The focus of the current paper is to explore the influence of meteorological variables on atmospheric CO2 and CH4 mean annual cycles at a rural site. Four variables were investigated: boundary layer height, recirculation factor, trajectory direction, and wind speed modelled at the altitude of the site. Boundary layer height and wind speed were provided by the METeorological data EXplorer (METEX) model. Recirculation factor and trajectory direction were obtained from calculations based on this trajectory model, and a nonparametric procedure was used to obtain a smooth evolution. The main results are higher concentrations obtained during the night, attributed to lower dispersion in this period. The smoothed values of the boundary layer height reached nearly 1200 m AGL during the day in August, and its low values caused high concentrations in spring. During the night, the recirculation factor and wind speed showed a sharp contrast between summer and winter. The average recirculation factor was low, 0.10, and average wind speed was 5.1 m·s−1. Trajectories were directionally distributed in four quadrants. Different tests were performed by selecting values of meteorological variables above or below certain thresholds. The influence of these variables reached values around 6.3 and 0.023 ppm for CO2 and CH4 average concentrations, respectively, during the day when the boundary layer was below 400 m. The main conclusion of this study is that the influence of meteorological variables should not be ignored. In particular, extremely low boundary layer heights may have noticeable effects on both gases.

1. Introduction

CO2 and CH4 are directly linked to climate change, are considered as trace gases in unpolluted environments, and are produced by natural sources at these sites. The contribution of water bodies to these gases is the target of intensive current research [1, 2]. In addition to emissions, their concentrations in the low atmosphere are determined by transport from sources such as populated regions [3], sinks such as vegetation, and soils [4], as well as dispersion in the low atmosphere.

The current paper focuses on the annual evolution of CO2 and CH4 measured in Valladolid (Spain), in southwestern Europe, a continent where research on said behaviour in both gases remains scarce [5]. Since the site is located in a rural area, anthropogenic influence is considered to be limited, allowing us to analyse the influence of certain atmospheric variables (boundary layer height, recirculation factor, air mass trajectory, and wind speed) on the concentrations of the two gases.

One key feature is that previous studies have investigated the daily cycle [6, 7]. Once this evolution is known, the current analysis considers the annual cycle. Different analyses reveal that it strongly depends on the site. This annual cycle is affected by a variety of parameters, the specific contribution of each proving rather difficult to distinguish.

When investigating the annual evolution, additional problems are the fast oscillations that hide this cycle. These oscillations may extend over several days and are produced by fronts that sweep the measurement site or the evolution of weather systems. One procedure which can be applied in order to minimize their impact is to use a polynomial fit [8]. However, the main disadvantage of this method is the gap which appears at the edge of the cycle. In the context of the present analysis, fast oscillations are filtered using a kernel function which, moreover, avoids this concentration gap. Another issue to be addressed in the analysis is the noticeable contribution of vegetation (photosynthesis uptake in the daytime and respiration at nighttime) to CO2, which suggests that the annual cycle should be split into daytime and nighttime periods.

Air parcel trajectory models are useful tools to investigate the influence of large-scale atmospheric circulation, not only on chemicals but also on local-scale meteorological processes or even living beings [9]. Moreover, trajectory analysis provides information concerning the contribution of local-scale processes with respect to long-range transport [10].

In the current paper, an air trajectory model is used for a twofold purpose. First, the model’s outputs are exploited to compute the locations of the air parcel travelling to the measurement site. These locations allow the trajectory direction and air recirculation to be calculated, a topic thus far scarcely investigated. Second, the air trajectory model provides meteorological variables, such as the boundary layer height and wind speed, which are not measured at the site.

The boundary layer height depends on thermodynamic and dynamic mechanisms, in addition to the latitude of the site [11]. The relationship between pollutant concentration and this variable has occasionally been considered. Lai [12] studied air quality in Banqiao, Taiwan, together with different meteorological variables and observed that the boundary layer height was nearly 400 m lower at PM2.5 events than at low PM2.5 level days. Moreover, low boundary layer height at night led to relatively high polycyclic aromatic hydrocarbon concentrations in Guangzhou City, South China [13]. By contrast, the daily evolution of the boundary layer may be inhibited by intensive transport in the upper levels, as observed in the southwestern Iberian Peninsula during intrusions of Saharan dust, where the dust was confined between 1500 and 5500 m [14].

One section of this paper is devoted to the relationship between CO2 and CH4 and the boundary layer height. Pérez et al. [15] analysed CO2 dilution rates in the atmospheric layer close to the surface by means of temperature and wind speed profiles measured with a sodar equipped with a radio-acoustic sounding system (RASS). The range reached by this device was very limited, and the current paper expands this analysis.

Another noticeable topic scarcely investigated to date is air mass recirculation. Coastal areas are suitable sites to analyse the relationship between recirculation and land-sea breeze. Levy et al. [16] considered seven sites in Israel during the period 2000–2004 and proposed a procedure to differentiate between synoptic scale, mesoscale, and local scales based on the mean and standard deviation of wind recirculation between sites. Surkova [17] used different stations on the northern coast of the Black Sea and concluded that recirculation is active in the least ventilated areas where wind speed was low. Breeze circulation was enhanced by relief, which was also responsible for the low impact of the large-scale atmospheric flow. Moreover, the author presented three periods of long-term changes in recirculation between 1900 and 2000, the most rapid increase occurring in the final quarter of the century. However, Papanastasiou and Melas [18] investigated sea breeze in the Volos area, Greece, and concluded that recirculation is not a specific factor of sea breeze days.

The relationship between recirculation and concentration has occasionally been studied. Pérez et al. [19] considered the critical values suggested by Allwine and Whiteman [20] for the wind run and the recirculation factor and found that CO2 concentration for recirculation was intermediate between concentration for ventilation and stagnation. Pérez et al. [21] calculated one trajectory each night from 20 to 5.30 GMT reaching the same site as the current paper, with CO2 concentration at 6 GMT being attributed to each trajectory. 200 back trajectories were considered to show two sources of noticeable impact: the first being the influence of recirculation in distances below 100 km and the second, the city of Valladolid. Pérez et al. [22] analysed the recirculation factor in the period 2004–2011 on the east coast of Gran Canaria Island, around 250 km from NW Africa, and concluded that high values showed an annual pattern, reaching their maximum in winter. Air pollutant accumulation and marked impact on air quality were favoured during these events. However, Karagiannidis et al. [23] did not find any successful relationship between the air quality described by the concentration of different pollutants and several meteorological parameters, in particular the recirculation factor, for winter and summer at two measuring stations in Patras, Greece, for the period 2008–2011. Another section of the current paper analyses the influence of recirculation on the CO2 and CH4 concentrations measured.

Directional analyses have proved useful for identifying pollution sources. Pérez et al. [24] obtained the histogram for CO2 concentrations above the 95th percentile to determine sources affecting the measurement site. Ashbaugh et al. [25] used conditional probability to determine the location of major pollutant sources. This probability was calculated by the relationship between the number of observations above a specific concentration, called the truncation level, and the total number of observations, both in a single wind sector. This procedure was used by Pérez et al. [26] to gain insights into CO2 concentration persistence. Finally, Donnelly et al. [27] used a directional analysis to investigate the influence of air masses on NO2 concentration at three sites in Ireland. Exploring the relationship between trajectory direction and concentrations of CO2 and CH4 is a further objective of the current paper.

Finally, the relationship between these concentrations and wind speed has scarcely been addressed to date. One example is the analysis by García et al. [28], which presented the relationship between CO2 and wind speed on semihourly means over a one-and-a-half-year period using an exponential function. The rest of this study considers the response of the annual cycle of both trace gases to changes in wind speed.

2. Materials and Methods

2.1. Experimental Description

CO2 and CH4 dry concentration was measured with a Picarro G1301 located at the Low Atmosphere Research Centre (CIBA) (41°48′50.25″N, 4°55′58.56″W; 850 m ASL) in Valladolid, Spain. The site is flat and surrounded by nonirrigated crops, with grass being the main vegetation. Commencing on 15 October 2010, the measuring campaign lasted three years. A noticeable gap in available observations was present in August 2013. This analyser was equipped with a valve sequencer to obtain measurements at three levels: 1.8, 3.7, and 8.3 m, although only the latter was used in this study. Observations lasted 10 min at each level. Around 30 values were sampled per minute, and the first 20 observations were discarded to avoid discontinuities when the level changed.

Calibrations were made every two weeks using three NOAA standards [29], and the concentration was corrected slightly using linear equations calculated from the calibrations.

Air mass trajectories and meteorological variables one-day prior to the arrival at the measuring site were provided by the METEX model [30]. The main features are its flexibility and ease-of-use. Calculations were made with a web-based version. Input requirements were date, interval between initializations, trajectory length, coordinates, and altitude of the site where the trajectory begins or ends, trajectory type (forward or backward), and model type. The kinematic model, selected in this paper, considers the trajectory dominated by the wind velocity components. However, the isentropic model employs an air parcel moving on isentropic surfaces.

Each trajectory’s coordinates were supplied by the model on an hourly basis together with certain meteorological variables, such as potential temperature and pressure although the present study only considers the boundary layer height and wind speed. Hourly averages of concentrations were calculated so as to combine them with variables provided by this model.

The Normalized Difference Vegetation Index (NDVI) was obtained from the MODIS on the TERRA satellite and downloaded from EOSDIS Reverb [31]. Each image corresponded to the MOD13 product, with a 16-day period, for the tile with coordinates h17v04. Values were extracted using the Windows Image Manager and Digital Array Viewer programs for the whole image. Software developed by the authors was used to extract the values for the measurement site and to check the quality control, which is available in the file.

Sunrise and sunset were obtained from the National Geographic Institute [32] for Valladolid (41°39′N, 4°43′W), a city located some 25 km SE of the measuring site.

2.2. Kernel Smoothing

When time or directional observations are handled, oscillations may hide the behaviour of the variable investigated. A moving average is the simplest procedure to filter these oscillations. However, this method poses two main drawbacks: the first is that only a small fraction of observations is involved in calculations, and the second is that the measurements averaged have the same weight. The Kernel smoothing method is a nonparametric procedure that calculates mean values by taking into account the proximity of neighbouring observations.

Average concentration, C, was calculated for each day of the year, t, by means of the following function described by Henry et al. [33] and Donnelly et al. [27]:where Ci is the concentration measured at time ti and h is the window width. Although Silverman [34] proposed a method to obtain this window width, the behaviour of the resulting function for different widths is the best selection procedure. Small values of h are sensitive to short-time fluctuations, whilst large values determine smoothed concentrations. A value of 20 days was used in this paper to retain the essential features of the annual cycle. The Gaussian kernel K is defined aswhere in equation (1).

Equation (1) was used to smooth global concentrations at noon for variables considered during the day, such as the boundary layer height. It was also used at midnight to obtain values of variables at night, such as wind speed.

2.3. Recirculation Factor

Allwine and Whiteman [20] defined this factor for each 24-hour backward air mass trajectory by

Its calculation is illustrated with Figure 1. L is the resulting transport distance, the distance between the beginning (24 h) and the end (0 h) of the trajectory, and S is the wind run, the addition of the distances between pairs of consecutive trajectory points:

L and Si may be calculated by the Sinnott equation [35]:where c is the distance between points and , with λ being the longitude and φ being the latitude.

The recirculation factor is calculated for each trajectory, and values obtained during the night were selected for this study.

2.4. Calculation of the Trajectory Direction

Directional calculations aim to determine the source of the concentrations recorded [24]. However, directions obtained at the measurement site may be affected by local flows. An air parcel trajectory may be slightly affected by local features, and its direction is more robust than that obtained at the measurement site.

The centroid of each trajectory was calculated by the mean of the trajectory points coordinates. Its direction, d, from the measuring site was then obtained by the law of cosines [35]:where cC is the distance between the trajectory centroid and the measurement site, with angles being measured in degrees.

3. Results

3.1. Characteristics of the Diurnal Cycle

Figure 2 presents the annual evolution of both trace gases, and Table 1 presents their corresponding average concentrations calculated from values provided by equation (1) together with their availabilities. The concentration during the day was lower than values observed during the night for both trace gases due to the low dispersion in this period. Noticeable discrepancies between day and night were observed for CO2 concentration from March to early July, attributed to intense vegetation development, described by the NDVI evolution whose smoothed curve was obtained by applying the Kernel smoothing methodology to the NDVI data provided each 16 days. According to Table 2, values above 0.4 correspond to abundant vegetation. The greatest difference was observed in early May, extending up to about 13 ppm between day and night. CH4 displayed less contrasting behaviour with day-night differences below 0.010 ppm most of the year. This behaviour was in agreement with the daily cycle presented by García et al. [37] for the same site and two years of measurements.

Regarding the annual evolution, minima were reached in summer for both trace gases. A marked evolution was observed for CO2 during the night, with a range of 16 ppm between a maximum in early May and a minimum in late August. Consequently, the annual evolution may be divided into two unequal periods: one with a fast decrease in concentration and the other with a slow increase. Another feature is the time difference between nighttime CO2 and NDVI maxima, which is around half a month, since the NDVI maximum was observed in late May. The CH4 cycle presented a similar evolution for the three situations. The annual cycle range was around 0.050 ppm between the maximum in winter and the minimum in summer, these being regularly distributed approximately every six months.

The analysis presented in this paper focused on the daytime for the boundary layer height due to the noticeable range of this variable during that period. However, the influence of the remaining variables was considered during the night due to the characteristic CO2 annual pattern, whose values were considerably higher than those during the day.

3.2. Boundary Layer Height

The METEX model provides the boundary layer heights, the most noticeable changes of this variable being observed during the day. Figure 3 presents the boundary layer evolution smoothed with the Kernel methodology. During winter, its minimum was in December, at about 400 m. However, it increased gradually in winter and at a lower rate in spring and summer, reaching nearly 1200 m in August. After this value, the boundary layer fell sharply during the rest of the year. Its values were similar to that reached at some European sites [38, 39].

Regression analysis between concentration during the day and boundary layer height shown in Figure 3 revealed an inverse relationship between the two variables, with correlation coefficients of 0.919 and 0.974, for CO2 and CH4, respectively. This behaviour is in agreement with Pérez et al. [15] and Sreenivas et al. [40]. In summer, plant activity was the lowest and the boundary layer height was greatest, leading to intensive dispersion. By contrast, the boundary layer height was lowest in winter, dispersion was small, and concentration increased due to larger emissions.

Two groups of situations with different thresholds of the boundary layer height were considered to investigate the response of equation (1). The first is formed by evolutions with boundary layer heights above certain thresholds, and the second considers boundary layer heights below the thresholds. An objective procedure for threshold selection was not achieved. Consequently, this should be chosen by taking into account of the frequency of observations and the changes observed in the concentration.

Table 3 presents the frequency of available observations, the number of days without observations (gaps) calculated for annual evolutions, and the differences between the average concentration with different boundary layer heights in 100 m intervals and the average diurnal value. With a high boundary layer height, strong dispersion caused low concentrations. Moreover, when the threshold for large values of the boundary layer increased, the number of available observations decreased. Furthermore, a noticeable gap was observed in autumn and winter when the threshold was above 800 m, since extensive development of the boundary layer is infrequent during this season. The annual evolution corresponding to this height is presented in Figure 3, whose average concentrations were 2.5 ppm lower for CO2 and 0.012 ppm lower for CH4 than those calculated for the diurnal observations. The seasonal pattern in this case was similar to that for diurnal values.

However, for heights below the threshold, concentrations increased. The behaviour of the available observations was the opposite to what emerged when the boundary layer height was above the threshold. In this case, when the threshold increased, the frequency of available values also increased, and a gap was observed in late summer-early autumn when the threshold was below 400 m. The evolutions corresponding to that height are shown in Figure 3. Their corresponding average concentrations increased 6.3 ppm for CO2 and 0.023 ppm for CH4. Moreover, a marked seasonal pattern was also observed for CO2, which may be explained by the daily evolution of the boundary layer height, whose lowest values are reached in early and late daytime. Under these conditions, photosynthesis is low and emissions prevail; hence, the CO2 maximum was observed in spring when vegetation is developing. This reached up to 13.4 ppm above the corresponding daytime concentration. Finally, similar values were obtained in winter for CO2 in the three evolutions shown in Figure 3. The seasonal pattern for CH4 was similar to that for diurnal values.

3.3. Recirculation Factor

The annual evolution of the recirculation factor was calculated using the Kernel smoothing methodology and presented in Figure 4(a). These values were lower than those calculated at different sites presented in Table 4, revealing that marked recirculations are infrequent. Moreover, their range is very narrow since the lowest value, around 0.07, was reached in February and the highest, nearly 0.12, in August.

In order to investigate the recirculation influence on concentrations, two situations were proposed: firstly by considering recirculation factors above certain thresholds (in steps of 0.05) and secondly, below others (in steps of 0.01). Table 5 presents the differences between the average concentration calculated for these situations and those obtained during the night together with their corresponding frequencies of available observations and gaps formed by days without observations.

Concentrations increased together with the recirculation factor for factors above the thresholds. Moreover, the frequency of available observations decreased when the threshold increased. Despite the high number of gaps for the 0.15 threshold, these were uniformly distributed along the year; hence, the small difference was observed in concentrations obtained with the following threshold. Figure 4 presents this evolution, whose concentration was 2.6 ppm higher for CO2 and 0.012 ppm higher for CH4 than their corresponding average calculated for nighttime.

CO2 was mainly affected by high recirculation in March-May and November, with concentrations reaching more than 4 ppm above those calculated with all observations. For CH4, the greatest difference was observed in late autumn and reached 0.035 ppm.

High recirculation should determine low dispersion and, consequently, a concentration increase. In this sense, high concentrations are reinforced by recirculation processes, such as in spring for CO2 and late autumn and early winter for CH4, added to which intermediate concentrations also grew, in autumn, for both gases.

When observations were selected below the threshold, the frequency of the available observations decreased following the threshold. Observation density was low when the recirculation factor was below 0.02. However, there were few days without observations, and these were uniformly distributed for this threshold. The corresponding annual evolution is presented in Figure 4. Under this condition, average concentrations were less modified than those obtained in the preceding test and were 1.7 ppm below the average for the annual cycle for CO2 and 0.008 ppm for CH4.

Minima of evolutions for CO2 presented in Figure 4 show an advancement of about one week between the cycle for 0.02 threshold and nighttime and between that and the evolution for 0.15 threshold. Moreover, the range for the cycle with the recirculation factor above 0.15 was 18.5 ppm and was greater than the range for the recirculation factor below 0.02, which was 16.1 ppm.

3.4. Trajectory Direction

A detailed analysis of direction does not seem recommendable for one-day trajectory, due to the wind direction change which may be significant for short trajectories. Following Lai [12], four quadrants were considered. Table 6 presents their corresponding availabilities, average wind speeds at the site, and the differences between the average calculated concentrations in the quadrant and for all nighttime observations. In this test, thresholds were not considered since trajectories are distributed in the quadrants. The most frequent sector was NW, with the second highest wind speed, and the least frequent SE, with the lowest wind speed. These frequencies are explained by the synoptic flow affecting the Iberian Peninsula where a western wind prevails [48]. The remaining sectors presented a similar and intermediate frequency. Days without observations, though noticeable for SE, were uniformly distributed, and equation (1) guarantees an accurate calculation.

The most noticeable contrasts were obtained for the directions presented in Figure 5. The average CO2 concentration for the SE quadrant was 2.5 ppm above the average for all nighttime observations and may be attributed to transport from the city of Valladolid [24]. Moreover, concentration increase in this sector was not uniformly distributed since the greatest differences were obtained from May to July. These differences ranged from 5 to 6 ppm and were probably due to the slow dispersion linked to the low wind speed in this sector [48]. CO2 concentration was intermediate and similar during autumn and winter. Another noticeable feature with respect to the cycle during the night was the delay observed in the maximum in May and the minimum in September. Differences between the values calculated with all the observations and the low concentration for NE were small for this gas, although they were above 1.5 ppm from March to October. For CH4, the contrast between sectors was also very small, as shown in Table 6 and Figure 5(b). For this gas, the highest concentration corresponded to NE trajectories and the lowest to NW, with a difference of 0.011 ppm.

3.5. Wind Speed

Wind speed during the night displayed the annual pattern shown in Figure 6. The range is very narrow, around 2.5 m·s−1. Large values, around 6 m·s−1 were observed in late autumn and winter. However, the lowest wind speed was observed in August, below 4 m·s−1. Consequently, its annual cycle evolution is asymmetric, with wind speed decreasing slowly from February to August and increasing sharply from August to November. This result is comparable to evolutions analysed in previous studies such as Lorente-Plazas et al. [49], who presented the annual cycle of wind speed for different regions in the Iberian Peninsula. The annual evolution for central sites is characterised by high values in March but low and similar values during the latter half of the year. However, the cycle obtained was similar to those observed in the north of the peninsula.

Table 7 presents the results of several tests performed with different thresholds of wind speed in steps of 1 m·s−1. Figure 6 presents the annual evolution for two selected thresholds in extreme conditions. When wind speeds were above 7 m·s−1, a noticeable gap in summer is observed linked with the frequent low wind speeds in this period, and wind speeds below 3 m·s−1 led to a low density of observations.

Calculated concentrations were 3.0 and 0.011 ppm lower than those obtained for all observations during the night for CO2 and CH4, respectively, when wind speed was above 7 m·s−1, indicating that dispersion was favoured under high wind speed. Conversely, calculated concentrations for low wind speeds were higher than those for all observations during the night, reaching 3.4 and 0.013 ppm for CO2 and CH4, respectively, when wind speed was below 3 m·s−1. These differences may be explained since stagnation conditions prevent dispersion of the two gases.

Several features are observed in the annual evolution. When wind speed was below 3 m·s−1, CO2 was around 5 ppm greater than the corresponding value for the nighttime evolution in late April and early May and a similar amount was lower when wind speed was above 7 m·s−1. Moreover, the minimum concentration was nearly one week later with wind speeds below 3 m·s−1 compared to the evolution for observations during the night, and it was early by a similar interval for wind speeds above 7 m·s−1. The low CO2 concentration in late summer is attributed to the extremely weak plant activity responsible for low emissions. Under this condition, concentration is low despite the low wind speed. CH4 behaviour was more irregular than CO2 evolution. Differences between concentrations for wind speeds below 3 m·s−1 and those obtained with all the observations were above 0.025 ppm in late autumn and winter. Moreover, the values in January, July, August, and December for wind speed above 7 m·s−1 were at least 0.015 ppm lower than those for all values during the night.

4. Conclusions

The key point of the current study is the combination of modelled and measured variables since the influence of meteorological variables on observed CO2 and CH4 concentrations is investigated. Prominent among the modelled variables provided by an air parcel trajectory model is boundary layer height, with its impact being quantified, whereas the shape of the trajectories is analysed from the recirculation factor, calculated from the geographical coordinates of such trajectories.

High concentrations during the night were attributed to the low atmospheric dispersion in this period. The sharp contrast between day and night observed in spring for CO2 was due to intense vegetation growth during this season that strengthened respiration during the night and photosynthesis during the day. Annual CH4 evolution remained nearly unchanged when only day or night was selected.

The annual pattern of the boundary layer height during the day evolved from 400 m in December-January, to nearly 800 m in March-April and reaching slightly below 1200 m in July-August, favouring dispersion in this period.

Trajectories reaching the measuring site recirculated slightly, and the annual wind speed pattern showed a small fluctuation range, 2.5 m·s−1 during the night. Despite their slight evolution, both variables showed opposite cycles since high wind speed is associated with trajectories that have only slight recirculation.

Trajectory direction showed a noticeable contrast since the NW sector was the most frequent, whereas the opposite sector, the SE sector, was the least frequent, in agreement with the synoptic flow affecting the Iberian Peninsula.

The kernel smoothing procedure emerges as a suitable procedure to investigate the response of the concentrations to different thresholds. As a result of the tests performed, a concentration increase was observed under meteorological conditions that inhibited dispersion. Particularly, low values of the boundary layer height were associated with noticeable increases in concentrations. However, slight displacements were observed when recirculation, direction, or wind speed was filtered. Moreover, CH4 was more robust to tests of meteorological values than CO2, whose concentration proved more sensitive.

Among the natural processes that determine the annual evolution of CO2 and CH4 at this site, meteorological variables, which have been analysed separately in this paper, may have a noticeable impact on concentrations of both greenhouse gases.

Data Availability

The CO2 and CH4 observations used in this study are available from the lead researcher of the project, Prof. M. Luisa Sánchez ([email protected]), upon request. METEX simulations were made from http://db.cger.nies.go.jp/metex/trajectory.html. NDVI data were downloaded from https://earthdata.nasa.gov/. Sunrise and sunset data were obtained from the National Geographic Institute (http://www.fomento.gob.es/).

Conflicts of Interest

The authors declare there are no conflicts of interest regarding publication of this paper.


The authors wish to acknowledge the financial support of the Ministry of Economy and Competitiveness and ERDF funds (projects CGL2009-11979 and CGL2014-53948-P).