Parya Broomandi1,12, Kaveh Mohammadpour 2,3, Dimitris G. Kaskaoutis4, Aram Fathian 5,6,7, Sabur F. Abdullaev8, Vladimir A. Maslov8, Amirhossein Nikfal9, Ali Jahanbakhshi10, Bakhyt Aubakirova1, Jong Ryeol Kim This email address is being protected from spambots. You need JavaScript enabled to view it.1, Alfrendo Satyanaga1, Alireza Rashki11, Nick Middleton13 1 Department of Civil and Environmental Engineering, School of Engineering and Digital Sciences, Nazarbayev University, Astana 010000, Kazakhstan
2 Department of Climatology, Faculty of Geographical Sciences, Kharazmi University, Tehran, Iran
3 Climate Change Technology Transfer to Developing Countries Group (SSPT-PVS), Department of Sustainability, Italian National Agency for New Technologies Energy and Sustainable Development, ENEA, C. R. Casaccia, 00123 Rome, Italy
4 Institute for Environmental Research and Sustainable Development, National Observatory of Athens, 15236 Athens, Greece
5 UNESCO Chair on Coastal Geo-Hazard Analysis, Research Institute for Earth Sciences, Tehran, Iran
6 Neotectonics and Natural Hazards Institute, RWTH Aachen University, Aachen, Germany
7 Water, Sediment, Hazards, and Earth-surface Dynamics (waterSHED) Lab, Department of Geoscience, University of Calgary, Canada
8 Department of Physical Atmosphere, Physical-Technical Institute, Academy of Sciences of Republic of Tajikistan, 734063, Dushanbe, Tajikistan
9 Atmospheric Science and Meteorological Research Centre (ASMRC), Tehran, Iran
10 School of Architecture, Building and Civil Engineering, Loughborough University, Loughborough, UK
11 Department of Desert and Arid Zones Management, Ferdowsi University of Mashhad, Mashhad, Iran
12 Department of Chemical Engineering, Masjed-Soleiman Branch, Islamic Azad University, Masjed-Soleiman, Iran
13 St Anne’s College, University of Oxford, Oxford OX2 6HS, UK
Received:
September 1, 2022
Copyright The Author(s). This is an open access article distributed under the terms of the Creative Commons Attribution License (CC BY 4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original author and source are cited.
Revised:
December 6, 2022
Accepted:
January 3, 2023
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||https://doi.org/10.4209/aaqr.220309
Broomandi, P., Mohammadpour, K., Kaskaoutis, D.G., Fathian, A., Abdullaev, S.F., Maslov, V.A., Nikfal, A., Jahanbakhshi, A., Aubakirova, B., Kim, J.R., Satyanaga, A., Rashki, A., Middleton, N. (2023). A Synoptic- and Remote Sensing-based Analysis of a Severe Dust Storm Event over Central Asia. Aerosol Air Qual. Res. https://doi.org/10.4209/aaqr.220309
Cite this article:
A severe dust storm blanketing Central Asia on 3–4 November 2021 was investigated employing satellite remote-sensing, synoptic meteorological observations, reanalysis and HYSPLIT back-trajectories. The prevailing meteorological conditions showed an intensification of air subsidence over eastern Kazakhstan, featured in a typical omega-blocking system over the region and two troughs to its west and east axis, one day before the dust storm. The prevailing high-pressure system and temperature gradients over Kazakhstan modulated the dominant anticyclonic wind pattern generated from the south Balkhash basin toward the Caspian Sea, causing a huge dust storm that covered the southern half of Kazakhstan and large parts of Uzbekistan, Tajikistan and Turkmenistan. The dust storm originated in the steppes of southern Kazakhstan by violent downdraft winds. Initially it swept over eastern parts and then the whole of Uzbekistan, reaching the Caspian Sea in the west. Meteorological measurements and HYSPLIT back-trajectories at selected sites in Central Asia (Turkmenabat, Khujand and Tashkent) showed a remarkable dust impact that reduced temperature (by 2–4°C) and visibility to below 1 km at different periods, as the thick dust plume expanded in various directions. The extremely high PM concentrations (PM10 > 10,000 µg m–3 in Tashkent) could endanger both human health and the environment, especially in a region suffering from high susceptibility to wind erosion and significant land degradation and desertification. Effective and immediate stabilising measures to control wind erosion in vulnerable areas of Central Asia are warranted.HIGHLIGHTS
ABSTRACT
Keywords:
Atmospheric circulation, Dust storms, HYSPLIT, Backward trajectory, Tashkent
The ambient air pollution induced by dust storms is associated with a wide range of human health disorders (Middleton, 2020) including (i) respiratory diseases such as bronchial asthma and chronic bronchitis (Al-Hemoud et al., 2018; Kang et al., 2012; Wang et al., 2014), (ii) cardiovascular diseases (Aghababaeian et al., 2021; Aili and Kim Oanh, 2015), (iii) psychological and cognitive disorders (Ghaisas et al., 2016; Gordeev et al., 2013) and (iv) neurodegenerative diseases (Aleya and Uddin, 2020; Chin-Chan et al., 2015; Galán-Madruga et al., 2020; Galán-Madruga and García-Cambero, 2022; Shafiee et al., 2021). Moreover, increased total non-accidental deaths in both adults and children are reported among exposed individuals in areas highly impacted by dust storms (Achilleos et al., 2019; Díaz et al., 2017; Galán-Madruga et al., 2022; Kashima et al., 2016; Perez et al., 2008). High ambient concentrations of dust particles caused by intense dust storms also lead to horizontal visibility reduction, which can have socio-economic impacts in several sectors, including aviation, transport, education, leisure construction and energy production (Middleton et al., 2021; Middleton, 2017; Middleton and Kang, 2017). Dust aerosols, originating from desert areas all over the world, can play an important role in altering Earth’s solar radiation balance and the primary productivity of oceans through iron fertilization (Jickells et al., 2005; Kok et al., 2018; Schepanski, 2018). Dust is a major type of tropospheric aerosol and the most common wind-induced climatic phenomenon in the hyperarid, arid and semi-arid regions of Central Asia (CA), accounting for ~25% of total global dust emissions, with significant impacts on regional climate, biogeochemical cycles, loess formation and the hydrological cycle (Booth et al., 2012; Ginoux et al., 2004; Li et al., 2021; Issanova and Abuduwaili, 2017; Uno et al., 2009). In recent times, dust generation and, consequently, population exposure in CA have escalated due to climate variability and land cover changes, as a result of rapid development, deforestation, enhanced aridity, mining and agricultural activities (Gao and Washington, 2009; Sternberg and Edwards, 2017; UN, 2010; Wiggs et al., 2003). Across CA, the most wind erosive areas and hotspots of dust storm activity are in Kazakhstan (areas surrounding the desiccated Aral Sea, known as the Aralkum Desert, Saryesik Atyrau Desert to the south of Lake Balkhash and Muyunkum Desert to its western end), Turkmenistan (Karakum Desert), Uzbekistan (Kyzylkum Desert), west of Mongolia and northwest China (Tarim Basin, Taklimakan and Gurbantunggut Deserts) (Gholami et al., 2021; Laurent et al., 2006; Song et al., 2021). Beyond climate change (decrease of precipitation and desertification over CA), human intervention, specifically the extended cultivation ploughing up of pastures during the Virgin Lands Programme of the 1950s, have played an important role in the increased wind erosion activity (Goudie and Middleton, 2006; Indoitu et al., 2012). For example, in Kazakhstan, different degrees of land degradation and desertification occur due to anthropogenic activities, unsustainable land practices such as agricultural activities, and non-rational use of natural sources such as water (Almaganbetov and Grigoruk, 2008; MARK, 2006; Lau et al., 2020; Madruga et al., 2019). Land degradation and desertification are mainly observed in regions under unfavourable ecological conditions such as Lake Balkhash, Caspian lowland and around the dried bed of the Aral Sea (GEF, 2003; NPRK, 2005). The areas in Kazakhstan most vulnerable to wind erosion are the western and southern parts, where the total wind-eroded lands are estimated at about 12.4 and 13.1 million hectares respectively (out of 273.5 million hectares of the Kazakhstan territory). In addition, wind eroded agricultural lands in the eastern and northern parts of the country occupy about 1.28 and 3.87 million hectares respectively, which are subject to accelerated desertification, including around 66% of Kazakhstan’s total area (Almaganbetov and Grigoruk, 2008; CSD, 2002). These conditions may lead to changes in regional terrestrial (desertification, wetness of topsoil, surface water resources, surface roughness) and climatic factors (wind and rainfall regimes), facilitating generation of dust storms over CA (Huang et al., 2016, 2017; Mahmoodirad and Sanei, 2016;Wang et al., 2017; Xi and Sokolik, 2015). Seasonal and inter-annual changes in atmospheric circulation patterns, along with changes in local topography, land use land cover (LULC) and long-term modulations of the climate system, control the dust activity over CA (Kaskaoutis et al., 2017; Nobakht et al., 2021; Shi et al., 2019; Zhang et al., 2020). Dust particles rising from Central Asia are held responsible for air-quality deterioration over Korea, Japan and Taiwan (Hashizume et al., 2010; Hasunuma et al., 2019), as well as northeast Iran-Afghanistan and other parts of southwest Asia (Kaskaoutis et al., 2016; Mohammadpour et al., 2022). Specific synoptic weather patterns may also favour dust from CA to be transported to the west, impacting Georgia, Belarus and Lithuania (Hongisto and Sofiev, 2004) or even the Balkans and Italy (Tositti et al., 2022). Furthermore, other studies showed that 3% of Asian dust can reach the western USA (Creamean et al., 2014). Dust-raising activity over CA occurs mostly during spring and summer, depending on area and meteorological conditions (Rupakheti et al., 2020, 2019), while dust-induced radiative forcing during intense dust events in Dushanbe, Tajikistan were estimated at –48 ± 12, –85 ± 24 and 37 ± 15 Wm–2 at the top of the atmosphere, surface and within the atmosphere, respectively, with even higher values during extreme dust events (Rupakheti et al., 2021). Although several aspects regarding dust sources, climatology of dust activity and dust impacts have been well documented in CA, as discussed above, case studies of severe and long-range transported dust events from this region are rare in the literature (Tositti et al., 2022). This work analyses a severe dust storm event over CA that affected a large area in southern Kazakhstan, Uzbekistan and Tajikistan on 3–4 November 2021 (Eurasianet, 2021; MKWEATHER, 2021) (Fig. 1). A massive dust storm covered Tashkent, the capital of Uzbekistan, where the horizontal visibility decreased to 200 meters and the PM10 concentrations spiked at 18,000 µg m–3 on 4 November 2021, 30 times above the Uzbekistan maximum acceptable level. Local authorities reported that it was the most extreme sand/dust storm during the last 150 years of monitoring in Tashkent (Uzhydromet, 2021). The true colour imagery of Terra-MODIS sensor, accessible from NASA Worldview (https://worldview.earthdata.nasa.gov) on 4 November 2021, showed a thick dust plume covering parts of south-eastern Kazakhstan, Uzbekistan and north Tajikistan around the Fergana valley (Fig. 1). People in Tashkent were advised to stay indoors, avoiding walks and physical activities. On 4 November 2021, the ambulance service received 687 calls from inhabitants in Tashkent seeking help for respiratory problems. Besides hospital admissions, local authorities reported car accidents and casualties due to low horizontal visibility (Uzhydromet, 2021). Moreover, on 5 November, the dust haze caused interruptions in drinking water supply in some districts of Tashkent due to the malfunction in the high-voltage power supply network (Eurasianet, 2021). Dust intrusion also caused a power outage in about 50 villages in the Turkestan region, southeast Kazakhstan, while drivers were stuck on the highway in traffic jams on 4 November 2021, due to reduced visibility (Eurasianet, 2021). Overall, this severe dust storm caused many socio-economic and health impacts for local inhabitants, beyond deterioration of air quality. This unprecedented dust event in CA undoubtedly needs further investigation of the meteorological conditions and driving mechanisms that initiated such a dust storm. This study investigates the synoptic meteorology and atmospheric circulation patterns that triggered this dust storm event and aims to detect the dust source and the expansion of the dust plumes via SEVIRI satellite imagery. Furthermore, it examines the impact of the dust storm on local meteorological conditions and visibility at specific sites in CA, and provides discussions about land degradation and increased dust activity over CA during the last decades. The Central Asian plains stretch from the shores of the Caspian Sea in the west to the foothills of Altai, Tian-Shan and Pamir Mountains in the east (Fig. 2). The Central Asian drylands cover an area of 1.890 million km2 and are home to about 40 million inhabitants (Indoitu et al., 2012). The area consists of various litho-edaphic desert types such as gravel-gypseous and gravel, sandy, sandy-pebble and pebble, loess, loamy, solonchakous and clayey deserts (Issanova and Abuduwaili, 2017; Gholami et al., 2021; Li et al., 2021). Based on different synoptic processes and meteorological conditions, CA is divided into two climatic zones of northern and southern (Issanova et al., 2015). The northern part has a dry and cold continental Central Asian climate, while the southern region is characterized by a dry and hot climate. In the northern part, the mean annual temperature varies between 5 and 11°C, while it increases to 13–16.6°C in the southern part. The annual precipitation over the whole region varies between 80 mm and 200 mm and it is below 100 mm in the desert regions of western Balkash shore, Kyzylkum, Karakum Deserts and Betpak-Dala (Indoitu et al., 2012; Issanova and Abuduwaili, 2017). In this study, ground-based hourly data of horizontal visibility, wind speed and temperature at selected stations in Central Asia (i.e., Tashkent, Uzbekistan; Khujand, Tajikistan; Turkmenabat, Turkmenistan) were obtained from the Iowa Environmental Mesonet (https://mesonet.agron.iastate.edu/ASOS/). Additionally, hourly PM2.5 data were obtained from the monitoring station in the United States Embassy in Tashkent, Uzbekistan (https://www.airnow.gov/international/us-embassies-and-consulates/). ERA-5 reanalysis (Hersbach et al., 2020) is produced by European Centre for Medium-Range Weather Forecasts (ECMWF) within the Copernicus Climate Change Service (C3S), which includes a detailed record of the global atmosphere and land surface from 1950 onwards (Hersbach et al., 2020). In this study, ERA-5 reanalysis data was used to obtain meteorological variables of (i) vertical velocity at 300 hPa, (ii) zonal wind at 250 hPa, (iii) geopotential heights at 500 and 850 hPa, (iv) air temperature at 2 m, (v) Mean Sea Level Pressure (MSLP) and (vi) surface vector winds, for the characterization of the daily synoptic conditions at 0.5° × 0.5° spatial resolution over CA during the dust storm event. The Modern-Era Retrospective Analysis for Research and Applications, version 2 (MERRA-2), is a long-term global reanalysis product with a horizontal resolution of 0.5° × 0.625° (latitude, longitude) and a temporal resolution varying from hour to month (Galán-Madruga, 2022; Gelaro et al., 2017; Sayer et al., 2019; Shafiee et al., 2019). In this study, the dust loading/dust column mass density (g m–2) was taken over CA on a daily basis around the dust storm event, as MERRA-2 has been proved as an accurate database for studying dust aerosols (Shaheen et al., 2020; Shi et al., 2019; Mahmoodirad et al., 2019). Visible/IR images of SEVIRI (Spinning Enhanced Visible and Infrared Imager) were employed to monitor the transport of the dust storm in high temporal resolution (~15 mins) (Schepanski et al., 2007, 2009). The infrared channel data from SEVIRI is based on RGB (red-green-blue) image compositions, and dusty pixels in pink or magenta colours are used to monitor the evolution of dust events during both day and night over desert areas (Martínez et al., 2009; Kaskaoutis et al., 2019). The HYSPLIT-4 (Hybrid Single-Particle Lagrangian Integrated Trajectory) model is widely used for analysis of the air-mass trajectories, dispersion and deposition of aerosols using the Global Forecast System (GFS) meteorological parameters as the initial background field (Ashrafi et al., 2014; Draxler and Hess, 1997). In this study, HYSPLIT air-mass back-trajectories were used at certain receptor sites in Central Asia like Tashkent (41.3°N, 69.26°E), Khujand (40.28°N, 69.63°E) and Turkmenabat (39.03°N, 63.56°E) on the dust storm day (4 November 2021), in order to investigate the dust source and the pathways of the expanded dust plumes that affected several regions in Central Asia (Rashki et al., 2015). SEVIRI Visible/IR imagery enables detection of slight or thick dust plumes, as well as subtle variations from one image to another, on high temporal resolution (Schepanski et al., 2009; Molla-Alizadeh-Zavardehi et al., 2014). In this study, SEVIRI imagery was deployed to monitor the evolution of the dust storm, aiming to identify the source origin, expansion of the dust plume and the affected areas in CA on 4 November 2021 (Fig. 3). Strong north-easterlies, which will be analysed in the next section, triggered dust-raising in Zhambyl region, and activated dust sources in Moiynkum, Kyzylorda and eastern Kyzylkum Deserts in the early morning of 4 November 2021 (04:00 UTC). The thick dust plume, shown in bold pink and magenta colours, reached Turkmenabat, Tashkent and Khujand at around 09:00 UTC, 11:00 UTC and 12:00 UTC, respectively. Terra-MODIS true-colour observations and SEVIRI RGB images corroborate detection of a very thick dust plume. However, the intensity of the pink/magenta colours associated with dust in RGB imagery does not absolutely agree with the dust intensity, since the RGB signal could be affected by dust mineralogy, low-temperature inversions and dust-layer height (Brindley et al., 2012; Solomos et al., 2018). The extensive cloudiness over the mountainous ranges is detected in ochre and brown colors in RGB imagery. Note also the change in the desert-surface reflectance colour from light cyan during the early morning hours to yellow, light orange during noon and early afternoon hours on 4 November (Fig. 3). This section analyses the atmospheric circulation patterns in the upper, middle, and lower troposphere during a 6-day period (1–6 November 2021) around the dust storm day (4 November 2021), aiming to reveal the dynamic conditions that were associated with the genesis, expansion and dissipation of the dust storm (Figs. 4–7). Prior to the dust storm, on 1 November, a typical cold atmospheric circulation formed over eastern Europe and the Balkan Peninsula, detected by a deep trough, which started to dissipate on 3 November (Fig. 4(a–c)). In the upper troposphere, these conditions were characterized by two relatively weak polar and subtropical jet streams over Russia and south Asia, respectively. The polar jet stream was progressively moving from central-west Siberia to east Kazakhstan, while marginal changes were observed in the sub-tropical jet stream, with a core of above 45 m s–1 over the Ganges valley and the Himalayas (Fig. 5(a–c)). The dynamic conditions created subsidence behind the subtropical jet core over the east of Iran, Afghanistan and Pakistan, while negative omega values at 300 hPa dominated over the Kazakhstan-Russia border, associated with the polar jet (Figs. 5(a–c)). In the meanwhile, the cold Siberian anticyclone was dominant over eastern Siberia, creating a strong gradient of geopotential heights across the Russia-Kazakhstan border. A high-pressure ridge prevailed on days prior to dust storm stretching from the Middle East and Iran to the Caspian Sea and western Russia, carrying warmer air masses over the region. These conditions created an omega blocking system over CA and Russia on days prior to the dust storm, while the axis of this ridge progressively shifted from southeast-to-northwest (1 November) to southwest-northeast on 4 November (Fig. 4), thus changing the upper-troposphere circulation. The upper-level conditions accompanied by stretching a trough in mid troposphere (500 hPa) over the northern borders of Kazakhstan, increased the instability along troposphere, which was induced to penetrate cold air masses from the Siberian region into CA. On 3 November, just prior to the dust storm, the polar jet, with a core of 35–45 m s–1, moved from south Russia to east Kazakhstan, causing negative omega at 300 hPa over the region (Figs. 5(a–c)). These conditions maximized air subsidence over the Kazakhstan-Russia border, which was accompanied by the eastward replacement of the polar jet with air upward motion over southeast Kazakhstan (Fig. 5(c)). The circulation at 500 hPa level featured a typical omega blocking pattern, with a large ridge over west Russia and two troughs to its west and east, whereas the latter was much deeper than the former extending into the whole territory of Kazakhstan. A strong surface-temperature gradient was created along north Kazakhstan, with the minimum temperature below −30°C, which was moving northwards affecting the central-eastern part of Kazakhstan on 3–4 November, with characteristics of a cold front associated with the Siberian anticyclone. Furthermore, the establishment of the polar jet stream strengthened the vertical instability, helping the convergence and invasion of cold air mass into east Kazakhstan. The atmospheric circulation on 4 November had a notable difference from that on 3 November, mostly detected by the strengthening of the jet stream over eastern Kazakhstan (wind speeds above 45 m s–1). This jet stream was expanded over a much lower area, which was affected by an intensified trough, as a tongue of cold-air intrusion from the Siberian anticyclone (Figs. 4(d) and 5(d)). These meteorological conditions triggered highest negative omega values highlighted an upward air motion in the upper troposphere over east Kazakhstan and surroundings and is likely to be highly associated with the dust storm outbreak, as also shown in previous studies over the Middle East and the Mediterranean (Kaskaoutis et al., 2019; Hamzeh et al., 2021). These dynamic conditions also induced an intense gradient between northern divergence and southern convergence in Central Asia. Furthermore, in the middle troposphere (500 hPa), the south-westward trough became deeper compared to previous day and it is stretched from Siberia to Iran, with the expanded ridge north-eastward, covering central Russia (Fig. 4(d)). The omega blocking system, accompanied with the Siberian anticyclone and favoured by the establishment of the upper-level jet stream over east Kazakhstan, seem to play a major role in the dust storm outbreak in east Kazakhstan. Although the atmospheric circulation patterns during intense dust storms in CA have not been well documented, being also variable depending on season and dust event (Kaskaoutis et al., 2019; Tositti et al., 2022), the role of the Siberian anticyclone, the position and movement of the upper-level jet stream seem to be very important factors controlling dust activity over CA during the cold period of the year. On 5 November, the strong zonal winds at 250 hPa (> 25 m s–1) covered an extended area from Italy toward western Russia (Fig. 5(e)), which was further extended to Siberia on the next day, while the upper-level jet over eastern Kazakhstan was dissipated and moved further to the south, practically merged with the subtropical upper-level jet over north India and the Tibetan Plateau (Fig. 5(f)). This weather pattern reflects rather stable upper-troposphere conditions accompanied by descending air, with positive omega values, over nearly the whole CA. The negative omega values prevailed in the northern edge of the subtropical jet (Fig. 5(e)), became more active air ascending over the trough-affected areas contributing to suction of cold air masses toward Tajikistan and northeast Pakistan on 5 November, when an expanded trough tongue covered the southeast Central Asian countries, extended over Iran (Fig. 4(e)). The omega blocking system over CA was significantly dissipated after the dust storm day and was limited to southern latitudes, as a ridge over the East Mediterranean-Middle East (EMME) region. These conditions limited invasion of polar cold air and transferred warmer air masses over CA and pushed the trough toward the east, while a zonal circulation was established at northern latitudes over Russia (Figs. 4(e, f)). The relative positions and intensity of the low- and high-pressure systems accompanied by the polar and subtropical jet streams at upper-levels, generally control the intensity of the surface regional winds and dust outbreaks (Mohammadpour et al., 2022). The meteorological conditions due to Caspian’s ridge at 500 hPa level facilitated the formation of high-pressure conditions at lower troposphere and at the surface over CA countries (Fig. 6). These conditions seem to modulate the dust activity over the region (Kaskaoutis et al., 2016; Shi et al., 2019). The dynamic pressure pattern on 2 November, which was a combination of two weak high-pressure systems over north Russia and CA on previous day, was characteristic of the omega blocking at the lower troposphere (850 hPa) and at the surface, with high-pressure conditions over central Siberia. The geopotential heights at 850 hPa presented even higher values on the next days (3 and 4 November 2021), with closed high-pressure systems over Kazakhstan, while at surface, high-pressure conditions of above 1040 hPa dominated over the whole Kazakhstan territory. The synoptic meteorology over the examined domain clearly dominated by this high-pressure system over CA, while lower pressure conditions prevailed in south Asia, the EMME region and in central/western Europe (Figs. 6(a–d)). This intense and expanded high-pressure system over CA (> 1600 gpm; > 1040 hPa over Kazakhstan), was a triggering dynamic for the formation of dust storm on 4 November 2021, while on the days after the dust storm, the core of the high-pressure system at 850 hPa was expanded over a larger area, slightly moved towards the east, and then significantly dissipated (Figs. 6(e–f)). These meteorological conditions were different from those usually prevailed during dust storms over southwestern CA in spring and summer that were attributed to high-pressure system over the Caspian Sea and thermal low-pressure over topographic-low areas in southern latitudes (Cheng et al., 2019; Li et al., 2019; Mohammadpour et al., 2022). Overall, MSLP dynamics highly controlled the wind regime on days prior, during and after the intense dust storm of 4 November 2021 over southeastern Kazakhstan. Fig. 6 shows the vector wind at the surface along with the spatial distribution of dust loading (in g m–2) obtained from MERRA-2 over Central Asia from 1 to 6 November 2021. The establishment of the high-pressure system over the northern part of CA on 2 November, modified the wind regime from the previous day, with a strong anticyclonic flow over Kazakhstan, which further intensified on 3 November. The easterly winds, propagated from the southern flanks of the high-pressure system over the southern part of CA, passed over Moiynkum, eastern Kyzylkum, Aralkum and Karakum Deserts (Zhou et al., 2019) and advected high dust loading covering a wide area till the shores of the Caspian Sea (Figs. 7(b–c)). At the same time, winter Shamal wind facilitated increased dust loading over the Syrian–Iraqi plains. A strong northerly/north-easterly flow dominated over the dust-source area, as well as over the alluvial dried beds in the Balkhash basin in east Kazakhstan, favouring dust emissions. On the dust storm day (4 November 2021), the associated changes in the distribution of G850, MSLP and wind regimes over the central Asian countries, indicated that the strengthened high-pressure system intensified the dominant anticyclonic wind pattern compared to previous days. The prevailing surface wind propagated from the southern Balkhash basin blowing toward the Caspian Sea and affected the southern half of Kazakhstan and nearly whole territories of Uzbekistan and Turkmenistan (Fig. 7(d)). These areas are covered by high columnar dust loading greater than 1.1 g m–2, probably emitted from the various deserts such as Aralkum, Kyzylkum, Trans-Unguz, and central Karakum and alluvial dried beds of the Caspian lowlands (Nobakht et al., 2021). Therefore, apart from the thick dust plume that covered the Tashkent area on 4 November 2021 and caused several socio-economic and health impacts on local population, the north-easterly/easterly flows generated from the centre of the anticyclone over Kazakhstan facilitated an extensive dust blanket over the southern parts of CA, also covering the Caspian Sea (Fig. 7(d)). The synoptic conditions on 5 November presented large similarities with the dust storm day, and this is also shown in the vector wind pattern, while the dust loading was progressively dissipated with lower values (~0.5 to 0.7 g m–2) over southern CA (Fig. 7(e)). MERRA-2 observations show high dust loading over the Tarim Basin and Taklimakan Desert, likely caused by convergence of winds over these desert areas and a significant dust transport from Libya towards south Italy and the Balkans due to strong southerlies. On the next day, 6 November 2021 (Fig. 7(f)), the dust loading over Central Asia was further reduced, while the dust hotspots over Taklimakan, central Mediterranean and the Indo-Gangetic plains intensified. Fig. 8 shows the variation of hourly PM2.5 concentrations from the air quality station located in the US embassy in Tashkent, Uzbekistan from 1 to 10 November 2021. The PM2.5 concentrations are color-coded with the Air Quality Index (AQI) data classified for the six AQI categories (good, satisfactory, moderate, poor, very poor and severe) related to various health clusters for the local population (from good to hazardous). Around 18:00 pm on 4 November 2021, there was a spike in PM2.5 levels caused by the arrival of the severe dust storm originated from southeast Kazakhstan. PM2.5 concentrations raised above 900 µg m–3 during the afternoon hours on 5 November. On 5 and 6 November, the AQI values were categorized in the very unhealthy and hazardous class for any group of population in Tashkent. There was a gap in PM2.5 recordings between 22:00 pm on 4 November and 17:00 pm on 5 November, probably attributable to instrument failure caused by the severe PM concentrations. The daily mean PM2.5 concentrations were 393 µg m–3 (26 times higher than the guideline level of 15 µg m–3 according to WHO), 215 µg m–3 (14 times higher) and 111 µg m–3 (7.5 times higher), on 6, 7 and 8 November, respectively (WHO, 2021). The intense dust haze (caused by particles raised into the atmosphere by a recent dust or sand storm) started dissipating in the evening hours of 6 November. Still, dust particles remained till about 15 November when heavy rain helped to wet deposition of PM. Similarly elevated PM2.5 concentrations during severe dust storms have been reported in other parts of the world (Dumka et al., 2019; Hussein et al., 2020; Wu et al., 2021). In Beijing, China, Wu et al. (2021) reported daily mean PM2.5 concentrations exceeding 200 µg m–3 on 15 March 2021 caused by an intense dust storm originating in Mongolia. In addition, PM2.5 levels were ~109 µg m–3 on 25 July 2018 in Amman, Jordan during a dust storm episode originating in the Sahara Desert (Hussein et al., 2020; Shafiee et al., 2017; Niroomand et al., 2020). Fig. 9 shows the hourly ground-based measurements of horizontal visibility and wind speed during 1–6 November 2021 at three sites in CA (Turkmenabat, Tashkent and Khujand) directly affected by the dust storm. In Turkmenabat, the dust arrived at around 09:00 UTC on 4 November and lasted for approximately 15 hours. During the arrival of the dust storm, visibility dropped drastically from about 10 km to 1 km, accompanied by a notable increase of wind speed from about 4 m s–1 to 10–12 m s–1 during the peak of the dust storm over the site (Fig. 8(a)). The minimum horizontal visibility was recorded at 15:00 UTC with a value of 692 m, when the wind speed was 12.5 m s–1. In Tashkent, horizontal visibility varied considerably on days prior to the dust storm, while the large gaps in visibility were accompanied by weak-to-calm winds (< 1–2 m s–1) that favoured the accumulation of anthropogenic aerosols and pollutants near the ground. This is a characteristic atmospheric condition in urban-polluted environments, where the weak winds and temperature inversions are responsible for trapping aerosols near the ground, which contribute to scattering of solar radiation and visibility degradation (Dumka et al., 2017; Liakakou et al., 2020). However, on 4 November the dramatic decrease in visibility was accompanied by a notable increase in wind speed (6–7 m s–1) signalling the arrival of the dust storm (Fig. 9(b)). As mentioned above, Tashkent was severely affected by this severe dust storm, which reduced visibility below 1000 m at 15:00 UTC and below 200 m between 16:00–18:00 UTC (4 November 2021). Dust aerosols over the city remained for the next 8 days, contributing to the reduced visibility (< 2–3 km; Fig. 9(b)) and the increased PM2.5 concentrations compared to pre dust storm days. In Khujand, the dust plume arrived at 12:00 UTC and immediately caused a reduction in visibility to below 2.5 km. As the dust plume thickened, visibility dropped below 1 km for about 7 hours. At the time of dust arrival, the wind speed in Khujand was 10 m s–1, while the changes in wind speed and visibility due to arrival of the dust storm were mostly similar in all the examined stations. This indicated that the thick dust plume that blanketed these sites was approaching in the form of a dust wall accompanied by strong near-surface winds, resulting in a strong negative correlation between wind speed and horizontal visibility. On the days prior to the dust storm, visibility records were mostly affected by local activities in the cities, while on the days after the dust storm, the visibility remained at general low levels, until atmospheric cleaning. Fig. 10 shows the temperature variation during the first half of November 2021 in Tashkent, Khujand, and Turkmenabat. The data showed that the dust intrusion on 4 November significantly changed the temperature regime in the region. As mentioned above, dust particles remained in the atmosphere for a long time, until heavy rain cleaned the air on 15 November 2021 in Tashkent and Khujand. In Turkmenabat, there was no rain, but horizontal visibility started to increase above 10 km from 14 November 2021, after the removal of dust aerosols. In Turkmenabat, the daytime air temperature decreased on 4 November 2021 compared to 3 November 2021 (before dust event) and 11 November 2021 (after dust event) by –11.8°C and –3.4°C, respectively. However, opposite changes in nighttime temperature occurred by +5.1°C and +10.4°C relative to the days before and after the dust event. A similar situation was observed in Tashkent, where the daytime temperature decreased by –9.8°C and –10.1°C relative to 2 November 2021 and 12 November 2021, while at night there was an increase in temperature by +2.3°C and +2.9°C, respectively. In Khujand, the dust storm on 4 November 2021, caused a notable decrease in daytime air temperature by –8.6°C and –12.5°C with respect to 2 and 13 November 2021. The respective nighttime air temperatures were higher on 4 November by +9.5°C and +8.4°C compared to aforementioned days. It should be noted that apart from the aforementioned temperature amplitudes between the dust day and specific days before and after the dust event, the arrival of the dust storm over each station caused a notable decrease in air temperature (Fig. 10), which is partly attributed to presence of a cold front associated with dust and to radiative impact of dust on solar radiation. Similar temperature changes with the arrival of intense dust storms have been reported at several sites worldwide (Alharbi et al., 2013; Kaskaoutis et al., 2019; Maghrabi et al., 2011; Prakash et al., 2015). Kaskaoutis et al. (2019) reported a considerable decrease in maximum temperature (~8–11°C) due to dust radiative cooling and the passage of a cold front on 5–6 February 2019 compared to 4 February 2019 in Zabol, Iran. The Middle East also experienced a remarkable reduction of −6.7°C in temperature due to the dust radiative cooling during severe dust storms from 18 to 22 March 2012 (Prakash et al., 2015). According to previous studies, mineral dust particles have an important role in global energy balance via both direct (on solar radiation) and indirect (on clouds) effects (Kok et al., 2018, 2017). Generally, when shortwave radiation encounters dust aerosols, cooling happens because some radiation does not reach the Earth’s surface. On the other hand, dust particles can also absorb longwave radiation, emitted by the earth, atmosphere and clouds, and contributes to planetary warming (Kok et al., 2018; Mahowald et al., 2014; Miller et al., 2006; Tegen and Lacis, 1996). To monitor the movement of the dust storm that affected the three receptor sites, the HYSPLIT-4 model was implemented to analyse the transport pathway of dust particles through 3-hour time intervals up to 48 hours before dust episodes reaching the study locations (Fig. 11). The starting point of trajectories was in Turkmenabat on 4/11/2021 at 09:00 UTC, in Tashkent on 4/11/2021 at 11:00 UTC, and in Khujand on 4/11/2021 at 12:00 UTC. The arriving height of the air masses at the receptor sites was set at mid boundary layer height to guarantee both transition and ending of dust trajectories in the boundary layer (Broomandi et al., 2021; Karaca et al., 2009). Turkmenabat, in central Turkmenistan, was hit by the dust plume on 4 November at 09:00 UTC, while the air masses at the altitude of 275 m originated from north/north-eastern directions, i.e., Qaraghandy and Pavlodar in Kazakhstan (Fig. 11(a)), passing over southeast Kazakhstan, where the dust storm was generated (Fig. 2(b)). Similar air mass pathways are observed in Tashkent (Fig. 11(b)), which was upwind of the dusty air masses that hit Turkmenabat. The starting points of the majority of the air masses at 130 m altitude (mid-boundary layer height) were from eastern and central Kazakhstan, and continued to the Almaty region, Jambyl and south Kazakhstan, before reaching Tashkent (Fig. 11(b)). The dusty air masses that hit Khujand travelled over the same regions (Fig. 11(c)), while the results of trajectories simulation were consistent with the SEVIRI Visible/IR imagery (Fig. 3) during the dust intrusion, indicating that air masses were mainly originated from south-western parts of Russia, as well as eastern, central, and southern Kazakhstan. While they were passing over dust sources located in south Kazakhstan, including Kyzylorda and Kyzylkum Deserts, the transport of dust particles was facilitated by the northeast winds toward Turkmenabat, Khujand and Tashkent in the afternoon of 4 November 2021. The 4 November severe dust storm over south-eastern Kazakhstan that affected a large area in CA, was a unique and rare phenomenon, in terms of its intensity, that happened in an area vulnerable to dust emissions and with continuous soil degradation during recent decades due to ongoing human interventions (Aiman et al., 2018; Baubekova et al., 2021; Guney et al., 2021; Kismelyeva et al., 2021; Ramazanova et al., 2021). Apart from the high PM concentrations during dust storms, potentially toxic elements (PTEs) as soil contaminants transported by dust may add more health and ecological concerns over the CA region. Due to the potentially toxic-contaminated soils in arid areas of CA, it is recommended to perform site-specific studies, also examining the chemical composition during intense dust storms. It is also highly recommended to take effective and immediate stabilising measures to control the wind erosion in vulnerable areas. Since sand and dust storm (SDS) activity is an alarming challenge to sustainable development in more than 150 countries that are directly affected by SDS worldwide (Middleton and Kang, 2017), it is necessary to prepare suitable climate adaptation and mitigation strategies, developing more reliable and accurate early warning systems and quantifying the impacts to societal implications in both national and regional scales. A transboundary multi-hazard risk assessment is also essential in analysing the cause-and-effect relationships and helping policymakers to fully understand the required dynamics and complexity of policy actions. Such transboundary dialogue and collaboration between the affected countries lead to policy interventions reflecting the geospatial link among the origins and receptors, which can positively influence both adaption and mitigation aspects. This study investigated a severe dust storm that occurred on 4 November 2021 over Central Asia, a phenomenon unprecedented in this region over the last 150 years (Eurasianet, 2021) that caused an increase of PM10 concentrations above 18,000 µg m–3 in Tashkent, Uzbekistan. Meteorological measurements at selected sites in Central Asia including Turkmenabat in Turkmenistan, Khujand in Tajikistan and Tashkent in Uzbekistan showed that a large part of Central Asia was highly impacted by this unique dust storm, which reduced horizontal visibility to 200–1000 m and daytime temperature by 2–4°C at different time periods. The thick dust plume that blanketed these sites approached in the form of a dust wall accompanied by strong near-surface winds. Favourable meteorological conditions for the formation of an intense dust storm prevailed both in the upper and lower troposphere over Central Asia and more specifically over the eastern Kazakhstan, which was detected by SEVIRI imagery as the main dust-source region. A high-pressure ridge prevailed during the day prior to the dust storm, stretching from the Middle East and Iran to the Caspian Sea and west Russia, creating a typical omega blocking pattern at 500 hPa level, with a large ridge over west Russia and two troughs to its west and east. The axis of the ridge progressively shifted from southeast-to-northwest (1 November) to southwest-northeast on 4 November, resulting in a strong surface air-temperature gradient and invasion of cold air masses associated with the anticyclonic system over Kazakhstan. The intense high-pressure system over CA was a triggering dynamic force for the formation of the dust storm on 4 November 2021, due to strong easterly winds from the southern flanks of the high-pressure system toward the southern part of CA, passing over Aralkum, Moiynkum, Kyzylorda, eastern Kyzylkum, Trans-Unguz, and central Karakum Deserts. On the dust storm day, an intense jet stream with core wind values of about 4 m s–1 was located just above the dust-source region in southeastern Kazakhstan. HYSPLIT air-mass back trajectories at the receptor sites of Turkmenabat, Khujand, and Tashkent were consistent with SEVIRI satellite data regarding the apportionment of the dust intrusions at each site, indicating that the dusty air masses mainly originated from the south-eastern parts of Kazakhstan, including Kyzylorda and Kyzylkum Deserts. The transport of dust plumes was facilitated by the northeast winds toward Turkmenabat, Khujand, and Tashkent in the afternoon of 4 November 2021. Central Asia is considered a highly sensitive area in view of climate change due to projections of precipitation decrease and increased possibility of prolonged droughts. Under such climatic conditions in the future, severe dust storms in the area will inevitably follow an increasing frequency, causing large deterioration to atmospheric environment and major socio-economic issues in the countries of Central Asia. The authors acknowledge the financial support for the NU projects (Nazarbayev Research Fund SOE2017003 & 11022021CRP1512). Kawe | Kaveh M. acknowledges grant support by Iran National Science Foundation (INSF) under post-doctoral project No. 4001142. A.R acknowledges support by Iran National Science Foundation (INSF) under project No 99003984. The authors thank Earth data, NASA, the ECMWF and Copernicus teams for providing the MODIS, MERRA-2 and ERA-5 products used in this work. The authors declare that they have no conflict of interest. Parya Broomandi: Conceptualization, Methodology, Software, Data Curation, Formal Analysis, Validation, Investigation, Visualization, Writing - Original Draft. Kaveh Mohammadpour: Conceptualization, Methodology, Software, Data Curation, Formal Analysis, Validation, Investigation, Visualization, Writing - Original Draft. Dimitris G. Kaskaoutis: Conceptualization, Methodology, Validation, Writing - Review & Editing. Sabur F. Abdullaev: Formal Analysis, Data Curation, Resources. Vladimir A. Maslov: Formal Analysis, Data Curation, Resources. Amirhossein Nikfal: Data Curation, Software. Aram Fathian: Data Curation, Software. Ali Jahanbakhshi: Data Curation, Software. Bakhyt Aubakirova: Data Curation. Jong Ryeol Kim: Funding acquisition, Project administration Resources. Alfrendo Satyanaga: Funding acquisition, Project administration, Resources. Alireza Rashki: Formal Analysis, Visualization. Nick Middleton: Original concept, Supervision, Validation, Writing - Review & Editing.1 INTRODUCTION
Fig. 1. True colour image from the Terra-MODIS sensor (https://worldview.earthdata.nasa.gov) on 4 November 2021, focused on the dust storm.
2 METHODS
2.1 Study RegionFig. 2. Physiographic map of the study area highlighting the Central Asian countries.
2.2 Ground-based Observations
2.3 Reanalysis Data
2.4 Satellite Remote Sensing Observations/Products
2.5 HYSPLIT Model
3 RESULTS AND DISCUSSION
3.1 Satellite Remote Sensing ObservationsFig. 3. SEVIRI satellite images over Central Asia at different hours on 4 November 2021, detecting the evolution of the thick dust plume (in pink/magenta). The key receptor sites of Tashkent in Uzbekistan, Khujand in Tajikistan and Turkmenabat in Turkmenistan are also shown.
3.2 Atmospheric Dynamics during the Dust StormFig. 4. (a–f) Composite maps of geopotential heights at 500 hPa (black contours) and surface temperature (shaded area) from 1 to 6 November 2021.
Fig. 5. (a–f) Composite maps of omega at 300 hPa (shaded area) and zonal wind at 250 hPa (blue contours) from 1 to 6 November 2021.
Fig. 6. (a–f) Composite maps of geopotential heights at 850 hPa (dash black contours) and mean sea-level pressure (MSLP, shaded area) from 1 to 6 November 2021.
Fig. 7. (a–f) Composite maps of dust load (g m–2) and surface vector winds (m s–1) from 1 to 6 November 2021.
3.3 Ground-based Meteorological Observations
PM2.5 concentrations in TashkentFig. 8. Hourly PM2.5 concentrations in Tashkent around the dust storm day (4 November 2021), color-coded with the AQI values.
3.3.1 Changes in horizontal visibility and 10-m wind speedFig. 9. Hourly ground-based measurements of wind speed and horizontal visibility at stations in Central Asia, (a) Turkmenabat, (b) Tashkent and (c) Khujand during 1-6 November 2021.
3.3.2 Variations in surface air-temperatureFig. 10. The hourly ground-based measurements (2-m temperature) for the study stations of (a) Turkmenabat, (b) Tashkent, and (c) Khujand between 1–15 November 2021.
3.4 Backward Trajectory AnalysisFig. 11. Backward trajectory analysis by HYSPLIT model at receptor sites of (a) Turkmenabat, (b) Tashkent, and (c) Khujand on 4 November 2021 (the dust storm day).
3.5 Land Degradation in Central Asia and Future Projections
4 CONCLUSIONS
ACKNOWLEDGMENTS
ADDITIONAL INFORMATION AND DECLARATIONS
Conflict of Interest
Credit Authorship Contribution Statement
REFERENCES