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Remote Sensing of Air-Sea Fluxes

A special issue of Remote Sensing (ISSN 2072-4292). This special issue belongs to the section "Biogeosciences Remote Sensing".

Deadline for manuscript submissions: closed (31 January 2021) | Viewed by 39959

Special Issue Editor


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Guest Editor
Department of Ocean Sciences, Rosenstiel School of Marine and Atmospheric Science, University of Miami, Miami, FL, USA
Interests: satellite remote sensing of sea-surface temperature; ship-board hyperspectral radiometry; air–sea fluxes; ocean thermal skin layer

Special Issue Information

Dear Colleagues,

The ocean–atmosphere interface marks the boundary between the two major fluid components of the climate system. Exchange of heat, moisture, momentum, gases and solid particles between the ocean and atmosphere are of fundamental importance to better understanding and improved forecasting of the weather and climate change. Satellite remote sensing provides global data with rapid sampling at useful accuracies for many studies, and remote sensing from planes, aerial drones, and other platforms is used to study important processes and critical regions. Currently, we are in a fortunate position as remote sensing of the ocean surface and lower atmosphere has provided us with time series of consistent, accurate fields of two to three decades, and new satellites recently launched or in development are opening new research opportunities. Algorithm developments are improving the accuracy of measurements relevant to remote sensing of surface exchanges.

This idea of this Special Issue grew from the session at the ESA Living Planet Symposium 2019 on Surface Ocean—Lower Atmosphere Study (SOLAS) research, but prospective authors are not limited to this session. The journal welcomes contributions related to all aspects of remote sensing of the ocean surface and lower atmosphere for this Special Issue.

Dr. Peter Minnett
Guest Editor

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Keywords

  • Sea surface variables
  • Lower atmosphere variables
  • Surface radiative fluxes
  • Air–sea exchanges
  • Weather forecasting
  • Climate monitoring
  • Remote sensing theory
  • Satellite instruments

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Published Papers (8 papers)

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Research

19 pages, 5572 KiB  
Article
Air–Sea Interaction in the Central Mediterranean Sea: Assessment of Reanalysis and Satellite Observations
by Salvatore Marullo, Jaime Pitarch, Marco Bellacicco, Alcide Giorgio di Sarra, Daniela Meloni, Francesco Monteleone, Damiano Sferlazzo, Vincenzo Artale and Rosalia Santoleri
Remote Sens. 2021, 13(11), 2188; https://doi.org/10.3390/rs13112188 - 3 Jun 2021
Cited by 6 | Viewed by 3501
Abstract
Air–sea heat fluxes are essential climate variables, required for understanding air–sea interactions, local, regional and global climate, the hydrological cycle and atmospheric and oceanic circulation. In situ measurements of fluxes over the ocean are sparse and model reanalysis and satellite data can provide [...] Read more.
Air–sea heat fluxes are essential climate variables, required for understanding air–sea interactions, local, regional and global climate, the hydrological cycle and atmospheric and oceanic circulation. In situ measurements of fluxes over the ocean are sparse and model reanalysis and satellite data can provide estimates at different scales. The accuracy of such estimates is therefore essential to obtain a reliable description of the occurring phenomena and changes. In this work, air–sea radiative fluxes derived from the SEVIRI sensor onboard the MSG satellite and from ERA5 reanalysis have been compared to direct high quality measurements performed over a complete annual cycle at the ENEA oceanographic observatory, near the island of Lampedusa in the Central Mediterranean Sea. Our analysis reveals that satellite derived products overestimate in situ direct observations of the downwelling short-wave (bias of 6.1 W/m2) and longwave (bias of 6.6 W/m2) irradiances. ERA5 reanalysis data show a negligible positive bias (+1.0 W/m2) for the shortwave irradiance and a large negative bias (−17 W/m2) for the longwave irradiance with respect to in situ observations. ERA5 meteorological variables, which are needed to calculate the air–sea heat flux using bulk formulae, have been compared with in situ measurements made at the oceanographic observatory. The two meteorological datasets show a very good agreement, with some underestimate of the wind speed by ERA5 for high wind conditions. We investigated the impact of different determinations of heat fluxes on the near surface sea temperature (1 m depth), as determined by calculations with a one-dimensional numerical model, the General Ocean Turbulence Model (GOTM). The sensitivity of the model to the different forcing was measured in terms of differences with respect to in situ temperature measurements made during the period under investigation. All simulations reproduced the true seasonal cycle and all high frequency variabilities. The best results on the overall seasonal cycle were obtained when using meteorological variables in the bulk formulae formulations used by the model itself. The derived overall annual net heat flux values were between +1.6 and 40.4 W/m2, depending on the used dataset. The large variability obtained with different datasets suggests that current determinations of the heat flux components and, in particular, of the longwave irradiance, need to be improved. The ENEA oceanographic observatory provides a complete, long-term, high resolution time series of high quality in situ observations. In the future, more similar sites worldwide will be needed for model and satellite validations and to improve the determination of the air–sea exchange and the understanding of related processes. Full article
(This article belongs to the Special Issue Remote Sensing of Air-Sea Fluxes)
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Figure 1

Figure 1
<p>Pictorial view of the air–sea heat exchange components.</p>
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<p>The Oceanographic Observatory (OO, left panel) and its position near Lampedusa Island. AO indicates the position of the Atmospheric observatory. The Lampedusa island picture was taken from the International Space Station (picture ISS 024-E-10246; see acknowledgments).</p>
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<p>Comparison between key meteorological variables contributing to air–sea heat flux estimates from ERA5 and from in situ observations. Air temperature (<b>a</b>), dew point temperature (<b>b</b>), atmospheric pressure at sea level (<b>c</b>), wind intensity (<b>d</b>), sea surface temperature (<b>e</b>). The (hourly) SST was inferred from the “skin” SST by adding the mean value of the difference with the “subskin” (0.17 °C) to make it more comparable with the sensor measurement at 1 m depth. Dot color indicates data density, increasing from white to black. Data refer to the period 3 June 2017–3 June 2018. Boxes within each plot include statistics of differences between ERA5 estimates and in situ measurements. Negative bias values indicate underestimates of the reanalysis.</p>
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<p>Comparison between hourly shortwave (<b>a</b>) and longwave (<b>b</b>) irradiance estimated by ERA5 and corresponding values measured on the buoy. Dot color indicates data density, increasing from white to black. Data refer to the period 4 June 2017–3 June 2018. Units are W/m<sup>2</sup>. Boxes within each plot include statistics of differences between ERA5 estimates and in situ measurements of shortwave and longwave irradiance.</p>
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<p>Comparison between hourly shortwave (<b>a</b>) and longwave (<b>b</b>) irradiances estimated by SEVIRI and the corresponding values measured on the buoy. Dot color indicates data density, increasing from white to black. Data refer to the period June 2017–3 June 2018. Units are W/m<sup>2</sup>. Boxes within each plot include statistics of differences between satellite estimates and in situ measurements of shortwave and longwave irradiances.</p>
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<p>In situ CTD casts made from 3 June 2017 at 14:00 UTC to 4 June 2017 at 07:56:00 UTC close to the Oceanographic Observatory. Dots represent individual CTD casts. The black lines represent the average profiles for temperature (<b>a</b>) and salinity (<b>b</b>) used as initial condition for the simulation.</p>
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<p>Comparison between in situ measurements of water temperature at 1 m depth (black curves in (<b>a</b>–<b>c</b>)) and GOTM simulated water temperatures at the same depth obtained as follows: (<b>a</b>) Simulations using air–sea heat and momentum fluxes computed by the model at each time step, using bulk formulae with ERA5 meteorological parameters (experiment 1, red line) or bulk formulae with in situ meteorological parameters (experiment 2, blue line). (<b>b</b>) Simulations imposing air–sea heat and momentum fluxes obtained by ERA5 (experiment 3, red line), by ERA5 except for the shortwave irradiance, which is from in situ measurements (experiment 4, blue line) and by ERA5 except for the shortwave irradiance, which is estimated by SEVIRI (experiment 5, green line). (<b>c</b>) Simulations imposing air–sea heat and momentum fluxes obtained by ERA5 (experiment 3, red line), by ERA5 except for the longwave irradiance, which is form in situ observations at the buoy (experiment 6, blue line), by ERA5 except for the longwave irradiance, which is estimated by SEVIRI (experiment 7, green line). The differences between measured and simulated temperatures at 1 m depth are reported in panels d, e, f, for: (<b>d</b>) Experiment 1 (red) and experiment 2 (blue). (<b>e</b>) Experiment 3 (red), experiment 4 (blue) and experiment 5 (green). (<b>f</b>) Experiment 3 (red), experiment 6 (blue) and experiment 7 (green). (<b>g</b>) Ocean heat flux loss (latent + sensible + net longwave) computed by the model for experiment 1 (red) and experiment 2 (blue). (<b>h</b>) Shortwave component of the heat fluxes from in situ measurements (blue), ERA5 (red) and SEVIRI (green). (<b>i</b>) Ocean heat flux loss (latent+sensible+net longwave) for experiment 3 (red), experiment 6 (blue) and experiment 7 (green) A 10 days moving average filter has been applied to curves in panels (<b>g</b>–<b>i</b>) to enhance readability.</p>
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<p>ERA5 minus buoy wind speed (<b>a</b>) and ERA5 minus buoy heat loss (Latent + Sensible + net Longwave) as a function of the in situ measured wind speed (<b>b</b>). Averages and standard deviations over 1 m/s intervals are shown as blue squares and red bars, respectively.</p>
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28 pages, 72526 KiB  
Article
Emerging Pattern of Wind Change over the Eurasian Marginal Seas Revealed by Three Decades of Satellite Ocean-Surface Wind Observations
by Lisan Yu
Remote Sens. 2021, 13(9), 1707; https://doi.org/10.3390/rs13091707 - 28 Apr 2021
Cited by 3 | Viewed by 3428
Abstract
This study provides the first full characterization of decadal changes of surface winds over 10 marginal seas along the Eurasian continent using satellite wind observations. During the three decades (1988–2018), surface warming has occurred in all seas at a rate more pronounced in [...] Read more.
This study provides the first full characterization of decadal changes of surface winds over 10 marginal seas along the Eurasian continent using satellite wind observations. During the three decades (1988–2018), surface warming has occurred in all seas at a rate more pronounced in the South European marginal seas (0.4–0.6 °C per decade) than in the monsoon-influenced North Indian and East Asian marginal seas (0.1–0.2 °C per decade). However, surface winds have not strengthened everywhere. On a basin average, winds have increased over the marginal seas in the subtropical/mid-latitudes, with the rate of increase ranging from 11 to 24 cms−1 per decade. These upward trends reflect primarily the accelerated changes in the 1990s and have largely flattened since 2000. Winds have slightly weakened or remained little changed over the marginal seas in the tropical monsoonal region. Winds over the Red Sea and the Persian Gulf underwent an abrupt shift in the late 1990s that resulted in an elevation of local wind speeds. The varying relationships between wind and SST changes suggest that different marginal seas have responded differently to environmental warming and further studies are needed to gain an improved understanding of climate change on a regional scale. Full article
(This article belongs to the Special Issue Remote Sensing of Air-Sea Fluxes)
Show Figures

Figure 1

Figure 1
<p>The 10 major semi-enclosed and enclosed marginal seas that surround the Eurasian continent. Left to right: the Mediterranean Sea, the Black Sea, the Caspian Sea, the Red Sea, the Persian Gulf, the Arabian Sea, the Bay of Bengal, the South China Sea, the East China Sea, and the Sea of Japan. The colors denote ocean floor (blues and whites) and land (greens, browns, and purples).</p>
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<p>Mean global wind speed (colored background) and direction vector averaged over 1988–2018. The superimposed magenta squares denote the locations of moored surface buoys used as validation (NDBC buoys are not shown). The large black box denotes the focal area of this study.</p>
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<p>Left column: time series plots of daily buoy winds (thin black) versus OAFlux-HR winds (thin red). Right column: scatter plots of collocated pairs at the Red-Sea buoy location 22°N, 39°E. (<b>a</b>,<b>b</b>) zonal wind component, (<b>c</b>,<b>d</b>) meridional wind component, (<b>e</b>,<b>f</b>) wind speed. Thick smoother lines in (<b>a</b>,<b>c</b>,<b>e</b>) denote a 21-day running mean with black for buoy and red for OAFlux-HR.</p>
Full article ">Figure 4
<p>Left column: time series plots of daily buoy winds (thin black) versus OAFlux-HR winds (thin red). Right column: scatter plots of collocated pairs at the Arabian Sea buoy location 16°N, 62°E (<b>a</b>,<b>b</b>) zonal wind component, (<b>c</b>,<b>d</b>) meridional wind component, (<b>e</b>,<b>f</b>) wind speed. Thick smoother lines in (<b>a</b>,<b>c</b>,<b>e</b>) denote a 21-day running mean with black for buoy and red for OAFlux-HR.</p>
Full article ">Figure 5
<p>Left column: time series plots of daily buoy winds (thin black) versus OAFlux-HR winds (thin red). Right column: scatter plots of collocated pairs at the Bay of Bengal buoy location 18°N, 89°E. (<b>a</b>,<b>b</b>) zonal wind component, (<b>c</b>,<b>d</b>) meridional wind component, (<b>e</b>,<b>f</b>) wind speed. Thick smoother lines in (<b>a</b>,<b>c</b>,<b>e</b>) denote a 21-day running mean with black for buoy and red for OAFlux-HR.</p>
Full article ">Figure 6
<p>Mean wind speed (shaded by colors) and direction. (<b>a</b>) Annual mean, (<b>b</b>) winter season (DJF), and (<b>c</b>) summer season (JJA).</p>
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<p>Standard deviation (STD) of seasonal variability of (<b>a</b>) zonal wind (<span class="html-italic">u</span>), (<b>b</b>) meridional wind (<span class="html-italic">v</span>), and (<b>c</b>) wind speed (<span class="html-italic">w</span>).</p>
Full article ">Figure 8
<p>Linear trends of surface wind speed and vector for (<b>a</b>) annual mean, (<b>b</b>) the winter season (December-January-February), (<b>c</b>) the summer season (June-July-August). The green dotted areas denote the linear trends of wind speed that are significant at the 90% confidence interval. The ocean regions outside of the marginal seas are shaded.</p>
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<p>(<b>a</b>) Linear trends of annual-mean surface wind speed and vector subsetted from <a href="#remotesensing-13-01707-f008" class="html-fig">Figure 8</a>a for the South European marginal seas. The magenta dotted areas denote the linear trends of wind speed that are significant at the 90% confidence interval. (<b>b</b>–<b>d</b>) Bar plots of the basin-averaged mean values (blue bars, left <span class="html-italic">y</span>-axis) and linear trends (red and gray bars, right axis) of wind speed in four seasons: December-January-February (DJF), March-April-May (MAM), June-July-August (JJA), and September-October-November (SON) and the total annual mean (ANN) for (<b>b</b>) the Mediterranean Sea (MED), (<b>c</b>) the Black Sea (BLACK), and (<b>d</b>) the Caspian Sea (CASPIAN). Error bars denote the upper and lower limits of the 90% confidence intervals. Linear trends that are statistically significant (not significant) are colored by red (gray).</p>
Full article ">Figure 10
<p>(<b>a</b>) Linear trends of annual-mean surface wind speed and vector subsetted from <a href="#remotesensing-13-01707-f008" class="html-fig">Figure 8</a>a for the North Indian Ocean marginal seas. The magenta dotted areas denote the linear trends of wind speed that are significant at the 90% confidence interval. (<b>b</b>–<b>d</b>) Bar plots of the basin-averaged mean values (blue bars, left <span class="html-italic">y</span>-axis) and linear trends (red and gray bars, right axis) of wind speed in four seasons: December-January-February (DJF), March-April-May (MAM), June-July-August (JJA), and September-October-November (SON) and the total annual mean (ANN) for (<b>b</b>) ARABIAN: the Arabian Sea; (<b>c</b>) BoB: the Bay of Bengal; (<b>d</b>) RED: the Red Sea; and (<b>e</b>) PERSIAN: the Persian Gulf. Error bars denote the upper and lower limits of the 90% confidence intervals. Linear trends that are statistically significant (not significant) are colored by red (gray).</p>
Full article ">Figure 11
<p>(<b>a</b>) Linear trends of annual-mean surface wind speed and vector subsetted from <a href="#remotesensing-13-01707-f008" class="html-fig">Figure 8</a>a for the East Asian marginal seas. The magenta dotted areas denote the linear trends of wind speed that are significant at the 90% confidence interval. (<b>b</b>–<b>d</b>) Bar plots of the basin-averaged mean values (blue bars, left <span class="html-italic">y</span>-axis) and linear trends (red and gray bars, right axis) of wind speed in four seasons: December-January-February (DJF), March-April-May (MAM), June-July-August (JJA), and September-October-November (SON) and the total annual mean (ANN) for (<b>b</b>) A SCS: the South China Sea; (<b>c</b>) ECS: the East China Sea; and (<b>d</b>) JAPAN: the Sea of Japan. Error bars denote the upper and lower limits of the 90% confidence intervals. Linear trends that are statistically significant (not significant) are colored by red (gray).</p>
Full article ">Figure 12
<p>Linear trends of annual mean SST for 1988–2018. The green dotted areas denote the linear trends of wind speed that are significant at the 90% confidence interval. The ocean regions outside of the marginal seas are shaded.</p>
Full article ">Figure 13
<p>Basin-averaged annual time series (black line) of (<b>a</b>–<b>c</b>) SST and (<b>d</b>–<b>f</b>) wind speed for the South European marginal seas. (<b>a</b>,<b>d</b>) MED: the Mediterranean Sea. (<b>b</b>,<b>e</b>) BLACK: the Black Sea. (<b>c</b>,<b>f</b>) CASPIAN: the Caspian Sea. The shaded area denotes one standard deviation of annual-mean variability. The red line denotes the linear trend over 1988–2018, and the dashed blue lines are the linear trends over 1988–2000 and 2001–2018, respectively. Linear trend estimates for the three periods are listed: 1988–2000 (top line), 2001–2018 (middle line), and 1988–2018 (bottom line), colored by red if the trend is statistically significant (<span class="html-italic">p</span> &lt; 0.1) or by black if the trend is statistically not significant (<span class="html-italic">p</span> &gt; 0.1). The value in the parentheses is the percentage increase.</p>
Full article ">Figure 14
<p>Basin-averaged annual time series (black line) of (<b>a</b>–<b>c</b>) SST and (<b>d</b>–<b>f</b>) wind speed for the North Indian Ocean marginal seas. (<b>a</b>,<b>e</b>) RED: the Red Sea. (<b>b</b>,<b>f</b>) PERSIAN: the Persian Gulf. (<b>c</b>,<b>g</b>) ARABIAN: the Arabian Sea. (<b>d</b>,<b>h</b>) BoB: the Bay of Bengal. The shaded area denotes one standard deviation of annual-mean variability. The red line denotes the linear trend over 1988–2018, and the dashed blue lines are the linear trends over 1988–2000 and 2001–2018, respectively. Linear trend estimates for the three periods are listed: 1988–2000 (top line), 2001–2018 (middle line), and 1988–2018 (bottom line), colored by red if the trend is statistically significant (<span class="html-italic">p</span> &lt; 0.1) or by black if the trend is statistically not significant (<span class="html-italic">p</span> &gt; 0.1). The value in the parentheses is the percentage increase.</p>
Full article ">Figure 15
<p>Basin-averaged annual time series (black line) of (<b>a</b>–<b>c</b>) SST and (<b>d</b>–<b>f</b>) wind speed for the East Asian marginal seas. (<b>a</b>,<b>d</b>) SCS: the South China Sea. (<b>b</b>,<b>e</b>) ECS: the East China Sea. (<b>c</b>,<b>f</b>) JAPAN: the Sea of Japan. The shaded area denotes one standard deviation of annual-mean variability. The red line denotes the linear trend over 1988–2018, and the dashed blue lines are the linear trends over 1988–2000 and 2001–2018, respectively. Linear trend estimates for the three periods are listed: 1988–2000 (top line), 2001–2018 (middle line), and 1988–2018 (bottom line), colored by red if the trend is statistically significant (<span class="html-italic">p</span> &lt; 0.1) or by black if the trend is statistically not significant (<span class="html-italic">p</span> &gt; 0.1). The value in the parentheses is the percentage increase.</p>
Full article ">Figure 16
<p>Schematic depiction of the decadal changes in annual-mean winds averaged over each of the 10 marginal seas for SST (left) and wind speed (right) in three periods: (<b>a</b>,<b>d</b>): 1988–2018; (<b>b</b>,<b>e</b>): 1988–2000; (<b>c</b>,<b>f</b>): 2001–2018. Areas colored in red (blue) denote that the rate of increase (reduction) in SST and wind speeds is statistically significant at the 90% confidence interval. The areas colored in gray denote that the changes in the SST or wind speed are not significant.</p>
Full article ">
23 pages, 4825 KiB  
Article
Air-Sea Interactions over Eddies in the Brazil-Malvinas Confluence
by Ronald Souza, Luciano Pezzi, Sebastiaan Swart, Fabrício Oliveira and Marcelo Santini
Remote Sens. 2021, 13(7), 1335; https://doi.org/10.3390/rs13071335 - 31 Mar 2021
Cited by 19 | Viewed by 3917
Abstract
The Brazil–Malvinas Confluence (BMC) is one of the most dynamical regions of the global ocean. Its variability is dominated by the mesoscale, mainly expressed by the presence of meanders and eddies, which are understood to be local regulators of air-sea interaction processes. The [...] Read more.
The Brazil–Malvinas Confluence (BMC) is one of the most dynamical regions of the global ocean. Its variability is dominated by the mesoscale, mainly expressed by the presence of meanders and eddies, which are understood to be local regulators of air-sea interaction processes. The objective of this work is to study the local modulation of air-sea interaction variables by the presence of either a warm (ED1) and a cold core (ED2) eddy, present in the BMC, during September to November 2013. The translation and lifespans of both eddies were determined using satellite-derived sea level anomaly (SLA) data. Time series of satellite-derived surface wind data, as well as these and other meteorological variables, retrieved from ERA5 reanalysis at the eddies’ successive positions in time, allowed us to investigate the temporal modulation of the lower atmosphere by the eddies’ presence along their translation and lifespan. The reanalysis data indicate a mean increase of 78% in sensible and 55% in latent heat fluxes along the warm eddy trajectory in comparison to the surrounding ocean of the study region. Over the cold core eddy, on the other hand, we noticed a mean reduction of 49% and 25% in sensible and latent heat fluxes, respectively, compared to the adjacent ocean. Additionally, a field campaign observed both eddies and the lower atmosphere from ship-borne observations before, during and after crossing both eddies in the study region during October 2013. The presence of the eddies was imprinted on several surface meteorological variables depending on the sea surface temperature (SST) in the eddy cores. In situ oceanographic and meteorological data, together with high frequency micrometeorological data, were also used here to demonstrate that the local, rather than the large scale forcing of the eddies on the atmosphere above, is, as expected, the principal driver of air-sea interaction when transient atmospheric systems are stable (not actively varying) in the study region. We also make use of the in situ data to show the differences (biases) between bulk heat flux estimates (used on atmospheric reanalysis products) and eddy covariance measurements (taken as “sea truth”) of both sensible and latent heat fluxes. The findings demonstrate the importance of short-term changes (minutes to hours) in both the atmosphere and the ocean in contributing to these biases. We conclude by emphasizing the importance of the mesoscale oceanographic structures in the BMC on impacting local air-sea heat fluxes and the marine atmospheric boundary layer stability, especially under large scale, high-pressure atmospheric conditions. Full article
(This article belongs to the Special Issue Remote Sensing of Air-Sea Fluxes)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Mean maps: (<b>a</b>) sea surface temperature (SST), (<b>b</b>) sea level anomaly (SLA) and (<b>c</b>) surface wind of the Brazil–Malvinas Current (BMC), respectively, representing these variables’ mean fields during the INTERCONF-32 campaign. The black line represents the ship’s track. White dots represent the coincident radiosonde and XBT/CTD launching positions. SST is an 8-day mean of MODIS image between 16–23 October 2013; SLA is a daily composite of 17 October 2013 and wind is an ASCAT 3-day mean between 16–18 October 2013. Warm core eddy (ED1) and cold core eddy (ED2) locations are indicated by the black arrows.</p>
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<p>Micrometeorological tower with sensors mounted on the Polar Ship Almirante Maximiano’s bow. The tower is 9 m tall and the upper sensors are about 15 m above the sea level. The micrometeorological data used in this study were obtained with these instruments.</p>
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<p>(<b>a</b>) Translational trajectories of the ED1 (22 September to 13 November 2013, red line) and ED2 (13 September to 1 November 2013, blue line) superimposed onto the bathymetry (m) of the Southwestern Atlantic Ocean. The ship’s track during the INTERCONF-32 campaign with the radiosonde and XBT/CTD launching positions (white circles) between 16–18 October 2013 are also shown. (<b>b</b>) Zoomed trajectories of ED1 and ED2 in the BMC: circles and triangles indicate the initial and final positions of the eddies, respectively. During their lifespans, SLA data indicated that ED1 diameters varied between 86 (day 1) and 122 km (day 53); ED2 diameters varied between 95 (day 1) and 114 km (day 50).</p>
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<p>SLA (<b>a</b>–<b>e</b>), ASCAT (<b>f</b>–<b>i</b>) and WindSat (<b>k</b>–<b>o</b>) wind magnitude maps of the BMC throughout ED1 and ED2 life spans. Columns from left to right indicate consecutive dates in 1 October, 11 October, 21 October, 31 October and 10 November 2013, respectively. ED1 and ED2 translational trajectories (<a href="#remotesensing-13-01335-f003" class="html-fig">Figure 3</a>) are also represented here.</p>
Full article ">Figure 5
<p>Time series of (<b>a</b>) ERA5 sea level pressure; (<b>b</b>) Sea level anomaly; (<b>c</b>) ASCAT wind magnitude; (<b>d</b>) WindSat wind magnitude; (<b>e</b>) ERA5 wind magnitude of both ED1 (red lines) and ED2 (blue lines) measured along their trajectories during their life spans. The green lines represent the time series of the same variables derived from ERA5 reanalysis at the neutral region of the Zapiola Rise (45 °S, 42 °W) during the same period when both eddies were tracked.</p>
Full article ">Figure 6
<p>Time series of ERA5: (<b>a</b>) the sea level air temperature (T<sub>air</sub>); (<b>b</b>) dew point temperature; (<b>c</b>) SST; (<b>d</b>) SST-T<sub>air</sub>; (<b>e</b>) air-sea sensible heat flux; (<b>f</b>) air-sea latent heat flux of both ED1 (red lines) and ED2 (blue lines) measured along their trajectories during their lifespans. The green lines represent the time series of the same variables derived from ERA5 reanalysis at the neutral region of the Zapiola Rise (45 °S, 42 °W) during the same period when both eddies were tracked.</p>
Full article ">Figure 7
<p>Synoptic characteristics of the coupled air-sea system in the BMC observed during the INTERCONF-32 campaign. Water temperatures were obtained from a combination of XBT and CTD data while the air temperature and the meridional component of the wind were obtained from radiosondes launched along the ship’s trajectory (<a href="#remotesensing-13-01335-f001" class="html-fig">Figure 1</a>). ED1 and ED2 positions in 16 and 17 October 2013, respectively, are denoted by the black arrows.</p>
Full article ">Figure 8
<p>ERA5 weather maps at 00Z during days 16 (<b>a</b>), 17 (<b>b</b>) and 18 (<b>c</b>) October 2013. Black lines represent the atmospheric pressure (hPa), the black arrows represent the surface wind vectors (m s<sup>−1</sup>) and the color scale from red to blues represent the thermal advection from warm to cold (°C day<sup>−1</sup>). The black dots represent the ship’s position in the study area at 00Z every day during the entire INTERCONF-32 campaign (14–20 October 2013) along the ship’s track (green line).</p>
Full article ">Figure 9
<p>Time series of meteorological and derived heat flux variables measured or computed along the ship’s track during the INTERCONF-32 campaign. (<b>a</b>) SLP (grey line) and the wind magnitude at 10 m level (U<sub>10</sub>, black line); (<b>b</b>) T<sub>10</sub> (grey line) and SST; (<b>c</b>) wind vector; (<b>d</b>) SST-T<sub>10</sub> (grey line) and relative humidity at 10 m level (RH<sub>10</sub>, black line); (<b>e</b>) <span class="html-italic">H<sub>EC</sub></span> (grey line) and <span class="html-italic">H<sub>bulk</sub></span> (black line); (<b>f</b>) <span class="html-italic">Hl<sub>EC</sub></span> (grey line) and <span class="html-italic">Hl<sub>bulk</sub></span> (black line); (<b>g</b>) <span class="html-italic">H<sub>b</sub></span>-<span class="html-italic">H<sub>EC</sub></span> (grey line) and <span class="html-italic">Hl<sub>b</sub></span>-<span class="html-italic">Hl<sub>EC</sub></span> biases (black line); (<b>h</b>) Monin–Obukhov stability parameter ζ.</p>
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15 pages, 4302 KiB  
Article
Mesoscale Temporal Wind Variability Biases Global Air–Sea Gas Transfer Velocity of CO2 and Other Slightly Soluble Gases
by Yuanyuan Gu, Gabriel G. Katul and Nicolas Cassar
Remote Sens. 2021, 13(7), 1328; https://doi.org/10.3390/rs13071328 - 31 Mar 2021
Cited by 3 | Viewed by 2857
Abstract
The significance of the water-side gas transfer velocity for air–sea CO2 gas exchange (k) and its non-linear dependence on wind speed (U) is well accepted. What remains a subject of inquiry are biases associated with the form of the non-linear [...] Read more.
The significance of the water-side gas transfer velocity for air–sea CO2 gas exchange (k) and its non-linear dependence on wind speed (U) is well accepted. What remains a subject of inquiry are biases associated with the form of the non-linear relation linking k to U (hereafter labeled as f(U), where f(.) stands for an arbitrary function of U), the distributional properties of U (treated as a random variable) along with other external factors influencing k, and the time-averaging period used to determine k from U. To address the latter issue, a Taylor series expansion is applied to separate f(U) into a term derived from time-averaging wind speed (labeled as U, where . indicates averaging over a monthly time scale) as currently employed in climate models and additive bias corrections that vary with the statistics of U. The method was explored for nine widely used f(U) parameterizations based on remotely-sensed 6-hourly global wind products at 10 m above the sea-surface. The bias in k of monthly estimates compared to the reference 6-hourly product was shown to be mainly associated with wind variability captured by the standard deviation σσU around U or, more preferably, a dimensionless coefficient of variation Iu= σσU/U. The proposed correction outperforms previous methodologies that adjusted k when using U only. An unexpected outcome was that upon setting Iu2 = 0.15 to correct biases when using monthly wind speed averages, the new model produced superior results at the global and regional scale compared to prior correction methodologies. Finally, an equation relating Iu2 to the time-averaging interval (spanning from 6 h to a month) is presented to enable other sub-monthly averaging periods to be used. While the focus here is on CO2, the theoretical tactic employed can be applied to other slightly soluble gases. As monthly and climatological wind data are often used in climate models for gas transfer estimates, the proposed approach provides a robust scheme that can be readily implemented in current climate models. Full article
(This article belongs to the Special Issue Remote Sensing of Air-Sea Fluxes)
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Figure 1

Figure 1
<p>Conceptual diagram representing the bias in gas transfer velocity (k) estimates associated with averaging wind speed variability (adapted from [<a href="#B32-remotesensing-13-01328" class="html-bibr">32</a>]). The quadratic and cubic relations are in blue and orange, respectively.</p>
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<p>Bias in k of CO<sub>2</sub> due to wind speeds at varying spatial resolutions (0.5°<math display="inline"><semantics> <mrow> <mo> </mo> <mo>×</mo> <mo> </mo> </mrow> </semantics></math>0.5° and 5°<math display="inline"><semantics> <mrow> <mo> </mo> <mo>×</mo> <mo> </mo> </mrow> </semantics></math>5°) for 6-hourly and monthly gas transfer velocity (k), and temporal bias in k (6 hourly and monthly) at the spatial resolution of 0.5°<math display="inline"><semantics> <mrow> <mo> </mo> <mo>×</mo> <mo> </mo> </mrow> </semantics></math>0.5° and 5°<math display="inline"><semantics> <mrow> <mo> </mo> <mo>×</mo> <mo> </mo> </mrow> </semantics></math>5°. The k<sub>mon</sub> and k<sub>6h</sub> are gas transfer velocities averaged over all k values estimated from monthly and 6-hourly wind speed records, respectively. k<sub>5</sub><sub>°</sub> and k<sub>0.5</sub><sub>°</sub> are gas transfer velocities averaged over all k values estimated from 5° and 0.5° wind speed, respectively. The bias is estimated as △k*100/k<sub>6h,0.5°</sub> (k<sub>6h,0.5°</sub> is k at the resolution of 6-hourly and 0.5°<math display="inline"><semantics> <mrow> <mo> </mo> <mo>×</mo> <mo> </mo> </mrow> </semantics></math>0.5°).</p>
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<p>Mean bias in gas transfer velocity (k) for CO<sub>2</sub> estimated from term 1 (measured bias in f(U)) and term 2 (bias correction k<sub>b</sub> from new model) of Equation (9) over the period spanning 1990 to 2018 for the parameterizations presented in <a href="#remotesensing-13-01328-t001" class="html-table">Table 1</a>.</p>
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<p>Left panel: time series of global (<b>a</b>) monthly averaged wind speed <math display="inline"><semantics> <mrow> <mo stretchy="false">〈</mo> <mi mathvariant="normal">U</mi> <mo stretchy="false">〉</mo> </mrow> </semantics></math> (in black) and standard deviation (<math display="inline"><semantics> <mrow> <msub> <mi mathvariant="sans-serif">σ</mi> <mi mathvariant="normal">u</mi> </msub> <mo>,</mo> <mrow> <mo> </mo> <mi>in</mi> <mo> </mo> <mi>grey</mi> </mrow> </mrow> </semantics></math>) around <math display="inline"><semantics> <mrow> <mo stretchy="false">〈</mo> <mi mathvariant="normal">U</mi> <mo stretchy="false">〉</mo> </mrow> </semantics></math>, (<b>b</b>) monthly squared coefficient of variation <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">I</mi> <mi mathvariant="normal">u</mi> </msub> <msup> <mrow/> <mn>2</mn> </msup> <mo>=</mo> <msup> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="sans-serif">σ</mi> <mi mathvariant="normal">u</mi> </msub> <mo>/</mo> <mrow> <mo stretchy="false">〈</mo> <mi mathvariant="normal">U</mi> <mo stretchy="false">〉</mo> </mrow> <mo stretchy="false">)</mo> </mrow> <mn>2</mn> </msup> </mrow> </semantics></math> from 1990 to 2018 (note the small variations along the ordinate axis). The black and the grey dashed lines in (<b>b</b>) indicate the long-term trend (0.002 dec<sup>−1</sup>) and average (<math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">I</mi> <mi mathvariant="normal">u</mi> </msub> <msup> <mrow/> <mn>2</mn> </msup> <mo>=</mo> <mn>0.15</mn> </mrow> </semantics></math>), respectively. Right panel: spatial distribution of (<b>c</b>) trends in the wind speed standard deviation (<math display="inline"><semantics> <mrow> <msub> <mi mathvariant="sans-serif">σ</mi> <mi mathvariant="normal">u</mi> </msub> </mrow> </semantics></math>) around <math display="inline"><semantics> <mrow> <mo stretchy="false">〈</mo> <mi mathvariant="normal">U</mi> <mo stretchy="false">〉</mo> </mrow> </semantics></math>, (<b>d</b>) monthly averaged wind speed <math display="inline"><semantics> <mrow> <mrow> <mo stretchy="false">〈</mo> <mi mathvariant="normal">U</mi> <mo stretchy="false">〉</mo> </mrow> <mo>,</mo> </mrow> </semantics></math> and (<b>e</b>) monthly squared coefficient of variation <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="normal">I</mi> <mi mathvariant="normal">u</mi> </msub> <msup> <mrow/> <mn>2</mn> </msup> <mo>=</mo> <msup> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="sans-serif">σ</mi> <mi mathvariant="normal">u</mi> </msub> <mo>/</mo> <mrow> <mrow> <mo stretchy="false">〈</mo> <mi mathvariant="normal">U</mi> <mo stretchy="false">〉</mo> </mrow> </mrow> <mo stretchy="false">)</mo> </mrow> <mn>2</mn> </msup> </mrow> </semantics></math> from 1990 to 2018.</p>
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<p>Difference in 6-hourly k and corrected k for CO<sub>2</sub> applying five correction methodologies in reference to the 6-hourly k (in %) for k parameterizations listed in <a href="#remotesensing-13-01328-t001" class="html-table">Table 1</a>. The bias is estimated as △k*100/k<sub>6h,0.5°</sub>.</p>
Full article ">Figure 6
<p>(<b>a</b>) Spatial distribution of averaged variance of sea surface temperature (SST) (<math display="inline"><semantics> <mrow> <msubsup> <mi mathvariant="sans-serif">σ</mi> <mrow> <mi>SST</mi> </mrow> <mn>2</mn> </msubsup> </mrow> </semantics></math>) around monthly averaged <math display="inline"><semantics> <mrow> <mrow> <mo stretchy="false">〈</mo> <mi>SST</mi> <mo stretchy="false">〉</mo> </mrow> </mrow> </semantics></math>; (<b>b</b>) Time series of annual averaged variance of SST (<math display="inline"><semantics> <mrow> <msubsup> <mi mathvariant="sans-serif">σ</mi> <mrow> <mi>SST</mi> </mrow> <mn>2</mn> </msubsup> </mrow> </semantics></math>) around monthly averaged <math display="inline"><semantics> <mrow> <mrow> <mo stretchy="false">〈</mo> <mi>SST</mi> <mo stretchy="false">〉</mo> </mrow> </mrow> </semantics></math>, the dashed line indicates the long-term trend; (<b>c</b>) Spatial pattern of trend in averaged variance of SST (<math display="inline"><semantics> <mrow> <msubsup> <mi mathvariant="sans-serif">σ</mi> <mrow> <mi>SST</mi> </mrow> <mn>2</mn> </msubsup> </mrow> </semantics></math>) around monthly averaged <math display="inline"><semantics> <mrow> <mrow> <mo stretchy="false">〈</mo> <mi>SST</mi> <mo stretchy="false">〉</mo> </mrow> </mrow> </semantics></math> from 1990 to 2018.</p>
Full article ">Figure 7
<p>(<b>a</b>) Zonal profiles of corrected k for CO<sub>2</sub> using the five correction methodologies in comparison to annual k derived from 6-hourly (red solid curve) and monthly (red dashed curve) wind speed. Zonal variation in k estimated using method 1 (in black) is not visible because it overlaps with the 6-hourly k. Panels (<b>a1</b>–<b>a9</b>) show the latitudinal variations in nine k parameterizations listed in <a href="#remotesensing-13-01328-t001" class="html-table">Table 1</a>. (<b>b</b>) The RMSE of each method in corrected k from 6-hourly k.</p>
Full article ">Figure 8
<p>Coefficient of variation <math display="inline"><semantics> <mrow> <msubsup> <mi mathvariant="normal">I</mi> <mi mathvariant="normal">u</mi> <mn>2</mn> </msubsup> </mrow> </semantics></math> as a function of the averaging period <math display="inline"><semantics> <mrow> <mo>Δ</mo> <mrow> <mi mathvariant="normal">t</mi> <mo> </mo> </mrow> </mrow> </semantics></math>(from 6-hourly to monthly). Circles indicate the results from measurements, and the solid line represents a modelled fit through the measurements. For ∆t &gt; 18 days, I<sub>u</sub><sup>2</sup> becomes independent of ∆t. Global climate models operate on a ∆t = 30 days.</p>
Full article ">Figure 9
<p>Energy spectrum of global average 6-hourly wind speed. The spectrum is extrapolated from 12 h to a turbulence scale (seconds) via Kolmogorov’s –5/3 power law (f<sup>–5/3</sup>, blue dashed line). The resolved spectrum has an exponent of –3 from multi-day to 12 h (f<sup>–3</sup>, blue solid line) consistent with an enstrophy cascade in a quasi-geostrophic flow. The dashed vertical lines (right to left) indicate frequencies corresponding to the following timescales: sub-hour (=0.5 h), diurnal (=12 h), daily (=24 h), and annual (=8760 h), respectively. The <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="sans-serif">σ</mi> <mi mathvariant="normal">d</mi> </msub> <msup> <mrow/> <mn>2</mn> </msup> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="sans-serif">σ</mi> <mi mathvariant="normal">m</mi> </msub> <msup> <mrow/> <mn>2</mn> </msup> <mo>,</mo> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="sans-serif">σ</mi> <mi mathvariant="normal">t</mi> </msub> <msup> <mrow/> <mn>2</mn> </msup> <mo> </mo> </mrow> </semantics></math>refer to the variance at large (mesoscale to decadal), intermediate (12 h to turbulence), and small (turbulence) scales, respectively.</p>
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28 pages, 25436 KiB  
Article
Twenty-Seven Years of Scatterometer Surface Wind Analysis over Eastern Boundary Upwelling Systems
by Abderrahim Bentamy, Semyon A. Grodsky, Gildas Cambon, Pierre Tandeo, Xavier Capet, Claude Roy, Steven Herbette and Antoine Grouazel
Remote Sens. 2021, 13(5), 940; https://doi.org/10.3390/rs13050940 - 3 Mar 2021
Cited by 10 | Viewed by 3130
Abstract
More than twelve satellite scatterometers have operated since 1992 through the present, providing the main source of surface wind vector observations over global oceans. In this study, these scatterometer winds are used in combination with radiometers and synthetic aperture radars (SAR) for the [...] Read more.
More than twelve satellite scatterometers have operated since 1992 through the present, providing the main source of surface wind vector observations over global oceans. In this study, these scatterometer winds are used in combination with radiometers and synthetic aperture radars (SAR) for the better determination and characterization of high spatial and temporal resolution of regional surface wind parameters, including wind speed and direction, wind stress components, wind stress curl, and divergence. In this paper, a 27-year-long (1992–2018) 6-h satellite wind analysis with a spatial resolution of 0.125° in latitude and longitude is calculated using spatial structure functions derived from high-resolution SAR data. The main objective is to improve regional winds over three major upwelling regions (the Canary, Benguela, and California regions) through the use of accurate and homogenized wind observations and region-specific spatial and temporal wind variation structure functions derived from buoy and SAR data. The long time series of satellite wind analysis over the California upwelling, where a significant number of moorings is available, are used for assessing the accuracy of the analysis. The latter is close to scatterometer wind retrieval accuracy. This assessment shows that the root mean square difference between collocated 6-h satellite wind analysis and buoys is lower than 1.50 and 1.80 m s−1 for offshore and nearshore locations, respectively. The temporal correlation between buoy and satellite analysis winds exceeds 0.90. The analysis accuracy is lower for 1992–1999 when satellite winds were mostly retrieved from ERS-1 and/or ERS-2 scatterometers. To further assess the improvement brought by this new wind analysis, its data and data from three independent products (ERA5, CMEMS, and CCMP) are compared with purely scatterometer winds over the Canary and Benguela regions. Even though the four products are generally similar, the new satellite analysis shows significant improvements, particularly in the upwelling areas. Full article
(This article belongs to the Special Issue Remote Sensing of Air-Sea Fluxes)
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Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>National Data Buoy Center (NDBC) buoy locations. Red and blue symbols show coastal (&lt;50 km of coastlines) and offshore buoys, respectively. (<b>a</b>) Panel shows all buoy locations, while (<b>b</b>) shows only buoys located in the Californian basin.</p>
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<p>Spatial scales (km) of 10m wind speed (<b>a</b>,<b>d</b>,<b>g</b>), zonal wind (<b>b</b>,<b>e</b>,<b>h</b>), and meridional wind (<b>c</b>,<b>f</b>,<b>i</b>) structure functions estimated from Sentinel-1a and Sentinel-1b synthetic aperture radar (SAR) IW retrievals during 2017–2019 over Benguela (top), Canary (middle), and California (bottom) upwelling zones.</p>
Full article ">Figure 2 Cont.
<p>Spatial scales (km) of 10m wind speed (<b>a</b>,<b>d</b>,<b>g</b>), zonal wind (<b>b</b>,<b>e</b>,<b>h</b>), and meridional wind (<b>c</b>,<b>f</b>,<b>i</b>) structure functions estimated from Sentinel-1a and Sentinel-1b synthetic aperture radar (SAR) IW retrievals during 2017–2019 over Benguela (top), Canary (middle), and California (bottom) upwelling zones.</p>
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<p>Spatial distribution of lagged temporal correlations of 10 m wind speed (<b>a</b>,<b>d</b>,<b>g</b>), zonal wind (<b>b</b>,<b>e</b>,<b>h</b>), and meridional wind (<b>c</b>,<b>f</b>,<b>i</b>) estimated from homogenized remotely sensed winds [<a href="#B8-remotesensing-13-00940" class="html-bibr">8</a>] in January and July 2000 over Benguela (top), Canary (middle), and California (bottom) upwelling zones. Time lag is included in each panel.</p>
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<p>Offshore comparisons of 6-hourly averaged buoy and on one hand IFREMER satellite analyses (left column), and on other hand ERA5 re-analyses (right column). Panels (<b>a</b>,<b>b</b>) illustrate wind speed comparisons, (<b>c</b>,<b>d</b>) illustrate zonal wind component comparisons, and (<b>e</b>,<b>f</b>) illustrate meridional wind component comparisons. Colors indicate sampling length values. Black and green lines indicate the perfect and symmetrical regression lines, respectively.</p>
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<p>As <a href="#remotesensing-13-00940-f004" class="html-fig">Figure 4</a> but for nearshore comparisons.</p>
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<p>Spatial distribution of root mean square difference (RMSD) between 10 m neutral wind speed from collocated scatterometer retrievals and (<b>a</b>–<b>c</b>) IFREMER satellite wind analysis, (<b>d</b>–<b>f</b>) ERA5 reanalysis, (<b>g</b>–<b>i</b>) CMEMS satellite wind analysis, and (<b>j</b>–<b>l</b>) CCMP analysis over the Canary upwelling zone. Note that retrievals from different scatterometers are used in 1996 (ERS2, left column), 2006 (QuikSCAT, middle column), and 2016 (ASCAT, right column). Colors indicate RMSD in m s<sup>−1</sup>. Note that color scale limits for 1996 are different from those in 2006 and 2016.</p>
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<p>The same as in <a href="#remotesensing-13-00940-f006" class="html-fig">Figure 6</a> but for the Benguela upwelling region.</p>
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<p>July 2006 mean of wind stress curl estimated from (<b>a</b>) scatterometer (QuikSCAT) and collocated (<b>b</b>) Ifremer, (<b>c</b>) ERA-5, and (<b>d</b>) CCMP analyses over the Canary zone. Colors indicate curl amplitude in N/m<sup>3</sup>.</p>
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<p>The same as in <a href="#remotesensing-13-00940-f008" class="html-fig">Figure 8</a> but over the Benguela zone in January 2006.</p>
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<p>Diurnal 10 m wind speed anomaly (shaded, m s<sup>−1</sup>) estimated as the difference between the seasonal mean for a given synoptic time and the seasonal mean for all synoptic times for January, and the seasonal mean wind velocity for each synoptic time. Results are based on the IFREMER wind analysis, seasonal means are computed over 2000–2018.</p>
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<p>The same as in <a href="#remotesensing-13-00940-f010" class="html-fig">Figure 10</a> but for the Benguela region in July.</p>
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<p>The three EBUS zones of interest: California, Canary, and Benguela are shown as red rectangles.</p>
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<p>Comparison, illustrated through QQplot result, between temporal correlation estimated from NDBC buoy wind measurements and from homogenized remotely sensed wind data.</p>
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<p>Monthly averaged wind speeds estimated from 6-hourly buoy, moored at 34.88°N and 120.87°W, and IFREMER satellite analyses for 00 h:00 and 12 h:00 UTC.</p>
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<p>Spatial distributions of root mean square of zonal wind component differences between collocated scatterometer retrievals and satellite wind analyses, referenced as Ifremer, (<b>a</b>–<b>c</b>), ERA5 wind estimates (<b>d</b>–<b>f</b>), CMEMS winds (<b>g</b>–<b>i</b>), and CCMP winds (<b>j</b>–<b>l</b>). The results are drawn from data occurring, over the Canary zone, in 1996 (panels in left column), 2006 (middle column), and 2016 (right column). Color indicates RMSD values in m/s. One should notice that the color bar associated with 1996 is different from the 2006 and 2016 ones.</p>
Full article ">Figure A5
<p>Spatial distributions of root mean square of meridional wind component differences between collocated scatterometer retrievals and satellite wind analyses, referenced as Ifremer, (<b>a</b>–<b>c</b>), ERA5 wind estimates (<b>d</b>–<b>f</b>), CMEMS winds (<b>g</b>–<b>i</b>), and CCMP winds (<b>j</b>–<b>l</b>). The results are drawn from data occurring, over Canary zone, in 1996 (panels in left column), 2006 (middle column), and 2016 (right column). Color indicates RMSD values in m/s. One should notice that the color bar associated with 1996 is different from the 2006 and 2016 ones.</p>
Full article ">Figure A6
<p>Spatial distributions of root mean square of zonal wind component differences between collocated scatterometer retrievals and satellite wind analyses, referenced as Ifremer, (<b>a</b>–<b>c</b>), ERA5 wind estimates (<b>d</b>–<b>f</b>), CMEMS winds (<b>g</b>–<b>i</b>), and CCMP winds (<b>j</b>–<b>l</b>). The results are drawn from data occurring, over Benguela zone, in 1996 (panels in left column), 2006 (middle column), and 2016 (right column). Color indicates RMSD values in m/s. One should notice that the color bar associated with 1996 is different from the 2006 and 2016 ones.</p>
Full article ">Figure A7
<p>Spatial distributions of root mean square of meridional wind component differences between collocated scatterometer retrievals and satellite wind analyses, referenced as Ifremer, (<b>a</b>–<b>c</b>), ERA5 wind estimates (<b>d</b>–<b>f</b>), CMEMS winds (<b>g</b>–<b>i</b>), and CCMP winds (<b>j</b>–<b>l</b>). The results are drawn from data occurring, over the Benguela zone, in 1996 (panels in left column), 2006 (middle column), and 2016 (right column). Color indicates RMSD values in m/s. One should notice that the color bar associated with 1996 is different from the 2006 and 2016 ones.</p>
Full article ">Figure A8
<p>Monthly-averaged mean of wind stress curl estimated from collocated (<b>a</b>) scatterometer (ASCAT), (<b>b</b>) Ifremer, (<b>c</b>) ERA-5, and (<b>d</b>) CCMP wind data occurring in July 2016 over the Canary zone. Colors indicate curl amplitudes in N/m<sup>3</sup>. White and black colors indicate curl values lower than −1.210<sup>−6</sup> N/m<sup>3</sup> and higher than 1.210<sup>−6</sup> N/m<sup>3</sup>, respectively.</p>
Full article ">Figure A9
<p>Monthly-averaged mean of wind stress curl estimated from collocated (<b>a</b>) scatterometer (ASCAT), (<b>b</b>) Ifremer, (<b>c</b>) ERA-5, and (<b>d</b>) CCMP wind data occurring in January 2016 over Benguela zone. Colors indicate curl amplitudes in N/m<sup>3</sup>. White and black colors indicate curl values lower than −1.210<sup>−6</sup> N/m<sup>3</sup> and higher than 1.210<sup>−6</sup> N/m<sup>3</sup>, respectively.</p>
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22 pages, 10015 KiB  
Article
The Impact of the Madden–Julian Oscillation on Cyclone Amphan (2020) and Southwest Monsoon Onset
by Heather L. Roman-Stork and Bulusu Subrahmanyam
Remote Sens. 2020, 12(18), 3011; https://doi.org/10.3390/rs12183011 - 16 Sep 2020
Cited by 15 | Viewed by 3480
Abstract
Cyclone Amphan was an exceptionally strong tropical cyclone in the Bay of Bengal that achieved a minimum central pressure of 907 mb during its active period in May 2020. In this study, we analyzed the oceanic and surface atmospheric conditions leading up to [...] Read more.
Cyclone Amphan was an exceptionally strong tropical cyclone in the Bay of Bengal that achieved a minimum central pressure of 907 mb during its active period in May 2020. In this study, we analyzed the oceanic and surface atmospheric conditions leading up to cyclogenesis, the impact of this storm on the Bay of Bengal, and how the processes that led to cyclogenesis, such as the Madden–Julian Oscillation (MJO) and Amphan itself, in turn impacted southwest monsoon preconditioning and onset. To accomplish this, we took a multiparameter approach using a combination of near real time satellite observations, ocean model forecasts, and reanalysis to better understand the processes involved. We found that the arrival of a second downwelling Kelvin wave in the equatorial Bay of Bengal, coupled with elevated upper ocean heat content and the positioning of the convective phase of the MJO, helped to create the conditions necessary for cyclogenesis, where the northward-propagating branch of the MJO acted as a trigger for cyclogenesis. This same MJO event, in conjunction with Amphan, heavily contributed atmospheric moisture to the southeastern Arabian Sea and established low-level westerlies that allowed for the southwest monsoon to climatologically onset on June 1. Full article
(This article belongs to the Special Issue Remote Sensing of Air-Sea Fluxes)
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Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>National Oceanic and Atmospheric Administration (NOAA) Coastwatch gap-filled ocean color chlorophyll-a (CHL-a; shaded; mg/m<sup>3</sup>) for the difference between May 28, 2020 and May 8, 2020 in the Bay of Bengal overlaid with NOAA Satellite Services Division (SSD) best track data from the Joint Typhoon Warning Center (JTWC) for Cyclone Amphan (2020).</p>
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<p>Multiparameter analysis of the Bay of Bengal on May 12, 2020 prior to cyclogenesis in (<b>A</b>) Global Precipitation Measurement (GPM) precipitation rate (mm/day); (<b>B</b>) Copernicus Marine and Environment Monitoring Service (CMEMS) sea level anomalies (SLAs) (cm) overlaid with geostrophic currents (cm/s); (<b>C</b>) Nucleus for the European Modeling of the Ocean (NEMO) sea surface temperature (SST) data (°C); (<b>D</b>) NEMO sea surface salinity (SSS) data (psu); (<b>E</b>) 0–30 m ocean heat content (OHC; J/m<sup>2</sup> * 10<sup>9</sup>) calculated from NEMO; (<b>F</b>) barrier layer thickness (BLT; m) calculated from NEMO; (<b>G</b>) mixed layer depth (MLD; m) calculated from NEMO; (<b>H</b>) isothermal layer depth (ILD; m) calculated from NEMO; (<b>I</b>) Cross-Calibrated Multi-Platform version 2 (CCMPv2) surface wind magnitude (m/s; shaded) and vectors; (<b>J</b>) ERA5 instantaneous moisture flux (kg/m<sup>2</sup>*day*10<sup>−3</sup>); (<b>K</b>) ERA5 surface sensible heat flux (J/m<sup>2</sup> * 10<sup>6</sup>); and (<b>L</b>) ERA5 surface latent heat flux (J/m<sup>2</sup> * 10<sup>7</sup>).</p>
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<p>Multiparameter analysis of the Bay of Bengal on May 19, 2020 at the peak of the storm in (<b>A</b>) Global Precipitation Measurement (GPM) precipitation rate (mm/day); (<b>B</b>) Copernicus Marine and Environment Monitoring Service (CMEMS) sea level anomalies (SLAs) (cm) overlaid with geostrophic currents (cm/s); (<b>C</b>) Nucleus for the European Modeling of the Ocean (NEMO) sea surface temperature (SST) data (°C); (<b>D</b>) NEMO sea surface salinity (SSS) data (psu); (<b>E</b>) 0–30 m ocean heat content (OHC; J/m<sup>2</sup> * 10<sup>9</sup>) calculated from NEMO; (<b>F</b>) barrier layer thickness (BLT; m) calculated from NEMO; (<b>G</b>) mixed layer depth (MLD; m) calculated from NEMO; (<b>H</b>) isothermal layer depth (ILD; m) calculated from NEMO; (<b>I</b>) Cross-Calibrated Multi-Platform version 2 (CCMPv2) surface wind magnitude (m/s; shaded) and vectors; (<b>J</b>) ERA5 instantaneous moisture flux (kg/m<sup>2</sup>*day*10<sup>−3</sup>); (<b>K</b>) ERA5 surface sensible heat flux (J/m<sup>2</sup> * 10<sup>6</sup>); and (<b>L</b>) ERA5 surface latent heat flux (J/m<sup>2</sup> * 10<sup>7</sup>).</p>
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<p>Multiparameter analysis of the Bay of Bengal on May 23, 2020 after the storm in (<b>A</b>) Global Precipitation Measurement (GPM) precipitation rate (mm/day); (<b>B</b>) Copernicus Marine and Environment Monitoring Service (CMEMS) sea level anomalies (SLAs) (cm) overlaid with geostrophic currents (cm/s); (<b>C</b>) Nucleus for the European Modeling of the Ocean (NEMO) sea surface temperature (SST) data (°C); (<b>D</b>) NEMO sea surface salinity (SSS) data (psu); (<b>E</b>) 0–30 m ocean heat content (OHC; J/m<sup>2</sup> * 10<sup>9</sup>) calculated from NEMO; (<b>F</b>) barrier layer thickness (BLT; m) calculated from NEMO; (<b>G</b>) mixed layer depth (MLD; m) calculated from NEMO; (<b>H</b>) isothermal layer depth (ILD; m) calculated from NEMO; (<b>I</b>) Cross-Calibrated Multi-Platform version 2 (CCMPv2) surface wind magnitude (m/s; shaded) and vectors; (<b>J</b>) ERA5 instantaneous moisture flux (kg/m<sup>2</sup>*day*10<sup>−3</sup>); (<b>K</b>) ERA5 surface sensible heat flux (J/m<sup>2</sup> * 10<sup>6</sup>); and (<b>L</b>) ERA5 surface latent heat flux (J/m<sup>2</sup> * 10<sup>7</sup>).</p>
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<p>Box-averaged NEMO salinity (psu; shaded) overlaid with NEMO temperature contours (°C) and calculated mixed layer depth (m; white line) in the Bay of Bengal (86–88°E, 14°N) with depth from May 1 to June 5, 2020.</p>
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<p>Box-averaged time series from May 9 to May 27, 2020 in the northern (86–88°E, 15–20°N; black), central (86–88°E, 10–15°N; blue), and southern (86–88°E, 5–10°N; red) Bay of Bengal for (<b>A</b>) GPM precipitation (mm/day); (<b>B</b>) CCMPv2 surface wind magnitude (m/s); (<b>C</b>) CMEMS geostrophic surface currents (cm/s); (<b>D</b>) CMEMS SLA (cm); (<b>E</b>) OISST (°C); and (<b>F</b>) SMAP SSS (psu).</p>
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<p>Box-averaged time series from May 9 to May 27, 2020 in the northern (86–88°E, 15–20°N; black), central (86–88°E, 10–15°N; blue), and southern (86–88°E, 5–10°N; red) Bay of Bengal for: (<b>A</b>) NEMO-derived BLT (m); (<b>B</b>) NEMO-derived MLD (m); (<b>C</b>) NEMO-derived ILD (m); (<b>D</b>) NEMO-derived 0–30 m OHC (J/m<sup>2</sup> * 10<sup>9</sup>); (<b>E</b>) ERA5 instantaneous moisture flux (kg/m<sup>2</sup>*day*10<sup>−3</sup>); (<b>F</b>) ERA5 surface sensible heat flux (J/m<sup>2</sup> * 10<sup>6</sup>); and (<b>G</b>) ERA5 surface latent heat flux (J/m<sup>2</sup> * 10<sup>7</sup>).</p>
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<p>Time–latitude plots of (<b>a</b>) GPM precipitation rate (mm/day), (<b>b</b>) CMEMS SLA (cm), (<b>c</b>) OISST (°C), and (<b>d</b>) SMAP SSS (psu) in the Bay of Bengal (86–88°E, −5–20°N) from April 1 to May 31, 2020 with the seasonal cycle removed.</p>
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<p>30–90-day bandpass filtered time–latitude plots of (<b>a</b>) GPM precipitation rate (mm/day), (<b>b</b>) CMEMS SLA (cm), (<b>c</b>) OISST (°C), and (<b>d</b>) SMAP SSS (psu) in the Bay of Bengal (86–88°E, −5–20°N) from April 1 to May 31, 2020 with the seasonal cycle removed.</p>
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<p>Time–latitude plots of (<b>a</b>) GPM precipitation rate (mm/day), (<b>b</b>) CMEMS SLA (cm), (<b>c</b>) OISST (°C), and (<b>d</b>) SMAP SSS (psu) in the southeastern Arabian Sea (65–70°E, −5–20°N) from April 1 to May 31, 2020 with the seasonal cycle removed.</p>
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<p>30–90-day filtered time–latitude plots of (<b>a</b>) GPM precipitation rate (mm/day), (<b>b</b>) CMEMS SLA (cm), (<b>c</b>) OISST (°C), and (<b>d</b>) SMAP SSS (psu) in the southeastern Arabian Sea (65–70°E, −5–20°N) from April 1 to May 31, 2020 with the seasonal cycle removed.</p>
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<p>Spatial plots of GPM precipitation rate (shaded; mm/day) for: (<b>A</b>) May 14, (<b>B</b>) May 15, (<b>C</b>) May 16, (<b>D</b>) May 17, (<b>E</b>) May 18, (<b>F</b>) May 19, (<b>G</b>) May 31, (<b>H</b>) June 1, and (<b>I</b>) June 2, with (<b>J</b>) a box-averaged time series of ERA5 instantaneous moisture flux data (kg/m<sup>2</sup>*s*10<sup>−3</sup>) in the southeastern Arabian Sea (65–70°E, 6–13°N) from May 1 to June 5, 2020.</p>
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17 pages, 2701 KiB  
Article
FluxSat: Measuring the Ocean–Atmosphere Turbulent Exchange of Heat and Moisture from Space
by Chelle L. Gentemann, Carol Anne Clayson, Shannon Brown, Tong Lee, Rhys Parfitt, J. Thomas Farrar, Mark Bourassa, Peter J. Minnett, Hyodae Seo, Sarah T. Gille and Victor Zlotnicki
Remote Sens. 2020, 12(11), 1796; https://doi.org/10.3390/rs12111796 - 3 Jun 2020
Cited by 24 | Viewed by 9884
Abstract
Recent results using wind and sea surface temperature data from satellites and high-resolution coupled models suggest that mesoscale ocean–atmosphere interactions affect the locations and evolution of storms and seasonal precipitation over continental regions such as the western US and Europe. The processes responsible [...] Read more.
Recent results using wind and sea surface temperature data from satellites and high-resolution coupled models suggest that mesoscale ocean–atmosphere interactions affect the locations and evolution of storms and seasonal precipitation over continental regions such as the western US and Europe. The processes responsible for this coupling are difficult to verify due to the paucity of accurate air–sea turbulent heat and moisture flux data. These fluxes are currently derived by combining satellite measurements that are not coincident and have differing and relatively low spatial resolutions, introducing sampling errors that are largest in regions with high spatial and temporal variability. Observational errors related to sensor design also contribute to increased uncertainty. Leveraging recent advances in sensor technology, we here describe a satellite mission concept, FluxSat, that aims to simultaneously measure all variables necessary for accurate estimation of ocean–atmosphere turbulent heat and moisture fluxes and capture the effect of oceanic mesoscale forcing. Sensor design is expected to reduce observational errors of the latent and sensible heat fluxes by almost 50%. FluxSat will improve the accuracy of the fluxes at spatial scales critical to understanding the coupled ocean–atmosphere boundary layer system, providing measurements needed to improve weather forecasts and climate model simulations. Full article
(This article belongs to the Special Issue Remote Sensing of Air-Sea Fluxes)
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Figure 1

Figure 1
<p>(<b>a</b>) Correlation between QuikScat wind speed [<a href="#B19-remotesensing-12-01796" class="html-bibr">19</a>] and NOAA Optimum Interpolated (OI) SST [<a href="#B20-remotesensing-12-01796" class="html-bibr">20</a>] using daily, 25-km-gridded data from 2000–2009. (<b>b</b>) The same data, using zonally high-pass-filtered (1000 km cutoff) data. A negative correlation coefficient is expected when the atmosphere forces the ocean (e.g., strong winds drive ocean mixing and cool SST), while a positive correlation coefficient is expected when the ocean forces the atmosphere (e.g., warm SST drives atmospheric mixing and entrainment of faster winds from aloft). (<b>a</b>) shows that, for most of the globe, the atmosphere is forcing the ocean. (<b>b</b>) focuses on mesoscale variability and shows a completely different view, with the ocean forcing the atmosphere almost globally, except in some well-known extreme conditions, e.g., Gulf of Tehuantepec wind jets. In <b>(b),</b> both the Tropical Pacific and western boundary current regions have the strongest link between the ocean and atmosphere.</p>
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<p>The standard deviation between the climatological mean surface latent heat fluxes between four satellite flux products (HOAPS4 [<a href="#B33-remotesensing-12-01796" class="html-bibr">33</a>,<a href="#B34-remotesensing-12-01796" class="html-bibr">34</a>], SeaFlux Climate Data Record (CDR) [<a href="#B35-remotesensing-12-01796" class="html-bibr">35</a>], IFREMER 4 [<a href="#B36-remotesensing-12-01796" class="html-bibr">36</a>,<a href="#B37-remotesensing-12-01796" class="html-bibr">37</a>], J-OFURO3 [<a href="#B38-remotesensing-12-01796" class="html-bibr">38</a>]), for the 1999–2008 mean. Some of the largest differences between different flux products occur in regions with the largest fluxes.</p>
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<p>Comparisons between ship-measured (circles) and satellite-derived SeaFlux V3 dataset [<a href="#B42-remotesensing-12-01796" class="html-bibr">42</a>] (triangle) across the Gulf Stream during the CLIMODE experiment [<a href="#B17-remotesensing-12-01796" class="html-bibr">17</a>] for (<b>a</b>) wind speed, (<b>b</b>) sea–air temperature difference, (<b>c</b>) sea–air specific humidity difference, (<b>d</b>) latent heat flux, and (<b>e</b>) sensible heat flux. The satellite-derived variables lack variability compared to the ship-measured variables, which results in reduced gradients in the calculated heat fluxes. The colors of the symbols correspond to the sea surface temperature of the input data stream (either ship or satellite).</p>
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<p>Effect of temporal offsets and spatial resolution on gradients of turbulent heat fluxes. Magnitude of the time–mean (<b>a</b>) latent and (<b>b</b>) sensible heat flux gradients calculated from simultaneous output of wind speed, SST, air temperature and relative humidity at 0.125° resolution. The RMSD in (<b>c</b>) latent and (<b>d</b>) sensible heat flux gradients, with and without offsetting the timing of wind speed from other variables by 3 hours at 0.125° resolution. Magnitude of the time–mean (<b>e</b>) latent and (<b>f</b>) sensible heat flux gradients calculated from simultaneous output of wind speed, SST, air temperature and relative humidity at 0.5° resolution. Note the different ranges in the color bars for latent and sensible heat flux gradients.</p>
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<p>Depiction of turbulent heat and moisture flux error sources and potential future mitigation solutions (e.g., digital backend [<a href="#B51-remotesensing-12-01796" class="html-bibr">51</a>]).</p>
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<p>Depiction of turbulent heat and moisture flux equations. The variables in red text need to be measured.</p>
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20 pages, 10393 KiB  
Article
CYGNSS Surface Heat Flux Product Development
by Juan A. Crespo, Derek J. Posselt and Shakeel Asharaf
Remote Sens. 2019, 11(19), 2294; https://doi.org/10.3390/rs11192294 - 1 Oct 2019
Cited by 30 | Viewed by 7215
Abstract
Ocean surface heat fluxes play a significant role in the genesis and evolution of various marine-based atmospheric phenomena, from the synoptic scale down to the microscale. While in-situ measurements from buoys and flux towers will continue to be the standard in regard to [...] Read more.
Ocean surface heat fluxes play a significant role in the genesis and evolution of various marine-based atmospheric phenomena, from the synoptic scale down to the microscale. While in-situ measurements from buoys and flux towers will continue to be the standard in regard to surface heat flux estimates, they commonly have significant gaps in temporal and spatial coverage. Previous and current satellite missions have filled these gaps; though they may not observe the fluxes directly, they can measure the variables needed (wind speed, temperature and humidity) to estimate latent and sensible heat fluxes. However, current remote sensing instruments have their own limitations, such as infrequent coverage, signals attenuated by precipitation or both. The Cyclone Global Navigation Satellite System (CYGNSS) mission overcomes these limitations over the tropical and subtropical oceans by providing improved coverage in nearly all weather conditions. While CYGNSS (Level 2) primarily estimates surface winds, when coupled with observations or estimates of temperature and humidity from reanalysis data, it can provide estimates of latent and sensible heat fluxes along its orbit. This paper describes the development of the Surface Heat Flux Product for the CYGNSS mission, its current results and expected improvements and changes in future releases. Full article
(This article belongs to the Special Issue Remote Sensing of Air-Sea Fluxes)
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Graphical abstract

Graphical abstract
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<p>Full day observations of Latent (<b>a</b>,<b>c</b>) and Sensible (<b>b</b>,<b>d</b>) Heat Fluxes [W/m<sup>2</sup>] from Cyclone Global Navigation Satellite System (CYGNSS) (FDS version) on 1 January 2018 from 0000–1159 UTC (<b>a</b>,<b>b</b>) and 1200–2359 UTC (<b>c</b>,<b>d</b>).</p>
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<p>Full day observations of Latent (<b>a</b>,<b>c</b>) and Sensible (<b>b</b>,<b>d</b>) Heat Fluxes [W/m<sup>2</sup>] from CYGNSS (FDS version) on 1 July 2018 from 0000–1159 UTC (<b>a</b>,<b>b</b>) and 1200–2359 UTC (<b>c</b>,<b>d</b>).</p>
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<p>CYGNSS Surface Heat Flux Observations of Hurricane Florence on 14 September 2018. Contours of sea level pressure [black lines] at 1800 UTC with CYGNSS observations spanning ±3 hours around this time. (<b>a</b>) LHF with FDS winds, (<b>b</b>) SHF with FDS winds; (<b>c</b>) LHF with YSLF winds; (<b>d</b>) SHF with YSLF winds.</p>
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<p>CYGNSS Flux Observations of an extratropical cyclone (ETC) on 4 January 2018. Contours of sea level pressure [black lines] at 1500 UTC with CYGNSS observations spanning ±3 hours from this period. (<b>a</b>) LHF with FDS winds, (<b>b</b>) SHF with FDS winds; (<b>c</b>) LHF with YSLF winds; (<b>d</b>) SHF with YSLF winds.</p>
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<p>Location of buoys used for CYGNSS Flux Product validation.</p>
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<p>Two dimensional-density plot of collocated CYGNSS and Buoy surface latent (<b>a</b>,<b>c</b>) and sensible (<b>b</b>,<b>d</b>) surface heat fluxes. Comparisons for both versions of CYGNSS Fluxes (top: Fully Developed Seas, bottom: Young Seas with Limited Fetch). The diagonal gray line is the 1:1 agreement.</p>
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<p>Histogram of surface latent (<b>a</b>,<b>c</b>) and sensible (<b>b</b>,<b>d</b>) surface heat flux comparisons, binned at 25 W/m<sup>2</sup>, between CYGNSS and buoy data as seen in <a href="#remotesensing-11-02294-f005" class="html-fig">Figure 5</a>, with buoy on the left and CYGNSS right in each plot.</p>
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<p>Differences in fluxes (CYGNSS-Buoy) and how they vary with increasing wind speed observations from the buoy data. This is done for LHF (<b>a</b>,<b>c</b>) and SHF (<b>b</b>,<b>d</b>) and their respective FDS (<b>a</b>,<b>b</b>) and YSLF (<b>c</b>,<b>d</b>) products.</p>
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<p>Latent (LHF) and sensible (SHF) heat flux residual dependency for each bulk component. Residual data were normalized to the range of −10 to 10. The slope of the linear fit and correlation values (star marks show statistically significant value at 95% level) are included in the bottom right of each respective plot. Flux differences (CYGNSS–buoy) for (<b>a</b>–<b>c</b>) LHF FDS, (<b>d</b>–<b>f</b>) LHF YSLF, (<b>g</b>–<b>i</b>) SHF FDS and (<b>j</b>–<b>l</b>) SHF YSLF and how they all vary with wind (Δ<span class="html-italic">U</span>). Specific humidity at 10-meters (Δ<span class="html-italic">q<sub>a</sub></span>) and surface (Δ<span class="html-italic">q<sub>s</sub></span>) is shown for LHF and temperature at the surface (Δ<span class="html-italic">T<sub>a</sub></span>) and 10-meters (Δ<span class="html-italic">T<sub>s</sub></span>) for SHF. The solid line represents the linear regression.</p>
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