1. Introduction
The MENA region is a critical area for developing a better understanding of the factors involved in the generation of large dust events because it is considered a principal source of atmospheric dust and includes nearly every type of known dust source due to its varied landforms [
1,
2]. However, data related to the nature of land surfaces in North Africa and to the conditions that lead to the generation of dust storm events are scarce. Numerical models are considered vital tools for forecasting dust storms. Here, the regional climate model version 4, hereinafter, “RegCM4.4” [
3], was run with different meteorological initial and boundary conditions with two dust schemes.
This study aimed to improve the daily dust forecast over the MENA region by testing different options in the RegCM4.4 model to determine the optimum conditions. For this purpose, four experiments were performed with different criteria, as illustrated later in the following sections.
2. Data and Methodology
2.1. The Dust Model (RegCM4.4)
RegCM4 is a hydrostatic limited area model for a compressible atmosphere and has been used in various studies of dust emission in various regions of the world. Ref. [
4] studied the changes in dust load over some arid regions in India. Ref. [
5] used the RegCM4 model to study the impacts of land use change on dust emission in Kuwait, and ref. [
6] compared the performance of two dust schemes in RegCM4 for Turkey.
Two dust emission schemes were used in the current study; one (Scheme1) is based on studies by [
7,
8,
9], and the other (Scheme2) is based on a study by [
10].
In RegCM4.4, dust mobilization is parameterized as a function of wind speed exceeding a threshold value, surface roughness, minimum friction velocity [
11], and soil moisture [
12], while the horizontal mass flux is parameterized in terms of friction velocity, according to [
13]. The dust particles are divided into four size bins (0.1–1.0 μm, 1.0–2.5 μm, 2.5–5.0 μm, and 5.0–20 μm). The radiative flux estimation follows the NCAR-CCM3 scheme [
14]. Land surface processes are represented by the biosphere–atmosphere transfer scheme “BATS” [
15] (Dickinson et al., 1993). The processes in the planetary boundary layer are parameterized using [
16], and the cumulus convection processes are described by [
17]. The model includes a large-scale, resolvable subgrid explicit moisture scheme (SUBEX) [
18].
The studied domain covered North Africa, South Europe, and the Middle East (10° N–60° N, 25° W–60° E), with a resolution of 45 km and 18 vertical sigma levels, with the model top set at 50 hPa. The studied period was from 5 May 2014 to 31 May 2014, and each day, a forecast was made for the next 4 days, but the analysis was conducted using data from the first 24 h of each run.
2.2. Meteorological Data
In this experiment, we used two different sources for the initial and lateral boundary conditions of the atmospheric variables (geopotential height, temperature, relative humidity, and wind). One was the NCEP global forecast system (GFS) with a resolution of 1 degree, and the other consisted of the reanalysis data of ERA-Intrim, with a resolution of 1.5 degrees; the lateral boundary conditions were updated every 6 h.
2.3. AERONET Data
Version 2 Level 1.5 of AERONET products “
https://aeronet.gsfc.nasa.gov/ (accessed on 26 August 2023)” was used for the model evaluation over twelve stations, as mentioned in
Table 1. The observations were assigned to the nearest hour, and in the case that more than one observation was assigned to the same hour, the average of the measured values was considered. The aerosol optical depth at 550 nm (AOD
550) was calculated using AOD at 440, 675, and 870 nm (hereafter AOD
440, AOD
675, AOD
870), and the Ångström exponent 440-870 (AE_440_870) was determined using the Ångström law, as in Equation (1).
2.4. MODIS Data
The daily means of combined dark target and deep blue aerosol optical depths at 550 nm for land and ocean, calculated by Terra and Aqua MODIS, with a resolution of 1° × 1°, downloaded from “
https://giovanni.gsfc.nasa.gov/giovanni/ (accessed on 26 August 2023)”, were used to compare the AOD values with those forecasted by RegCM4.4. The AOD values obtained with Terra and Aqua MODIS were compared with the simulated AOD values at the hours of 9 and 12 UTC, respectively, since these two hours were the nearest times to that of MODIS determinations.
3. Results and Discussion
3.1. Two Different Datasets of the Meteorological Field
Figure 1 shows a comparison of the DOD values resulting from RegCM4.4 using GFS (red line) and ERA-Interim (green line) and AOD at 550 nm calculated through AERONET measurements using Equation (1) (blue dots), in addition to the Ångström exponent at 440–870 nm (purple dots), indicating the particle size (fine or coarse) at the 12 stations listed in
Table 1 in the same order.
As shown in
Figure 1, the behavior of DOD using GFS and ERA-Interim was not consistent in most cases in the selected stations; however, approximately the same behavior was found at the station of IER_Cinzana during the period of 14–20 May 2014, with different values of DOD; with GFS, DOD exceeded 2, but with ERA-Interim its value was less than 0.5, which was more consistent with the AOD obtained with AERONET. At the station of Izana, DOD resulting from ERA-Interim was near the measured AOD value, whereas at the stations of Cairo_EMA_2, Dakar, El_Farafra, Hada_El-Sham, Saada, and SEDE_BOKER, RegCM4.4 with GFS provided DOD values near the observed ones. Moreover, at Zinder_Airport station, RegCM4.4 using GFS captured high values of DOD on 9 and 21 May 2014, which agreed with the AERONET data and the measured Ångström exponent (AE) (AE_440-870 < 0.5), indicating that the high values of AOD corresponded to dust events. In contrast, RegCM4.4 with ERA resulted in lower values of DOD.
3.2. Two Different Dust Emission Schemes
In this experiment, RegCM4.4 was run using GFS data from two dust emission schemes.
Figure 2 shows the DOD values produced by RegCM4.4 using scheme1 (red line) and scheme2 (green line), the AERONET AOD at 550 nm (blue dots), and the Ångström exponent at 440–870 nm (purple dots). One can notice that the two schemes resulted in the same behavior at all stations but with different values of dust optical depth, as in the stations of Cairo_EMA_2 and El_Farafra on 29 and 31 May 2014, when DOD with scheme1 exceeded 1, whereas DOD with scheme2 was more consistent with AOD from AERONET. In the station of IER_Cinzana, the two schemes resulted in more dust causing high values of DOD exceeding 1.5 in the period of 15–19 May 2014, whereas the AERONET AOD values were ≤0.5. Moreover, the same was observed at the station of Izana on 10–22 May 2014 and at the station of Zinder_Airport on 12–19 May 2014.
3.3. Two Values for the Dust Emission Adjustment Factor
The dust flux is directly proportional to the fraction of erodible surface (E), which is related to the fraction of the uncovered surface according to the presence of roughness elements and the exposure to wind erosion. Ref. [
19] showed that the fraction of erodible surface roughly decreases as a function of the roughness length (Z0) in desert regions. When Z0 is less than 3 × 10
−3 cm, the desert surface can be considered as totally erodible (E = 1), whereas when Z0 exceeds 3 × 10
−3 cm, E can be calculated as a linear function of the logarithm of Z0 according to the equation of [
20]:
In this experiment, the RegCM4.4 model was run using GFS data and scheme1, but with two values of the dust emission adjustment factor (or soil erodibility), i.e., 1 and 0.5.
Figure 3 shows the DOD values obtained with RegCM4.4 assuming the adjustment factor equaled 1 and 0.5, represented in red and green lines, respectively, the AERONET AOD at 550 nm (blue dots), and the Ångström exponent at 440–870 nm (purple dots).
From the previous experiments, one can notice the high values of AOD that exceeded 2 in some cases, in contrast with those provided by AERONET. Therefore, these values could cause a false alarm, forecasting the arrival of a severe dust storm.
The changes in the erodibility factor had an effective influence on the DOD values. Using the erodibility factor of 0.5 resulted in a noticeable decrease in DOD at the stations of Cairo_EMA_2 and El-Farafra in the last days of May, in addition to the stations of IER_Cinzana, Izana, Ouarzazate, and Zinder_Airport in the middle of May.
3.4. Comparison with MODIS/Aqua Measurements
The average AOD values in the whole studied period were calculated using Terra and Aqua MODIS, and then the difference between DOD values obtained with RegCM4.4 at 9 and 12 UTC and the calculated average AOD values of Terra and Aqua MODIS, respectively, was calculated, as shown in
Figure 4 and
Figure 5, respectively. It can be noticed that AOD values resulting from the GFS_1_0.5 experiment (GFS data and scheme1 with erodibility factor = 0.5) for Sahara have low bias compared with those obtained in the other experiments.
4. Conclusions
In this study, different options were chosen to run the RegCM4.4 model to forecast dust emissions over the MENA region. These options included: (1) data from two meteorological fields, i.e., the NCEP-GFS forecast and the ERA-Interim reanalysis, (2) two different dust emission schemes, (3) two values of the soil erodibility factor. These experiments were limited to only one month of daily dust forecast.
The high values of dust optical depth that were obtained posed the most noticeable problem in our forecast. Therefore, by testing different options, we found that changing the erodibility factor value, while using the first dust scheme, caused a significant reduction in AOD at some AERONET stations. Also, the two dust emission schemes resulted in the same behavior at all stations but with different values of dust optical depth.
Finally, it is necessary to perform more experiments using different planetary boundary layer schemes, land surface models, convection schemes, and the radiation schemes available in RegCM4.4 over a long period to improve the forecast of dust emissions using RegCM4.4.
Funding
This research received no external funding.
Data Availability Statement
Data are available in this manuscript, in the mentioned websites.
Acknowledgments
The author thanks the principal investigators and their staff for establishing and maintaining the AERONET sites considered in this investigation. Public access to the Global Forecast System (GFS) forecast meteorological data provided by the National Center for Environmental Prediction (NCEP) and the ERA Interim Reanalysis dataset provided by the European Center for Medium-Range Weather Forecasts (ECMWF) is gratefully acknowledged.
Conflicts of Interest
The author declares no conflicts of interest.
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