Evaluation of the Wind Fields in the Semi-Arid Region in Northeastern Brazil Using RAMS Model

Avaliação do Modelo RAMS em Simulações dos Campos de Ventos na Região Semiárida do Nordeste do Brasil

Abstract

The use of wind power has increased significantly around the world over the last few years. Some estimates state that about 12% of all energy generated in the world will come from wind energy conversion systems, corresponding to an installed capacity of 1,200 GW. The installed wind power capacity in Brazil is low, being equal to 11300 MW in 2017. Even though Brazilian wind potential is not spread all over the country, some regions are quite interesting for the installation of wind farms, especially the Northeast region, which aggregates about 53% of the national potential. This work aims to identify patterns of variability of the wind regime, as well as potential sites for the generation of wind power in semi-arid northeastern Brazil. In order to achieve it, numerical simulations are performed using the Regional Atmospheric Modeling System (RAMS). During simulations, both turbulence parameterization and Newtonian relaxation time scale are evaluated. It is worth to mention that obtained data are compared with those provided by the National Institute of Meteorology (INMET) through static indexes.

Keywords:
wind fields; semi-arid; atmospheric modeling

Resumo

A geração de energia elétrica a partir dos ventos está em uma crescente mundial, estimativas indicam que em 2020, cerca de 12% de toda a energia gerada no mundo será proveniente da conversão eólica, o que representaria uma capacidade instalada de 1.200 GW. No Brasil, a capacidade instalada ainda é pouco representativa e, em 2017, totalizava cerca de 11300 MW. A região nordeste possui um grande potencial para a geração eólica, tendo cerca de 53% do potencial nacional. Este trabalho tem por objetivo identificar padrões de variação do regime de ventos, bem como identificar potenciais sítios para geração de energia eólica em regiões contidas no semiárido nordestino. Para tanto, foram realizadas simulações numéricas utilizando o modelo atmosférico regional RAMS (Regional Atmospheric Modeling System) sobre região semiárida do Nordeste do Brasil. Nas simulações, foram avaliadas a parametrização de turbulência e escala de tempo do relaxamento newtoniano. A destreza das diferentes configurações do modelo foi verificada através da utilização de dados de superfície coletados por estacoes meteorológicas do Instituto Nacional de Meteorologia - INMET, que foram comparados aos dados simulados através do calculo de diversos índices estatísticos.

Palavras-chave:
ventos; Semiárido; modelagem atmosférica

1. Introduction

When determining the wind potential of a given region, it is necessary to know the respective variability of wind regime. This information can be obtained from meteorological stations installed in private or public sites. However, this strategy is not viable in many cases due to the distance among the data collection points, as there is little confidence in acquired data.

Therefore, weather forecast models are a prominent alternative to provide information that can be of great help in the design of future wind power plants, they are able to predict both speed fields and wind direction.

Numerical simulations use global or regional atmospheric models or even a combination of both in a technique known as downscaling. Such models reproduce the physical process that occur in atmosphere and other factors that influence directly on atmospheric circulation in computer environment (Gomes Filho et al., 1996; Marengo, 2001; Melo and Marengo, 2007; Menezes Neto et al., 2009).

Alves et al. (2003) tested the downscaling technique by combining the RSM97 (regional) and ECHAM4.5 (global) models to perform climate simulations in northern and northeastern Brazil. The obtained results have shown improved performance when representing the fields of some atmospheric variables such as rainfall levels and wind speed if compared with output fields of the global models (Silva et al., 2004)

The numerical modeling has great applicability in the energy sector, because it can be used in the prediction and planning for the utilization of existing energy resources in a given region, as well as to assess the impacts caused by them. Therefore, the simulation of wind fields is a prominent tool in the assessment of energy potential for the possible installation of wind farms (Martins et al., 2007).

The state of the art presents some studies on the subject that aim at establishing settings and analyzing the performance of climate simulations regarding the wind fields in the Semi-Arid Region in Northeastern Brazil (SARNB) when performed by several, global and regional numerical models, while some cases employ the downscaling technique (Cuadra and Rock, 2005; Alcântara and Souza, 2007; Santiago de Maria, 2008; Oliveira and Costa, 2011).

This work presents the performance analysis of climate simulations regarding wind fields in SARNB using the regional model described by (Pielke, 1991; Pielke et al., 1992; Cotton et al., 1995). Besides, distinct turbulence parameterizations and settings for the Newtonian relaxation time scale are evaluated in order to determine which configuration presents the best performance in the representation of wind fields in SARNB.

For this purpose, simulations are performed considering the turbulence settings used by Smagorinsky (1963) and Mellor and Yamada (1974). The first one has local influence and depends on the components of local winds. The second one considers the potential temperature and turbulent kinetic energy as the variables necessary for the calculation of diffusion coefficients.

The Newtonian relaxation time scales considered in the tests correspond to 12 h and 48 h, which are chosen in order to verify the influence of such parameter on the local wind fields of the region. It is worth to mention that 12 h correspond to a more intense nudging than 48 h.

The validation of the simulation results is performed through comparisons performed between output data obtained from RAMS model and those acquired from meteorological stations of the Brazilian National Institute of Meteorology (INMET) located in the studied regions.

The performance of simulations is evaluated through statistical analysis, which provides the degree of relationship between the series of simulated and observed values. Eight statistical rates are calculated and proper weights are assigned to such quantities according to the respective relevance. Then it is possible to identify the wind regime profile, as well as potential sites for wind energy generation in SARNB, while it allows to determine possible settings for operational routines in order to predict the use of wind resources.

2. Materials and Methods

2.1. Parameterization used in the simulation tests

Two nested grids were used in the simulations performed with model RAMS 6.0. The first one presents a horizontal spacing of 20 km, covering large part of northeast region, except for the state of Bahia (Fig. 1a). The second one used a horizontal spacing of 5 km, which covers the south portion of Ceará state, the west portion of Pernambuco state and the north portion of Bahia (Fig. 1b). Vertically, there are 54 levels with an expansion rate of 1.1 and initial grid spacing of 20 m, initially, which can be extended to a maximum spacing of 1000 m. The model was then configured with 11 soil layers. The Table 1 presents the settings for the two remaining grids.

Figura 1
Grids used in the simulation. (a) Grid with horizontal spacing of 20 km, (b) Grid with horizontal spacing of 5 km.

Tabela 1
Specifications of the used grids in the simulations, where NNXP, NNYP and NNZP represent the number of points of the grid in x and y directions and the number of points in the vertical grade, respectively; DELTA provides the grid spacing; DZRAT is the rate of vertical expansion, DZMAX is the maximum vertical spacing; CENTLAT and CENTLON provide us the coordinates of the center of the grids.

	Grid 1	Grid 2		Grid 1	Grid 2
NNXP	100	118	DELTAZ (m)	20	20
NNYP	100	182	DZRAT	1.1	1.1
NNZP	54	54	DZMAX (m)	1000	1000
DELTAX (km)	20	5	CENTLAT	- 5.67	- 5.99
DELTAY (km)	20	5	CENTLON	- 40.33	- 39.64

Short and long wave radiations were parameterized according to the scheme presented by Chen and Cotton et al., 1983, being updated every 20 min of simulation. This frequency was also used to update the settings for cumulus cloud types, while Kuo scheme is applicated in this case, described in Kuo et al. (1974). For shallow convection parameterization is used the scheme described in Souza and Silva, 2003.

For turbulent diffusion parameterization, two distinct settings were tested. The first one uses the anisotropic version of the scheme proposed by Smagorinsky (1963). According to Santiago de Maria (2008), this setting is recommended for cases where the horizontal and vertical spacing have quite distinct dimensions. Being this is a local scheme, the mixture coefficients depend only on the local and the properties of the current flux.

In the second setting, the turbulent diffusion was parameterized according to Mellor and Yamada (1974), whose scheme uses the horizontal wind fields, the potential temperature, and the turbulent kinetic energy provided by the model to calculate the diffusion coefficients.

Two settings were tested for the Newtonian relaxation. In the first case, the time scale was 12 h, while the second was 48 h. The Newtonian relaxation has unity weight, being applied to the center and the top of the grid. This feature is used to ensure that the simulation results do not diverge from the input data used in the model initialization.

The fields of the meteorological variables from the National Center for Environmental Prediction (NCEP) were used to initialize the model. The fields topography, soil, sea temperature, vegetation, and normalized vegetation difference index (NVDI) are provided by Atmospheric Meteorological, and Environmental Technologies (ATMET).

2.2. Surface data

In order to evaluate the simulation performance, data from four meteorological stations located at SARNB (Fig. 2), which were obtained from INMET website for the period of one year comprised between May 2009 and May 2010.

Figura 2
Location of automatic stations in the first grid of the RAMS model.

2.3. Analysis of the simulations

In order to properly evaluate the simulation tests and determine which one presents the best configuration for the parameterization of turbulent diffusion and the Newtonian relaxation, among the assessed variables, a statistical analysis has been performed by the calculation of the following statistical indexes: Bias, Mean Absolute Error, Mean Square Error, rate between the simulated and observed standard deviations, Mean Absolute Error between the deviations, Mean Square Error between the deviations, concordance index, and correlation index. Such coefficients allow comparing two or more data groups and determining existing relationships among them.

According to Xavier (2000), the statistical bias (b) represents a comparison between the mean values of a variable obtained by the simulation and the observed mean value. This statistical variable can also be expressed as the rate between the number of predictions and the number of times that a given event has occurred.

If there is no bias, b = 1, showing that the event was predicted the same number of times it was observed. Bias does not provide information on the correspondence between predictions and observations in particular cases, what makes it an inaccurate measure.

By defining the value of a given variable observed at the i-th instant of time, and the same variable simulated by the model at the same instant and point in space, statistical bias can be expressed as:

(1) $$b=\frac{1}{N}{\displaystyle \sum _{i=1}^N({\text{ϕ}}_i-{\text{ψ}}_i)}$$

where N is the number of time instants in the series.

A more accurate error measure is the Mean Absolute Error (MAE), which is the average of the absolute values for the differences between prediction and observation. The MAE is zero if prediction is perfect and increases as the difference between the simulated and observed values also does.

(2) $$MAE=\frac{1}{N}{\displaystyle \sum _{i=1}^N|{\text{ϕ}}_i-{\text{ψ}}_i|}$$

The Mean Square Error (MSE) is the average of the squared difference among pairs of simulated and observed values and defined as follows:

(3) $$MSE={\left[\frac{1}{N}{\displaystyle \sum _{i=1}^N({\text{ϕ}}_i-{\text{ψ}}_i)}\right]}^{1\text{/}2}$$

As the square of error products are positive terms, MSE is zero for perfect predictions and increases rapidly as the difference between prediction and observation becomes higher.

Another error estimate proposed by Santiago de Maria (2008) and Lima and Alves (2009) is the rate between the simulated and observed standard deviations. According to Lima and Alves (2009), this is due to the fact that similar measures of standard deviations are associated with the similarity between the series. The standard deviations σ_ϕ and σ_ψ are given by:

(4) $${\text{σ}}_{\text{ϕ}}={\left[\frac{1}{N}{\displaystyle \sum _{i=1}^N{({\text{ϕ}}_i-\overline{\text{ϕ}})}^2}\right]}^{1\text{/}2}$$

(5) $${\text{σ}}_{\text{ψ}}={\left[\frac{1}{N}{\displaystyle \sum _{i=1}^N{({\text{ψ}}_i-\overline{\text{ψ}})}^2}\right]}^{1\text{/}2}$$

Therefore, the rate between the standard deviations is defined as R_s:

(6) $$R_{\text{σ}}=\frac{{\text{σ}}_{\text{ψ}}}{{\text{σ}}_{\text{ϕ}}}$$

This quantity is dimensionless and can assume any nonnegative value. The closer it is to unity, the higher is the similarity between the standard deviations.

According to Walko et al. (2001), the systematic error of the model can be reduced through the removal of statistical bias i.e. considering that the error measures are only calculated for the series deviations. Consequently, by reformulating indexes like MAE and MSE in order to eliminate bias, the Deviation Mean Absolute Error (DMAE) and the Deviation Mean Square Error (DMSE) can be obtained as defined by the following expressions:

(7) $$DMAE=\frac{1}{N}{\displaystyle \sum _{i=1}^N\text{|}{\text{ϕ}}_i^{\text{'}}{–\text{ψ}}_i^{\text{'}}\text{|}}$$

(8) $$DMAE={\left[\frac{1}{N}{\displaystyle \sum _{i=1}^N\text{(}{\text{ϕ}}_i^{\text{'}}{–\text{ψ}}_i^{\text{'}}\text{)}}\right]}^{1\text{/}2}$$

where ${\phi }_i^{\text{'}}$ and ${\psi }_i^{\text{'}}$ are the deviations of the simulated and observed series, given by Walko et al. (2001), Gobble (2006) and Devore (2006), respectively.

(9) $${\mathrm{\varphi }}_i^{\text{'}}={\text{ϕ}}_i-{\overline{\text{ϕ}}}_i$$

(10) $${\text{ψ}}_i^{\text{'}}={\text{ψ}}_i-{\overline{\text{ψ}}}_i$$

The concordance index I_C is a dimensionless measure and can assume values between 0 and 1, and it approaches 1 as the similarity between the series increases.

(11) $$I_C=1-\frac{{\displaystyle \sum _{i=1}^N\text{|}{\text{ϕ}}_i-{\text{ψ}}_i{\text{|}}^2}}{{\displaystyle \sum _{i=1}^N{(\text{|}{\text{ϕ}}_i–{\overline{\text{ψ}}}_i\text{|}+{\text{|ψ}}_i-{\overline{\text{ψ}}}_i\text{|})}^2}}$$

The correlation index (r) is the most relevant metric of comparison among all the previously presented ones Devore (2006) being defined as:

(12) $$r=\frac{1}{N}{\displaystyle \sum _{i=1}^N\frac{{\text{ϕ}}_i^{\text{'}}{\text{ψ}}_i^{\text{'}}}{{\text{σ}}_{\text{ϕ}}{\text{σ}}_{\text{ψ}}}}$$

This index can assume values between −1 and 1, thus indicating values between perfect anticorrelation and perfect correlation, respectively. When it equals zero, the total absence of correlation is verified. This index is capable of detecting the phase correspondence between the series, being inherently insensible to bias errors. Its classification is shown in Table 2.

Tabela 2
Person's Correlation Coefficient

Range	Classification
1	Perfect
0.9 to 1	Very Strong
0.7 to 0.89	Strong
0.4 to 0.69	Moderate
0.2 to 0.39	Weak
0.0 to 0.19	Very Weak

Devore (2006)

The aforementioned statistical indexes were calculated using simulated data and observed ones from the meteorological stations under study in order to verify the performance of simulations. Weights are assigned to each calculated index, in such a way that the higher the weight, the more relevant the index is as proposed by Santiago de Maria (2008). Thus, the configuration that obtains the highest weight is supposed to present the highest similarity with the observed series. Table 3 lists all statistical indexes and their respective weights.

Tabela 3
Statistical Indexes and their respective scores.

Simbol	Index	Scores
b	Statistical Bias	1
EAM	Mean Absolute Error	1
EQM	Mean Sque Error	1
R	Rate between Standard Deviations	1
EAMD	Mean Absolute Error of the Deviations	2
EQMD	Mean Square Error of the Deviations	2
Ic	Concordance Index	3
r	Correlation Index	4

Santiago de Maria (2008)

3. Results and Discussions

3.1. Sensibility of the model to the turbulence parameterization

In order to determine the adequate parameterization of turbulence for climate simulations of the wind fields in the region of study, the results for simulations using Mellor and Yamada's parameterizations (1974) and Smagorinsky's (1963) ones are compared with observations obtained from INMET's meteorological stations, which are shown in Fig. 2.

Figure 3-a presents the daily averages of wind speed including simulated and observed values corresponding to July 2009, August 2009, and September 2009. It can be observed that the simulated values of wind speeds in Barbalha/CE are higher than those observed during the whole period.

Figura 3
Daily average of simulated and observed wind speed at 10 m high to the 5 km grade for the quarter of July. August and September of 2009 to the localities of (a) Barbalha and (b) Cabrobó.

The statistical value shown in Table 4 confirms the overestimation of observed values over the simulation ones in both cases. The mean absolute and mean square values also denote such difference between the simulated and observed series. The obtained statistical correlation coefficients are considered strong according to Devore (2006)i.e. 0.77 and 0.73, showing that the simulated series follows the tendency of the observed values.

Tabela 4
Calculated statistical indexes. to the measurements of wind speed. for the parameterized model according to Mellor-Yamada (M-Y). and for the model according to Smagorinsky (SMA). in the locality of Barbalha and Cabrobo. The presented indexes are the statistical bias (b). Mean Absolute Error. Mean Square Error. rate between Standard Deviation. Mean Absolute Error of the Deviations. Mean Square Errors of the Deviations. Concordance Index and Correlation Index. The Total of Scores obtained by each variable are also shown.

Barbalha/CE	b	EAM	EQM	R	EAMD	EQMD	Ic	r	Pesos
M-Y	2.11	2.11	2.19	0.59	0.47	0.56	0.33	0.77	9
SMA	1.83	1.83	1.95	0.53	0.57	0.68	0.37	0.73	6
Cabrobó/PE
M-Y	0.16	0.53	0.69	1.16	0.51	0.67	0.78	0.63	9
SMA	0.42	0.60	0.77	1.17	0.54	0.65	0.75	0.65	6

In essence, the results in Table 4 show that the simulated values using Mellor and Yamada's parameterization present higher weights, that is, RAMS model presents improved performance when using such settings if compared with the observations from the meteorological station of Barbalha/CE.

Figure 3-b shows the simulation and the observation results for wind speeds obtained from the meteorological station of Cabrobó/PE. It can be stated that the simulated values are close to the observed ones. The simulated values using Mellor and Yamada's scheme present an average of 4.3 m/s, while the average for Smagorinsky's scheme is 4.6 m/s. It is also worth to mention that the average speed for the observed values corresponds to 4.1 m/s during the considered period.

The statistical indexes calculated in this case as shown in Table 4 evidence that the simulated values with both parameterization methods present little bias, as confirmed by the concordance indexes and the correlation coefficients classified as moderated (0.63 and 0.65). In general, the simulations using Mellor and Yamada's parameterizations provide higher weights in the indexes counting, thus showing that the RAMS model presents improved performance when representing the observations in the region wind fields.

3.2. Sensitivity of the model in relation to time scale of the Newtonian Relaxation

The simulated data series using different turbulence parameterizations shown in the previous session used a Newtonian relaxation time scale of 12 h. As it was seen, the use of Mellor and Yamada's parameterization implied better performance if compared to the observed data. Therefore, the simulated series in this session uses Mellor and Yamada's scheme considering time scales of 12 and 48 h.

Figure 4-a presents the series of daily average wind speeds for simulated and observed data. It can be stated that varying the Newtonian relaxation time scale causes higher bias errors in Barbalha/CE station, while the mean absolute and mean square errors also increase according to Table 4. There are low concordance indexes in this case, even though there are strong correlation coefficients in both time scales. It can be also seen that RAMS model presents better performance when configured with relaxation time of 12 h according to the presented methodology.

Figura 4
Daily Average of wind speed simulated at 10 m high for the grade of 5 km for the quarter of July. August and September of 2009 for the localities of Barbalha (a) and Cabrobo (b).

The results for Cabrobó/PE show that the simulated series follow the observed values (Fig. 4-b). According to Table 5, the highest weights for the statistical indexes occur when relaxation time scale of 12 h is considered for the simulated data, thus providing the accurate representation of the wind regime in the study region.

Tabela 5
Calculated Statistical Indexes. for the measurements of wind speed. for the model configurer with a Newtonian Relaxation time scale of 15 h (RN 12 h). And for a configuration of Newtonian Relaxation of 48 h (RN 48 h). in the locality of Barbalha and Cabrobó. The presented indexes are the statistical bias (b). Mean Absolute Error (EAM). Mean Square Error (EQM). rate between Standard Deviation (R). Mean Absolute Error of the Deviations (EAMD). Mean Square Errors of the Deviations (EQMD). Concordance Index (Ic) and Correlation Index. The Total of Scores obtained by each variable are also shown.

Barbalha/CE	b	EAM	EQM	R	EAMD	EQMD	Ic	r	Pesos
RN 12 h	2.11	2.11	2.19	0.59	0.47	0.56	0.34	0.77	11
RN 48 h	2.10	2.10	2.18	0.60	0.48	0.58	0.33	0.73	4
Cabrobó/PE
RN 12 h	0.16	0.53	0.69	1.16	0.51	0.67	0.78	0.63	12
RN 48 h	0.15	0.55	0.68	1.33	0.54	0.66	0.76	0.62	3

3.3. Adjustment of the simulated series

The results presented in the previous sessions have shown that RAMS model has the ability to preview the wind fields in the study region. Although, the series of simulated values presents bias and statistical errors, what makes it diverge from the observed one. Therefore, once the goal is to approximate the simulated values to the observed ones, curve fitting is performed using the linear regression theory.

A similar approach was proposed by Lira et al. (2011). In this case, the calibration period for the linear regression comprehends the wind speed data obtained during July 2009 and August 2009. On the other hand, the validation period aggregates the values corresponding to September 2009. Once the curves are fitted, the statistical indexes for the adjusted series can be calculated.

The series of adjusted values have as a base the simulated values using the model configured with Mellor and Yamada's parameterization and a Newtonian relaxation time scale of 12 h, since RAMS model has presented better performance when representing the wind speed fields in the investigated regions.

Figure 5 shows the series of simulated, observed and adjusted values by the linear regression method in the study regions. Table 5 presents the statistical indexes calculated between the values of the adjusted series and the observed one. On the other hand, the comparison between simulated and observed values is given in Table 4 considering that the Newtonian relaxation time scale is 12 h.

Figura 5
Daily Average of wind simulated and wind speed observed at 10 meters high for the grade of 5 km to the quarter of July. August and September of 2009 for the localities of Barbalha (a) and Cabrobo (b).

Considering the comparison between the adjusted values and the obtained ones in the meteorological station of Barbalha/CE, it can be seen that curve fitting allows decreasing the statistical bias between the series, and consequently higher values for the statistical correlation coefficient (0.86) and the concordance index (0.89) could be obtained (Table 6).

Tabela 6
Calculated statistical indexes. for the simulated and previewd by linear regression wind speed. in the locality of Barbalha. The presented indexes are the statistical bias (b). Mean Absolute Error (EAM). Mean Square Error (EQM). rate between Standard Deviation (R). Mean Absolute Error of the Deviations (EAMD). Mean Square Errors of the Deviations (EQMD). Concordance Index (Ic) and Correlation Index. The Total of Scores obtained by each variable are also shown.

	b	EAM	EQM	R	EAMD	EQMD	Ic	r
Barbalha/CE	-0.07	0.20	0.24	1.35	0.20	0.23	0.89	0.86
Cabrobó/PE	0.023	0.61	0.81	1.98	0.61	0.81	0.70	0.66

The fitted curve for Cabrobó/PE causes the statistical bias to decrease, while a small increase occurs between the standard deviations. Besides, there is a slight decrease of the concordance index for the adjusted series if compared with the observed one (Table 6).

4. Conclusion

According to the obtained results, it can be concluded that the model is able to detect the variability tendency of the observed series of wind speeds in all the tested configurations, as the statistical correlation coefficient is classified from moderated to strong, with values higher than 0.5 in every case.

Considering the sensibility to the turbulence parameterization where Mellor and Yamada's and Smagorinsky's schemes have been tested, the statistical analysis has shown that the first one presents better performance in the representation of wind speed fields.

Although values for the correlation coefficients could be classified from moderate to strong, the series of simulated values in the performed tests has presented appreciable bias and statistical errors in some cases. This fact is evidenced by the differences between the curves in Figs. 3 and 4, which cause low values of concordance index.

The sensibility test to the Newtonian relaxation time scale has revealed slight differences between the simulated series with time scales of 12 and 48 h. In such cases, the simulated values overestimate the observed wind speeds in the stations, even though the series of simulated values seems to follow the variability tendency of the observed values graphically.

The statistical analysis has also demonstrated that the model configured with Newtonian relaxation time scale of 12 h is more accurate in the representation of the wind fields for two investigated regions because higher weights are assigned in this analysis.

Therefore, through the analysis of obtained results with sensibility tests performed using the RAMS model configured with the previously mentioned turbulence parameterizations and Newtonian relaxation time scales, it can be stated that such regional model is able to represent the wind fields observed in the meteorological stations of Bracalha/CE and Cabrobó/PE more accurately. For this purpose, Mellor and Yamada's scheme (1974) and a Newtonian relaxation time scale of 12 h are used. Such results are in accordance with the analysis carried out by Santiago de Maria (2008) and Oliveira and Costa (2011).

It can be also concluded that the application of the method proposed by Lira et al. (2011) for curve fitting purposes causes the statistical bias between the studied series to be reduced. This fact can be observed graphically in the presented curves, while the correlation coefficients between the series of adjusted and observed values are increased.

Finally, it is worth to mention that the analysis carried in this work evidences that the regional model RAMS can be used as an auxiliary tool in the prediction and planning for the energetic sector in SARNB, being able to assess potential sites for the installation of wind farms in agreement with the proposal of Martins et al. (2007).

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Publication Dates

• Publication in this collection
  Jul-Sep 2017

History

• Received
  18 Mar 2017
• Accepted
  19 Aug 2017