Redha Belhadji’s research while affiliated with Université Paris Cité and other places

What is this page?


This page lists works of an author who doesn't have a ResearchGate profile or hasn't added the works to their profile yet. It is automatically generated from public (personal) data to further our legitimate goal of comprehensive and accurate scientific recordkeeping. If you are this author and want this page removed, please let us know.

Publications (12)


Figure 1: Horizontal evolution of the vortex shown with relative vorticity (a) and ozone mixing ratio (b), data from ECMWF-IFS reanalyses. The background shows the relative vorticity and ozone mixing ratio on 07 January 2020 18UTC, at 75.2 hPa (~18 km altitude, thus at the vertical location of the vortex) corresponding to the level of highest vorticity and lowest concentration of ozone in the vortex. The boxes show the vorticity field and the ozone anomaly at other indicated times as horizontal sections at the vertical level of the vortex centroid projected onto the background field. The green curve is the daily-sampled trajectory of the vortex 155
Figure 2: OMPS-LP ozone anomalies for selected days following the Australian fires, with a latitude/altitude plot (left column). OMPS-LP ozone observation concentration at the core vortex altitude from ECMWF IFS (right column). The circle represents the 180
Figure 3: TROPOMI total ozone column observations, for four selected days in January 2020 (see labels over the individual panels). The inner and outer circles show the averaged regions for the total ozone columns in the case of the in-vortex ozone minihole and the background, respectively. The red and black stars show the center of the vortex according to the ECMWF-IFS 195
Figure 4: IASI partial stratospheric ozone column, defined using the vortex altitude derived with ECMWF-IFS reanalyses, for four selected days in January 2020 (see labels over the individual panels). The depth of the partial stratospheric ozone column is 6 km, located at 14.3-20.3 km, 16.6-22.6 km, 16.8-22.8 km and 17.6-23.6 km, for the different days in the panels. The inner and outer circles show the averaged regions for the total ozone columns in the case of the in-vortex ozone mini-hole and the background, respectively. The red and black stars show the center of the vortex according to the ECMWF-IFS reanalyses at 6UTC and 18UTC, 220
Figure 5: IASI partial stratospheric ozone column anomaly, based on the temporal background approach, defined using the vortex altitude derived with ECMWF-IFS reanalyses, for four selected days in January 2020 (see labels over the individual panels). The depth of the partial stratospheric ozone column is 6 km, located at 14.3-20.3 km, 16.6-22.6 km, 16.8-22.8 km and 17.6-23.6 km, for the different days in the panels. The anomaly in 2020 is estimated with respect to 2010-2019 averages. The red circles show the 235

+4

Early evolution of the ozone mini-hole generated by the Australian bushfires 2019–2020 observed from satellite and ground-based instruments
  • Preprint
  • File available

April 2025

·

18 Reads

Redha Belhadji

·

·

·

[...]

·

The intense wildfires in Australia, during the 2019–2020 fire season, generated massive Pyro-cumulonimbus (pyro-Cb) clouds, and injected an unprecedented amount of smoke aerosols into the upper troposphere–lower stratosphere (UTLS). The smoke aerosols produced a self-sustaining confined anticyclonic vortex, that ascended up to 35 km altitude by March 2020 by diabatic heating of radiation absorbing aerosols. This vortex transported ozone-poor tropospheric air into the ozone-rich stratosphere, thus forming a transient ozone mini-hole. This study investigates the early evolution of the dynamically-generated ozone mini-hole, using satellite and ground-based observations, supported by modelling information. Ozone anomalies within the vortex are tracked and quantified by satellite observation. In particular, ad-hoc in-vortex observations are derived by coupling the IASI (Infrared Atmospheric Sounding Interferometer) satellite observations and meteorological reanalysis information of the vortex. With these observations, a 30–40 % ozone depletion is observed in a 6-km partial stratospheric column, which exponentially decreased to ~7 % by the end of January with an e-folding time of about one week, as the vortex ascended in the stratosphere. A total ozone column depletion of ~7 %, immediately after the pyro-Cb injection, was observed with IASI and the TROPOMI (TROPOspheric Monitoring Instrument) satellite instrument. Consistently, ground-based measurement at Lauder, New Zealand showed a localised ozone depletion reaching ~10 % (total column) and ~20 % (in-vortex stratospheric partial column) associated with two vortex overpasses. These results provide insights into the impacts of extreme wildfires and pyro-Cbs on the dynamics and composition of the stratosphere.

Download

(a) Monthly mean SA OD (at 8.5 μm) anomaly from IASI observations in 2022, from 10°N to 70°S. (b) Zonal average SA OD anomaly from IASI observations in 2022, in the same latitude range as panel (a). The month/latitude position of the Hunga eruption is indicated as a black triangle.
Regional monthly mean IASI SA OD in 2022 (blue lines and crosses), and median values (black lines and crosses), 5–95 (dark gray shaded area), 10–90 (medium gray shaded area) and 30–70 (light gray shaded area) percentiles intervals for the period 2007–2018, in the five latitude regions: northern hemispheric high‐latitudes (60°N–90°N, panel (a)), northern hemispheric mid‐latitudes (30°N–60°N, panel (b)), tropics (30°N–30°S, panel (c)), southern hemispheric mid‐latitudes (30°S–60°S, panel (d)) and southern hemispheric high‐latitudes (60°S–90°S, panel (e)).
(a, b) Short term (January and February 2022) temporal evolution of SO2 (panel a) and SA (panel b) total anomaly masses due to the Hunga eruption, estimated using daily average IASI SO2 total column and SA OD observations. (c) Long term (year 2022) temporal evolution of SA total anomaly mass due to the Hunga eruption, estimated using monthly average IASI SA OD observations. In panels (a–c), fit of parameterization functions of the total masses evolution is also shown, see text for more details (sampled at the end of each month for Figure 3c). The total sulfur (S) mass is indicated for both SO2 and SA in panels a–c.
Observing the SO2 and Sulfate Aerosol Plumes From the 2022 Hunga Eruption With the Infrared Atmospheric Sounding Interferometer (IASI)

October 2024

·

62 Reads

·

2 Citations

Plain Language Summary The eruption of the submarine Hunga volcano in January 2022 polluted the global stratosphere with a large amount of water vapor and significantly perturbed the stratospheric aerosol layer. In this paper, we present a 1‐year long aftermath study of the stratospheric sulfur pollution from this volcanic eruption using observations from the Infrared Atmospheric Sounding Interferometer (IASI) satellite‐borne instrument. Gaseous and aerosol sulfur emissions are observed simultaneously using the specific potential of this sensor. These observations provide unique capabilities to characterize the aerosol type in the Hunga plume and the sulfur cycle associated with the volcanic emissions. An extremely rapid conversion of gaseous sulfur emissions to aerosols is observed, leading to larger than expected and persistent anomalies of the stratospheric aerosol layer (compared with a consistent long‐term climatology), still noticeable in the Southern Hemisphere after 1 year. The total mass of the emitted sulfur in gas and aerosol state is also simultaneously estimated, for the first time.


The optical properties of stratospheric aerosol layer perturbation of the Hunga volcano eruption of January 15th, 2022

July 2024

·

20 Reads

The Hunga volcano violently erupted on January 15th, 2022, and produced the largest stratospheric aerosol layer perturbation of the last 30 years. One notable effect of the Hunga eruption was the significant modification of the size distribution (SD) of the stratospheric aerosol layer with respect to background conditions and other recent moderate stratospheric eruptions, with larger mean particles size and smaller SD spread for Hunga. Starting from satellite-based SD retrievals, and the assumption of pure sulphate aerosol layers, in this work we calculate the optical properties of both background and Hunga-perturbed stratospheric aerosol scenarios using a Mie code. We found that the intensive optical properties of the stratospheric aerosol layer (i.e., single scattering albedo, asymmetry parameter, aerosol extinction per unit mass and the broad-band average Ångström exponent) were not significantly perturbed by the Hunga eruption, with respect to background conditions. The calculated Ångström exponent was found consistent with multi-instrument satellite observations of the same parameter. Thus, the basic impact of the Hunga eruption on the optical properties of the stratospheric aerosol layer was an increase of the stratospheric aerosol extinction (or optical depth), without any modification of the shortwave and longwave relative absorption, angular scattering and broad-band spectral trend of the extinction, with respect to background. This highlights a marked difference of the Hunga perturbation of the stratospheric aerosol layer and those from other larger stratospheric eruptions, like Pinatubo 1991 and El Chichon 1982. With simplified radiative forcing estimations, we show that the Hunga eruption produced an aerosol layer likely 3–10 times more effective in producing a net cooling of the climate system with respect to Pinatubo and El Chichon eruptions, due to more effective shortwave scattering. As intensive optical properties are seldom directly measured, e.g. from satellite, our calculations can support the estimation of radiative effects for the Hunga eruption with climate or offline radiative models.


Radiative impacts of the Australian bushfires 2019–2020 – Part 2: Large-scale and in-vortex radiative heating

December 2023

·

48 Reads

·

6 Citations

Record-breaking wildfires ravaged south-eastern Australia during the fire season 2019–2020. The intensity of the fires reached its paroxysmal phase at the turn of the year 2019–2020, when large pyro-cumulonimbi developed. Pyro-convective activity injected biomass burning aerosols and gases in the upper-troposphere–lower-stratosphere (UTLS), producing a long-lasting perturbation to the atmospheric composition and the stratospheric aerosol layer. The large absorptivity of the biomass burning plume produced self-lofting of the plume and thus modified its vertical dynamics and horizontal dispersion. Another effect of the in-plume absorption was the generation of compact smoke-charged anticyclonic vortices which ascended up to 35 km altitude due to diabatic heating. We use observational and modelling description of this event to isolate the main vortex from the dominant Southern Hemispheric biomass burning aerosol plume. Entering this information into an offline radiative transfer model, and with hypotheses on the absorptivity and the angular scattering properties of the aerosol layer, we estimate the radiative heating rates (HRs) in the plume and the vortex. We found that the hemispheric-scale plume produced a HR of 0.08±0.05 K d-1 (from 0.01 to 0.15 K d-1, depending on the assumption on the aerosol optical properties), as a monthly average value for February 2020, which is strongly dependent on the assumptions on the aerosol optical properties and therefore on the plume ageing. We also found in-vortex HRs as large as 15–20 K d-1 in the denser sections of the main vortex (8.4±6.1 K d-1 on average in the vortex). Our results suggest that radiatively heated ascending isolated vortices are likely dominated by small-sized strongly absorbing black carbon particles. The hemispheric-scale and in-vortex HR estimates are consistent with the observed ensemble self-lofting (a few kilometres in 4 months) and the main isolated vortex rise (∼ 20 km in 2 months). Our results also show evidence of the importance of longwave emission in the net HR of biomass burning plumes.


(a) The solid curves correspond to Mie calculations of the extinction ratios 448/755 nm and 1,543/755 nm for constant values of the width σ. The dashed curves correspond to constant values of the mean radius rm. This panel uses the same axis as Figure 2a of Wrana et al. (2021). The numbers and letters show SAGE III measured ratios for each latitude band (color coded) and month at the central level of maximum 755 nm extinction for each month. The months are coded as Y and Z for November and December 2021, as 1 to 9 between January and September 2022 and alphabetically from A to I between October 2022 and June 2023. For each latitude band, the altitude levels for months before February 2022 (and March for the 40°S band) are chosen to be the same as the central level for the first detection in March 2022 (or April for the 40°S band). (b) Comparison of SAGE III (solid) and modeled (dash) normalized extinctions for all nine aerosol channels of SAGE III. The curves are shown for the latitude band 30°–10°S using the values of σ and rm determined from the diagram (a). We show the background case of February 2022 (blue) and the earliest and latest case of the plume in March 2022 (orange) and June 2023 (green). (c, d) are respectively zooms on the “background zone” and the “plume zone” of panel (a).
Zonal altitude‐time sections averaged over 20° latitude bands between 50°S and 30°N from November 2021 to June 2023. The first row represents the aerosol extinction kext (km⁻¹) provided by SAGE III at 755 nm. The second row represents the mode width σ of the particle size distribution (PSD) retrieved from SAGE III extinction ratios. The third row represents the particle effective radius reff (μm). The fourth row represents the total number density N0 (cm⁻³) of the PSD retrieved from SAGE III extinction ratios and 755 nm extinction kext.
Monthly averaged particle size distributions from the retrieved particle size distribution parameters in the 30°–10°S latitude range. Orange curve corresponds to background conditions at 24.5 km averaged between months of November 2021 and January 2022, blue curve corresponds to plume conditions at altitude of maximum extinction averaged between months of June and August 2022.
(a) Orange curves: evolution of the H2SO4 total mass contained in the plume sulfates for a H2SO4 weight percentage ws = 70%, according to SAGE III, eliminating surrounding pixels with radius rm less than 0.2 μm considered as background. Blue curves: background contribution within the volume of the plume with σ = 1.4, rm = 0.15 μm, and N0 = 1 cm⁻³. The latitude range is 50°S–30°N for solid curves and 70°S–30°N for dashed curves. (b) Evolution of the H2SO4 total mass per latitude band. The contribution from the 50°–70°S is zero before May 2022, then is missing until August and contaminated by polar stratospheric clouds until September. It is shown only from October 2022 to April 2023.
Observation of the Aerosol Plume From the 2022 Hunga Tonga—Hunga Ha'apai Eruption With SAGE III/ISS

September 2023

·

144 Reads

·

12 Citations

Plain Language Summary We study the stratospheric aerosol plume produced by the Hunga Tonga–Hunga Ha'apai eruption on 15 January 2022 based on the high quality solar occultation measurements of the instrument SAGE III (Stratospheric Aerosol and Gas Experiment) onboard the International Space Station. These data reveal that the aerosol sizes are about twice as large as after other documented volcanic eruptions and that the total mass of H2SO4 in the liquid droplets of sulfate in the stratosphere has been very stable from March 2022, when it started to be well homogeneized in longitude, to November 2022, when it started to decay. The total mass of 0.66 Tg of H2SO4 is in good agreement with the early estimates of a stratospheric emission of 0.4–0.5 Tg of SO2. The implication is that the aerosol radiative impact will not mask the persisting warming effect of the water vapor injected in the stratosphere by the eruption.


Observing the SO2 and Sulphate Aerosol Plumes from the 2022 Hunga Tonga-Hunga Ha'apai Eruption with IASI

August 2023

·

79 Reads

·

4 Citations

The Hunga Tonga-Hunga Ha’apai volcano violently erupted on 15 January 2022, producing the largest perturbation of the stratospheric aerosol layer since Pinatubo 1991, despite the estimated modest injection of SO2. Here we present novel SO2 and sulphate aerosol (SA) co-retrievals from the Infrared Atmospheric Sounding Instrument, and use them to study the dispersion of the Hunga Tonga plume over the entire year 2022. We observe rapid conversion of SO2 (e-folding time: 17.1±0.6 days) to sulphate aerosols (SA), with an initial injected burden of >1.0 Tg. This points at larger SO2 injections than previously thought. A long-lasting SA plume was observed, with a meridional dispersion of marked anomalies from the tropics to the higher southern hemispheric latitudes. A very small SA removal is observed after 1-year dispersion. The total SA mass burden was estimated at 1.6 ± 0.1 Tg in total column, with a build-up e-folding time of about 2 months.


Figure 3. Monthly averaged particle size distributions from the retrieved PSD parameters in the 30°S -10°S latitude range. Orange curve corresponds to background conditions at 24.5 km averaged between months of November 2021 and January 2022, blue curve corresponds to plume conditions at altitude of maximum extinction averaged between months of June and August 2022.
Observation of the aerosol plume from the 2022 Hunga Tonga - Hunga Ha’apai eruption with SAGE III/ISS

June 2023

·

77 Reads

·

2 Citations

The Tonga eruption of 15 January 2022 has released a long-lived stratospheric plume of sulfate aerosols. More than 15 months after, we focus on the high quality data series of SAGE III/ISS to determine the mean radius and size distribution of the aerosols and their total mass. We show that the persisting aerosols – with a mode width of 1.25 and an effective radius of 0.4 µm – differ from the significantly smaller background aerosols and from those measured during other recent stratospheric eruptions. The sulfuric acid mass between 50°S and 30°N is estimated to be very stable in spite of considerable redistribution in latitude at a value of 0.66 Tg ± 0.1 Tg, corresponding to an initial sulfur dioxide emission of 0.44 Tg. Such properties are expected to induce a small negative aerosol radiative forcing, thus facilitating the persistence of a climate warming due to the volcanic water vapour.


Radiative impacts of the Australian bushfires 2019–2020 – Part 2: Large-scale and in-vortex radiative heating

June 2023

·

65 Reads

·

2 Citations

Record-breaking wildfires ravaged south-eastern Australia during the fire season 2019–2020. The intensity of the fires reached its paroxysmal phase at the turn of the year 2019–2020, when large pyro-cumulonimbi developed. Pyro-convective activity injected biomass burning aerosols and gases in the upper-troposphere—lower-stratosphere (UTLS), producing a long-lasting perturbation to the atmospheric composition and the stratospheric aerosol layer. The large absorptivity of the biomass burning plume produced self-lofting of the plume and thus modified its vertical dynamics and horizontal dispersion. Another effect of the in-plume absorption was the generation of compact smoke-charged anticyclonic vortices which ascended up to 35 km altitude due to diabatic heating. We use observational and modelling description of this event to isolate the dominant Southern-Hemispheric biomass burning aerosol plume from the main isolated vortex. Entering this information into an offline radiative transfer model, and with hypotheses on the absorptivity and the angular scattering properties of the aerosol layer, we estimate the radiative heating rates (HR) in the plume and the vortex. We found that the hemispheric-scale plume produced a HR of 0.08±0.05 K/d, which is strongly dependent on the assumptions on the aerosol optical properties and then on the plume ageing, in our simulations. We also found in-vortex HR as large as 15–20 K/d in the denser sections of the main vortex (8.4±6.1 K/d on average in the vortex). Our results suggest that radiatively-heated ascending isolated vortices are likely dominated by small-sized strongly absorbing black carbon particles. The hemispheric-scale and in-vortex HR estimates are consistent with the observed ensemble self-lofting (a few km in 4 months) and the main isolated vortex rise (~20 km in 2 months). Our results also put in evidence the importance of longwave emission in the net HR of biomass burning plumes.


Volcanic injection and initial HT plume evolution
Selected Ash RGB Himawari images for three sequences of the initial dispersion of the HT volcanic plume (15th January at 4:40 to 20th January at 14:00). a HT explosion and plume rise; b disappearing ash/ice signal; c sulphur-rich plume dispersion across Australia. All times are UTC. By a RGB band combination, this product allows to qualitatively distinguish thick ash plumes or ice clouds (brown), thin ice clouds (dark blue) and sulphur-containing plumes (green). Mixed ash/sulphur-containing volcanic species would appear in reddish and yellow shades.
The physicochemical properties of the early HT plume
IMS/IASI SO2 (a) and sulfate-specific AOD (b) observations for 16th January at 23:07 UTC. a, b the red line is CALIOP track for the same day at 15:41 UTC. OMPS-LP integrated SAOD (c) and vertical aerosol extinction profile (central detector, d) for 16th January at 2:03 and 3:27 UTC. d the red line is tropopause height. Attenuated CALIOP backscatter at 532 nm (e), and integrated in-plume AOD (f), corrected transmission (g) extinction (h) and depolarisation (i) in the two identified plumes sections (pink and green squares). The CALIOP track of e–i is the one identified in a and b. Due to the time mismatch between CALIOP and IASI orbits, the CALIOP trace actually crossed both the eastern part of the aerosol plume in a, b (lower plume at 27 km) and the western part (upper plume at 30 km) which has already reached Australia in the display.
Longer-term HT plume evolution and its comparison with recent past events
Zonal average IMS/IASI SO2 observations (a), sulfate-specific AOD (b) and their ratio (c), for the first month of HT plume dispersion. Black triangles in a–c indicate the main HT eruption of January 15th (large triangle) and the previous smaller event of January 14th (that had a small but visible impact on the SO2 distributions). Time series of the OMPS-LP zonal average SAOD (d) and tropical (Tropics: 30°N–30°S, red line), Northern Hemisphere (NH: 0–80°N, blue line), Southern Hemisphere (SH: 0–80°S, green line) and global (Global: 80°N–80°S, black line) SAOD (e). The OMPS-LP time series are updated to 15th June 2022. Global, Tropical, Northern Hemispheric and Southern Hemispheric peak SAOD values for the stratospheric events: HT eruption in 2022 (HT2022), Australian fires in 2019-2020 (AF2020), Raikoke eruption in 2019 (Ra2019), Nabro eruption in 2011 (Na2011), from OMPS-LP observations, and Pinatubo eruption in 1991 (Pi1991) and El Chichon eruption in 1982 (EC1982), from the GloSSAC database (f).
Water vapour in the HT plume
Water vapour radio-sounding observations over western Australia on 18th January (unperturbed background in RF estimations, black line), 19th (dark red line), 20th (red line), and 8th February (yellow line), and over Saint Helena island (blue line) (a). Plume and sounding positions (red crosses) are shown in b–f, using IMS/IASI SO2 and sulfate-specific AOD observations.
Stratospheric radiative cooling due to the HT plume and plume descent
Aerosol (a), water vapour (b) and total plume (c) LW (dashed lines), SW (dotted lines) and total (solid lines) radiative heating rates (HR) for the basic cases discussed in the text: fresh plume, higher section (dark red), fresh plume, lower section (red) and aged plume (orange). The additional case of the southern Atlantic profile is presented for water vapour only in b (blue). The CALIOP aerosol observations and water vapour radio-sounding, even if representative of the same plume sections, are taken at different time intervals (radio-soundings are taken 2 days later than CALIOP overpasses of the early plume), thus CALIOP profiles are vertically shifted to match the water vapour enhancements observed with radio-sounding. CALIOP 532 nm attenuated backscatter ratio (SR) averaged daily over all night traces in the zonal direction and between 15°S and 25°S in latitude (d). The fit is performed over all pixels where SR > 4 and for the two periods Jan 28–Feb 09 (green line, −11.3 K/d) and Feb 10–28 (blue line, −3.6 K/d).
The unexpected radiative impact of the Hunga Tonga eruption of 15th January 2022

November 2022

·

322 Reads

·

104 Citations

The underwater Hunga Tonga-Hunga Ha-apai volcano erupted in the early hours of 15th January 2022, and injected volcanic gases and aerosols to over 50 km altitude. Here we synthesise satellite, ground-based, in situ and radiosonde observations of the eruption to investigate the strength of the stratospheric aerosol and water vapour perturbations in the initial weeks after the eruption and we quantify the net radiative impact across the two species using offline radiative transfer modelling. We find that the Hunga Tonga-Hunga Ha-apai eruption produced the largest global perturbation of stratospheric aerosols since the Pinatubo eruption in 1991 and the largest perturbation of stratospheric water vapour observed in the satellite era. Immediately after the eruption, water vapour radiative cooling dominated the local stratospheric heating/cooling rates, while at the top-of-the-atmosphere and surface, volcanic aerosol cooling dominated the radiative forcing. However, after two weeks, due to dispersion/dilution, water vapour heating started to dominate the top-of-the-atmosphere radiative forcing, leading to a net warming of the climate system.


Radiative impacts of the Australian bushfires 2019–2020 – Part 1: Large-scale radiative forcing

July 2022

·

101 Reads

·

25 Citations

As a consequence of extreme heat and drought, record-breaking wildfires developed and ravaged south-eastern Australia during the fire season 2019–2020. The fire strength reached its paroxysmal phase at the turn of the year 2019–2020. During this phase, pyrocumulonimbus clouds (pyroCb) developed and injected biomass burning aerosols and gases into the upper troposphere and lower stratosphere (UTLS). The UTLS aerosol layer was massively perturbed by these fires, with aerosol extinction increased by a factor of 3 in the visible spectral range in the Southern Hemisphere, with respect to a background atmosphere, and stratospheric aerosol optical depth reaching values as large as 0.015 in February 2020. Using the best available description of this event by observations, we estimate the radiative forcing (RF) of such perturbations of the Southern Hemispheric aerosol layer. We use offline radiative transfer modelling driven by observed information of the aerosol extinction perturbation and its spectral variability obtained from limb satellite measurements. Based on hypotheses on the absorptivity and the angular scattering properties of the aerosol layer, the regional (at three latitude bands in the Southern Hemisphere) clear-sky TOA (top-of-atmosphere) RF is found varying from small positive values to relatively large negative values (up to -2.0 W m-2), and the regional clear-sky surface RF is found to be consistently negative and reaching large values (up to -4.5 W m-2). We argue that clear-sky positive values are unlikely for this event, if the ageing/mixing of the biomass burning plume is mirrored by the evolution of its optical properties. Our best estimate for the area-weighted global-equivalent clear-sky RF is -0.35±0.21 (TOA RF) and -0.94±0.26 W m-2 (surface RF), thus the strongest documented for a fire event and of comparable magnitude with the strongest volcanic eruptions of the post-Pinatubo era. The surplus of RF at the surface, with respect to TOA, is due to absorption within the plume that has contributed to the generation of ascending smoke vortices in the stratosphere. Highly reflective underlying surfaces, like clouds, can nevertheless swap negative to positive TOA RF, with global average RF as high as +1.0 W m-2 assuming highly absorbing particles.


Citations (8)


... This injection of smoke aerosols produced the strongest documented large-scale radiative forcing for a fire event, of comparable magnitude with the strongest volcanic eruptions of the post-Pinatubo era (Sellitto et al., 2022). In addition, the absorption of solar radiation diabatically heated these large amounts of injected absorbing aerosols (Sellitto et al., 2023) and generated an anticyclonic self-maintained ellipsoidal vortex of 1000 km in diameter (Podglajen et al., 2024), who 50 travelled around the Southern Hemisphere and ascended up to 35 km altitude by March 2020 (Kablick et al., 2020;Khaykin et al., 2020). In his way up to the deep stratosphere, the anticyclonic vortex dragged large amounts of ozone-poor tropospheric air masses who temporarily diluted the ozone-rich stratospheric air and generated an ozone mini-hole (Bernath et al., 2022;Khaykin et al., 2020;Ohneiser et al., 2022;Solomon et al., 2022;Yu et al., 2021). ...

Reference:

Early evolution of the ozone mini-hole generated by the Australian bushfires 2019–2020 observed from satellite and ground-based instruments
Radiative impacts of the Australian bushfires 2019–2020 – Part 2: Large-scale and in-vortex radiative heating

... However, we also compare our results with other satellite products, including MLS for H₂O and O₃ (Supplementary Figs. 3,(11)(12)(13)(14) and SAOD measurements from multiple instruments, such as OMPS-SASK, OMPS-NASA, and GloSSAC, to ensure consistency and to assess and highlight uncertainties across different datasets (Supplementary Fig. 2; Table 1). ...

Observation of the Aerosol Plume From the 2022 Hunga Tonga—Hunga Ha'apai Eruption With SAGE III/ISS

... Hunga also injected at least 0.5 Tg of SO 2 into the stratosphere (Carn et al., 2022) although this amount may have been as much as 1.5 Tg (Sellitto et al., 2024). SO 2 oxidation forms a sulfate aerosol layer that was detected by the Ozone Mapping and Profile Suite limb profiler (OMPS) shortly after the eruption. ...

Observing the SO2 and Sulphate Aerosol Plumes from the 2022 Hunga Tonga-Hunga Ha'apai Eruption with IASI
  • Citing Preprint
  • August 2023

... In the case of the plumes from the 2020 Australian fires, this appears as a reasonable approximation, since CALIOP shows limited attenuation of the lidar beam at 532 nm (Section 2). Furthermore, Sellitto et al. (2023) recently reported that the radiative properties of the aerosols remained stable over time-scales ranging from weeks to months, which justifies using a constant . Finally, it should be mentioned that, besides simplifying the heating induced by the absorbing/emitting layer, Equation (21) also ignores the radiative damping of the temperature anomaly associated with the anticyclone (Lestrelin et al., 2021). ...

Radiative impacts of the Australian bushfires 2019–2020 – Part 2: Large-scale and in-vortex radiative heating

... Pinatubo, Parker et al., 1996) a significantly lower amount of SO2 (~0.42 Tg) was detected in the atmosphere. In contrast, a surprisingly large quantity of water vapor was measured (146 ± 5 Tg, ~10% of the total stratospheric burden) (Millán et al., 2022;Sellitto et al., 2022). ...

The unexpected radiative impact of the Hunga Tonga eruption of 15th January 2022

... Kloss et al., 2021). This injection of smoke aerosols produced the strongest documented large-scale radiative forcing for a fire event, of comparable magnitude with the strongest volcanic eruptions of the post-Pinatubo era (Sellitto et al., 2022). In addition, the absorption of solar radiation diabatically heated these large amounts of injected absorbing aerosols (Sellitto et al., 2023) and generated an anticyclonic self-maintained ellipsoidal vortex of 1000 km in diameter (Podglajen et al., 2024), who 50 travelled around the Southern Hemisphere and ascended up to 35 km altitude by March 2020 (Kablick et al., 2020;Khaykin et al., 2020). ...

Radiative impacts of the Australian bushfires 2019–2020 – Part 1: Large-scale radiative forcing

... Water vapor is radiatively active in the infrared, contributing to the total radiative cooling in the stratosphere, which is dominated by the effects of carbon dioxide and ozone (e.g., Gille & Lyjak, 1986). These large perturbations in water vapor are expected to increase the amount of radiation lost to space, locally cooling the stratosphere (Schoeberl et al., 2022;Sellitto et al., 2022). This study attempts to quantify this impact on the temperature, as well as the subsequent changes to the stratospheric circulation, during the first 6 months after the eruption. ...

The unexpected radiative impact of the Hunga Tonga eruption of January 15th, 2022

... Fresh and aged biomass burning plumes produce diabatic radiative heating, e.g., [1], and then can lead to self-lofting of the plume, e.g., [2]. They can produce a warming or cooling radiative forcing, depending on their optical properties and then their atmospheric lifetime [3]. If vertically and horizontally co-located with clouds, they may modify their properties and precipitation by acting as cloud condensation nuclei, e.g., [4], depending on the age and the composition of the particles, e.g., [5]. ...

Radiative impacts of the Australian bushfires 2019–2020 – Part 1: Large-scale radiative forcing