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Remote Sensing of Atmospheric Components and Water Vapor

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

Deadline for manuscript submissions: closed (31 March 2020) | Viewed by 43190

Special Issue Editors


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Guest Editor
Department of Experimental Sciences Teaching, University of Valladolid, Valladolid, Spain
Interests: radiometry; radiative transfer; remote sensing; aerosols; water vapor; ozone; clouds; solar and UV radiation

Special Issue Information

Dear Colleagues

This is an invitation to contribute to the Special Issue, “Remote Sensing of Atmospheric Components and Water Vapor”, regarding the retrieval, analysis and validation of atmospheric components (gases) by remote sensing technique: Water vapor (H2O(v)), CO2 and CH4 as representatives of greenhouse gases; SO2, NO2, CO, HCHO, as main trace gases, and obviously ozone and those related with its decline, such as OCl, OClO, OBr, and CFCs. A wide set of different techniques may be considered, mainly those based on radiometry, spectroscopy (i.e., DOAS, FTS, etc.) in the solar or infrared spectral range, and also including LIDAR and related techniques of general applications for probing the atmosphere. Other techniques, such as GPS and radiosounding are necessary for water vapor retrieval. These techniques may be applied from local to global scales as the main tool for the monitoring of these atmospheric constituents: From surface local measurements, usually arranged into regional or global networks (NDAC, TCCON, Brewer network, etc.) to the great variety of Earth Observing satellite sensors. When long-term data are available, climatology studies, seasonal cycles, and trend analyses will be also welcome. Although clouds and aerosols are not considered as this issue is focused on gases, their effects or interactions in the determination of atmospheric gases are also of great interest. Monitoring of atmospheric gas composition is of vital importance in climate change.

Dr. Victoria E. Cachorro
Guest Editor
Dr. Manuel Antón
Co-Guest Editor

Manuscript Submission Information

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Keywords

  • remote sensing
  • atmosphere
  • atmospheric gases
  • ozone
  • water vapor
  • radiometry
  • spectroscopy
  • satellite sensors
  • Lidar

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Published Papers (12 papers)

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Editorial

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6 pages, 215 KiB  
Editorial
Editorial for the Special Issue “Remote Sensing of Atmospheric Components and Water Vapor”
by Victoria E. Cachorro and Manuel Antón
Remote Sens. 2020, 12(13), 2074; https://doi.org/10.3390/rs12132074 - 28 Jun 2020
Viewed by 1835
Abstract
The observation/monitoring of atmospheric components and water vapor in the atmosphere is today open to very different remote sensing techniques, most of them based on the radiation-matter interaction covering the full electromagnetic spectrum. This SI collects some papers regarding the retrieval, calibration, validation, [...] Read more.
The observation/monitoring of atmospheric components and water vapor in the atmosphere is today open to very different remote sensing techniques, most of them based on the radiation-matter interaction covering the full electromagnetic spectrum. This SI collects some papers regarding the retrieval, calibration, validation, analysis of data and uncertainties, as well as comparative studies on atmospheric gases and water vapor by remote sensing techniques, where different types of sensors, instruments, and algorithms are used or developed. Full article
(This article belongs to the Special Issue Remote Sensing of Atmospheric Components and Water Vapor)

Research

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21 pages, 2716 KiB  
Article
Column Integrated Water Vapor and Aerosol Load Characterization with the New ZEN-R52 Radiometer
by Antonio Fernando Almansa, Emilio Cuevas, África Barreto, Benjamín Torres, Omaira Elena García, Rosa Delia García, Cristian Velasco-Merino, Victoria Eugenia Cachorro, Alberto Berjón, Manuel Mallorquín, César López, Ramón Ramos, Carmen Guirado-Fuentes, Ramón Negrillo and Ángel Máximo de Frutos
Remote Sens. 2020, 12(9), 1424; https://doi.org/10.3390/rs12091424 - 30 Apr 2020
Cited by 10 | Viewed by 3807
Abstract
The study shows the first results of the column-integrated water vapor retrieved by the new ZEN-R52 radiometer. This new radiometer has been specifically designed to monitor aerosols and atmospheric water vapor with a high degree of autonomy and robustness in order to allow [...] Read more.
The study shows the first results of the column-integrated water vapor retrieved by the new ZEN-R52 radiometer. This new radiometer has been specifically designed to monitor aerosols and atmospheric water vapor with a high degree of autonomy and robustness in order to allow the expansion of the observations of these parameters to remote desert areas from ground-based platforms. The ZEN-R52 device shows substantial improvements compared to the previous ZEN-R41 prototype: a smaller field of view, an increased signal-to-noise ratio, better stray light rejection, and an additional channel (940 nm) for precipitable water vapor (PWV) retrieval. PWV is inferred from the ZEN-R52 Zenith Sky Radiance (ZSR) measurements using a lookup table (LUT) methodology. The improvement of the new ZEN-R52 in terms of ZSR was verified by means of a comparison with the ZEN-R41, and with the Aerosol Robotic Network (AERONET) Cimel CE318 (CE318-AERONET) at Izaña Observatory, a Global Atmosphere Watch (GAW) high mountain station (Tenerife, Canary Islands, Spain), over a 10-month period (August 2017 to June 2018). ZEN-R52 aerosol optical depth (AOD) was extracted by means of the ZEN–AOD–LUT method with an uncertainty of ±0.01 ± 0.13*AOD. ZEN-R52 PWV extracted using a new LUT technique was compared with quasi-simultaneous (±30 s) Fourier Transform Infrared (FTIR) spectrometer measurements as reference. A good agreement was found between the two instruments (PWV means a relative difference of 9.1% and an uncertainty of ±0.089 cm or ±0.036 + 0.061*PWV for PWV <1 cm). This comparison analysis was extended using two PWV datasets from the same CE318 reference instrument at Izaña Observatory: one obtained from AERONET (CE318-AERONET), and another one using a specific calibration of the 940-nm channel performed in this work at Izaña Atmospheric Research Center Observatory (CE318-IARC), which improves the PWV product. Full article
(This article belongs to the Special Issue Remote Sensing of Atmospheric Components and Water Vapor)
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Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>Monthly precipitable water vapor (PWV) and aerosol optical depth (AOD)<sub>500</sub> averages (solid lines) and corresponding standard deviations (error bars) at Izaña station. PWV annual cycle given by Total Column Carbon Observing Network (TCCON) Fourier Transform Infrared (FTIR) (blue line) has been calculated for 2007–2019. Aerosol Robotic Network (AERONET) PWV (orange line) and AOD<sub>500</sub> (red line) have been calculated for 2005-2019.</p>
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<p>ZEN-R52 picture.</p>
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<p>ZEN quality control (ZEN-QC) scheme flowchart.</p>
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<p>AOD at 500 nm for a 10-month period (August 2017 to June 2018) at Izaña station obtained from ZEN-R52 and CE318-AERONET radiometers. Grey crosses represent ZEN-R52 unfiltered AOD data, red solid circles depict ZEN-R52 AOD after applying the ZEN-QC algorithm, and blue squares show CE318-AERONET level 2.0 AOD data.</p>
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<p>Coincidences (%) between AERONET and ZEN quality control algorithms for eight solar zenith angle (SZA) intervals. The black line represents the average of 68.8% of the coincidences.</p>
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<p>ZSR relative differences between (<b>a</b>) ZEN-R52 and (<b>b</b>) ZEN-R41 against CE318-AERONET ((ZSR<sub>ZEN-R</sub>-ZSR<sub>CE318</sub>)/ ZSR<sub>CE318</sub>) in logarithmic scale at the four coincident channels: 870 nm (grey crosses), 675 nm (red circles), 440 nm (blue squares), and 500 nm (green triangles).</p>
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<p>AOD scatter plot between AERONET and ZEN-R52 at 440 nm (<b>a</b>) and 870 nm (<b>b</b>) nominal wavelengths. The red line shows the linear fit equation, the broken grey line shows the diagonal and the colour bar indicates the density of data. ZEN-R52–AERONET AOD differences against the solar zenith angle are shown in (<b>c</b>) for 440 nm and in (<b>d</b>) for 870 nm, where the colour bar indicates AERONET AOD.</p>
Full article ">Figure 8
<p>Standard deviation of the AOD differences between CE318-AERONET and ZEN-R52 for different AOD intervals of 0.05 between zero and 0.6. Data at 440, 500, 675, and 870 nm, are represented by blue squares, green triangles, red circles, and grey crosses, respectively. The black solid line represents the fitting equation for the standard deviation of the AOD differences for AOD values between zero and 0.2, while the broken black line depicts the fitting equation for the standard deviation of the AOD differences for higher AOD values (0.25 to 0.55).</p>
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<p>PWV scatterplots between ZEN-R52, CE318-AERONET, CE318-IARC and FTIR at Izaña over a 10-month period (August 2017 to June 2018 <b>a</b>–<b>f</b>). The red line shows the linear fit equation, the broken grey line shows the diagonal and the colour bar indicates the density of data.</p>
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<p>Standard deviation of the PWV differences between FTIR and ZEN-R52 (blue dots) for PWV intervals of 0.1 cm between 0 and 1.3 cm approximately. Numbers near the dots indicate the number of data included in each interval. The black solid line represents the fitting equation for the standard deviation of the PWV differences for PWV values between 0.1 and 1.0 cm. The broken grey line depicts the standard deviation of PWV differences between FTIR and ZEN-R52 for the full dataset.</p>
Full article ">
19 pages, 13590 KiB  
Article
Assessment of Sampling Effects on Various Satellite-Derived Integrated Water Vapor Datasets Using GPS Measurements in Germany as Reference
by Cintia Carbajal Henken, Lisa Dirks, Sandra Steinke, Hannes Diedrich, Thomas August and Susanne Crewell
Remote Sens. 2020, 12(7), 1170; https://doi.org/10.3390/rs12071170 - 6 Apr 2020
Cited by 9 | Viewed by 3007
Abstract
Passive imagers on polar-orbiting satellites provide long-term, accurate integrated water vapor (IWV) data sets. However, these climatologies are affected by sampling biases. In Germany, a dense Global Navigation Satellite System network provides accurate IWV measurements not limited by weather conditions and with high [...] Read more.
Passive imagers on polar-orbiting satellites provide long-term, accurate integrated water vapor (IWV) data sets. However, these climatologies are affected by sampling biases. In Germany, a dense Global Navigation Satellite System network provides accurate IWV measurements not limited by weather conditions and with high temporal resolution. Therefore, they serve as a reference to assess the quality and sampling issues of IWV products from multiple satellite instruments that show different orbital and instrument characteristics. A direct pairwise comparison between one year of IWV data from GPS and satellite instruments reveals overall biases (in kg/m 2 ) of 1.77, 1.36, 1.11, and −0.31 for IASI, MIRS, MODIS, and MODIS-FUB, respectively. Computed monthly means show similar behaviors. No significant impact of averaging time and the low temporal sampling on aggregated satellite IWV data is found, mostly related to the noisy weather conditions in the German domain. In combination with SEVIRI cloud coverage, a change of shape of IWV frequency distributions towards a bi-modal distribution and loss of high IWV values are observed when limiting cases to daytime and clear sky. Overall, sampling affects mean IWV values only marginally, which are rather dominated by the overall retrieval bias, but can lead to significant changes in IWV frequency distributions. Full article
(This article belongs to the Special Issue Remote Sensing of Atmospheric Components and Water Vapor)
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Figure 1

Figure 1
<p>Examples of spatial sampling for IASI, MIRS and MODIS for 24 April 2013 over a German domain, at overpass times of about 19:34 UTC, 20:30 UTC and 12:30 UTC, respectively. On the right are the GPS stations (circles) from the German GPS network used in this study and corresponding IWV values at the MODIS overpass time. For this day IWV products from 236 GPS stations were available. Areas in grey indicate that no (successful) IWV retrievals were performed or obtained.</p>
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<p>Temporal sampling of the IASI, MIRS and MODIS instruments at all GPS stations combined for one year, assuming for each satellite overpass a maximum distance of 20 km and a maximum time difference of 7.5 min between satellite pixel and GPS station.</p>
Full article ">Figure 3
<p>2D histograms and probability density functions for IWV GPS vs. IWV from IASI, MIRS, MODIS and MODIS-FUB. The dashed black-white diagonal line is the 1:1 line, while the dashed red-blue line presents a linear fit through the data. Corresponding statistical quantities can be found in <a href="#remotesensing-12-01170-t002" class="html-table">Table 2</a>.</p>
Full article ">Figure 4
<p>Bias (inner circle colors ranging from blue to red) and standard deviation (std; outer circle colors in greyish colors) at each GPS station for all matched IWV observations within one year. Only the GPS stations are included with at least 20 valid satellite-GPS data pairs.</p>
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<p>Comparison of monthly mean of IWV from GPS to IASI, MIRS, MODIS and MODIS-FUB for all months from June 2012 to May 2013. The error bars show the standard deviation. Bias and root mean square error (RMSE) are given in kg/m<math display="inline"><semantics> <msup> <mrow/> <mn>2</mn> </msup> </semantics></math>.</p>
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<p>Averaging time period vs. error (using as reference GPS climatologies computed from all 15 min IWV values within an averaging time period) obtained from bootstrap using a sample size of 10,000 for each averaging time period. The dots show the median and the bars indicate the 5% and 95% confidence levels. <b>Left:</b> for GPS IWV values for all matched satellite pixels. <b>Middle:</b> for GPS IWV values for all matched satellite pixels with successfully retrieved satellite IWV values. <b>Right:</b> satellite IWV values for all matched satellite pixels and successfully retrieved satellite IWV values</p>
Full article ">Figure 7
<p>IWV distributions for all GPS IWV observations, for all GPS IWV observations during daytime as well as for certain clear-sky and certain cloudy cases.</p>
Full article ">Figure 8
<p>Hourly deviations from the IWV daily mean (zero black dashed line) computed using all 15 min GPS IWV values from the one-year time period (black line) and using all 15 min GPS IWV values from the years 2007–2013 (grey line). Overlaid are the deviations of the satellite daily means, computed using the GPS IWV values for matched GPS-satellite cases, to the GPS daily mean from the one-year time period (colored horizontal lines). The relative frequency of occurrence of satellite IWV values at corresponding hourly time intervals is shown in the lower parts of the panels. Results are presented for local time (LT) for four seasons: June–July–August (JJA), September–October–November (SON), December–January–February (DJF), March–April–May (MAM).</p>
Full article ">Figure 9
<p>IWV distributions for GPS IWV values for all GPS time steps (black), for GPS IWV values for all time steps matched with satellite observations (green), for GPS IWV values for all timesteps matched with satellite observations with valid IWV retrieval (blue), and for all matched valid satellite IWV values (red).</p>
Full article ">
26 pages, 5897 KiB  
Article
Satellite-Observed Variations and Trends in Carbon Monoxide over Asia and Their Sensitivities to Biomass Burning
by Xun Zhang, Jane Liu, Han Han, Yongguang Zhang, Zhe Jiang, Haikun Wang, Lingyun Meng, Yi Chen Li and Yi Liu
Remote Sens. 2020, 12(5), 830; https://doi.org/10.3390/rs12050830 - 4 Mar 2020
Cited by 35 | Viewed by 6873
Abstract
As the carbon monoxide (CO) total column over Asia is among the highest in the world, it is important to characterize its variations in space and time. Using Measurements of Pollution in the Troposphere (MOPITT) and Atmospheric InfraRed Sounder (AIRS) satellite data, the [...] Read more.
As the carbon monoxide (CO) total column over Asia is among the highest in the world, it is important to characterize its variations in space and time. Using Measurements of Pollution in the Troposphere (MOPITT) and Atmospheric InfraRed Sounder (AIRS) satellite data, the variations and trends in CO total column over Asia and its seven subregions during 2003–2017 are investigated in this study. The CO total column in Asia is higher in spring and winter than in summer and autumn. The seasonal maximum and minimum are in spring and summer respectively in the regional mean over Asia, varying between land and oceans, as well as among the subregions. The CO total column in Asia shows strong interannual variation, with a regional mean coefficient of variation of 5.8% in MOPITT data. From 2003 to 2017, the annual mean of CO total column over Asia decreased significantly at a rate of (0.58 ± 0.15)% per year (or −(0.11 ± 0.03) × 1017 molecules cm−2 per year) in MOPITT data, resulting from significant CO decreases in winter, summer, and spring. In most of the subregions, significant decreasing trends in CO total column are also observed, more obviously over areas with high CO total column, including eastern regions of China and the Sichuan Basin. The regional decreasing trends in these areas are over 1% per year. Over the entire Asia, and in fire-prone subregions including South Siberia, Indo-China Peninsula, and Indonesia, we found significant correlations between the MOPITT CO total column and the fire counts from the Moderate Resolution Imaging Spectroradiometer (MODIS). The variations in MODIS fire counts may explain 58%, 60%, 36%, and 71% of the interannual variation in CO total column in Asia and these three subregions, respectively. Over different land cover types, the variations in biomass burning may explain 62%, 52%, and 31% of the interannual variation in CO total column, respectively, over the forest, grassland, and shrubland in Asia. Extremes in CO total column in Asia can be largely explained by the extreme fire events, such as the fires over Siberia in 2003 and 2012 and over Indonesia in 2006 and 2015. The significant decreasing trends in MODIS fire counts inside and outside Asia suggest that global biomass burning may be a driver for the decreasing trend in CO total column in Asia, especially in spring. In general, the variations and trends in CO total column over Asia detected by AIRS are similar to but smaller than those by MOPITT. The two datasets show similar spatial and temporal variations in CO total column over Asia, with correlation coefficients of 0.86–0.98 in the annual means. This study shows that the interannual variation in atmospheric CO in Asia is sensitive to biomass burning, while the decreasing trend in atmospheric CO over Asia coincides with the decreasing trend in MODIS fire counts from 2003 to 2017. Full article
(This article belongs to the Special Issue Remote Sensing of Atmospheric Components and Water Vapor)
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Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>(<b>a</b>) Land cover types over Asia in 2015. The boxed areas indicate the subregions, namely, South Siberia, India, Indo-China Peninsula, Indonesia, the Sichuan Basin, North China, and South China. (<b>b</b>) The annual total fire counts from the Moderate Resolution Imaging Spectroradiometer (MODIS) data [<a href="#B46-remotesensing-12-00830" class="html-bibr">46</a>] and (<b>c</b>) the annual total carbon monoxide (CO) emissions from biomass burning (BB) from the Global Fire Emissions Database (GFED) data [<a href="#B27-remotesensing-12-00830" class="html-bibr">27</a>]. The grid size is 1° × 1°. The values in (<b>b</b>) and (<b>c</b>) are the means over 2003–2017.</p>
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<p>Spatial distributions of the seasonal total fire counts in (<b>a</b>) spring, (<b>b</b>) summer, (<b>c</b>) autumn and (<b>d</b>) winter from the MODIS data [<a href="#B46-remotesensing-12-00830" class="html-bibr">46</a>]. The values are the mean over 2003–2017. The grid size is 1° × 1°.</p>
Full article ">Figure 3
<p>(<b>a</b>) MODIS total fire counts and (<b>b</b>) GFED4 total CO emissions from biomass burning (BB). The fractional contribution of each land cover type to the total fire counts (<b>c</b>) and to the total CO emissions from BB (<b>d</b>). The bars in (<b>a</b>) and (<b>b</b>) indicate the standard deviation. All the values are the means over 2003–2017.</p>
Full article ">Figure 4
<p>Spatial distributions of annual and seasonal mean CO total columns in Asia averaged over 2003–2017 from the Measurements of Pollution in the Troposphere (MOPITT) (the 1st column) and Atmospheric InfraRed Sounder (AIRS) (the 2nd column). Correlation coefficients (r) between MOPITT and AIRS CO total column (the 3rd column). The shadow areas indicate that the r is statistically significant (p &lt; 0.05). The corresponding annual mean is shown in (<b>a</b>–<b>c</b>) (the 1st row). The corresponding seasonal mean is shown in (<b>d</b>–<b>f</b>) for spring (the 2nd row), in (<b>g</b>–<b>i</b>) for summer (the 3rd row), in (<b>j</b>–<b>l</b>) for autumn (the 4th row) and in (<b>m</b>–<b>o</b>) for winter (the 5th row).</p>
Full article ">Figure 5
<p>Comparison of CO total column between MOPITT and AIRS data averaged over (<b>a</b>) Asia, (<b>b</b>) the land of Asia and (<b>c</b>) the oceans of Asia, from 2003 to 2017. The correlation coefficients (r) with an asterisk indicate a significance level at over 95% (p &lt; 0.05).</p>
Full article ">Figure 6
<p>The annual mean and seasonal variations in MOPITT and AIRS CO total columns averaged over Asia and its subregions during 2003–2017: (<b>a</b>) Asia, (<b>b</b>) the land of Asia, (<b>c</b>) the ocean of Asia, (<b>d</b>) South Siberia,(<b>e</b>) India, (<b>f</b>) North China, (<b>g</b>) South China, (<b>h</b>) the Sichuan Basin, (<b>i</b>) Indo-China Peninsula and (<b>j</b>) Indonesia. The bar indicates the standard deviation. The values in (<b>a</b>), (<b>b</b>), and (<b>c</b>) are for the mean CO total column from MOPITT data.</p>
Full article ">Figure 7
<p>Interannual variations in MOPITT and AIRS CO total column averaged over Asia during 2003–2017. The bar indicates the standard deviation. CV is the ratio of the standard deviation to the long-term mean.</p>
Full article ">Figure 8
<p>Based on MOPITT data: (<b>a</b>) Spatial distribution of CV of the annual CO total column over 2003–2017. (<b>b</b>) The means CV of CO total column in Asia, its subregions, and the world. The bar indicates the standard deviation of the mean CV. CV is the ratio of the standard deviation to the long-term mean.</p>
Full article ">Figure 9
<p>Horizontal distributions of the trends in CO total column during 2003–2017 from MOPITT (left column: (<b>a</b>) annual, (<b>c</b>) spring, (<b>e</b>) summer, (<b>g</b>) autumn, and (<b>i</b>) winter) and AIRS (right column: (<b>b</b>) annual, (<b>d</b>) spring, (<b>f</b>) summer, (<b>h</b>) autumn and (<b>j</b>) winter). The shadow indicates that the trends are statistically significant (p &lt; 0.05).</p>
Full article ">Figure 10
<p>Trends in CO total columns (in %) from MOPITT and AIRS data averaged over Asia and its subregions during 2003–2017: (<b>a</b>) Asia, (<b>b</b>) the land of Asia, (<b>c</b>) the ocean of Asia, (<b>d</b>) South Siberia, (<b>e</b>) India, (<b>f</b>) North China, (<b>g</b>) South China, (<b>h</b>) the Sichuan Basin, (<b>i</b>) Indo-China Peninsula and (<b>j</b>) Indonesia. The red star indicates that the trend is statistically significant at 95% level (p &lt; 0.05). The bar indicates the 95% confident interval.</p>
Full article ">Figure 11
<p>Interannual variations in the annual fire counts and annual CO emissions from biomass burning (BB) over Asia during 2003–2017.</p>
Full article ">Figure 12
<p>Correlation between CO total column and the MODIS fire counts (left column: (<b>a</b>) annual, (<b>c</b>) spring, (<b>e</b>) summer, (<b>g</b>) autumn and (<b>i</b>) winter) and between CO total column and the GFED4 CO emissions from biomass burning (right column: (<b>b</b>) annual, (<b>d</b>) spring, (<b>f</b>) summer, (<b>h</b>) autumn, and (<b>j</b>) winter) averaged over the land of Asia during 2003–2017. The star indicates that the trend is statistically significant at 95% level (p &lt; 0.05). The number beside each dot denotes the last two digits of the year.</p>
Full article ">Figure 13
<p>Monthly variations in the anomalies of (<b>a</b>) MOPITT CO total column, (<b>b</b>) fire counts, and (<b>c</b>) CO emissions from biomass burning (BB) averaged over 60–140°E during 2003–2017. Rectangles mark the extreme fire events.</p>
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<p>Interannual variations and trends in MODIS fire counts and GFED4 fire emissions in the annual mean and by season: (<b>a</b>) fire counts inside Asia, (<b>b</b>) fire CO emissions inside Asia, (<b>c</b>), fire counts outside Asia, (<b>d</b>) fire CO emissions outside Asia. The black star indicates that the trend is statistically significant (p &lt; 0.05).</p>
Full article ">
18 pages, 9278 KiB  
Article
Evaluation of Environmental Moisture from NWP Models with Measurements from Advanced Geostationary Satellite Imager—A Case Study
by Xiaowei Jiang, Jun Li, Zhenglong Li, Yunheng Xue, Di Di, Pei Wang and Jinlong Li
Remote Sens. 2020, 12(4), 670; https://doi.org/10.3390/rs12040670 - 18 Feb 2020
Cited by 9 | Viewed by 3132
Abstract
The distribution of tropospheric moisture in the environment is highly associated with storm development. Therefore, it is important to evaluate the uncertainty of moisture fields from numerical weather prediction (NWP) models for better understanding and enhancing storm prediction. With water vapor absorption band [...] Read more.
The distribution of tropospheric moisture in the environment is highly associated with storm development. Therefore, it is important to evaluate the uncertainty of moisture fields from numerical weather prediction (NWP) models for better understanding and enhancing storm prediction. With water vapor absorption band radiance measurements from the advanced imagers onboard the new generation of geostationary weather satellites, it is possible to quantitatively evaluate the environmental moisture fields from NWP models. Three NWP models—Global Forecast System (GFS), Unified Model (UM), Weather Research and Forecasting (WRF)—are evaluated with brightness temperature (BT) measurements from the three moisture channels of Advanced Himawari Imager (AHI) onboard the Himawari-8 satellite for Typhoon Linfa (2015) case. It is found that the three NWP models have similar performance for lower tropospheric moisture, and GFS has a smaller bias for middle tropospheric moisture. Besides, there is a close relationship between moisture forecasts in the environment and the tropical cyclone (TC) track forecasts in GFS, while regional WRF does not show this pattern. When the infrared and microwave sounder radiance measurements from polar orbit satellite are assimilated in regional WRF, it is clearly shown that the environment moisture fields are improved compared with that with only conventional data are assimilated. Full article
(This article belongs to the Special Issue Remote Sensing of Atmospheric Components and Water Vapor)
Show Figures

Graphical abstract

Graphical abstract
Full article ">Figure 1
<p>(<b>a</b>) Himawari-8 true-color Red/Green/Blue (RGB) full-disk image at 0340 UTC. The tropical cyclone in the black box is typhoon Linfa. (<b>b</b>) The best track of typhoon Linfa. Images from the Cooperative Institute for Meteorological Satellite Studies (CIMSS)/Space Science and Engineering Center (SSEC)/University of Wisconsin-Madison.</p>
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<p>The water vapor (WV) Jacobian Function of Advanced Himawari Imager (AHI) calculated from a tropical atmospheric profile using the fast-radiative transfer model, hyperspectral infrared (IR) all-sky radiative transfer model (HIRTM).</p>
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<p>Brightness temperature (BT) images from three water vapor channels of AHI for (upper panel) all skies and (lower panel) clear skies on 5 July 2015 at 1800 UTC. The lower panels are limited to the satellite zenith angle of 67 degree.</p>
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<p>BT sensitivity to moisture with (<b>a</b>) increasing moisture from 0% to 50%, and (<b>b</b>) decreasing moisture from 0% to −50%. Blue line is for AHI Channel 8, green line is for AHI Channel 9 and red line is for AHI Channel 10. A tropical atmospheric profile is used in the calculations.</p>
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<p>(upper right) AHI/Himawari-8 channel 8 BT measurements, (upper) calculated BTs from GFS, UM and WRF (GTS only) 12-h forecasts (07-05-2015 1800 UTC [06 UTC+12 h]), and (bottom) the corresponding BT difference (BTD; model - observation) using HIRTM. GFS = Global Forecast System; UM = Unified Model; WRF = Weather Research and Forecasting; GTS = Global Telecommunication System.</p>
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<p>Same as <a href="#remotesensing-12-00670-f005" class="html-fig">Figure 5</a> but for AHI channel 9.</p>
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<p>Same as <a href="#remotesensing-12-00670-f005" class="html-fig">Figure 5</a> but for AHI channel 10.</p>
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<p>(upper right) AHI/Himawari-8 channel 8 BT measurements, (upper) calculated BTs from WRF (GTS only) and WRF (GTS+JPSS) 12-h forecasts (07-05-2015 1800 UTC [06 UTC+12 h]), and (bottom) the BTD (model—observation) using HIRTM. JPSS = Joint Polar Satellite System.</p>
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<p>Same as <a href="#remotesensing-12-00670-f008" class="html-fig">Figure 8</a> but for AHI channel 9.</p>
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<p>Same as <a href="#remotesensing-12-00670-f008" class="html-fig">Figure 8</a> but for AHI channel 10.</p>
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<p>Time series of BT bias between models calculations (from GFS, UM, WRF (GTS only) and WRF (GTS+JPSS)) and AHI observations for the three WV absorption bands of 72-h forecasts started from 1800 UTC 5 July 2015. The x-axis represents for the forecast time (unit: UTC) and y-axis represents for the BT bias (unit: K).</p>
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<p>Root mean square error (RMSE) of (<b>a</b>) track (km) and (<b>b</b>) intensity (characterized by maximum wind speed, m/s) between the Japan Meteorological Administration (JMA) best track data for typhoon Linfa (2015) and the 72 h forecasts (started from Jul-05-2015 1800 UTC) from GFS, UM, WRF (GTS only) and WRF (GTS+JPSS).</p>
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<p>The correlation between moisture forecast bias (absolute value) and track forecast bias of GFS (blue line) and WRF with conventional data and JPSS satellite data assimilation (red line) for three WV absorption bands. The x-axis represents for the brightness temperature bias (unit: K) and y-axis represents for the track bias (unit: km).</p>
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<p>Same as <a href="#remotesensing-12-00670-f013" class="html-fig">Figure 13</a> but the y-axis is for intensity bias.</p>
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21 pages, 15213 KiB  
Article
Preliminary Evaluation of the Error Budgets in the TALIS Measurements and Their Impact on the Retrievals
by Wenyu Wang, Zhenzhan Wang and Yongqiang Duan
Remote Sens. 2020, 12(3), 468; https://doi.org/10.3390/rs12030468 - 2 Feb 2020
Cited by 6 | Viewed by 2331
Abstract
The THz Atmospheric Limb Sounder (TALIS) is a Chinese sub-millimeter limb sounder being designed by National Space Science Center of the Chinese Academy of Sciences to measure the temperature and chemical constituents vertically in the middle and upper atmosphere, with good precision and [...] Read more.
The THz Atmospheric Limb Sounder (TALIS) is a Chinese sub-millimeter limb sounder being designed by National Space Science Center of the Chinese Academy of Sciences to measure the temperature and chemical constituents vertically in the middle and upper atmosphere, with good precision and vertical resolution. This paper presents a simulation study that assesses the measurement errors and their impacts on the retrievals. Three error sources, including instrument uncertainties, calibration errors and a priori errors, are considered. The sideband weight uncertainty, the local oscillator, the pointing angle offsets and the measurement noise (NEDT), are considered as instrument uncertainties. Calibration errors consist of the hot target offset, the nonlinearity residual of the two-point calibration, use of the Rayleigh–Jeans (R–J) approximation and the choice of the antenna pattern. A priori profile errors of temperature, pressure and species are also considered. The results suggest that the antenna pattern mainly affects the retrievals in the troposphere. The NEDT is a major error source affecting all of the retrievals. The R–J approximation has a great impact upon the retrievals at 643 GHz, and should not be used. The local oscillator offset leads to an obvious error above 50 km. The effect of nonlinearity residuals cannot be neglected above 70 km. The impact of the sideband weight uncertainty and the hot target offset are relatively small. The pointing and the a priori errors can be neglected in most observation regions. Full article
(This article belongs to the Special Issue Remote Sensing of Atmospheric Components and Water Vapor)
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Figure 1

Figure 1
<p>Schematic of two-point calibration.</p>
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<p>The variations of calibration errors with temperature and the count ratio induced by the R–J approximation: (<b>a</b>) variations with temperature; (<b>b</b>) variations with the count ratio. Here <math display="inline"><semantics> <mrow> <msubsup> <mi>T</mi> <mi>B</mi> <mo> </mo> </msubsup> </mrow> </semantics></math> is calculated by Equation (3), and <math display="inline"><semantics> <mrow> <msubsup> <mi>T</mi> <mrow> <mi>R</mi> <mi>J</mi> </mrow> <mo> </mo> </msubsup> </mrow> </semantics></math> is obtained from replacing <math display="inline"><semantics> <mi>I</mi> </semantics></math> by <math display="inline"><semantics> <mi>T</mi> </semantics></math> with <math display="inline"><semantics> <mrow> <msubsup> <mi>T</mi> <mi>C</mi> <mo> </mo> </msubsup> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msubsup> <mi>T</mi> <mi>H</mi> <mo> </mo> </msubsup> </mrow> </semantics></math> set to 2.73 and 300 K, respectively. The count ratio means <math display="inline"><semantics> <mrow> <mfrac> <mrow> <msub> <mi>C</mi> <mi>A</mi> </msub> <mo>−</mo> <msub> <mi>C</mi> <mi>C</mi> </msub> </mrow> <mrow> <msub> <mi>C</mi> <mi>H</mi> </msub> <mo>−</mo> <msub> <mi>C</mi> <mi>C</mi> </msub> </mrow> </mfrac> </mrow> </semantics></math>.</p>
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<p>The antenna pattern of TALIS: (<b>a</b>) the 118 GHz antenna pattern; (<b>b</b>) the 190 GHz antenna pattern; (<b>c</b>) the 240 GHz antenna pattern; (<b>d</b>) the 643 GHz antenna pattern.</p>
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<p>The retrieval precision of the four radiometers with different retrieval grids, and only random noises are added: (<b>a</b>) 118 GHz temperature retrieval; (<b>b</b>) 190 GHz H2O retrieval; (<b>c</b>) 240 GHz O3 retrieval; (<b>d</b>) 643 GHz HCl retrieval. The 1 km, 2.5 km, 5 km represent the different retrieval grids. The “Profile” represents the typical profile.</p>
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<p>The temperature retrieval errors induced by different instrument uncertainty sources: (<b>a</b>) absolute and (<b>b</b>) relative retrieval errors. The uncertainties assumed are summarized in <a href="#remotesensing-12-00468-t003" class="html-table">Table 3</a>.</p>
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<p>The brightness temperature difference <math display="inline"><semantics> <mrow> <msubsup> <mi>T</mi> <mi>A</mi> <mtext> </mtext> </msubsup> </mrow> </semantics></math> − <math display="inline"><semantics> <mrow> <msubsup> <mi>T</mi> <mi>B</mi> <mtext> </mtext> </msubsup> </mrow> </semantics></math> at various tangent height measured by the 118 GHz radiometer: (<b>a</b>) 10 km; (<b>b</b>) 20 km; (<b>c</b>) 30 km; (<b>d</b>) 50 km; (<b>e</b>) 70 km; (<b>f</b>) 90 km.</p>
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<p>The temperature retrieval errors induced by different calibration error sources: (<b>a</b>) absolute and (<b>b</b>) relative retrieval errors. The uncertainties assumed are summarized in <a href="#remotesensing-12-00468-t004" class="html-table">Table 4</a>.</p>
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<p>The temperature retrieval errors induced by external error sources: (<b>a</b>) absolute and (<b>b</b>) relative retrieval errors. The uncertainties assumed are summarized in <a href="#remotesensing-12-00468-t005" class="html-table">Table 5</a>.</p>
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<p>The H<sub>2</sub>O retrieval errors induced by different instrument uncertainty sources: (<b>a</b>) absolute and (<b>b</b>) relative retrieval errors. The uncertainties assumed are summarized in <a href="#remotesensing-12-00468-t003" class="html-table">Table 3</a>.</p>
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<p>The brightness temperature difference <math display="inline"><semantics> <mrow> <msubsup> <mi>T</mi> <mi>A</mi> <mtext> </mtext> </msubsup> </mrow> </semantics></math> − <math display="inline"><semantics> <mrow> <msubsup> <mi>T</mi> <mi>B</mi> <mtext> </mtext> </msubsup> </mrow> </semantics></math> at various tangent height measured by 190 GHz radiometer (183 GHz spectrometer): (<b>a</b>) 10 km; (<b>b</b>) 20 km; (<b>c</b>) 30 km; (<b>d</b>) 50 km; (<b>e</b>) 70 km; (<b>f</b>) 90 km.</p>
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<p>The H<sub>2</sub>O retrieval errors induced by different calibration error sources: (<b>a</b>) absolute and (<b>b</b>) relative retrieval errors. The uncertainties assumed are summarized in <a href="#remotesensing-12-00468-t004" class="html-table">Table 4</a>.</p>
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<p>The H<sub>2</sub>O retrieval error induced by external error source: (<b>a</b>) absolute and (<b>b</b>) relative retrieval errors. The uncertainties assumed are summarized in <a href="#remotesensing-12-00468-t005" class="html-table">Table 5</a>.</p>
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<p>The O<sub>3</sub> retrieval errors induced by different instrument uncertainty sources: (<b>a</b>) absolute and (<b>b</b>) relative retrieval errors. The uncertainties assumed are summarized in <a href="#remotesensing-12-00468-t003" class="html-table">Table 3</a>.</p>
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<p>The brightness temperature difference <span class="html-italic">T<sub>A</sub></span> − <span class="html-italic">T<sub>B</sub></span> at various tangent height measured by 240 GHz radiometer (235 GHz spectrometer): (<b>a</b>) 10 km; (<b>b</b>) 20 km; (<b>c</b>) 30 km; (<b>d</b>) 50 km; (<b>e</b>) 70 km; (<b>f</b>) 90 km.</p>
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<p>The O<sub>3</sub> retrieval errors induced by different calibration error sources: (<b>a</b>) absolute and (<b>b</b>) relative retrieval errors. The uncertainties assumed are summarized in <a href="#remotesensing-12-00468-t004" class="html-table">Table 4</a>.</p>
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<p>The O<sub>3</sub> retrieval error induced by external error source: (<b>a</b>) absolute and (<b>b</b>) relative retrieval errors. The uncertainties assumed are summarized in <a href="#remotesensing-12-00468-t005" class="html-table">Table 5</a>.</p>
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<p>The HCl retrieval errors induced by different instrument uncertainty sources: (<b>a</b>) absolute and (<b>b</b>) relative retrieval errors. The uncertainties assumed are summarized in <a href="#remotesensing-12-00468-t003" class="html-table">Table 3</a>.</p>
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<p>The brightness temperature difference −<math display="inline"><semantics> <mrow> <msubsup> <mi>T</mi> <mi>B</mi> <mtext> </mtext> </msubsup> </mrow> </semantics></math> at various tangent height measured by 643 GHz radiometer (625 GHz spectrometer): (<b>a</b>) 10 km; (<b>b</b>) 20 km; (<b>c</b>) 30 km; (<b>d</b>) 50 km; (<b>e</b>) 70 km; (<b>f</b>) 90 km.</p>
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<p>The HCl retrieval errors induced by different calibration error sources: (<b>a</b>) absolute and (<b>b</b>) relative retrieval errors. The uncertainties assumed are summarized in <a href="#remotesensing-12-00468-t004" class="html-table">Table 4</a>.</p>
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<p>The HCl retrieval error induced by external error source: (<b>a</b>) absolute and (<b>b</b>) relative retrieval errors. The uncertainties assumed are summarized in <a href="#remotesensing-12-00468-t005" class="html-table">Table 5</a>.</p>
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<p>The overall retrieval errors estimation: (<b>a</b>) 118 GHz temperature retrieval; (<b>b</b>) 190 GHz H<sub>2</sub>O retrieval; (<b>c</b>) 240 GHz O<sub>3</sub> retrieval; (<b>d</b>) 643 GHz HCl retrieval. The errors are calculated by using the sum of squared errors.</p>
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18 pages, 4546 KiB  
Article
Intercomparison of Integrated Water Vapor Measurements at High Latitudes from Co-Located and Near-Located Instruments
by Ermanno Fionda, Maria Cadeddu, Vinia Mattioli and Rosa Pacione
Remote Sens. 2019, 11(18), 2130; https://doi.org/10.3390/rs11182130 - 13 Sep 2019
Cited by 7 | Viewed by 2827
Abstract
Data from global positioning system (GPS) ground-based receivers, ground-based microwave radiometers (MWRs), and radiosondes (RS) at two high-latitude sites were compared. At one site, the North Slope of Alaska (NSA), Barrow, Alaska (USA), the instruments were co-located, while at the other site, the [...] Read more.
Data from global positioning system (GPS) ground-based receivers, ground-based microwave radiometers (MWRs), and radiosondes (RS) at two high-latitude sites were compared. At one site, the North Slope of Alaska (NSA), Barrow, Alaska (USA), the instruments were co-located, while at the other site, the second ARM Mobile Facility (AMF2), Hyytiälä, Finland, the GPS receiver was located about 20 km away from the MWRs and RS. Differences between the GPS-derived integrated water vapor (IWV) and the other three instruments were analyzed in terms of mean differences and standard deviation. A comparison of co-located and near-located independently calibrated instruments allowed us to isolate issues that may be specific to a single system and, to some extent, to isolate the effects of the distance between the GPS receiver and the remaining instruments. The results showed that at these two high-latitude sites, when the IWV was less than 15 kg/m2, the GPS agreed with other instruments within 0.5–0.7 kg/m2. When the variability of water vapor was higher, mostly in the summer months, the GPS agreed with other instruments within 0.8–1 kg/m2. The total random uncertainty between the GPS and the other systems was of the order of 0.6–1 kg/m2 and was the dominant effect when the IWV was higher than 15 kg/m2. Full article
(This article belongs to the Special Issue Remote Sensing of Atmospheric Components and Water Vapor)
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Figure 1

Figure 1
<p>(<b>a</b>) From left to right, 2C and 3C radiometers at the AMF2 site (Hyytiälä, Finland). The enclosure near the three-channel radiometer (3C) contains the control computer, meteorological sensors, and infrared thermometer. (<b>b</b>) A view of the north slope of Alaska (NSA) facilities in Barrow, Alaska (USA): in the foreground the G-Band Vapor Radiometer Profiler (GVRP), in the background the 2C radiometer.</p>
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<p>Latitude and longitude of the NSA (<b>a</b>) and AMF2 (<b>b</b>) sites (black star), the GPS (black square), and the RS at an 8-km height. The shaded brown area represents the approximate FOV of the GPS for a cut-off angle of 3°. The star and square overlap at the NSA.</p>
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<p>(<b>a)</b> Scatterplot of the IWV from the GPS (<span class="html-italic">x</span> axis) and from all operated radiometers (<span class="html-italic">y</span> axis) at the NSA (blue) and AMF2 (orange). The dashed black line represents a 1:1 ratio. (<b>b</b>) The number of occurrences of absolute differences between the microwave radiometers (MWRs) and the GPS. The red solid line represents the normal distribution fit. The normal distribution had a mean of 0.191 kg/m<sup>2</sup> [0.181, 0.200] with an SD of 0.756 kg/m<sup>2</sup> [0.750, 0.763]. The intervals next to the parameter estimates are the 95% confidence intervals for the distribution parameters.</p>
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<p>(<b>a</b>): Monthly mean of differences; (<b>b</b>) monthly mean of the standard deviation of the differences.</p>
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<p>Density plots of differences between: (<b>a</b>) 3C and GPS at AMF2; (<b>b</b>) 2C and GPS at AMF2; (<b>c</b>) 3C and GPS at AMF2; (<b>d</b>) GVRP and GPS at NSA; (<b>e</b>) 2C and GPS at NSA; (<b>f</b>) GVRP and 2C at NSA. All difference binned by IWV bins of 5 kg/m<sup>2</sup>.</p>
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<p>Left three panels: GPS and radiometers comparison. (<b>a</b>) Standard deviation of differences as a function of IWV; (<b>b</b>) percent of cloudy cases; (<b>c</b>) number of cases in each bin. Right panels: RS, GPS, and radiometers comparison. (<b>d</b>) Standard deviation of differences as a function of IWV; (<b>e</b>) number of cases in each bin. In all panels, IWV bins are 5 kg/m<sup>2</sup>, brown symbols refer to the NSA, and black symbols refer to the AMF2.</p>
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<p>Differences between original and corrected IWV (kg/m<sup>2</sup>) at the AMF2 (all data).</p>
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<p>Distribution of daytime (11:00–17:00 UTC) GPS–RS mean differences before (gray) and after (red) the dry bias correction at the AMF2 (data are for May–September 2014).</p>
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<p>Density plots of differences between: (<b>a</b>) GPS and RS at AMF2; (<b>b</b>) 2C and RS at AMF2; (<b>c</b>) 3C and RS at AMF2; (<b>d</b>) GPS and RS at NSA; (<b>e</b>) 2C and RS at NSA; (<b>f</b>) GVRP and RS at NSA. All difference binned by IWV bins of 5 kg/m<sup>2</sup>.</p>
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14 pages, 794 KiB  
Article
Water Vapor Calibration: Using a Raman Lidar and Radiosoundings to Obtain Highly Resolved Water Vapor Profiles
by Birte Solveig Kulla and Christoph Ritter
Remote Sens. 2019, 11(6), 616; https://doi.org/10.3390/rs11060616 - 13 Mar 2019
Cited by 9 | Viewed by 4705
Abstract
We revised the calibration of a water vapor Raman lidar by co-located radiosoundings for a site in the high European Arctic. For this purpose, we defined robust criteria for a valid calibration. One of these criteria is the logarithm of the water vapor [...] Read more.
We revised the calibration of a water vapor Raman lidar by co-located radiosoundings for a site in the high European Arctic. For this purpose, we defined robust criteria for a valid calibration. One of these criteria is the logarithm of the water vapor mixing ratio between the sonde and the lidar. With an error analysis, we showed that for our site correlations smaller than 0.95 could be explained neither by noise in the lidar nor by wrong assumptions concerning the aerosol or Rayleigh extinction. However, highly variable correlation coefficients between sonde and consecutive lidar profiles were found, suggesting that small scale variability of the humidity was our largest source of error. Therefore, not all co-located radiosoundings are useful for lidar calibration. As we assumed these changes to be non-systematic, averaging over several independent measurements increased the calibration’s quality. The calibration of the water vapor measurements from the lidar for individual profiles varied by less than ±5%. The seasonal median, used for calibration in this study, was stable and reliable (confidence ±1% for the season with most calibration profiles). Thus, the water vapor mixing ratio profiles from the Koldewey Aerosol Raman Lidar (KARL) are very accurate. They show high temporal variability up to 4 km altitude and, therefore, provide additional, independent information to the radiosonde. Full article
(This article belongs to the Special Issue Remote Sensing of Atmospheric Components and Water Vapor)
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Graphical abstract

Graphical abstract
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<p>Exemplary lidar profile used for calibration (20 February 2018). Bins used for calibration (<math display="inline"><semantics> <msub> <mi>z</mi> <mi>i</mi> </msub> </semantics></math>) are highlighted with green points. Conditions under which heights are excluded from calibration as in <a href="#remotesensing-11-00616-t001" class="html-table">Table 1</a> due to deficiencies in lidar (green) or radiosonde data (blue) are marked.</p>
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<p>Pearson correlation coefficient between log<math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <msub> <mi>w</mi> <mrow> <mi>R</mi> <mi>S</mi> </mrow> </msub> <mo stretchy="false">)</mo> </mrow> </semantics></math> and log<math display="inline"><semantics> <mrow> <mo stretchy="false">(</mo> <msub> <mi>S</mi> <mi>lidar</mi> </msub> <mo stretchy="false">)</mo> </mrow> </semantics></math> at heights where data would fulfill all other criteria to be selected for calibration (<math display="inline"><semantics> <msub> <mi>z</mi> <mi>i</mi> </msub> </semantics></math>) during the nights from 3 March 2018 to 4 March 2018, 6 March 2018 to 7 March 2018 and 11 March 2018 to 12 March 2018. Colors indicate the temporal difference between the start of the radiosonde and the lidar measurement. Red line shows the threshold for minimal correlation applied here. Start of radiosounding measurement indicated by black, dashed line.</p>
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<p>Calibration factor for winter 2017/2018. Light green I: median of all <math display="inline"><semantics> <msub> <mi>C</mi> <mi>i</mi> </msub> </semantics></math>; dark green I: median of <math display="inline"><semantics> <msub> <mi>C</mi> <mi>i</mi> </msub> </semantics></math>, when using only one profile at a time; grey: seasonal median of <math display="inline"><semantics> <msub> <mi>C</mi> <mi>i</mi> </msub> </semantics></math> ±3%; black: seasonal median of <math display="inline"><semantics> <msub> <mi>C</mi> <mi>i</mi> </msub> </semantics></math> ±5%.</p>
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<p>Probability density function of <math display="inline"><semantics> <msub> <mi>C</mi> <mi>i</mi> </msub> </semantics></math> for different years and different radiosonde products as reference datasets. Respective median <span class="html-italic">C</span> indicated by an I.</p>
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<p>(<b>a</b>) Exemplary lidar profile used for calibration (20 February 2018); (<b>b</b>) ratio between the calibrated lidar signal and radiosounding measurement, with (green) and without (orange) overlap correction for all profiles with parallel measurements in 2018; and (<b>c</b>) probability density function (PDF) of ratio between radiosounding and the uncorrected (orange) and corrected (green) lidar signal in the lowermost 400 m. The ratio between the signals in the altitudes chosen for calibration is shown as a reference (dark green).</p>
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<p>(<b>a</b>) PDF of Pearson correlation coefficient how different realizations of noise in the lidar degrade a perfect r = 1 correlation; (<b>b</b>) PDF of the error due to different Rayleigh atmospheres; (<b>c</b>) median (dotted) and 95% percentile (dashed) of the error due to aerosol extinction as a function of altitude; (<b>d</b>) PDF of the aerosol induced error from AOD and Ångström exponent; (<b>e</b>) PDF of Pearson correlation coefficient of the combined error due to noise and aerosol; and (<b>f</b>) accuracy for the determination of the lidar calibration constant.</p>
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<p>Water vapor mixing ratio dynamics over Ny-Ålesund during the nights from 3 March 2018 to 4 March 2018, 6 March 2018 to 7 March 2018 and 11 March 2018 to 12 March 2018. Times of radiosounding measurements indicated by black, dashed line.</p>
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25 pages, 3867 KiB  
Article
Evaluation of Bias Correction Methods for GOSAT SWIR XH2O Using TCCON data
by Tran Thi Ngoc Trieu, Isamu Morino, Hirofumi Ohyama, Osamu Uchino, Ralf Sussmann, Thorsten Warneke, Christof Petri, Rigel Kivi, Frank Hase, David F. Pollard, Nicholas M. Deutscher, Voltaire A. Velazco, Laura T. Iraci, James R. Podolske and Manvendra K. Dubey
Remote Sens. 2019, 11(3), 290; https://doi.org/10.3390/rs11030290 - 1 Feb 2019
Cited by 2 | Viewed by 4877
Abstract
This study evaluated three bias correction methods of systematic biases in column-averaged dry-air mole fraction of water vapor (XH2O) data retrieved from Greenhouse Gases Observing Satellite (GOSAT) Short-Wavelength Infrared (SWIR) observations compared with ground-based data from the Total Carbon Column Observing [...] Read more.
This study evaluated three bias correction methods of systematic biases in column-averaged dry-air mole fraction of water vapor (XH2O) data retrieved from Greenhouse Gases Observing Satellite (GOSAT) Short-Wavelength Infrared (SWIR) observations compared with ground-based data from the Total Carbon Column Observing Network (TCCON). They included an empirically multilinear regression method, altitude bias correction method, and combination of altitude and empirical correction for three cases defined by the temporal and spatial collocation around TCCON site. The results showed that large altitude differences between GOSAT observation points and TCCON instruments are the main cause of bias, and the altitude bias correction method is the most effective bias correction method. The lowest biases result from GOSAT SWIR XH2O data within a 0.5° × 0.5° latitude × longitude box centered at each TCCON site matched with TCCON XH2O data averaged over ±15 min of the GOSAT overpass time. Considering land data, the global bias changed from −1.3 ± 9.3% to −2.2 ± 8.5%, and station bias from −2.3 ± 9.0% to −1.7 ± 8.4%. In mixed land and ocean data, global bias and station bias changed from −0.3 ± 7.6% and −1.9 ± 7.1% to −0.8 ± 7.2% and −2.3 ± 6.8%, respectively, after bias correction. The results also confirmed that the fine spatial and temporal collocation criteria are necessary in bias correction methods. Full article
(This article belongs to the Special Issue Remote Sensing of Atmospheric Components and Water Vapor)
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Graphical abstract
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<p>Global map of the ground-based Total Carbon Column Observing Network (TCCON) sites used for correction and validation of Greenhouse Gases Observing Satellite (GOSAT) data.</p>
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<p>Scatter plots between original GOSAT SWIR XH<sub>2</sub>O data and TCCON XH<sub>2</sub>O data for case 1 (GOSAT data retrieved within ±1° latitude/longitude boxes centered at each TCCON site and the mean of TCCON XH<sub>2</sub>O values within ±30 min of the GOSAT overpass time) at the 18 TCCON sites from April 2009 to December 2017. GOSAT land data (gain H) are shown by red circles and GOSAT mixed data (gain H) are shown by black circles. The regression lines fitted to the data are dotted and the solid lines show one-to-one correspondence.</p>
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<p>Scatter plots between original GOSAT SWIR XH<sub>2</sub>O data and TCCON XH<sub>2</sub>O data for case 1 (GOSAT data retrieved within ±1° latitude/longitude boxes centered at each TCCON site and the mean of TCCON XH<sub>2</sub>O values within ±30 min of the GOSAT overpass time) at the 18 TCCON sites from April 2009 to December 2017. GOSAT land data (gain H) are shown by red circles and GOSAT mixed data (gain H) are shown by black circles. The regression lines fitted to the data are dotted and the solid lines show one-to-one correspondence.</p>
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<p>Scatter plots between ΔXH<sub>2</sub>O calculated from original GOSAT SWIR XH<sub>2</sub>O data (left panels) or from GOSAT SWIR XH<sub>2</sub>O data corrected by bias-correction method (E) (right panels) and auxiliary parameters (<b>a</b>) AOD<sub>1.6</sub>, (<b>b</b>) surface pressure, (<b>c</b>) temperature shift, (<b>d</b>) air mass, (<b>e</b>) altitude, (<b>f</b>) Alb<sub>1</sub>, and (<b>g</b>) Alb<sub>2</sub> for case 1. Red symbols indicate GOSAT gain H land data, and black symbols indicate GOSAT gain H mixed for case 1. Red symbols indicate GOSAT gain H land data and black symbols indicate GOSAT gain H mixed data. The dotted lines are the fitted regression lines. ΔXH<sub>2</sub>O = GOSAT XH<sub>2</sub>O − TCCON XH<sub>2</sub>O.</p>
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<p>Scatter plots between ΔXH<sub>2</sub>O calculated from original GOSAT SWIR XH<sub>2</sub>O data (left panels) or from GOSAT SWIR XH<sub>2</sub>O data corrected by bias-correction method (E) (right panels) and auxiliary parameters (<b>a</b>) AOD<sub>1.6</sub>, (<b>b</b>) surface pressure, (<b>c</b>) temperature shift, (<b>d</b>) air mass, (<b>e</b>) altitude, (<b>f</b>) Alb<sub>1</sub>, and (<b>g</b>) Alb<sub>2</sub> for case 0. Red symbols indicate GOSAT gain H land data, and black symbols indicate GOSAT gain H mixed for case 0. Red symbols indicate GOSAT gain H land data and black symbols indicate GOSAT gain H mixed data. The dotted lines are the fitted regression lines. ΔXH<sub>2</sub>O = GOSAT XH<sub>2</sub>O − TCCON XH<sub>2</sub>O.</p>
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<p>Correlations between GOSAT SWIR XH<sub>2</sub>O and TCCON XH<sub>2</sub>O for case 2 (<b>a</b>–<b>d</b>), case 1 (<b>a</b>–<b>d</b>), and case 0 (<b>a</b>–<b>d</b>). (<b>a</b>) Original GOSAT SWIR XH<sub>2</sub>O and TCCON XH<sub>2</sub>O, (<b>b</b>) GOSAT SWIR XH<sub>2</sub>O corrected by bias correction method (E) and TCCON XH<sub>2</sub>O, (<b>c</b>) GOSAT SWIR XH<sub>2</sub>O corrected by bias correction method (A) and TCCON XH<sub>2</sub>O, and (<b>d</b>) GOSAT SWIR XH<sub>2</sub>O corrected by bias correction method (A + E) and TCCON XH<sub>2</sub>O. Red symbols indicate GOSAT gain H land data and black symbols indicate GOSAT gain H mixed data. The dotted lines are the fitted regression lines and the solid lines show one-to-one correspondence.</p>
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<p>Correlations between GOSAT SWIR XH<sub>2</sub>O and TCCON XH<sub>2</sub>O for case 2 (<b>a</b>–<b>d</b>), case 1 (<b>a</b>–<b>d</b>), and case 0 (<b>a</b>–<b>d</b>). (<b>a</b>) Original GOSAT SWIR XH<sub>2</sub>O and TCCON XH<sub>2</sub>O, (<b>b</b>) GOSAT SWIR XH<sub>2</sub>O corrected by bias correction method (E) and TCCON XH<sub>2</sub>O, (<b>c</b>) GOSAT SWIR XH<sub>2</sub>O corrected by bias correction method (A) and TCCON XH<sub>2</sub>O, and (<b>d</b>) GOSAT SWIR XH<sub>2</sub>O corrected by bias correction method (A + E) and TCCON XH<sub>2</sub>O. Red symbols indicate GOSAT gain H land data and black symbols indicate GOSAT gain H mixed data. The dotted lines are the fitted regression lines and the solid lines show one-to-one correspondence.</p>
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19 pages, 7435 KiB  
Article
A Retrieval of Glyoxal from OMI over China: Investigation of the Effects of Tropospheric NO2
by Yapeng Wang, Jinhua Tao, Liangxiao Cheng, Chao Yu, Zifeng Wang and Liangfu Chen
Remote Sens. 2019, 11(2), 137; https://doi.org/10.3390/rs11020137 - 11 Jan 2019
Cited by 7 | Viewed by 3523
Abstract
East China is the ‘hotspot’ of glyoxal (CHOCHO), especially over the Pearl River Delta (PRD) region, where glyoxal is yielded from the oxidation of aromatics. To better understand the glyoxal spatial-temporal characteristics over China and evaluate the effectiveness of atmospheric prevention efforts on [...] Read more.
East China is the ‘hotspot’ of glyoxal (CHOCHO), especially over the Pearl River Delta (PRD) region, where glyoxal is yielded from the oxidation of aromatics. To better understand the glyoxal spatial-temporal characteristics over China and evaluate the effectiveness of atmospheric prevention efforts on the reduction of volatile organic compound (VOC) emissions, we present an algorithm for glyoxal retrieval using the Ozone Monitoring instrument (OMI) over China. The algorithm is based on the differential optical absorption spectroscopy (DOAS) and accounts for the interference of the tropospheric nitrogen dioxide (NO2) spatial-temporal distribution on glyoxal retrieval. We conduct a sensitively test based on a synthetic spectrum to optimize the fitting parameters set. It shows that the fitting interval of 430–458 nm and a 4th order polynomial are optimal for glyoxal retrieval when using the daily mean value of the earthshine spectrum in the Pacific region as a reference. In addition, tropospheric NO2 pre-fitted during glyoxal retrieval is first proposed and tested, which shows a ±10% variation compared with the reference scene. The interference of NO2 on glyoxal was further investigated based on the OMI observations, and the spatial distribution showed that changes in the NO2 concentration can affect the glyoxal result depending on the NO2 spatial distribution. A method to prefix NO2 during glyoxal retrieval is proposed in this study and is referred to as OMI-CAS. We perform an intercomparison of the glyoxal from the OMI-CAS with the seasonal datasets provided by different institutions for North China (NC), South China (SC), the Yangtze River Delta (YRD) and the ChuanYu (CY) region in southwestern China in the year 2005. The results show that our algorithm can obtain the glyoxal spatial and temporal variations in different regions over China. OMI-CAS has the best correlations with other datasets in summer, with the correlations between OMI-CAS and OMI-Harvard, OMI-CAS and OMI-IUP, and OMI-CAS and Sciamachy-IUP being 0.63, 0.67 and 0.67, respectively. Autumn results followed, with the correlations of 0.58, 0.36 and 0.48, respectively, over China. However, the correlations are less or even negative for spring and winter. From the regional perspective, SC has the best correlation compared with other regions, with R reaching 0.80 for OMI-CAS and OMI-IUP in summer. The discrepancies between different glyoxal datasets can be attributed to the fitting parameters and larger glyoxal retrieval uncertainties. Finally, useful recommendations are given based on the results comparison according to region and season. Full article
(This article belongs to the Special Issue Remote Sensing of Atmospheric Components and Water Vapor)
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Figure 1

Figure 1
<p>The study region.</p>
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<p>Absorption intensity of atmospheric components between 300 nm and 500 nm. The slant columns were taken as 10<sup>14</sup> molec/cm<sup>2</sup> for BrO, 2 × 10<sup>16</sup> molec/cm<sup>2</sup> for HCHO, 2 × 10<sup>16</sup> molec/cm<sup>2</sup> for NO<sub>2</sub>, 2 × 10<sup>43</sup> molec<sup>2</sup>/cm<sup>5</sup> for O<sub>4</sub> and 2 × 10<sup>15</sup> molec/cm<sup>2</sup> for CHOCHO.</p>
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<p>The logarithm of the ratio of the synthetic spectrum to the solar reference spectrum.</p>
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<p>(<b>a</b>–<b>c</b>) Color mapping of CHOCHO SCD retrieved from a synthetic spectrum for wavelength intervals with starting limits of 420–436 nm, ending limits of 444–460 nm, and polynomial orders of 3, 4 and 5; (<b>d</b>) same as <b>a</b>–<b>c</b>, but without NO<sub>2</sub> cross-section in the retrieval; and (<b>e</b>,<b>f</b>) the relative difference between the CHOCHO SCD retrieved from a synthetic spectrum and the SCD in (<b>b</b>).</p>
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<p>The selected fitting interval.</p>
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<p>The differential ACS of NO<sub>2</sub> and CHOCHO with respect to the differential spectra (DF). (<b>Left</b>) CHOCHO and differential spectrum; (<b>right</b>) NO<sub>2</sub> and differential spectrum.</p>
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<p>(<b>a</b>) The relative change in the CHOCHO SCD caused by a 50% decrease in NO<sub>2</sub> values. (<b>b</b>) The relative change in the CHOCHO SCD caused by a 100% increase in NO<sub>2</sub> values.</p>
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<p>(<b>a</b>) The results of OMI-CAS. (<b>b</b>) The results from OMI-Harvard. (<b>c</b>) A scatterplot of OMI-CAS and OMI-Harvard as a function of latitude.</p>
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<p>The fitted spectrum compared with the differential spectrum (DF): (<b>a</b>) with SCD<sub>glyoxal</sub> = 3.73 × 10<sup>15</sup> molec/cm<sup>2</sup>; (<b>b</b>) with SCD<sub>glyoxal</sub> = 2.74 × 10<sup>15</sup> molec/cm<sup>2</sup>.</p>
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<p>The seasonal distribution of glyoxal in China in 2005. From left to right: OMI-CAS, OMI-Harvard, OMI-IUP, and Sciamachy-IUP; From top to bottom: spring (MAM), summer (JJA), autumn (SON) and winter (DJF).</p>
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<p>Glyoxal monthly mean variations in the selected regions.</p>
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<p>Seasonal variations of glyoxal based on the four datasets.</p>
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<p>OMI-CAS glyoxal correlation with different datasets over China (<b>Left</b>: OMI-CAS and OMI-Harvard; <b>Middle</b>: OMI-CAS and OMI-IUP; <b>Right</b>: OMI-CAS and Sciamachy-IUP; Resolution = 2.5° × 2.5°; Top to bottom: spring (MAM), summer (JJA), autumn (SON), winter (DJF)).</p>
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12 pages, 462 KiB  
Letter
Evaluation of Water Vapor Radiative Effects Using GPS Data Series over Southwestern Europe
by Javier Vaquero-Martínez, Manuel Antón, Arturo Sanchez-Lorenzo and Victoria E. Cachorro
Remote Sens. 2020, 12(8), 1307; https://doi.org/10.3390/rs12081307 - 21 Apr 2020
Cited by 9 | Viewed by 2520
Abstract
Water vapor radiative effects (WVRE) at surface in the long-wave (LW) and short-wave (SW) spectral ranges under cloud and aerosol free conditions are analyzed for seven stations in Spain over the 2007–2015 period. WVRE is calculated as the difference between the net flux [...] Read more.
Water vapor radiative effects (WVRE) at surface in the long-wave (LW) and short-wave (SW) spectral ranges under cloud and aerosol free conditions are analyzed for seven stations in Spain over the 2007–2015 period. WVRE is calculated as the difference between the net flux obtained by two radiative transfer simulations; one with water vapor from Global Positioning System (GPS) measurements and the other one without any water vapor (dry atmosphere). The WVRE in the LW ranges from 107.9 Wm 2 to 296.7 Wm 2 , while in the SW it goes from 64.9 Wm 2 to 6.0 Wm 2 . The results show a clear seasonal cycle, which allows the classification of stations in three sub-regions. In general, for total (SW + LW) and LW WVRE, winter (DJF) and spring (MAM) values are lower than summer (JJA) and autumn (SON). However, in the case of SW WVRE, the weaker values are in winter and autumn, and the stronger ones in summer and spring. Positive trends for LW (and total) WVRE may partially explain the well-known increase of surface air temperatures in the study region. Additionally, negative trends for SW WVRE are especially remarkable, since they represent about a quarter of the contribution of aerosols to the strong brightening effect (increase of the SW radiation flux at surface associated with a reduction of the cloud cover and aerosol load) observed since the 2000s in the Iberian Peninsula, but with opposite sign, so it is suggested that water vapor could be partially masking the full magnitude of this brightening. Full article
(This article belongs to the Special Issue Remote Sensing of Atmospheric Components and Water Vapor)
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Graphical abstract

Graphical abstract
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<p>Map of the Global Positioning System (GPS) stations included in this work. Zones are: North atlantic (NA), Mediterranean Sea (MS) and interior (I).</p>
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<p>Water vapor radiative effects (WVRE) seasonal evolution in the regions considered in this study, in the form of a box-plot.</p>
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<p>Time-series of station-averaged integrated water vapor (IWV) and WVRE (SW, LW and total regimes) anomalies. Values are in cm for IWV and in <math display="inline"><semantics> <msup> <mi>Wm</mi> <mrow> <mo>−</mo> <mn>2</mn> </mrow> </msup> </semantics></math> for WVRE. Blue solid lines point out the linear trends (see text).</p>
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9 pages, 1107 KiB  
Letter
Worldwide Evaluation of Ozone Radiative Forcing in the UV-B Range between 1979 and 2014
by David Mateos and Manuel Antón
Remote Sens. 2020, 12(3), 436; https://doi.org/10.3390/rs12030436 - 29 Jan 2020
Cited by 4 | Viewed by 2388
Abstract
Ultraviolet (UV) radiation plays a key role in different planetary mechanisms, thus necessitating a worldwide analysis of this solar spectrum interval. This study offers a worldwide and long-term analysis of ozone radiative forcing (ORF) in the UV-B range between 1979 and 2014. The [...] Read more.
Ultraviolet (UV) radiation plays a key role in different planetary mechanisms, thus necessitating a worldwide analysis of this solar spectrum interval. This study offers a worldwide and long-term analysis of ozone radiative forcing (ORF) in the UV-B range between 1979 and 2014. The method uses monthly total ozone column (TOC) values obtained from the ERA-Interim reanalysis data collection and radiative transfer simulations. A global mean ORF of 0.011 Wm−2 is obtained, with marked differences between mid-latitude and tropical areas. The mid-latitude belts in the Northern and Southern Hemispheres exhibit the following statistically significant ORF trends between 1982 and 2014 with respect to pre-1980 values: 0.007 Wm−2 per decade in the 60–45°S belt and around 0.004 Wm−2 per decade in the 45–30°S and 45–60°N belts. The increase observed in the net UV-B radiation levels at the troposphere might have relevant photochemical effects that impact climate change. Full article
(This article belongs to the Special Issue Remote Sensing of Atmospheric Components and Water Vapor)
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Graphical abstract
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<p>Ozone radiative forcing (ORF; in W m<sup>−2</sup>) for three different periods: (<b>a</b>) ORF<sub>2-1</sub> between 1979–1981 and 1994–1996, (<b>b</b>) ORF<sub>3-2</sub> between 1994–1996 and 2012–2014, and (<b>c</b>) ORF<sub>3-1</sub> between 1979–1981 and 2012–2014. See Equations (1)–(3).</p>
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<p>Evolution of yearly ORF in the UV-B range at four latitudinal bands.</p>
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