From 25 April 2022 to 30 April 2023, observations were conducted on wind direction, wind speed, and sand transport in the blowout of Xilinguole grassland. And an automatic weather station (TZXBF01102W, United States) was established in the blowout observation area. These stations are capable of simultaneously observing conventional meteorological factors such as temperature, wind direction, wind speed, solar radiation, ground temperature, and evaporation. The scanning frequency of the automatic weather station was 2 min, and the recorded data was the average value of the data within 30 min. The monitoring data were obtained from the website (http://cloud.usr.cn/). The observation periods panned 12 months, from 2022 to 2023.

The objective of this study was to examine changes in wind speed and airflow patterns, the structure of wind-blown sand flow, and variations in sand transport rates in the depositional lobes outside the blowout, on the slope of the blowout, and in different deflation basins within the blowout. The aim was to elucidate the dynamics of wind-blown sand in the blowout. To monitor wind direction and speed variations within the blowout, 23 observation points were established at various locations. These points were monitored at heights of 0.1 m, 0.3 m, 0.5 m, 1.0 m, and 2.0 m, with five different wind cup heights installed at each point for wind speed measurements. Additionally, 12 wind direction indicators were positioned at a height of 0.3 m within the blowout and at 0.3 m and 2 m in the reference tower to track wind direction changes. These observation points included positions such as the front of the blowout, the air inlet, the slopes on both sides, the bottom of the blowout, the air outlet, and the depositional lobe behind the blowout (Figure 2). The observation setup mirrored that of the reference tower, positioned 5 m from the blowout inlet. Observations were conducted using three cup anemometer of HOBO S-WSB-M003 model and wind vanes of the HOBO S-WDA-M003 model. All observation instruments were connected using the data collector of the HOBO H21 model, and all instruments were calibrated before the experiment. The wind direction and wind speed observation data are recorded at a 5-s interval, with continuous observations conducted every 30 min. For analysis purposes, the average value of each set of observation data is used. The rate of wind speed acceleration serves as an indicator of wind speed changes at each position within the blowout and is crucial for assessing airflow alterations. In this study, the wind speed acceleration rate was calculated using the formula defined by (Jackson and Hunt (1975): ∆ S = u z − U z U z where, Represents the wind speed acceleration rate, denotes the measured wind speed at height z (m·s⁻¹), and represents the measured wind speed (m·s⁻¹) at the same height of the reference station.

The research utilized a self-made sand accumulation instrument to monitor sand transport at various locations within the blowout. Positioned effectively at 30 cm above ground level, the instrument featured collection tubes measuring 2 cm × 2 cm in cross-section. The collection pipes of each layer of the sand accumulation instrument are kept parallel to the blowout sand surface, and the pipe mouth of the sand accumulation instrument is aligned with the incoming wind direction. Aligned with wind speed points, the sand accumulation observation point corresponded, and the instrument automatically adjusted its orientation to accumulate sand in accordance with wind direction (Figure 2). Observational data were collected based on wind direction and speed stability, along with ground sand conditions. Sand accumulation was conducted three times, spaced 30 min apart. Sand samples were collected, air-dried, and then weighed with a precision of 0.001 g using a balance.

At a height of 2 m above ground level, wind speed and direction changes were monitored at the reference tower (Figure 3). Throughout the observation period, wind conditions remained stable, with speeds predominantly exceeding 6 m·s⁻¹, concentrated mainly between 7 and 9 m·s⁻¹. Wind direction varied between W-NW (270.9°–313.2°), with the prevailing direction originating from WNW (279.1°–300.3°).

Figure 4 shows the composite wind direction at a reference station located 2 m above the ground and the corresponding wind direction changes at different observation points along the blowout, positioned at a height of 0.3 m above the ground. In Figure 4A, it is evident that when the synthesized wind direction of the blowout inflow is basically parallel to the long axis (270.9°≤θ < 281.4°), the measuring point G7 at the west inlet deviates towards the north wall, and the airflow direction at G1 and G8 aligns closely with the long axis of the blowout and moves towards the east outlet direction. When the airflow enters the bottom of the blowout, G11 and G12 erode along the wind direction of the walls on both sides, G4 continues to erode towards the east exit direction, and deviates towards the southeast direction at the position of G6 at the east exit. The composite wind direction at G15, G6, and G16 is W-WNW, while the composite wind direction at observation point G17 in the depositional lobe is WNW. These findings indicate that the airflow undergoes a significant change in wind direction after the blowout. When there is an angle between the synthesized wind direction of the incoming flow and the long axis direction of the blowout (281.4°≤θ < 293.6°), a significant change in airflow direction is observed at the west inlet of the blowout (G7, G1, G8) compared to Figure 4A. Specifically, G7 and G1 are eroded towards the north side wall, while G8 is deflected towards the south side wall. When the airflow reaches the bottom of the blowout, the airflow direction on the north wall G11 contracts inward, while the bottom measuring point G4 continues to deflect towards the north wall. As a result, the airflow blows out parallel to the long axis of the blowout at the east outlet G15, while G6 blows out in a southeast direction. These findings emphasize the influence of the deviation in inflow direction on the wind direction observed at each measuring point within the blowout.

Figure 4C shows the variation inside the blowout in the composite wind direction of the incoming flow (293.6°≤θ < 300.3°). When compared with Figure 4B, it is observed that the wind direction alters in the west inlet G1 and G8. Specifically, the wind direction at G1 changes from WSW to WNW, while at G8 it blows towards the south wall. The wind direction from G7 to G11 extends from the north wall to the inside of the blowout, and at observation points G4 and G6, the airflow direction is parallel to the major axis and blows out from the east outlet. When the angle between the synthesized wind direction of the incoming flow and the major axis is at its maximum, the direction of the airflow inside the blowout changes significantly. Particularly, the angle between the wind direction at the observation point G8, situated at the west inlet, and the south wall is at its maximum, resulting in airflow blowing out from the south wall. The airflow direction at G1-G4-G6 is WNW, while G11 and G12 experience airflow towards the southeast wall. During variations in the incoming wind direction (270.9°≤θ < 313.2°), the composite airflow direction at the depositional lobe (G17) is W-WNW and consistent with the trend of the incoming wind direction.

Figure 5 illustrates the change in wind speed acceleration rate at each measuring point along the longitudinal section of the blowout. Concurrently, the wind direction and speed at control observation points outside the blowout are synchronously observed. At the control observation points located at 0.1 m, 0.3 m, 0.5 m, 1 m, and 2 m, the wind speeds are measured at 2.59 m s⁻¹, 4.80 m s⁻¹, 4.85 m s⁻¹, 6.44 m s⁻¹, and 7.50 m s⁻¹, respectively. The synthetic wind direction of the wind flow into the blowout is 294.7°. On the vertical section of the blowout, Figures 5A–C) depict the changes in wind speed on the north wall, the central axis section, and the south wall of the blowout, respectively. On the central axis section (Figure 5B), the wind speed increases rapidly by 27%–54% at each height when the airflow enters from the west entrance (G1) of the blowout. As the airflow enters the front bottom section (G2) of the blowout, the wind speed at heights of 0.1 m and 0.3 m near the surface increases by 11% and 5% respectively, while the wind speed at other heights gradually decreases. When the airflow enters the bottom of the blowout (G3, G4), the wind speed gradually decreases, with the maximum wind speed at 2 m decreasing by 29%. Until the airflow reaches the eastern outlet of the rear section of the blowout (G5, G6), the wind speed gradually increases. In the depositional lobe, the wind speed increases rapidly from the edge of the blowout to the top of the depositional lobe (G17). The wind speed at 0.1 m near the surface increases by 58%, and the wind speed decreases rapidly at the upper section of the leeward slope (G18) in the depositional lobe, before increasing again after the leeward slope. From measuring point G1 in the deflation basin of the blowout to measuring point G19 in the depositional lobe of the blowout, the airflow exhibits a pattern of initially increasing, then decreasing, and then increasing again. Across the deflation basin to the depositional lobe, the changes in height at each observation point indicate that the closer the measuring point is to the surface wind speed, the more pronounced the change, with the lowest wind speed acceleration rate occurring at the bottom of the blowout (G3, G4).

The airflow along the north and south walls in the longitudinal section of the blowout (Figures 5A, C) was directed from west to east. Wind speed acceleration in the deflation basin of the north wall gradually increased, reaching its peak at the eastern exit of the blowout (G15). Conversely, in the deflation basin of the south wall, wind speed acceleration initially increased, then decreased, with the highest rate occurring in the middle of the blowout (G12). In the depositional lobe, the height of each measuring point on the north wall exhibited a pattern of initial decrease followed by an increase. Conversely, the variation in height for each measuring point on the south wall was opposite to that of the north wall. Apart from the measuring points on the leeward slope (G22 and G23) in the depositional lobe of the blowout, there was a noticeable correlation between the observation height of the north and south walls and the magnitude of wind speed change.

To better comprehend the relationship between sand concentration and height at various locations of blowouts, a histogram was constructed depicting the relationship between cumulative sediment transport rate and height. Analysis of Figure 6 reveals that sand flow migration primarily occurs near the surface across different positions of the blowout. Across varied wind directions and speeds, over 90% of sediment transport takes place within the 0–25 cm height range. Noticeable disparities exist in the vertical sand flow structure at distinct observation points of the blowout. Figures 6A–C illustrates the sand transport height at the north (G7), middle (G2), and south (G8) observation points on the cross-section at the western entrance of the blowout. Across the three wind directions and speeds, more than 50% of sediment transport occurs within the 0–5 cm height range, while over 75% of sediment transport at G7 and G8 transpires within the 0–10 cm height range. Additionally, more than 90% of sediment transport falls within the 0–15 cm height range, and over 95% within the 0–20 cm height range. Notably, over 75% of sand transport height at G2 lies within the 0–15 cm range, with over 90% and 95% of sand transport height occurring within the 0–25 cm and 0–30 cm ranges respectively. As wind speed increases, sand transport height also rises, with the total sand transport height at G2 surpassing that of G7 and G8. At the three observation points of the eastern outlet of the blowout (G15, G6, G16), more than 50% of sand transport height at the southern section (G16) falls within the 0–5 cm range, while over 75%, 90%, and 95% fall within the 0–10 cm, 0–15 cm, and 0–25 cm ranges respectively. The total sand transport range of G16 is lower than that of G15, and G15 is lower than G6.

At observation point G17, situated on the central axis section atop the blowout (Figures 6G–I), more than 75% of sand transport occurs within the height range of 0–10 cm, with over 95% within 0–20 cm. The total sediment transport height at the north and south sections (G20, G21) exceeds that at the central axis point (G17). Similarly, on the leeward slope of the depositional lobe (G22, G18, G23), the total sediment transport height at the central axis point is lower than that at the north and south points, with the north section slightly lower than the south. In summary, the total sediment transport height at the north and south sections of the west entrance (G7, G2, G8) and the east exit (G15, G6, G16) of the blowout is lower than at the central axis section. Conversely, the total sediment transport height at the north and south sections atop the depositional lobe (G20, G17, G21) and on its leeward slope (G22, G18, G23) surpasses that of the central axis section. Additionally, sediment transport height at different measuring points increases with wind speed.

The sediment transport rate per unit width refers to the amount of sediment transported per unit width perpendicular to the wind direction within a specific time frame. Figures 7D–F depict the sediment transport rate alongside the corresponding wind speed along the longitudinal axis of the blowout, specifically within 0.3 m of height near the surface. Figures 7A–C illustrate the changes in wind direction at the control measuring point during three observation periods. Throughout these observation periods, in Observation 1 (Figure 7A), the primary wind direction is WNW with wind speeds ranging from 4 to 10 m s⁻¹, with over 45% of the winds clocking in at 6–8 m s⁻¹. In Observation 2 (Figure 7B), the prevailing wind direction shifts slightly to W-WNW, with wind speeds ranging from 4 to 8 m s⁻¹, and nearly 30% of the time, the wind speed falls within the range of 4–6 m s⁻¹. During Observation 3, the dominant wind direction is W, with wind speeds concentrated between 2 and 6 m s⁻¹. Across these observations, the trend in wind speed and sediment transport rate fluctuates, initially decreasing, then increasing, and finally decreasing again from the west entrance to the east exit of the blowout. The peak values for wind speed and sediment transport rate occur in Observation 1, as depicted in Figure 7D, whereas the trough values are observed in Observation 3, illustrated in Figure 7F. In both Observation one and Observation 2, the lowest sediment transport rate is observed at the bottom of the blowout (G4) within the deflation basin, while the highest rate occurs at the top of the dune (G17) in the sand accumulation zone, aligning with changes in wind speed. However, in Observation 3, although the lowest sediment transport rate still appears at the bottom of the blowout (G4) within the wind deflation basin, the lowest wind speed occurs at point (G3). Furthermore, across the three observations, the greater the wind speed at the west entrance (G1) of the blowout deflation basin, the larger the disparity in sand transport rate between the east exit of the deflation basin (G6) and the top of the depositional lobe (G17).

Figure 8 illustrates the variations in wind speed and sand transport rate across two selected cross sections within the blowout deflation basin and the depositional lobe. In the deflation basin (Figures 8A–F), the lowest sand transport rates are observed at positions G2 and G6. Along the cross section, the sand transport rate is higher on the north and south walls compared to the central axis section. At measurement points G7, G2, and G8, the sand transport rate correlates closely with wind speed. However, at measurement points G15, G6, and G16, the sand transport rate on the north wall significantly exceeds that on the south wall, desblowoute insignificant changes in wind speed. In the depositional lobe (Figures 8G–1), the pattern of sediment transport rate variation is opposite to that observed in the deflation basin. The highest sediment transport rate occurs in the central axis section (G17), while the sediment transport rates on the north and south sides of the dune top (G20, G21) are notably lower than those in the central axis section (G17). On the cross section of the leeward slope of the dune, apart from observation 1 (Figure 8J) at G18, where the sediment transport rate is significantly higher than at G22 and G23, the variations in sediment transport rate are similar across the other two observations.

Based on the results depicted in Fig.7and8, the variation in sediment transport rate and wind speed is evident in both longitudinal and cross-sectional analyses. It is observed that the change in sediment transport rate aligns closely with fluctuations in wind speed, particularly from the blowout deflation basin to the sand accumulation zone. The airflow gradually intensifies from the western to the eastern directions along both the southern and northern walls, reaching its peak at the hill’s summit before diminishing. This pattern mirrors the observed changes in the horizontal airflow field as outlined in the longitudinal section analysis. Furthermore, the sediment transport rate is notably higher on the north and south peripheries of the deflation basin compared to the central axis section. Conversely, in the depositional lobe, the sediment transport rate is lower on the north and south sides than on the central axis section.

The airflow observation results reveal that the interaction between wind from various directions and the terrain induces substantial alterations in the airflow structure within the blowout, consequently impacting the distribution of wind speed within it. In the entire blowout airflow study (Figure 4), we observed that the clearest rotation of wind direction occurred at point G1 on the central axis when the airflow entered from the west entrance of the blowout. This can be attributed to the topographical characteristics of the area. The slope, on the windward side, which does not enter the blowout, is relatively gentle, while the slope at the west entrance is leeward and the entrance itself is narrow. The airflow is affected by the terrain and slope, with the northwest wall having a higher terrain. Therefore, when the incoming airflow aligns closely with the west wind, the deviation in wind direction at point G1 is minimal. Conversely, when the incoming airflow aligns with the northwest wind, the deviation in airflow direction is more pronounced. Notably, the direction of airflow is also greatly influenced by the direction of incoming flow, especially the angle between the incoming flow direction and the long axis of the blowout. This angle directly affects the airflow direction inside the blowout, causing significant changes in the direction of observation points on the north and south walls. When the angle between the incoming wind direction and the major axis is close to parallel (Figure 4A), the airflow on both sides of the walls cascades in parallel and diffuses towards the east exit. However, when the angle between the incoming wind direction and the major axis is less than 15° (Figure 4B), the airflow direction of the west inlet on the north and south walls first blows along the slopes on both sides, and then the airflow direction on the north wall deflects inward. The north wall is influenced not only by the incoming flow direction but also by its leeward slope. The most significant expansion of the blowout terrain occurs at measurement point G11 on the north wall. Moreover, when the angle between the incoming flow direction and the major axis is greater than 15° (Figures 4C, D), the G8 point on the south wall deviates from its typical direction along the slope towards the south wall, and the terrain on the south wall is lower than that on the north wall. The airflow blows out at the G8 point.

Along the longitudinal axis of the blowout, the near-surface wind speed change curve exhibits consistency with the terrain alteration trend, as depicted in Figure 5. As the airflow approaches the western edge of the erosion blowout, it undergoes acceleration, followed by rapid expansion and deceleration upon entering the blowout’s bottom. Subsequently, the airflow accelerates towards the east along the bottom and the north and south walls of the erosion blowout, as shown in Figure 5A, C, in agreement with the findings of Hugenholtz and Wolfe (Hugenholtz and Wolfe, 2006). Upon ascending from the rear section of the erosion blowout to the windward surface of the dune within the depositional lobe, the airflow experiences compression and acceleration due to the abrupt elevation change in terrain, resulting in maximum wind speed atop the dune. Upon traversing the dune’s summit, the airflow disperses and decelerates along the leeward slope, influenced by terrain and vegetation. This cyclic process perpetuates, leading to varying degrees of wind erosion expansion on both sides of the erosion blowout. The rear section of the erosion blowout extends continuously eastward, and the dunes within the depositional lobe migrate in the same direction. Consequently, the grassland on the plateau becomes buried beneath the advancing dunes. On both the north and south sides of the wall (Figures 5A, C), the wind speed acceleration rate at the same measuring point in the erosion blowout and depositional lobe increases with the observation height, while the wind speed acceleration rate in the two areas on the central axis section of the blowout decreases with observation height. This discrepancy arises due to the differing topographies of the central axis section compared to the north and south side walls. The airflow undergoes acceleration, deceleration, reacceleration, redeceleration, and recovery as it enters from the blowout entrance. Closer to the surface, the influence of wind speed acceleration rate becomes more pronounced.

The interaction between airflow and terrain is the main factor affecting the structure of wind-driven sand flow observed in blowout areas. Observation 1 (Figure 6A)exhibits the lowest wind speed, while observation 3 (Figure 6C) registers the highest. It is evident that higher wind speeds correspond to greater cumulative sediment transport heights. The total sediment transport height on the north and south sides of the western entrance (G7, G2, G8) and the eastern exit (G15, G6, G16) of the blowout is lower than that of the central axis section. This phenomenon can be attributed to the significant slope of the terrain, particularly at the central axis position of the west inlet and east outlet. The fast uplift of the airflow further contributes to the substantial amplitude of sand particle lift and the resulting high sediment transport height. Conversely, the total sediment transport height on the north and south sides of the top of the depositional lobe (G20, G17, G21) and the leeward slope of the depositional lobe (G22, G18, G23) surpasses that of the central axis section, contrary to the sediment transport rate of the blowout cross section. Due to greater sediment transport within 0–10 cm near the surface on both sides of the erosion blowout compared to the central axis, when the total sediment transport in the central axis reaches 95%, its total sediment transport height consistently exceeds that on both sides of the blowout. In the depositional lobe, 75% of sediment transport at the top of the dune (G17) occurs within a height of 10 cm, while the sediment transport height of G20 and G21 falls within the range of 0–15 cm, which is also related to the topography of depositional lobe shaped sand dunes.

During the observation of sediment transport rate, it is crucial to consider the accumulation of sediment in the depositional lobe, which primarily originates from the deflation basin. The variations in sediment transport rate are influenced by factors such as airflow direction, wind speed, vegetation coverage, and terrain. The wind speed in observation one is the highest with a wide range, while the wind speed in observation two is the second highest, and the wind speed in observation three is the smallest but more concentrated (Figures 7A–C). At each observation point in the deflation basin of the blowout and the depositional lobe behind the blowout, the variation trend of the sand transport rate and wind speed observed simultaneously is roughly the same. This indicates that when the incoming wind direction is W-WNW, wind speed becomes the primary factor affecting sediment transport in the blowout. Across the three observations, it is noticeable that the highest values of sand transport rate and wind speed occur at the top of the dune in the depositional lobe behind the blowout (G17). The wind speed at the dune’s apex is the fastest and most stable, consistent with the findings of Smyth et al. (2014). The more stable the wind speed at the blowout, the greater the sand transport rate. After a blowout event, the sand material on the top of the depositional lobe becomes highly mobile and devoid of vegetation coverage. However, on the leeward slope of the depositional lobe, the sand transport rate of G18 and G19 is lower than that of G17. In addition to airflow reasons, the sand material in the depositional lobe is covered by vegetation. At the measuring points G18 and G19, the sand dune thickness is lower and vegetation coverage is higher. Vegetation intercepts the sand material, resulting in a decrease in the sand transport rate. In the longitudinal section of the blowout (Figures 7D–F), the sediment transport rate aligns with the synchronous change in wind speed observed. In both the depositional lobe (Figures 8G–1) and deflation basin (Figures 8A–C) of the blowout’s cross-section, the sediment transport rate mirrors the trend in wind speed during the same time period. However, at the measuring point position of the cross-section in the deflation basin (Figures 8D–F), the sediment transport rate of the three observations does not consistently correspond with the change in wind speed. This disparity is attributed to factors beyond airflow influencing sediment transport rate. The sediment transport rate is not only affected by air flow and vegetation coverage, but also by terrain. Especially, in the deflation basin, the different heights and slopes of the two walls, as well as the differences in terrain between the two walls and the bottom, play a significant role. In previous studies of coastal blowouts (Hart et al., 2012; Halls and Bennett, 2012; Hernández-Cordero et al., 2015), the maximum sediment transport rate is typically found at the base of dunes and erosion blowouts in the depositional lobe. However, in this study, the sediment transport rate at the bottom of the erosion blowout is lower than that on the north and south sides, while the sediment transport rate at the top of the sand dune in the depositional lobe is higher than on the leeward side of the dune. This difference arises from the location of the blowout in a sandy grassland area, distinct from the coastal blowout’s geographical environment. Eddy currents form on both sides of the blowout as a result of the slope and vegetation cover. In the deflation basin, the sediment transport rate on the north side wall is basically higher than that on the south side wall. This discrepancy can be attributed to the steeper slope and higher elevation of the north-facing wall, resulting in a larger supply of sand material from this side. Additionally, the north-facing wall experiences higher wind speeds, further contributing to the variance in sediment transport rates between the two walls. Consequently, the sediment transport rate on both sides of the wall exceeds that at the bottom of the blowout. Moreover, the grassland on the leeward side of the depositional lobe remains uneroded with high vegetation coverage, creating turbulence to disperse and decelerate airflow. Hence, the sand transport rate on the leeward side of the depositional lobe is lower than at the dune’s peak.

Throughout the entire blowout process, the simultaneous occurrence and interplay of airflow and sediment transport are evident. This interaction between airflow and sediment transport plays a significant role in shaping the blowout When the airflow enters from the west end of the blowout, it accelerates and spreads towards three parts: the north and south walls, and the bottom of the central axis. Then, the wind speed weakens at the bottom of the blowout, and gradually increases. The wind speed accelerates and rushes out at the east exit of the transition between the deflation basin and the depositional lobe, reaching its maximum at the top of the depositional lobe. In a deflation basin, the wind speed and sediment transport on both sides of the wall are greater than those on the central axis section, while the wind speed and sediment transport on the north wall are greater than those on the south wall. Under continuous wind erosion, the bottom of the blowout continues to deepen, resulting in uneven development of the north and south walls. The composite wind direction at the eastern exit of the deflation basin is predominantly W-WNW, which drives the depositional lobe to develop toward southeast. The rapid increase in airflow at the eastern exit also contributes to the eastward extension of the sand dunes within the depositional lobe. Within the depositional lobe, airflow tends to veer towards the southeast, and the sediment transport rate is higher on the south side near the sand dune than on the north side. Consequently, this disparity in sediment transport rates leads to differences in the width of the sand dunes between the north and south sections of the depositional lobe.