Sea Surface Ka-Band Doppler Measurements: Analysis and Model Development
Multi-year field measurements of sea surface Ka-band dual-co-polarized (vertical transmit–receive polarization (VV) and horizontal transmit–receive polarization (HH)) radar Doppler characteristics from an oceanographic platform in the Black Sea are presented. The Doppler centroid...
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doaj-6ff0ce5dacf84475bdc1b77ae64c40be2020-11-24T21:20:57ZengMDPI AGRemote Sensing2072-42922019-04-0111783910.3390/rs11070839rs11070839Sea Surface Ka-Band Doppler Measurements: Analysis and Model DevelopmentYury Yu. Yurovsky0Vladimir N. Kudryavtsev1Semyon A. Grodsky2Bertrand Chapron3Remote Sensing Department, Marine Hydrophysical Institute of RAS, 2 Kapitanskaya St., 299011 Sevastopol, RussiaRemote Sensing Department, Marine Hydrophysical Institute of RAS, 2 Kapitanskaya St., 299011 Sevastopol, RussiaDepartment of Atmospheric and Oceanic Science, University of Maryland, College Park, MD 20740, USASatellite Oceanography Laboratory, Russian State Hydrometeorological University, 98 Malookhtinskiy Pr., 195196 St-Petersburg, RussiaMulti-year field measurements of sea surface Ka-band dual-co-polarized (vertical transmit–receive polarization (VV) and horizontal transmit–receive polarization (HH)) radar Doppler characteristics from an oceanographic platform in the Black Sea are presented. The Doppler centroid (DC) estimated using the first moment of 5 min averaged spectrum, corrected for measured sea surface current, ranges between 0 and ≈1 m/s for incidence angles increasing from 0 to <inline-formula> <math display="inline"> <semantics> <msup> <mn>70</mn> <mo>∘</mo> </msup> </semantics> </math> </inline-formula>. Besides the known wind-to-radar azimuth dependence, the DC can also depend on wind-to-dominant wave direction. For co-aligned wind and waves, a negative crosswind DC residual is found, ≈−0.1 m/s, at ≈20<inline-formula> <math display="inline"> <semantics> <msup> <mrow></mrow> <mo>∘</mo> </msup> </semantics> </math> </inline-formula> incidence angle, becoming negligible at ≈ 60<inline-formula> <math display="inline"> <semantics> <msup> <mrow></mrow> <mo>∘</mo> </msup> </semantics> </math> </inline-formula>, and raising to, ≈+0.5 m/s, at <inline-formula> <math display="inline"> <semantics> <msup> <mn>70</mn> <mo>∘</mo> </msup> </semantics> </math> </inline-formula>. For our observations, with a rather constant dominant wave length, the DC is almost wind independent. Yet, results confirm that, besides surface currents, the DC encodes an expected wave-induced contribution. To help the interpretation, a two-scale model (KaDOP) is proposed to fit the observed DC, based on the radar modulation transfer function (MTF) previously developed for the same data set. Assuming universal spectral shape of energy containing sea surface waves, the wave-induced DC contribution is then expressed as a function of MTF, significant wave height, and wave peak frequency. The resulting KaDOP agrees well with independent DC data, except for swell-dominated cases. The swell impact is estimated using the KaDOP with a modified empirical MTF.https://www.mdpi.com/2072-4292/11/7/839radarscatterometeroceanbackscatterDoppler shiftDoppler centroidsea surface currentwind driftmodulationtransfer functionempirical model |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Yury Yu. Yurovsky Vladimir N. Kudryavtsev Semyon A. Grodsky Bertrand Chapron |
spellingShingle |
Yury Yu. Yurovsky Vladimir N. Kudryavtsev Semyon A. Grodsky Bertrand Chapron Sea Surface Ka-Band Doppler Measurements: Analysis and Model Development Remote Sensing radar scatterometer ocean backscatter Doppler shift Doppler centroid sea surface current wind drift modulation transfer function empirical model |
author_facet |
Yury Yu. Yurovsky Vladimir N. Kudryavtsev Semyon A. Grodsky Bertrand Chapron |
author_sort |
Yury Yu. Yurovsky |
title |
Sea Surface Ka-Band Doppler Measurements: Analysis and Model Development |
title_short |
Sea Surface Ka-Band Doppler Measurements: Analysis and Model Development |
title_full |
Sea Surface Ka-Band Doppler Measurements: Analysis and Model Development |
title_fullStr |
Sea Surface Ka-Band Doppler Measurements: Analysis and Model Development |
title_full_unstemmed |
Sea Surface Ka-Band Doppler Measurements: Analysis and Model Development |
title_sort |
sea surface ka-band doppler measurements: analysis and model development |
publisher |
MDPI AG |
series |
Remote Sensing |
issn |
2072-4292 |
publishDate |
2019-04-01 |
description |
Multi-year field measurements of sea surface Ka-band dual-co-polarized (vertical transmit–receive polarization (VV) and horizontal transmit–receive polarization (HH)) radar Doppler characteristics from an oceanographic platform in the Black Sea are presented. The Doppler centroid (DC) estimated using the first moment of 5 min averaged spectrum, corrected for measured sea surface current, ranges between 0 and ≈1 m/s for incidence angles increasing from 0 to <inline-formula> <math display="inline"> <semantics> <msup> <mn>70</mn> <mo>∘</mo> </msup> </semantics> </math> </inline-formula>. Besides the known wind-to-radar azimuth dependence, the DC can also depend on wind-to-dominant wave direction. For co-aligned wind and waves, a negative crosswind DC residual is found, ≈−0.1 m/s, at ≈20<inline-formula> <math display="inline"> <semantics> <msup> <mrow></mrow> <mo>∘</mo> </msup> </semantics> </math> </inline-formula> incidence angle, becoming negligible at ≈ 60<inline-formula> <math display="inline"> <semantics> <msup> <mrow></mrow> <mo>∘</mo> </msup> </semantics> </math> </inline-formula>, and raising to, ≈+0.5 m/s, at <inline-formula> <math display="inline"> <semantics> <msup> <mn>70</mn> <mo>∘</mo> </msup> </semantics> </math> </inline-formula>. For our observations, with a rather constant dominant wave length, the DC is almost wind independent. Yet, results confirm that, besides surface currents, the DC encodes an expected wave-induced contribution. To help the interpretation, a two-scale model (KaDOP) is proposed to fit the observed DC, based on the radar modulation transfer function (MTF) previously developed for the same data set. Assuming universal spectral shape of energy containing sea surface waves, the wave-induced DC contribution is then expressed as a function of MTF, significant wave height, and wave peak frequency. The resulting KaDOP agrees well with independent DC data, except for swell-dominated cases. The swell impact is estimated using the KaDOP with a modified empirical MTF. |
topic |
radar scatterometer ocean backscatter Doppler shift Doppler centroid sea surface current wind drift modulation transfer function empirical model |
url |
https://www.mdpi.com/2072-4292/11/7/839 |
work_keys_str_mv |
AT yuryyuyurovsky seasurfacekabanddopplermeasurementsanalysisandmodeldevelopment AT vladimirnkudryavtsev seasurfacekabanddopplermeasurementsanalysisandmodeldevelopment AT semyonagrodsky seasurfacekabanddopplermeasurementsanalysisandmodeldevelopment AT bertrandchapron seasurfacekabanddopplermeasurementsanalysisandmodeldevelopment |
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