3. Results and Discussions
The EOF analysis applied to the fields of PBLH anomalies highlighted the existence of a small number of dominant modes of variability. The first five EOF modes explain approximately 80% of the total variance of the PBLH field and capture the main physical mechanisms that control the evolution of the PBL in Romania during the warm season.
The analysis focuses on the warm season (May - September, MJJAS) over a 30-year period (1989 - 2022) across Romania. The EOF decomposition was performed on data interpolated onto a regular spatial grid to ensure methodological consistency and to avoid biases associated with irregular spatial sampling.
Only the first five eigenmodes were retained for detailed examination (
Figure 1,
Figure 2,
Figure 3,
Figure 4 and
Figure 5), as they account for the largest fraction of the total variance in the dataset [
18]. These leading modes capture the most significant large-scale structures of variability, while higher-order modes, which explain progressively smaller portions of variance (
Table 1), were not considered further in order to maintain statistical robustness and physical interpretability.
The following EOF modes have the values:
Table 1.
Eigenvalues and explained variance for EOF modes 6 to 10.
Table 1.
Eigenvalues and explained variance for EOF modes 6 to 10.
| EOF Mode |
Daily (Value / Variance %) |
Diurnal (d) (Value/Variance %) |
Nocturnal (n) (Value/Variance %) |
| 6 |
0.9849E+05 / 2.41% |
0.2907E+06 / 2.10% |
0.2399E+05 / 3.40% |
| 7 |
0.8802E+05 / 2.16% |
0.2713E+06 / 1.96% |
0.1523E+05 / 2.16% |
| 8 |
0.7646E+05 / 1.87% |
0.2205E+06 / 1.59% |
0.1349E+05 / 1.91% |
| 9 |
0.6634E+05 / 1.63% |
0.2138E+06 / 1.54% |
0.1190E+05 / 1.68% |
| 10 |
0.5575E+05 / 1.37% |
0.1579E+06 / 1.14% |
0.1579E+06 / 1.30% |
Figure 1.
Spatial patterns (left) and corresponding Principal Component (PC) time series (right) for the first EOF mode. The three panels represent the daily (a), diurnal (b), and nocturnal (c) analysis.
Figure 1.
Spatial patterns (left) and corresponding Principal Component (PC) time series (right) for the first EOF mode. The three panels represent the daily (a), diurnal (b), and nocturnal (c) analysis.
Figure 2.
Spatial patterns (left) and corresponding PC2 time series (right) for the second EOF mode.
Figure 2.
Spatial patterns (left) and corresponding PC2 time series (right) for the second EOF mode.
Figure 3.
Spatial patterns (left) and corresponding PC3 time series (right) for the third EOF mode.
Figure 3.
Spatial patterns (left) and corresponding PC3 time series (right) for the third EOF mode.
Figure 4.
Spatial patterns (left) and corresponding PC4 time series (right) for the fourth EOF mode.
Figure 4.
Spatial patterns (left) and corresponding PC4 time series (right) for the fourth EOF mode.
Figure 5.
Spatial patterns (left) and corresponding PC4 time series (right) for the fourth EOF mode.
Figure 5.
Spatial patterns (left) and corresponding PC4 time series (right) for the fourth EOF mode.
3.1. Analysis of EOF 1: Influence of Large-Scale Atmospheric Circulation (NAO)
The first EOF mode (EOF1) represents the dominant structure of the PBLH variability during the warm season and explains 54.4% of the total variance of the PBLH field (
Figure 1a). The high proportion of explained variance indicates the existence of a large-scale control mechanism that acts relatively uniformly over the entire territory of Romania.
The spatial pattern associated with EOF1 (
Figure 1, left panels) highlights predominantly positive anomalies across the entire territory of the country, with the highest values being located in the extra-Carpathian regions, particularly in Moldavia region (north-east of the country), Oltenia region (south-west of the country between Carpahtians mountains and Danube), and southeastern Romania. The spatial distribution suggests the existence of a coherent response of the boundary layer to modifications in regional and hemispheric atmospheric circulation. The higher sensitivity of the extra-Carpathian regions can be explained by the reduced influence of orographic effects on turbulent mixing processes and by the direct exposure to the dominant atmospheric advections.
The temporal evolution of the principal component associated with EOF1 (PC1) highlights a pronounced variability at interannual and multiannual scales (PC1;
Figure 1, right panels). The predominantly negative values observed in the first part of the analyzed period are followed by a significant increase after the year 2000, with a significant maximum in the years 2000, 2007, and 2022. In contrast, pronounced minima are identified in the years 2005 and 2010, suggesting the existence of important modifications in the atmospheric forcing mechanisms responsible for the development of the boundary layer.
The comparison of the PC1 evolution with the North Atlantic Oscillation (NAO) index highlights a remarkable correspondence between the two time series. The main maxima and minima of PC1 coincide with the positive and negative phases of the NAO, suggesting that the first EOF mode reflects the response of the PBL to modifications in the atmospheric circulation from the North Atlantic sector.
NAO represents the primary mode of atmospheric variability in the North Atlantic region and significantly influences European atmospheric circulation by modifying the intensity and position of the westerly jet stream. During the positive phases of NAO, the westerly circulation is intensified, favoring more stable and drier atmospheric conditions in certain regions of Southeastern Europe.
These conditions lead to an increase in the surface sensible heat flux and to the development of a deeper boundary layer. Conversely, the negative phases of NAO favor increased cyclonic activity and atmospheric instability, which can limit the development of the boundary layer by increasing cloudiness and precipitation [
19].
This interpretation is supported by the behavior observed in the year 2010, when the NAO index recorded its most pronounced negative value across the entire analyzed period. Concurrently, Romania was affected by numerous episodes of heavy precipitation and widespread flooding, particularly in the extra-Carpathian regions. The associated atmospheric conditions favored a reduction in surface heating and restricted the development of the planetary boundary layer, which explains the pronounced negative values of PC1 (
Figure 6).
The separate analysis of the daytime and nighttime components shows that the EOF1 structure is dominated by the daytime contribution, which highlights the determining role of radiative surface heating in controlling PBLH variability. Nevertheless, the nighttime component contributes to the amplification or attenuation of the daily signal during certain periods, indicating that residual mixing processes and the persistence of atmospheric instability can influence the evolution of the boundary layer even after sunset.
Overall, EOF1 represents the signature of the primary control mechanism of PBLH variability in Romania during the warm season and reflects the direct influence of hemispheric-scale atmospheric circulation, represented by the North Atlantic Oscillation, on the development and structure of the planetary boundary layer.
3.2. Analysis of EOF 2: Regional Thermodynamic Forcing
The second EOF mode (EOF2) explains 9.8% of the total variance of the planetary boundary layer height and highlights a distinct regional pattern of variability (
Figure 2a). Unlike EOF1, which reflects the influence of a large-scale control mechanism, EOF2 describes regional contrasts generated by thermodynamic and hydrological processes (
Figure 2, left panels).
The spatial structure of EOF2 exhibits a clear bipolar configuration, characterized by negative anomalies in northeastern Romania, particularly in Moldavia, and positive anomalies in the southwestern part of the country, centered over Oltenia (southweastern Romania). This distribution suggests the existence of regional mechanisms that drive different responses of the boundary layer within these two regions.
The temporal evolution of the associated principal component (PC2) highlights the alternation between periods when the development of the boundary layer is favored in Moldavia and inhibited in Oltenia, and periods when the situation is reversed. Positive values of PC2 are associated with a relative reduction in the PBL height in northeastern Romania and an increase in the southwest, while negative values indicate a more pronounced development of the boundary layer in Moldova (
Figure 2, right panels).
To identify the physical mechanism responsible for this distribution, the total precipitable water (PW) fields were analyzed. The results show that the spatial pattern of EOF2 exhibits a significant correspondence with the regional distribution of atmospheric moisture. Years characterized by precipitable water deficits in northeastern Romania, such as 2003, 2009, and 2014, coincide with negative values of PC2 and the development of a deeper boundary layer in Moldavia.
From a physical perspective, the reduction in atmospheric moisture content favors an increase in the surface sensible heat flux and a decrease in the energy fraction utilized for evapotranspiration. Under these conditions, a higher proportion of the available energy is converted into heating the air near the surface, which leads to the intensification of convective turbulence and to an increase in the boundary layer height.
Conversely, periods characterized by positive anomalies of precipitable water (PW) and frequent convective activity lead to a reduction in radiative surface heating through increased cloudiness and precipitation. These processes limit the development of thermal convection and favor the occurrence of lower values of the boundary layer height. A representative example is the year 2021, when northeastern Romania was characterized by positive anomalies of PW and frequent frontal activity, conditions that contributed to the relative reduction of the PBLH in this region (
Figure 7).
The analysis of the daytime and nighttime components indicates that EOF2 is primarily controlled by daytime processes associated with surface heating and convection development. The high similarity between the daily EOF2 and daytime EOF2 structures confirms that the dominant mechanism is linked to convective processes that reach their maximum intensity during the day.
Nevertheless, the nighttime contribution is not negligible. The nighttime EOF2 explains more than 22% of the variance of the nighttime field and suggests that the effects of convective processes developed during the day can persist into the early hours of the night through the residual layer (
Figure 2c). In situations characterized by persistent atmospheric instability, convective activity can continue after sunset, influencing the structure and evolution of the nighttime boundary layer.
The obtained results indicate that EOF2 captures the response of the PBL to regional variations in the energy and hydrological balance, highlighting the central role of atmospheric moisture distribution and convective activity in controlling PBLH variability during the warm season. Thus, this mode represents the main regional mechanism that modulates the boundary layer's response to local atmospheric and thermodynamic forcings.
A distinct shift is observed during the warm season of 2021 (
Figure 7d), where northeastern Romania experienced higher PW anomalies (increased moisture) due to the passage of multiple frontal systems and enhanced convective activity [
15]. This resulted in a relative decrease in PBL height in the northeast compared to southwestern Romania, where PW amounts were lower. These patterns suggest a strong coupling between regional precipitation anomalies and PBL variability, highlighting the role of thermodynamic and convective processes in modulating boundary layer development during the warm season
3.3. Analysis of EOF 3: Thermal Advection and Heatwave Impact
The third EOF mode (EOF3) explains 7.2% of the total variance of the planetary boundary layer height and highlights the influence of extreme thermal processes on the boundary layer development in Romania (
Figure 3a). Unlike EOF1 and EOF2, which are associated with large-scale atmospheric circulation and regional moisture distribution respectively, EOF3 reflects the response of the PBLH to extreme heating episodes generated by persistent advections of tropical air [
20].
The spatial structure of EOF3 exhibits a bipolar configuration characterized by positive anomalies in southeastern Romania and slightly negative anomalies in the rest of the country. The highest values are identified in Dobrogea (south-east of the country, between Danube and Black Sea) and Muntenia (south of the country), regions that are frequently under the direct influence of tropical air advections originating from North Africa and the eastern basin of the Mediterranean Sea. This distribution suggests the existence of a direct link between the intensity of atmospheric heating and the development of the PBL.
The temporal evolution of the associated principal component (PC3) highlights pronounced negative values in the years 2000, 2007, 2012, and 2015 (
Figure 3, right panels). These years are well known in the climatology of Romania for the high frequency of heatwaves and for the extreme temperatures recorded during the warm season. The analysis of the air temperature fields at 2 m confirms the existence of extensive positive thermal anomalies, which locally exceed 2-3°C relative to the climatological means (
Figure 8a-c).
From a synoptic perspective, these episodes are associated with the development and persistence of the extended subtropical ridge from North Africa toward Southeastern Europe. The atmospheric configuration favors the transport of continental tropical air masses characterized by high temperatures, relatively low humidity, and pronounced stability in the free troposphere. Near the surface, however, the intense heating leads to an increase in the sensible heat flux and to the development of a deep convective layer.
Under these conditions, thermal turbulence becomes significantly more efficient, and the boundary layer height can increase substantially. Because heatwaves simultaneously affect extensive areas of Romania, local spatial variability is reduced, and the signal associated with extreme heating becomes dominant at a regional scale.
The comparative analysis of the daytime and nighttime components indicates that the EOF3 signal is primarily generated by daytime processes associated with intense radiative surface heating (
Figure 3b-c).
Nevertheless, the nighttime contribution is remarkable and explains an important fraction of the total variability. This result suggests that the effects of heatwaves are not limited to the daytime interval but persist during the night as well.
During severe heatwave episodes, nighttime radiative cooling is often reduced, and minimum temperatures remain high. This phenomenon favors the maintenance of a deeper residual layer and delays the stabilization of the lower atmosphere. Consequently, turbulent processes can continue into the early hours of the night, and the boundary layer height remains greater than under normal climatological conditions.
The year 2007 constitutes a representative example of this behavior (
Figure 8a). The succession of heatwaves and the persistence of high temperatures during the night contributed to the amplification of the nighttime component of EOF3. The results suggest that, in such situations, the processes associated with the residual layer and residual atmospheric instability can become comparable in importance to the daytime convective mechanisms.
The positive trend observed after the year 2016 in the evolution of the main component PC3 may indicate modifications in the frequency and intensity of heat episodes at a regional level. Although the analysis of climate trends does not represent the primary objective of the present study, this result is consistent with numerous research works that highlight the increasing frequency of heatwaves in Southeastern Europe over recent decades [
21].
Overall, EOF3 captures the influence of extreme thermal processes on the planetary boundary layer structure and highlights the role of tropical air advections and heatwaves in amplifying its vertical development. The results demonstrate that episodes of extreme temperatures represent one of the important regional mechanisms controlling PBLH variability in Romania during the warm season.
3.4. Analysis of EOF 4: Mixed Layer Humidity and Regional Moisture Budget
The fourth EOF mode (EOF4) explains 5.1% of the total variance of the PBLH and highlights the influence of processes associated with atmospheric moisture distribution and energy exchanges between the terrestrial surface and the atmosphere (
Figure 4a).
The spatial distribution of EOF4 is characterized by an almost monopolar mode, with predominant positive anomalies in southern and southeastern Romania and lower values in the other regions of the country. This configuration suggests the existence of a regional mechanism that simultaneously influences the development of the boundary layer over extensive areas.
In order, to physically interpret this mode, the composite fields of specific humidity at the 1000 hPa level were analyzed (
Figure 9). The results indicate a correspondence between EOF4 variability and the regional distribution of moisture within the lower layers of the atmosphere. However, the relationship between the moisture content and the boundary layer height is not a direct one but rather depends on how the energy available at the surface is partitioned between the sensible heat flux and the latent heat flux.
In years characterized by high moisture, such as 2001, evaporation and evapotranspiration contribute to an increase in the latent heat flux. Concurrently, additional moisture can favor the development of convection and turbulent mixing, especially under conditions of pronounced atmospheric instability [
22,
23]. In such situations, the boundary layer can become deeper due to the intensification of convective processes.
On the other hand, a more humid atmosphere can also favor the development of cloudiness, reducing the solar radiation available at the surface and limiting daytime heating. Consequently, the final effect of moisture on the PBLH depends on the balance between the cooling processes associated with evaporation and the destabilization processes generated by the release of latent heat.
In the case of the year 2001 (
Figure 4, right panels), the specific humidity distribution suggests that the more pronounced development of the boundary layer was associated with a favorable combination between moisture availability and regional convective conditions. In contrast, the year 2017, characterized by lower values of specific humidity, saw vertical mixing processes influenced by a different energetic regime, which led to modifications in the structure and depth of the boundary layer.
The temporal evolution of the main component PC4 indicates that the variability associated with this mode is dominated by the daytime component(
Figure 4b). This result is consistent with the fact that energy exchange processes between the surface and the atmosphere reach their maximum intensity during the day, when solar radiation controls both surface heating and the development of convective turbulence.
Nevertheless, the nighttime EOF4 analysis highlights the fact that the signal associated with moisture persists even after sunset (
Figure 4c). The moisture accumulated within the boundary layer during the day influences the properties of the residual layer and can modify nighttime atmospheric stability, thereby contributing to the maintenance of a portion of the variability observed during the daytime.
The results suggest that EOF4 reflects the coupling processes between the surface and the atmosphere via the regional energetic and hydrological balance. This mode underscores the fact that the variability of the PBL layer is not exclusively controlled by large-scale atmospheric circulation, but also by local and regional mechanisms associated with moisture availability and surface energy exchanges.
3.5. Analysis of EOF 5: Meridional Circulation and Topographic Interaction
The fifth EOF mode (EOF5) explains 3.7% of the total variance of the PBLH and describes a regional component of variability associated with the interaction between meridional circulation and the complex topography of Romania (
Figure 5a).
Although its contribution to the total variance is smaller compared to the preceding EOF modes, its well-defined spatial structure indicates the existence of distinct physical processes that influence the development of the boundary layer at a regional scale.
The spatial pattern of EOF5 exhibits a bipolar configuration characterized by negative anomalies in southern and eastern Romania and positive anomalies in the northern and western regions. This distribution suggests the existence of a regional redistribution mechanism of energy and air mass associated with variations in meridional circulation.
To investigate this mechanism, the composite anomalies of the meridional wind component at the 1000 hPa level were analyzed (
Figure 10 a–i). The results indicate that periods characterized by the intensification of the meridional flow are associated with the development of a deeper boundary layer in certain regions of the country, particularly in southeastern Romania.
From a dynamic perspective, meridional circulation favors the transport of air masses between different latitudes, contributing to the redistribution of heat and moisture within the lower troposphere. The intensification of this transport can modify atmospheric stability and can amplify vertical mixing processes, leading to an increase in the PBLH planetary boundary layer height.
The years 2009, 2017, 2018, 2021, and 2022 are representative examples of this behavior (
Figure 10b,
Figure 10e,
Figure 10f,
Figure 10h, and
Figure 10i). During these periods, a more active meridional circulation favored the development of more intense turbulence and a more efficient vertical exchange between the surface and the free atmosphere. As a result, the boundary layer height presented higher values in the regions directly influenced by these circulation configurations.
In contrast, periods characterized by the weakening of the meridional circulation or by the predominance of less mobile atmospheric regimes were associated with a reduction in vertical mixing and an increase in atmospheric stability. These conditions favor air accumulation within the lower layers and limit the vertical development of the boundary layer. Such situations were identified in the years 2007, 2010, and 2020 (
Figure 10a,
Figure 10c and
Figure 10g).
A particularly important aspect for the interpretation of EOF5 is represented by the role of the Carpathian arc. The Carpathians constitute the main orographic element of the region and exert a major influence on the atmospheric circulation in Romania. Depending on the direction of the dominant flow, it can act both as a barrier and as a channeling mechanism for the circulation [
24].
In situations characterized by intense meridional circulation, orographic effects can amplify air transport along depressional corridors and extra-Carpathian regions, favoring the local development of the boundary layer. Conversely, under conditions dominated by westerly circulation or weakly organized baric fields, the orographic influence can lead to the regional compartmentalization of air masses and to the emergence of significant spatial contrasts in the PBLH.
The analysis of the daytime and nighttime components indicates that the boundary layer's response to modifications in the meridional circulation is not exclusively limited to the daytime interval. In certain situations, such as the year 2002, the nighttime contribution becomes comparable to the daytime one, suggesting that advective transport and dynamic processes can maintain turbulent activity even in the absence of radiative surface heating.
Therefore, EOF5 can be interpreted as an expression of the interaction between the regional atmospheric circulation and the topography of Romania. This mode highlights the fact that the variability of the PBL is the result not only of large-scale atmospheric forcings and regional thermodynamic processes, but also of local dynamic mechanisms generated by the complex configuration of the relief.