.e., zero net mean upwelling flow.
“For zero heat fluxes the release of available potential energy by baroclinic instabilities is strongest and leads, near the coast, to nearly full cancellation of the Ekman cross-shore circulation by eddy effects, i.e., zero net mean upwelling flow.”
Quote in the paperSubstantial claimMay combine two claims.
Findingown dataWith increasing heat fluxes, eddy cancellation is reduced and the transverse flow progressively approaches the classical Ekman circulation.
“With increasing heat fluxes eddy cancellation is reduced and the transverse flow progressively approaches the classical Ekman circulation.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingnone givenThe first baroclinic Rossby Radius is around 57 km within the idealized setting.
“The first baroclinic Rossby Radius is around 57 km within our idealized setting.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown dataBecause the mean cross-shore buoyancy gradient b_y is weakly sensitive to resolution, similar reductions of about 25% are found for the intensity of C_TEM Eddy in the mixed layer.
“The mean cross-shore buoyancy gradient b y being weakly sensitive to resolution similar reductions of about 25% are found for the intensity of C TEM Eddy in the mixed layer (cf.Figs.7b,e).”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown dataAt the chosen location, eddies cancel between 72% (C_iso2y Eddy) and 87% (C_iso2h Eddy) of the Ekman transport for NF, while cancellation reduces to between 46% (C_iso2y Eddy) and 60% (C_iso2h Eddy) for MF.
“At the chosen location, the eddies cancel between 72% (C iso2y Eddy ) and 87% (C iso2h Eddy ) of the Ekman transport for NF while the cancellation reduces to between 46% (C iso2y Eddy ) and 60% (C iso2h Eddy )for MF (Fig. 10b).”
Quote in the paperSubstantial claimMay combine two claims.
Findingown dataC_TEM Eddy sign is systematically negative and almost mirrors the structure of the mean streamfunction C_Mean.
“Its sign is systematically negative, and it almost mirrors the structure of the mean streamfunction (C Mean ) shown in Fig. 8a.”
Quote in the paperSubstantial claimMay combine two claims.
Findingown dataSeveral smaller-scale cyclonic vortices are formed around the anticyclone with cold filaments at the edges of the mesoscale structures.
“Several smaller-scale cyclonic vortices are formed around the anticyclone with cold filaments at the edges of the mesoscale structures (Figs.6a,b).”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown dataBelow 125-m depth, domain-averaged w'b' curves for all air-sea flux cases show almost no difference and vanish at around 200-m depth.
“Below 125-m depth the domain-averaged w 0 b 0 curves for all airsea flux cases show almost no difference and vanish at around 200-m depth (Fig. 7c)”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingown dataWithin the filaments the SST can drop down to about 18°C.
“Within the filaments the SST can drop down to about 188C.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown dataAlthough a large degree of eddy-mean cancellation is still present at HF, its residual circulation has recovered a structure that more closely resembles the mean Ekman circulation, with some streamlines connecting the offshore-subsurface to the nearshore-surface sectors.
“Although a large degree of eddy-mean cancellation is still present at HF its residual circulation has recovered a structure that more closely resembles the mean Ekman circulation, with some streamlines unambiguously connecting the offshoresubsurface to the nearshore-surface sectors.”
Quote in the paperSubstantial claimMay combine two claims.
Findingown dataThe entire region of interest is in close proximity to the mean mixed-layer base and is subjected to intense intermittent mixing.
“Second, and more importantly, our entire region of interest is in close proximity to the mean ML base, and it is subjected to intense intermittent mixing.”
Quote in the paperSubstantial claimMay combine two claims.
Findingown dataEddy streamfunction reaches values down to -2.8 m2 s-1, stronger in opposing direction than the mean Eulerian streamfunction (2.3 m2 s-1).
“The eddy streamfunction reaches values down to 22.8 m 2 s 21 , which is stronger (in opposing direction) than the mean Eulerian streamfunction (2.3 m 2 s 21 , Fig. 5d).”
Quote in the paperSubstantial claimMay combine two claims.
Findingown dataThe Ekman cell (C_Mean) is closed by a return flow reaching down to 200-m depth and has a maximum strength of 2.3 m^2 s^-1 around 50-m depth.
“The Ekman cell (C Mean ) is closed by a return flow reaching down to 200-m depth and has a maximum strength of 2.3 m 2 s 21 around 50-m depth (Fig. 5d).”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Findingown dataSubmesoscale frontal dynamics are richer at the higher resolution.
“Submesoscale frontal dynamics are obviously richer at the higher resolution.”
Quote in the paperNot a substantial claimMay combine two claims.
Findingown dataThe eddies play an important role, so that the neglect of the bolus velocity in Eq. (A9) is invalid; this is also the case in the Southern Ocean.
“In contrast we find that the eddies play an important role so that the neglect of the bolus velocity in (A9) is invalid (this is also the case in Southern Ocean).”
Quote in the paperSubstantial claimMay combine two claims.
Findingown dataOver the relatively short study periods (40 days) analyzed, the temporal tendency term could contribute to the balance, but it is not found to be important.
“Over relatively short study periods (40 days for the analyses we carried out) temporal tendency could contribute to the balance but we do not find this term to be important.”
Quote in the paperNot a substantial claimClassified as probably not a substantial claim.
PremisereasoningIt is widely accepted that the sole knowledge of the wind forcing does not provide useful insight into the mean cross-frontal circulation of the Southern Ocean.
“As a result, it is widely accepted that the sole knowledge of the wind forcing does not provide useful insight into the mean cross-frontal circulation of the SO.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationThe initial temperature profile T_o(z) is typical of (sub)tropical eastern boundary upwelling systems.
“It is chosen to be typical of (sub)tropical EBUS.”
Quote in the paperNot a substantial claim0 of 2 sources checkedProbably not a substantial claim: may not pass S3 (load-bearing).
Premisenone givenThe first part of Eq. (3) prescribes the intensified stratification within the upper 250 m as typically found in eastern boundary systems.
“The first part of Eq. ( 3) prescribes the intensified stratification within the upper 250 m as typically found in eastern boundary systems.”
Quote in the paperNot a substantial claimClassified as probably not a substantial claim.
PremisecitationIn the Southern Ocean, transport transverse to the Antarctic Circumpolar Current axis computed in isopycnal coordinates is a small residual between the mean Ekman-driven circulation due to wind pumping/suction (the Deacon cell) and eddy-induced transfers of mass driven by baroclinic instability processes.
“In the SO, transport in the direction transverse to the Antarctic Circumpolar Current (ACC) axis computed in isopycnal coordinates is a small residual between the mean Ekman-driven circulation due to wind pumping/suction (the so-called Deacon cell) and eddy-induced transfers of mass driven by baroclinic instability processes (Marshall and Radko 2006;Marshall and Speer 2012).”
Quote in the paperSubstantial claim0 of 2 sources checkedProbably not a substantial claim: may not pass S4 (based). May combine two claims.
PremisereasoningDue to the turbulent nature of the ocean, eddy fluxes are not solely determined by the forcings and are subjected to intrinsic stochastic variability, in addition to not being in statistical equilibrium.
“Due to the turbulent nature of the ocean the eddy fluxes are not solely determined by the forcings and are subjected to intrinsic stochastic variability (in addition to not being in statistical equilibrium).”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Premiseown dataThese heat flux values are typical of net heat flux forcings in EBUS although large variability exists.
“These values are typical of net heat flux forcings in EBUS although large variability exists (Fig. 2).”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Fig. 2
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Classified as probably not a substantial claim.
Study design and conductnone givenEddy cancellation is consistently evaluated with three different methods that all account for the quasi-isopycnal nature of ocean circulation away from the surface.
“Eddy cancellation is consistently evaluated with three different methods that all account for the quasi-isopycnal nature of ocean circulation away from the surface.”
Quote in the paperSubstantial claimClassified as probably not a substantial claim.
Study design and conductcitationApplying all three approaches to determine residual overturning streamfunctions ensures that the main findings are robust.
“Thus, we apply all three of them to ensure that our main findings are robust, as previously done for the SO or in the atmosphere.”
Quote in the paperSubstantial claimMay combine two claims.
Interpretationnone givenThe choice of parameters makes the results applicable to the Peruvian, West African, and northern Benguelan upwelling systems, and the main findings should also be valid at higher latitude.
“This choice of parameters makes our results applicable to the Peruvian, West African, and northern Benguelan upwelling systems, but the main findings should also be valid at higher latitude.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
PremisecitationThe transformed Eulerian mean formulation explicitly involves the rate of APE release and is able to accommodate outcropping situations.
“The first formulation explicitly involves the rate of APE release and is able to accommodate outcropping situations.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Held and Schneider (1999) source
Probably not a substantial claim: may not pass S4 (based). May combine two claims.
Interpretationnone givenUpwelling systems lack the periodicity attribute, so the ACC framework and theory are not directly applicable.
“One practical difficulty is that upwelling systems lack the periodicity attribute, so the ACC framework and theory are not directly applicable.”
Quote in the paperNot a substantial claimMay combine two claims.
PremisecitationThe eddy-induced circulation attempts to flatten isopycnal surfaces, reduce available potential energy, and therefore largely opposes the thermally direct Deacon cell.
“The eddy-induced circulation attempts to flatten isopycnal surfaces, reduce available potential energy, and therefore largely opposes the thermally direct Deacon cell.”
Quote in the paperSubstantial claim0 of 2 sources checkedProbably not a substantial claim: may not pass S3 (load-bearing).
InterpretationcitationThe absence of beta effect is presumably responsible for eddy kinetic energy levels above typical values found in the real ocean for EBUS sectors.
“but is presumably responsible for eddy kinetic energy (EKE) levels above typical values found in the real ocean for EBUS sectors (Haney et al. 2001;Marchesiello et al. 2003;Gruber et al. 2011).”
Quote in the paperNot a substantial claim0 of 3 sources checkedClassified as probably not a substantial claim.
PremisecitationBaroclinic instability processes are essential in upwelling systems as a source of mesoscale and submesoscale turbulence.
“Baroclinic instability (hereafter BCI) processes are known to be essential in upwelling systems as a source of mesoscale and submesoscale turbulence (Marchesiello et al. 2003).”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Marchesiello et al. 2003 source
Classified as probably not a substantial claim.
Study design and conductreasoningThe model uses 100 vertical sigma levels for all configurations to resolve sharp vertical velocity and temperature gradients in the upper ocean.
“To resolve sharp vertical velocity and temperature gradients in the upper ocean, we use 100 vertical sigma levels for all configurations.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationRare occurrences of warm water conditions at the surface strongly imprint on the form of C_iso2h_Res and its remapping.
“In addition, rare occurrences of warm water conditions at the surface strongly imprint on the form of C iso2h Res and its remapping (Nurser and Lee 2004a).”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Nurser and Lee 2004a
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
Probably not a substantial claim: may not pass S4 (based).
Study design and conductnone givenPerforming 12 ensemble runs for each experiment provides statistically reliable averages.
“to get statistically reliable averages.Thus we perform 12 ensemble runs for each experiment listed in Table 1.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S4 (based).
Interpretationnone givenThe rate at which water is transferred from the ocean interior into the mixed layer may not be simply related to the Ekman transport.
“However, the rate at which water is being transferred from the ocean interior into the mixed layer may not be simply related to the Ekman transport.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S4 (based).
Study design and conductnone givenThe degree of resemblance between C_TEM_Eddy, C_iso2h_Eddy, and C_iso2y_Eddy will be considered as an indication of robustness.
“The degree of resemblance between C TEM Eddy , C iso2h Eddy , and C iso2y Eddy will be considered as an indication of robustness.”
Quote in the paperNot a substantial claimMay combine two claims.
Study design and conductown dataThe circulation pattern is very similar for C_iso2y Eddy and C_iso2h Eddy, providing confidence in its robustness despite the proximity of the ocean surface and coastline.
“This circulation pattern is very similar for C iso2y Eddy and C iso2h Eddy which provides confidence in its robustness, despite the proximity of the ocean surface and coastline.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationThe result is consistent with the limited vertical extension of submesoscale turbulence, which is typically confined into the mixed layer in most oceanic regimes.
“Although this may seem surprising given the shallow nature of the problem under consideration, this is consistent with the limited vertical extension of submesoscale turbulence, which is typically confined into the mixed layer in most oceanic regimes [see Capet et al. (2016) for a counterexample where Charney instability is present].”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Capet et al. (2016) source
May combine two claims.
Interpretationown dataThe level of cancellation can be subjected to spatiotemporal modulations due to air-sea buoyancy flux variability, which can lead to changes in the degree to which eddy fluxes counteract the mean advection by the Ekman flow central in coastal upwelling dynamics.
“and (ii) the level of cancellation can be subjected to spatiotemporal modulations due to air-sea buoyancy flux variability, which can lead to changes in the degree to which eddy fluxes counteract the mean advection by the Ekman flow that is central in coastal upwelling dynamics.”
Quote in the paperSubstantial claimMay combine two claims.
InterpretationcitationIn the mixed layer, C_iso2y Res displays a reduction of the submesoscale restratification tendency consistent with theory, confirming the superiority of this formulation near the ocean surface.
“In the mixed layer, C iso2y Res displays a reduction of the submesoscale restratification tendency consistent with theory, which confirms the superiority of this formulation near the ocean surface (Held and Schneider 1999).”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Held and Schneider 1999 source
Probably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
Study design and conductown dataEddy and residual streamfunctions exhibit small spatial variations in their cross-shore-depth structures at different resolution, so the single-point comparison in Fig. 10 should not be overinterpreted.
“Also note that eddy and residual streamfunctions exhibit small spatial variations in their crossshore-depth structures at different resolution, so the single point comparison in Fig. 10 should not be overinterpreted.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationIsothermal averaging at constant z is strongly impacted near side boundaries where the structure of C_iso2y_Res can be difficult to interpret.
“On the other hand, isothermal averaging at constant z is strongly impacted near side boundaries where the structure of C iso2y Res can be difficult to interpret (Nurser and Lee 2004a;Lee and Nurser 2012).”
Quote in the paperNot a substantial claim0 of 2 sources checked- cites Nurser and Lee 2004a
Couldn’t be matched to a paper in Crossref, so it can’t be checked.
- cites Lee and Nurser 2012 source
Probably not a substantial claim: may not pass S3 (load-bearing).
InterpretationcitationEddy fluxes may also have an appreciable time-averaged effect on tracer advection in sectors of the California Current System where standing meanders yield intensified mesoscale and submesoscale activity.
“Eddy fluxes may also have an appreciable timeaveraged effect on tracer advection in sectors of the California Current System where standing meanders yield intensified mesoscale and submesoscale activity (Centurioni et al. 2008;Colas et al. 2013).”
Quote in the paperNot a substantial claim0 of 2 sources checkedProbably not a substantial claim: may not pass S3 (load-bearing).
InterpretationreasoningIn the northern Benguela and southern Canary Current sectors, where eddy cancellation is particularly weak, the alongshore pressure gradient effect and its temporal variability may be difficult to discern.
“In the northern Benguela and southern Canary current sectors where the eddy cancellation is particularly weak this effect and its temporal variability may thus be difficult to discern.”
Quote in the paperNot a substantial claimMay combine two claims.
Interpretationown dataThe modulation of the eddy cancellation process in response to environmental changes should occur on synoptic and longer time scales, including seasonal and interannual, but not on shorter time scales such as a diurnal cycle.
“From this we infer that the modulation of the eddy cancellation process in response to environmental changes should occur on synoptic and longer times scales (including seasonal and interannual) but not on shorter time scales, e.g., as a response to a diurnal cycle.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
InterpretationreasoningIn the real ocean, wind and air-sea buoyancy flux variability may be correlated and combine to produce results distinct from those found in this study.
“In the real ocean wind and air-sea buoyancy flux variability may be correlated and combine to produce results distinct from those found in this study.”
Quote in the paperNot a substantial claimMay combine two claims.
Interpretationown dataThe results point to the possible importance of eddy-induced circulations during periods when air-sea buoyancy forcings are weak and perhaps more so when they are temporarily negative.
“But they point to the possible importance of eddy-induced circulations during periods when air-sea buoyancy forcings are weak and perhaps more so when they are temporarily negative (see Fig. 2).”
Quote in the paperSubstantial claimMay combine two claims.
Interpretationown dataThe study suggests that a regional ocean model need not resolve submesoscale processes because eddy cancellation of the Ekman flow depends on subsurface turbulence that remains overwhelmingly linked to the mesoscale despite strong frontality.
“Our study suggests that such model need not resolve submesoscale processes: eddy cancellation of the Ekman flow depends on subsurface turbulence which, our study demonstrates, remains overwhelmingly linked to the mesoscale despite the strong frontality of the environment under investigation.”
Quote in the paperSubstantial claimMay combine two claims.
InterpretationcitationCancellation estimates derived from Fig. 11 ignore that beta drift is more effective at low latitude, which fundamentally alters the w'b'-EKE relationship.
“Thus, cancellation estimates derived from Fig. 11 ignore, for instance, the fact that beta drift is more effective at low latitude which fundamentally alters the w 0 b 0 -EKE relationship.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationAlongshore pressure gradient variability is another factor that can modulate upwelling intensity on synoptic, seasonal, and longer time scales, frequently in the sense of an upwelling reduction.
“Finally, note that alongshore pressure gradient variability is another factor that can modulate upwelling intensity on synoptic, seasonal, and longer time scales (Werner and Hickey 1983;Huyer et al. 1987;Colas et al. 2008;Marchesiello et al. 2010;McCabe et al. 2015;Jacox et al. 2018), frequently in the sense of an upwelling reduction.”
Quote in the paperNot a substantial claim0 of 3 sources checkedClassified as probably not a substantial claim.
InterpretationreasoningIdentifying and quantifying eddy cancellation in realistic model simulations is far more difficult, mainly because the alongshore periodicity of the numerical configuration offers a much simpler framework for analyses.
“Identifying and quantifying eddy cancellation in realistic model simulations is far more difficult, mainly because the alongshore periodicity of our numerical configuration offers a much simpler framework for analyses.”
Quote in the paperSubstantial claimProbably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
Study design and conductnone givenLimitations imposed by the idealized framework do not allow the study to work in steady state and limit the duration of experiments to periods of tens of days.
“Limitations imposed by our idealized framework do not allow us to work in steady state and limit the duration of our experiments to periods of tens of days.”
Quote in the paperNot a substantial claimMay combine two claims.
Study design and conductown dataThe study used three different standard methods and found good agreement between them in the idealized setting.
“Concerned by the methodological limitations inherent to eddy flux estimations and descriptions we used three different standard methods and found good agreement between them in our idealized setting.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Premiseown dataIn all EBUS, air-sea buoyancy fluxes exhibit fluctuations of large magnitude on synoptic and seasonal time scales.
“In all EBUS air-sea buoyancy fluxes exhibit fluctuations of large magnitude on synoptic and seasonal time scales as illustrated in Fig. 2 for nearshore sites.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningThe findings on the cancellation process itself do not specifically depend on the 40-day time scale, but the modulation of cancellation in response to air-sea buoyancy fluctuations may.
“Our findings on the cancellation process itself do not specifically depend on this particular time scale but the modulation of the cancellation in response to air-sea buoyancy fluctuations may.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Interpretationown dataIn the northern Humboldt, eddy cancellation is presumably stronger but still modest in magnitude, about 10%-20%.
“In the northern Humboldt the eddy cancellation is presumably stronger but still modest in magnitude (;10%-20%,”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S1 (asserted), S3 (load-bearing), S4 (based).
Premisenone givenStrong ocean cooling events from -200 to -500 W m-2 can occasionally occur in three of the four EBUS.
“Strong ocean cooling events (from 2200 to 2500 W m 22 ) can occasionally occur in three of the four EBUS.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
PremisecitationCorrelations between wind and air-sea buoyancy flux variability vary from place to place.
“Such correlations vary from place to place (Send et al. 1987;Beardsley et al. 1998;Flynn et al. 2017;Lübbecke et al. 2019).”
Quote in the paperNot a substantial claim0 of 3 sources checkedProbably not a substantial claim: may not pass S3 (load-bearing). May combine two claims.
Study design and conductreasoningWind variability has been ignored throughout the study, whereas it is an important aspect of upwelling dynamics.
“Third, for simplicity, wind variability has been ignored throughout the study whereas it is an important aspect of upwelling dynamics.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationcitationThe results can be interpreted using steady-state Walin-type reasoning: given the mean frontal thermohaline structure of an upwelling system, vanishing or negative air-sea buoyancy fluxes would imply that the surface Ekman flow produces diapycnal transport of mass unless counteracted by eddy transport, resulting in partial or total cancellation of mean buoyancy advection by the Ekman flow.
“our results can be interpreted using a steady-state Walin type reasoning (Marshall 1997): given the mean frontal thermohaline structure of an upwelling system vanishing (or negative) air-sea buoyancy fluxes would imply that the surface Ekman flow produces diapycnal transport of mass unless it is counteracted by eddy transport, resulting in partial or total cancellation of the mean buoyancy advect”
Quote in the paperSubstantial claim0 of 1 sources checked- cites Marshall 1997 source
May combine two claims.
InterpretationcitationBy analogy with Southern Ocean functioning and general understanding of baroclinic processes, the intensity of eddy cancellation mechanisms should roughly scale with that of the Ekman flow, so that increasing upwelling winds steepen isopycnals and increase the counteracting effect of eddies.
“By analogy with the SO functioning and in agreement with the general understanding of baroclinic processes the intensity of the eddy cancellation mechanisms shall roughly scale with that of the Ekman flow, i.e., we expect compensation (Marshall and Radko 2003) to occur whereby increasing upwelling winds steepens the isopycnals which increases the counteracting effect of eddies.”
Quote in the paperNot a substantial claim0 of 1 sources checked- cites Marshall and Radko 2003 source
Probably not a substantial claim: may not pass S3 (load-bearing).
Premisenone givenThe two studies (Nagai et al. 2015 and Colas et al. 2013) use very similar numerical configurations.
“Note that the two studies use very similar numerical configurations.”
Quote in the paperNot a substantial claim0 of 2 sources checkedMay combine two claims.
Interpretationown dataNet heat flux values are more typically in the range 0-150 W m-2, consistent with the forcings used in this study, so the results should be relevant to the real ocean provided that the rescaling of cancellation based on EKE levels is correct.
“Net heat fluxes values are more typically in the range 0-150 W m 22 (Fig. 2b), i.e., consistent with the forcings used in this study whose results should therefore be relevant to the real ocean, provided that the rescaling of cancellation based on EKE levels proposed above is correct.”
Quote in the paperSubstantial claim- The authors state this as an assumption: The intensity of the eddy overturning streamfunctions scales linearly with EKE.
- Rests on an assumption: The rescaling of cancellation based on EKE levels proposed in the study is correct.
May combine two claims.
Interpretationnone givenUpper range values correspond to situations with about zero net air-sea buoyancy fluxes, which are not very common in the California Current System when upwelling conditions prevail.
“Upper range values correspond to situations with '0 net air-sea buoyancy fluxes, which are not very common in this latter system when upwelling conditions prevail.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S3 (load-bearing).
Study design and conductown dataThe study was based on numerical simulations analyzed only over specific time periods of 40 days.
“Second, our study was based on numerical simulations that were analyzed only over specific time periods of 40 days.”
Quote in the paperNot a substantial claimProbably not a substantial claim: may not pass S2 (checkable).
Study design and conductreasoningThe simplifications taken advantage of have important implications in terms of model realism.
“However, the simplifications we take advantage of have important implications in terms of model realism.”
Quote in the paperNot a substantial claimMay combine two claims.
InterpretationreasoningIn real upwelling systems the eddy terms are not as strong as in the idealized simulations, but the upper-ocean buoyancy balance can also involve a mean alongshore advection term because of lack of periodicity.
“In real upwelling systems the eddy terms are not as strong (see section 4), but the upper-ocean buoyancy balance can also involve mean alongshore advection term because of lack of periodicity.”
Quote in the paperNot a substantial claim
The paper relies on this without support.
Coastal upwelling rates are classically determined by the intensity of the upper-ocean offshore Ekman transport.
“Coastal upwelling rates are classically determined by the intensity of the upper-ocean offshore Ekman transport.”
The authors state this as an assumption.
The net buoyancy supply to the mixed layer (B_ml) mainly results from air-sea exchanges in the sector where coastal upwelling is taking place.
“The term B ml is the net buoyancy supply to the mixed layer, supposed to mainly result from air-sea exchanges sector where coastal upwelling is taking place (Fig. 2).”
The paper relies on this without support.
Net buoyancy input can arise from lateral fluxes at the northern and southern edges of the upwelling region, and this is an important source of complication.
“Net buoyancy input can arise from lateral fluxes at the northern and southern edges of the upwelling region, and this is an important source of complication.”
The paper relies on this without support.
Twelve ensemble runs per experiment are sufficient to obtain statistically reliable averages.
“Thus we perform 12 ensemble runs for each experiment listed in Table 1.”
The paper relies on this without support.
Simple Eulerian averaging produces transport fields with unrealistically large diapycnal components.
“Simple Eulerian averaging is well known to produce transport fields with unrealistically large diapycnal components (i.e., the flow associated with C Mean crosses the mean isopycnal surfaces and is therefore inconsistent with the weakly diabatic nature of interior ocean circulation).”
The paper relies on this without support.
The ocean sector where upwelling takes place is in close proximity to the eastern boundary and not situated very deep below the surface, with the depth range of interest from below the mixed layer down to 150-200 m or less.
“The ocean sector where upwelling takes place is in close proximity to the eastern boundary and not situated very deep below the surface.Indeed we are typically interested in the depth range from below the mixed layer down to 150-200-m depth or less, i.e., the source region of the upwelled water.”
The paper relies on this without support.
Submesoscale permitting simulations represent the turbulent processes more accurately.
“This is done for the submesoscale permitting simulations which represent the turbulent processes more accurately.”
The paper relies on this without support.
The proximity to the ocean surface has no effect on the isopycnal averaging at constant height method.
“The proximity to the ocean surface has no effect on this method.”
The authors state this as an assumption.
The intensity of the eddy overturning streamfunctions scales linearly with EKE.
“To make progress despite this important caveat we assume that the intensity of the eddy overturning streamfunctions scales linearly with EKE.”
The paper relies on this without support.
The rescaling of cancellation based on EKE levels proposed in the study is correct.
“provided that the rescaling of cancellation based on EKE levels proposed above is correct.”
The authors state this as an assumption.
The upwelling channel is alongshore periodic, making the alongshore eddy flux component u0b0 irrelevant.
“taking advantage of the alongshore periodicity of our upwelling channel (which makes the eddy flux component in that direction u 0 b 0 irrelevant)”
The authors state this as an assumption.
The flow is 2D laminar and steady-state, with Ekman circulation as the only flow component.
“In the situation of a 2D laminar and steady-state upwelling where the Ekman circulation is the only flow component”
The authors state this as an assumption.
The buoyancy gradient in the mixed layer is horizontal (no vertical stratification) and independent of depth.
“the buoyancy gradient is supposed to be horizontal (no vertical stratification) and independent of depth”
The authors state this as an assumption.
Heat is neglected in the mixed layer integration.
“neglecting heat”
Self-check
Percentages, sums and reported differences re-computed from the paper’s own numbers.
Each contradiction between two passages listed here was confirmed by an independent check.
Heat-flux relaxation coefficient has conflicting units
MinorThe methods describe dQ/dT in W K−1, whereas Table 1 labels the same parameter in W m−2 K−1.
“with dQ/dT being the relaxation coefficient (W K 21 ), and SST m the model SST”
“| (W m 22 K 21 ) | (N m 22 ) |”
Table lists 80-day runs, but the text describes 120-day runs
MinorTable 1 gives a duration of 80 days for every run, while the text says the experiments run for 120 days, including an 80-day spinup.
“| Submesoscale no flux, NF | 794 | 504, 756, 100 | 80 | 80 | 12 | 0 | 0.075 |”
“we restrict the duration of our experiment to 120 days (including a spinup of 80 days)”
Sponge-layer endpoints imply 94 km, not 96 km
MinorThe stated sponge layer begins at 506 km and ends at the boundary at 600 km, giving a width of 94 km rather than 96 km.
Reported 96 · recomputed 94
“a sponge layer of width equal to 96 km is included”
Figure 8 assigns panel (k) to two different results
MinorThe caption labels panel (k) as the HF residual streamfunction and also as the HF-minus-NF difference.
“and (c),(g),(k) HF air-sea buoyancy forcing.”
“(d),(h),(k) The difference between HF and NF forcing experiments.”
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Flagged first, then by citations
Research works printed but not linked: 65
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- Lübbecke, 2019, Causes and evolution of the southeastern tropical Atlantic warm event in early 2016, Climate Dyn., 53, 261, 10.1007/s00382-018-4582-8 · DOI
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- Colas, 2013, Mesoscale eddy buoyancy flux and eddy-induced circulation in eastern boundary currents, J. Phys. Oceanogr., 43, 1073, 10.1175/JPO-D-11-0241.1 · DOI · Paper page
- Karsten, 2002, Constructing the residual circulation of the ACC from observations, J. Phys. Oceanogr., 32, 3315, 10.1175/1520-0485(2002)032<3315:CTRCOT>2.0.CO;2 · DOI
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- McCabe, 2015, Seasonal cross-shelf flow structure, upwelling relaxation, and the alongshelf pressure gradient in the northern California Current System, J. Phys. Oceanogr., 45, 209, 10.1175/JPO-D-14-0025.1 · DOI
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Cited by
Sorted by citations
Physical processes and biological productivity in the upwelling regions of the tropical Atlantic
Brandt, P. N., Alory, G., Awo, F. M., Dengler, M., Djakouré, S., Koungue, R. A. I., Jouanno, J., Körner, M., Roch, M., & Rouault, M. P. (2023) · Ocean science · doi:10.5194/os-19-581-2023 · Cited by 52 · see citing works
Körner, M., Brandt, P. N., Illig, S., Dengler, M., Subramaniam, A., Bachèlery, M., & Krahmann, G. (2024) · Science Advances · doi:10.1126/sciadv.adj6686 · Cited by 35 · see citing works
“This can prolong the time upwelled nitrate-rich water spends near the surface before being subducted ( 60 ).”
BackgroundHow the Source Depth of Coastal Upwelling Relates to Stratification and Wind
He, J., & Mahadevan, A. (2021) · Journal of Geophysical Research Oceans · doi:10.1029/2021jc017621 · Cited by 28 · see citing works
Seasonal cycle of sea surface temperature in the tropical Angolan Upwelling System
Körner, M., Brandt, P. N., & Dengler, M. (2023) · Ocean science · doi:10.5194/os-19-121-2023 · Cited by 21 · see citing works
“, 2015) as well as the influence of lateral eddy fluxes (Thomsen et al., 2021).”
BackgroundOn the Pathways of Wind-Driven Coastal Upwelling: Nonlinear Momentum Flux and Baroclinic Instability
Li, D., & Ruan, X. (2023) · Journal of Physical Oceanography · doi:10.1175/jpo-d-23-0098.1 · Cited by 12 · see citing works
Chabert, P., Capet, X., Échevin, V., Lazar, A., Hourdin, C., & Ndoye, S. (2022) · Journal of Physical Oceanography · doi:10.1175/jpo-d-22-0092.1 · Cited by 7 · see citing works
Self-citationDynamics of Upwelling and Downwelling in a Channel Basin of the Baltic Sea
Masini, M., Koszalka, I. M., Nilsson, J., et al. (2025) · Tellus A Dynamic Meteorology and Oceanography · doi:10.16993/tellusa.4070 · Cited by 5 · see citing works
Formation of Eastern Boundary Undercurrents via Mesoscale Eddy Rectification
Stewart, A. L., Wang, Y., Solodoch, A., Chen, R., & McWilliams, J. C. (2024) · Journal of Physical Oceanography · doi:10.1175/jpo-d-23-0196.1 · Cited by 4 · see citing works
Fearon, G., Herbette, S., Veitch, J., Cambon, G., & Vichi, M. (2022) · Ocean Modelling · doi:10.1016/j.ocemod.2022.102069 · Cited by 3 · see citing works
Xie, C., Wei, H., & Wang, Y. (2023) · Journal of Physical Oceanography · doi:10.1175/jpo-d-23-0017.1 · Cited by 4 · see citing works
Chabert, P., Échevin, V., Aumont, O., Person, R., Hourdin, C., Pous, S., Machu, É., & Capet, X. (2024) · Journal of Plankton Research · doi:10.1093/plankt/fbae054 · Cited by 2 · see citing works
Self-citationThe Importance of Eddy Stirring in Wind-Driven Coastal Upwelling
Li, D., Wei, H., & Ruan, X. (2024) · Journal of Physical Oceanography · doi:10.1175/jpo-d-24-0066.1 · Cited by 3 · see citing works
Red Sea warming and its links to the Red Sea dipole and upwelling mechanisms
Kenawy, A. E., Bordbar, M. H., Mohamed, E. K., et al. (2025) · Journal of Marine Systems · doi:10.1016/j.jmarsys.2025.104066 · Cited by 1 · see citing works
The Upwelling Source Depth Distribution and Its Response to Wind Stress and Stratification
Weeks, E. M., Lösch, M., & Tziperman, E. (2024) · Journal of Physical Oceanography · doi:10.1175/jpo-d-23-0171.1 · Cited by 1 · see citing works
“These submesoscale eddies then drive a circulation that acts to restratify the upper ocean, countering the effects of the wind-driven Ekman circulation (Marshall and Radko 2003; Capet et al. 2008; Thomsen et al. 2021).”
InfluentialNonlinear Dynamics over the Inner Shelf and in the Surface Boundary Layer during Coastal Upwelling
Connolly, T. (2025) · Journal of Physical Oceanography · doi:10.1175/jpo-d-24-0042.1 · Cited by 1 · see citing works
Singular Phenomenon Analysis of Wind-Driven Circulation System Based on Galerkin Low-Order Model
Feng, P., Cao, S., & Liu, Z. (2024) · Applied Sciences · doi:10.3390/app14167329
- Authors
- Thomsen, S., Capet, X., & Echevin, V.
- Affiliations
- LOCEAN-IPSL, IRD/CNRS/Sorbonne Universités (UPMC)/MNHN, UMR 7159, Paris, France
- Centre National de la Recherche Scientifique (FR)
- Venue
- Journal of Physical Oceanography
- Publisher
- American Meteorological Society
- Published
- 2021-09-02
- ISSN
- 0022-3670 (ISSN-L)
- 1520-0485
- OpenAlex
- W3198774622
- Cited by
- 17
- References
- 65
- Citations by year
- 2025: 3 · 2024: 6 · 2023: 5 · 2022: 2 · 2021: 1
- FWCI
- 1.68
- Type
- journal article
- Language
- en
- Open access
- hybrid
- doi.org
- Licence
- other-oa
- Locations
- Journal of Physical Oceanography (publishedVersion, other-oa)
- HAL (Le Centre pour la Communication Scientifique Directe) (submittedVersion)
- Funders
- European Commission (HORIZON2020, 749699)
- Deutsche Forschungsgemeinschaft (SFB‐754)
- Topics
- Physical Sciences › Earth and Planetary Sciences › Oceanography › Oceanographic and Atmospheric Processes
- Physical Sciences › Earth and Planetary Sciences › Atmospheric Science › Meteorological Phenomena and Simulations
- Physical Sciences › Earth and Planetary Sciences › Oceanography › Ocean Waves and Remote Sensing
- Keywords
- coastal upwelling, baroclinic instability, Ekman transport, air-sea heat flux, buoyancy forcing, submesoscale turbulence, mesoscale eddies, available potential energy
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