1 Introduction

The reference crop evapotranspiration (ETo) is essential for characterizing the local climate and for computing crop and vegetation evapotranspiration, water and irrigation requirements as well as for crop water management, irrigation planning and management, hydrologic and water balance studies, climate characterization, and climate change analysis. Following conceptual and computational discussions by Pereira et al. (1999, 2015), a brief review was presented in the companion paper (Paredes et al. 2017) focusing on the estimation of the actual vapor pressure (e a, kPa), short wave radiation (R s, MJ m2 day−1), and wind speed at 2 m height (u 2, m s−1) when observations data are not available. The accuracy of using those estimates for computing ETo replacing the respective missing variables in the PM-ETo, as recommended by Allen et al. (1998), was assessed by comparing the respective results with those obtained with the PM-ETo with full data sets. The results for accuracy were very good for all the three estimated variables, particularly considering the monthly variability of weather variables in Azores (Fig. S1 in the Supplementary Material).

The use of the referred approaches for estimating the parameters of the PM-ETo equation allows computing ETo with temperature data only as proposed in FAO56 (Allen et al. 1998). This approach to cope with missing weather data is known as reduced set PM equation or PM temperature approach (PMT) as in the current paper. As analyzed by Annandale et al. (2002), errors resulting from estimating weather parameters are “somewhat compensated for by the absence of error that would have been resident in the measurements”. Hargreaves and Allen (2003) also compared the Hargreaves-Samani equation (11) with the PMT approach following that the HS equation was proposed in FAO56 as an alternative for ETo computation when only temperature data are available (Allen et al. 1998). The referred assessments evidence the need for good quality of weather data.

Researchers have generally not adhered to using the methods proposed in FAO56 (Allen et al. 1998) to estimate the missing variables and adopting the PMT approach; instead, they easily adopted the HS equation, simpler and easier to use than the PMT approach, and/or searched for alternative ET equations and numerical and heuristic methods for estimating ETo as revised by Pereira et al. (2015). Nevertheless, as stated by these authors, while using different equations and estimation methods may ease computational approaches, there is no replacement for basic Physics as it is represented in the PM-ETo formulation. Using alternative equations may induce changes in the basic Physics relationships as expressed by the non-linearity of relations between HS and PM-ETo equations shown by Raziei and Pereira (2013a), particularly for locations marked by aridity and wind speed. Differently, adopting estimated values for the missing variables, particularly R s and e a, has the merit of allowing explicit review of the estimates and their behavior and accuracies prior to computations, e.g., Paredes et al. (2017), as well as to approach the basic Physics represented in the PM-ETo equation (Pereira et al. 2015). Likely for this reason, trends in ETo computed with the HS equation differ of PM-ETo largely more than those computed with PMT (Ren et al. 2016). Meanwhile, using geostationary satellite imagery (De Bruin et al. 2010; Cammalleri and Ciraolo 2013) is a good alternative for reduced data sets, and using gridded data sets and reanalysis weather products consist of computational alternatives that do not require new equations or new numerical methods but just applies the PM-ETo directly and accurately (Raziei and Pereira 2013b; Martins et al. 2017).

Few attempts to assess the accuracy of the PMT method are available in literature; contrarily, the performance of the HS equation is often reported in literature, including for humid climates. Irmak et al. (2003) for Florida, Yoder et al. (2005) in humid Southeast United States, and Trajkovic and Kolakovic (2009) in Western Balkans found poor performance of HS equation for humid conditions. Differently, other authors found good results for humid climates when calibrating the Hargreaves coefficient (Sentelhas et al. 2010; Tabari et al. 2013), or the k Rs coefficient (Todorovic et al. 2013; Raziei and Pereira 2013a; Almorox and Grieser 2016; Ren et al. 2016), and/or when replacing the exponent of (T max − T min) by a value smaller than the original 0.5 (Trajkovic 2007; Almorox and Grieser 2016). However, for an exponent different of 0.5 (Eqs. 9 and 11), the k Rs coefficient varies in a much wider interval (e.g., Almorox et al. 2016) and cannot be considered anymore as to reflect the volumetric heat capacity of the atmosphere. Our approaches to compute the HS equation (Raziei et al. 2013a; Ren et al. 2016) were also applied by Almorox et al. (2016) and their results confirmed ours when calibrating k Rs but not when changing the exponent. However, as discussed by Hargreaves and Allen (2003), recalibrations increase the complexity of the HS equation.

The first PMT studies closely followed the recommendations provided by Allen et al. (1998) and include those reported by Liu and Pereira (2001) and Pereira et al. (2003) for China, Popova et al. (2006) for Bulgaria, all referring to humid or sub-humid locations, and Jabloun and Sahli (2008), which also covered arid climates. All these studies have shown a better performance of the PMT approach relative to the HS equation. Moreover, those studies assessed positively the replacement of missing variables by their estimators as proposed by Allen et al. (1998): R s computed from the T max and T min difference, ea computed with T min replacing dew point temperature (T dew), as well as assuming the world average value of u 2 = 2 m s−1. Earlier studies by Annandale et al. (2002) were the first proposing a software to perform computations of ETo with the PM-ETo method and where missing variables were computed with those approaches. Another similar software was lately developed by Gocic and Trajkovic (2010), also including the HS equation.

ETo was estimated with the PM-ETo equation using daily weather forecast messages, i.e., R s was estimated from the forecasted cloudiness and T max and T min; the actual vapor pressure, e a, was estimated assuming T dew = T min, and u 2 was computed from the forecasted wind speed (Cai et al. 2007). This study referred to various Chinese sites with climates ranging from desert to humid. Errors of estimation of R s and e a were small and those for estimation of ETo were also small excepting for a hyper-arid location. Further, Cai et al. (2009) used daily weather forecast messages to estimate R s, e a, and u 2 for computing ETo used as input to a water balance model adopted for real time management of various field irrigation treatments of wheat. Good performances of the ETo and of its use in modeling were obtained (Cai et al. 2009). More recent studies have demonstrated that better performance of PMT is obtained when calibrating k Rs and adopting appropriate approaches to correct temperature when estimating e a (Todorovic et al. 2013; Raziei and Pereira 2013a; Ren et al. 2016). In addition, these studies have shown that k Rs varies with climate aridity. Differently, when there is no correction of T min as estimator of T dew and if k Rs is not calibrated, e.g., Martínez and Thepadia (2010), a poor performance of the PMT method may result.

Considering the discussion above on alternative procedures to compute ETo with reduced data sets and to estimate the missing variables as in the companion paper by Paredes et al. (2017) which provided for the first time appropriate information on estimating ETo and related missing variables in humid islands environments, the objectives of this study consist of (a) evaluating the accuracy of estimating daily ETo with the HS equation and the PMT approach and (b) assessing the impacts of wind speed estimation on the accuracy of the PMT approach. Computations apply to full weather data sets from 20 meteorological stations located in eight out of the nine islands of Azores.

2 Materials and methods

2.1 Study area and data

The archipelago of Azores comprises nine islands and is located in the North Atlantic at latitudes 36° 45′ N to 39° 43′ N and longitudes 24° 45′ W to 31° 17′ W (Fig. S2 in Supplementary Material). A description of the climate of the archipelago and of the weather stations was provided in the companion paper (Paredes et al. 2017).

Daily data used in the present study was collected in 20 weather stations in eight islands whose locations, basic climate characteristics and size of data sets are described in Table 1. Data included precipitation (P), maximum and minimum air temperatures (T max and T min, °C), relative humidity (RH, %), wind speed (m s−1), and solar radiation (R s, Watt m−2) or sunshine duration (n, h). A supplemental description of weather stations is given in Table S1 (Supplementary Material).

Table 1 Weather stations characteristics and date ranges of the weather data series

The Azorean climate is strongly influenced by its location in the middle of the North Atlantic Ocean, in a transition region between the sub-tropical Azores high pressure system and the mid-latitude storm track, and shows two clear seasons, winter when Azores are frequently crossed by the North Atlantic storm track (October to March concentrates 75% of the precipitation and two thirds of rainy days) and summer when climate is particularly influenced by the Azores anticyclone (Santos et al. 2004). Main characteristics of weather variables used in this study were analyzed in the companion paper and are available in Fig. S1 (Supplementary Material). Considering the focus of this paper and the importance of knowing ETo for crop and vegetation studies, namely when looking to climate change impacts and adaptation (e.g., Santos et al. 2004; Miranda et al. 2006), Fig. 1 shows the box-and-whisker plots of monthly PM-ETo for selected stations and the period of observations used in this study. Stations were selected to represent most of islands and related effects of longitude, and low and high altitude. The importance given to altitude relates to the type of pasture land use. Data show a clear distinction between summer and winter months, that ETo is much smaller in stations at medium to high elevation (S. Caetano, S. Bárbara, Lagoa do Fogo, and Fontinhas), and that ETo has a great variability in every month, particularly during summer, which is due to the frequent occurrence of cloud cover and precipitation.

Fig. 1
figure 1

The box-and-whisker plots including outliers (○) of monthly PM-ETo for selected stations. a Santa Cruz, Flores Island. b Horta, Faial Island. c São Caetano, Pico island. d Santa Cruz, Graciosa Island. e Ribeirinha, Terceira Island. f Santa Bárbara, Terceira Island. g Lagoa do Fogo, São Miguel Island. h Fontinhas, Santa Maria Island. The periods of observations are those in Table 1

2.2 Reference evapotranspiration computations

Grass reference ETo was defined by FAO after parameterizing the Penman-Monteith equation for a cool season grass (FAO56, Allen et al. 1998). Following Allen et al. 1998, daily PM-ETo (mm day−1) is given as

$$ {\mathrm{ET}}_{\mathrm{o}}=\frac{0.408\Delta \left({R}_{\mathrm{n}}-G\right)+\upgamma\ \frac{900}{{\mathrm{T}}_{\mathrm{mean}}+273}{\mathrm{u}}_2\left({e}_{\mathrm{s}}-{e}_{\mathrm{a}}\right)}{\Delta +\upgamma\ \left(1+0.34\ {\mathrm{u}}_2\right)} $$
(1)

where R n is the net radiation at the crop surface (MJ m−2 day−1), G is the soil heat flux density (MJ m−2 day−1), T mean is the mean daily air temperature at 2 m height (°C), u2 is the wind speed at 2 m height (m s−1), e s is the saturation vapor pressure (kPa), e a is the actual vapor pressure (kPa), VPD or e s-e a is the saturation vapor pressure deficit (kPa), Δ is the slope vapor pressure curve (kPa °C−1), and γ is the psychrometric constant (kPa °C−1). For daily computations, G equals zero as the magnitude of daily soil heat flux beneath the grass reference surface is very small (Allen et al. 1998). Hence, computations of PM-ETo require observed data on T max and T min, R s or sunshine duration (n), RH or psychrometric data, and wind speed at 2 m height (u 2). Although T max and T min are commonly well observed in many locations, the other variables are often not observed with good quality, or data sets are short and/or have frequent gaps, and their acquisition may be very expensive.

Computations require the adoption of the standard methods proposed by Allen et al. (1998) for computing the various parameters of Eq. (1). The vapor pressure deficit (VPD, kPa), difference between the saturation vapor pressure (e s, kPa) and the actual vapor pressure (e a, kPa), is computed with e s given as

$$ {\mathrm{e}}_{\mathrm{s}}=\frac{{\mathrm{e}}^{\mathrm{o}}\left({\mathrm{T}}_{\mathrm{max}}\right)+{\mathrm{e}}^{\mathrm{o}}\left({\mathrm{T}}_{\mathrm{min}}\right)}{2} $$
(2)

where e o(T max) and e o(T min) are the saturation vapor pressure at respectively the maximum and minimum daily temperatures (kPa), and e a computed as

$$ {\mathrm{e}}_{\mathrm{a}}=\frac{{\mathrm{e}}^{\mathrm{o}}\left({\mathrm{T}}_{\mathrm{min}}\right)\frac{{\mathrm{RH}}_{\mathrm{max}}}{100}+{\mathrm{e}}^{\mathrm{o}}\left({\mathrm{T}}_{\mathrm{max}}\right)\frac{{\mathrm{RH}}_{\mathrm{min}}}{100}}{2} $$
(3)

when there are observations of maximum and minimum relative humidity, RH max and RH min (%), or as

$$ {\mathrm{e}}_{\mathrm{a}}=\frac{{\mathrm{RH}}_{\mathrm{mean}}}{100}\left[\frac{{\mathrm{e}}^{\mathrm{o}}\left({T}_{\mathrm{max}}\right)+{\mathrm{e}}^{\mathrm{o}}\left({T}_{\mathrm{min}}\right)}{2}\right] $$
(4)

when only the mean daily relative humidity (RH mean, %) was available.

Considering that e a = e o(T dew), T dew is computed from e a as

$$ {\mathrm{T}}_{\mathrm{dew}}=\frac{116.91+237.3\ \ln \left({\mathrm{e}}_{\mathrm{a}}\right)}{16.78-\ln \left({\mathrm{e}}_{\mathrm{a}}\right)} $$
(5)

When RH data are missing, considering the relations for T dew in moist air (Lawrence 2005), for humid climates T dew is above T min and can be approximated using an empirical temperature adjustment coefficient ad (°C) that was locally calibrated for Azores as described in the companion paper (Paredes et al. 2017). Thus, T dew is estimated as

$$ {\mathrm{T}}_{\mathrm{dew}}=\left(\frac{{\mathrm{T}}_{\mathrm{max}}+{\mathrm{T}}_{\mathrm{min}}}{2}\right)-{a}_d $$
(6)

resulting that the actual vapor pressure is estimated from T dew (e a Tdew) adjusted with the calibrated parameter ad as

$$ {\mathrm{e}}_{\mathrm{a}\ \mathrm{Tdew}}={\mathrm{e}}^{\mathrm{o}}\left({\mathrm{T}}_{\mathrm{d}\mathrm{ew}}\right)=0.611\ \exp \left[\frac{17.27\ \left({\mathrm{T}}_{\mathrm{mean}}-{\mathrm{a}}_{\mathrm{d}}\right)}{\ \left({\mathrm{T}}_{\mathrm{mean}}-{\mathrm{a}}_{\mathrm{d}}\right)+237.3}\right] $$
(7)

where T dew is replaced by its value given by Eq. 6. As described in the companion paper, that estimation procedure was performed with very good accuracy.

Solar radiation, R s, was observed in all but one weather stations, Lajes, where sunshine duration (n, h) was observed; hence, R s was calculated as

$$ {\mathrm{R}}_{\mathrm{s}}=\left({\mathrm{a}}_{\mathrm{s}}+{\mathrm{b}}_{\mathrm{s}}\frac{\mathrm{n}}{\mathrm{N}}\right)\kern0.22em {\mathrm{R}}_{\mathrm{a}} $$
(8)

where, in addition to variables previously defined, N is the maximum possible daylight hours [h], n/N is the relative sunshine duration [−], R a is the extraterrestrial radiation [MJ m−2 day−1], as is the fraction of extraterrestrial radiation reaching the earth on overcast days (n = 0), and as + bs is the fraction of extraterrestrial radiation reaching the earth on clear sky days (n = N). Despite knowing that a greater accuracy of calculations with Eq. 8 is obtained when parameters as and bs are locally calibrated, the default parameters as = 0.25 and bs = 0.50 were used as recommended by Allen et al. (1998).

In the absence of observations, Allen (1997) and Allen et al. (1998) proposed to estimate R s for use with the PM-ETo equation using the Hargreaves and Samani (1982) equation that expresses R s as a linear function of the square root of the temperature difference T max − T min:

$$ {\mathrm{R}}_{\mathrm{s}\ \mathrm{TD}}={\mathrm{k}}_{{\mathrm{R}}_{\mathrm{s}}}{\left({\mathrm{T}}_{\mathrm{max}}-{\mathrm{T}}_{\mathrm{min}}\right)}^{0.5}{\mathrm{R}}_{\mathrm{a}} $$
(9)

where k Rs is an empirical radiation adjustment coefficient (°C-0.5) and R a is the extraterrestrial radiation (MJ m2 day−1). In this study, as described in the companion paper, the ETo estimates using Eq. 9 have shown a very good accuracy when k Rs were calibrated for all locations used in this study (Paredes et al. 2017).

Allen et al. (1998) proposed the use of the world average wind speed value u 2 = 2 m s−1 as default value (u 2 def) when wind speed data are missing. This default value was adopted for all stations except those located in airports but over grass, where u 2 def = 3 m s−1 was adopted due to high exposure to winds of all directions. Another studied alternative refers to the average wind speed data (u 2 avg) as considered by Popova et al. (2006) and Jabloun and Sahli (2008). To adjust wind speed data obtained from instruments placed at heights other than the standard height of 2 m, the following logarithmic wind speed profile (Allen et al. 1998) was used:

$$ {\mathrm{u}}_2={\mathrm{u}}_{\mathrm{z}}\kern0.62em \frac{4.87}{\ln\;\left(\kern0.24em 67.8\kern1.12em z\kern1.12em -\kern1.12em 5.42\;\right)} $$
(10)

where u 2 is the wind speed at 2 m above ground surface [m s−1], uz is the measured wind speed at z m height [m s−1], and z is the height of measurement above ground surface [m].

The use of the above referred approaches for estimating the parameters of the PM-ETo equation allows computing ETo with temperature data only as proposed in FAO56 (Allen et al. 1998). This approach is known as reduced set PM equation or PM-ETo temperature approach (PMT) as in the current paper.

The Hargreaves-Samani equation (HS, Hargreaves and Samani 1985) is also used in the current study. The HS equation estimates ETo (ETo-HS, mm d−1) from T max − T min and is written (Todorovic et al. 2013) as

$$ {\mathrm{ET}}_{\mathrm{o}-\mathrm{HS}}=0.0135\ {\mathrm{k}}_{\mathrm{R}\mathrm{s}}\frac{{\mathrm{R}}_{\mathrm{a}}}{\uplambda}\ {\left({\mathrm{T}}_{\mathrm{max}}-{\mathrm{T}}_{\mathrm{min}}\right)}^{0.5}\ \left({\mathrm{T}}_{\mathrm{mean}}+17.8\right) $$
(11)

where λ is the latent heat of vaporization (MJ kg−1) for the mean air temperature T mean (°C) and assumed to be 2.45 MJ kg−1, and k Rs (°C-0.5) and Ra (MJ m2 d−1) as defined for Eq. 9. The constant 0.0135 is a factor for conversion from American to the International system of units. k Rs was calibrated for all locations and for two seasons, winter and summer as reported by Paredes et al. (2017). The calibrated k Rs values are used with the PMT approach but a distinct calibration was performed for the HS equation.

Results of both ETo temperature estimation approaches were compared with the PM-ETo using full data sets as described in the next section.

2.3 Accuracy indicators

The accuracy of ETo computations with the PMT method (ETo-PMT) and the HS equation (ETo HS) was evaluated by comparing their results with those of the PM-ETo equation using full data sets. As per previous applications to ETo studies, namely by Martins et al. (2017) and similarly to assessments reported in the companion paper (Paredes et al. 2017), accuracy was measured with several statistical indicators:

  1. 1.

    The regression coefficient (b0) of the regression forced to the origin (FTO) between daily PM-ETo computed with observed data, Oi, and daily ETo computed with predicted variables, Pi. Values of b0 near 1 indicates that Oi and Pi are statistically close while b0 > 1 suggests overestimation and b0 < 1 underestimation.

  2. 2.

    The determination coefficient (R 2) of the ordinary least squares (OLS) regression between Oi and Pi, where a value close to 1.0 indicates that most of the variation of the PM-ETo values is explained by the simplified computation approach.

  3. 3.

    The root mean square error (RMSE, mm day−1) measures overall discrepancies between observed and estimated values, thus should be as small as possible.

  4. 4.

    The percent bias (PBIAS, %), which is a normalized difference between the means of both sets Oi and Pi, that indicates the average tendency for Pi under- or over-estimate Oi.

  5. 5.

    The Nash and Sutcliffe (1970) modeling efficiency (EF, non-dimensional) that provides an indication of the relative magnitude of the mean square error (MSE = RMSE2) relative to the observed data variance (Legates and McCabe Jr. 1999). The best value is EF = 1.0 that represents a perfect match between Pi and Oi and EF close to 1 means that the “noise” is negligible relative to the “information’, implying that alternative-based values of ETo are good estimators of PM-ETo values.

The joint assessment of this set of indicators provides a good evaluation of the quality of ETo computed with the PMT and HS approaches as in previous applications (Martins et al. 2017).

3 Results and discussion

3.1 Accuracy of the FAO-PMT method for ETo estimations

As previously analyzed in Section 2.2, the PMT computations included the use of T mean for T dew and e a estimation (e a Tdew, Eqs. 6 and 7), of the squared root of the temperature difference T max − T min for Rs calculations (R s TD, Eq. 8), and of the u 2 avg and u 2 def, referring respectively to the local average and to the default wind speed. Both the temperature adjustment coefficient ad (Eq. 6) and the radiation adjustment factor k Rs (Eq. 8) were calibrated for all locations and both the winter and summer seasons (Paredes et al. 2017) and are used herein for ETo-PMT calculations.

ETo-PMT estimations using the winter and summer calibrated ad (Eq. 6) and kRs (Eq. 8) and both wind speed estimators u 2 avg and u 2 def yielded very good accuracy indicators as shown in Table 2. When winter and summer calibrated ad and/or k Rs were different, computations were performed assigning those different values to the corresponding winter and summer months. Indicators in Table 2 are somewhat different due to using both u 2 avg and u 2 def. A detailed analysis by location may be performed using Table 2 but a global analysis is easier when considering the frequency of the various indicators as depicted in Fig. 2.

Table 2 Accuracy of the ETo-PMT estimation using both the u 2 local average (u 2 avg) and a default value (u 2 def) considering the calibrated adjustment factors for T dew (ad) and for solar radiation (k Rs)
Fig. 2
figure 2

Frequency distribution of the accuracy indicators relative to the computation of ETo with the FAO-PMT approach comparing the use of the annual wind speed averages ( ) with the default wind speed value ( )

Accuracy indicators when u 2 avg was used (Table 2 and Fig. 2) were good, nevertheless with a slight tendency for underestimation of PM-ETo values, with b0 generally close to 1.0 but varying from 0.94 to 1.01. Coherently, PBIAS results indicate an underestimation bias ranging from − 5 to − 10.2% in 65% of the locations, and a quite low PBIAS, ranging from − 5 to 2.5%, in 35% of the locations. R 2 values are higher than 0.60 in 85% of cases, which indicates that the variance of PM-ETo is quite well explained by the OLS regression on ETo-PMT. Using the default wind speed u2 def, the underestimation tendency prevails, with b0 ranging from 0.93 to 1.0, although PBIAS varied in a wider interval of − 10.4 to 3.1%, so including a few overestimation bias. R 2 values have a distribution similar to that relative to u 2 avg, also with 85% of cases with R 2 > 0.60. Estimation errors are small for all locations, with RMSE ranging from 0.47 to 0.74 mm day−1 when u 2 avg is used, and 0.48 to 0.73 mm day−1 if u 2 def is used. EF values are good and also quite similar for both estimators, ranging from 0.49 to 0.75 and from 0.46 to 0.76 respectively when u 2 avg or u 2 def are used. It may be concluded that both wind speed estimators provide for similar accuracy indicators and therefore there is evidence that u 2 def may be commonly used with the PMT approach together with the estimators of actual vapor pressure and short wave radiation when both ad and k Rs are seasonally calibrated.

Similar to ours (0.48 to 0 73 mm day−1), RMSE values were reported for daily ETo computations using the PMT approaches in inland sub-humid climates (Popova et al. 2006, Jabloun and Sahli 2008; Ren et al. 2016). Poor results were reported by Sentelhas et al. (2010) with RMSE up to 1.218 mm day−1 likely due to absence of adjustments of T dew and k Rs. Differently, Almorox et al. (2016) reported lower RMSE values for humid climates when calibrating k Rs for local conditions as well as when using T dew = T min and T dew = T min−2. Also better results are reported by Raziei and Pereira (2013a) for humid climates of Iran. Using ANNs to estimate ETo for the Basque region, northern Spain, Landeras et al. (2008) reported RMSE averages similar to our results when computations were performed with temperature data only. For the same region, Shiri et al. (2012, 2013), reported slightly better RMSE averages, also similar to ours, when using gene expressing programming or a neuro-fuzzy model with T max and T min only. Referred studies are, however, for less humid and windy climates than Azores islands but allow to assume that our PMT results are good and may be used in Azores when only T max and T min data are available.

The scatter plots in Fig. 3 highlight good relationships between ETo PMT using u 2 def and PM-ETo. Moreover, plots allow perceiving that slight overestimations occur for the smaller values of ETo, and underestimations occur for the high ETo values. However, under- and overestimations are more important for the stations located in high elevations (S. Caetano, S. Bárbara, and Lagoa do Fogo).

Fig. 3
figure 3

Comparing ETo PMT with PM-ETo for eight selected locations in various islands and having different environments. Included the FTO and the OLS regression equations and the OLS determination coefficient R 2

3.2 Accuracy of ETo PMT when reduced data sets lack two variables

The accuracy of ETo PMT when data sets lack both RH and u 2 was assessed comparing with PM-ETo and ETo PMT when the latter is computed with observed solar R s and the actual vapor pressure is estimated with Eq. 7 (e a Tdew) with the parameter ad calibrated locally and for the winter and summer seasons as referred above. Wind speed was estimated with both the local daily average u 2 avg and the default u 2 def but, confirming results above reported for ETo PMT, there were no meaningful differences in accuracy relative to both u 2 estimators (Table S2 and Fig. 4). Hence, in the following, only u2 def is considered. Overall indicators are reported in Table S2 (Supplementary Material) and their frequency is summarized in Fig. 4.

Fig. 4
figure 4

Frequency distribution of accuracy indicators relative to the computation of ETo PMT with observed solar radiation and using the estimator e a Tdew for actual vapor pressure and both wind speed estimators u 2 avg ( ) and u2 def ( )

It could be observed that the regression coefficient b0 ranged from 0.94 to 1.02 with 45% of cases within the shortest interval of 0.99 to 1.01. Therefore, with b0 values close to 1.0, a slightly underestimation trend occurs, with 85% of locations presenting a PBIAS ranging from − 5 to 2.5%. R 2 is generally high, ranging from 0.75 to 0.98 and most values above 0.80. In 95% of cases results have shown RMSE < 0.50 mm day−1 with all values ranging from 0.17 to 0.57 mm day−1; hence, errors are small. The modeling efficiency was very good, varying from 0.74 to 0.97, and 95% of cases with EF > 0.80. These indicators evidence that approaches used when both RH and u 2 data are missing are appropriate for Azores humid and windy climate conditions.

When observations of R s and u 2 are missing, ETo PMT was computed with observed e a data. R s was estimated with the R s TD estimator (Eq. 9) with k Rs calibrated for every local and for summer and winter conditions, as described before. As analyzed above, the estimator u 2 def was used for wind speed; nevertheless, the comparative analysis in Fig. 5 also includes u 2 avg. Overall accuracy indicators are reported in Table S3 (Supplementary Material) and their frequency is summarized in Fig. 5.

Fig. 5
figure 5

Frequency distribution of accuracy indicators of ETo-PMT estimation with observed RH and using the estimators R s TD for solar radiation and both the u 2 avg ( ) and u 2 def ( ) for wind speed

Values of b0 range between 0.92 and 1.01, which identifies a slight tendency for underestimation of PM-ETo. Consequently, in 60% of cases PBIAS ranges from − 5 to 2.5%, confirming the tendency for underestimation. R 2 is quite high, varying within the interval 0.70 to 0.90 in 90% of cases. Errors are small, with RMSE within the interval 0.30 to 0.50 mm day−1 in 65% of locations. EF was generally high since for 90% of cases it ranged from 0.70 to 0.90. Therefore, the above referred ETo PMT approach when e a is observed is quite accurate and appropriate for the humid and windy islands of Azores.

When only wind speed is available, the ETo-PMT was used with the estimators R s TD and e a Tdew. The accuracy indicators are shown in Table SI-4 and their frequency is summarized in Fig. 6. In agreement with previous analysis, a slight tendency for underestimation of ETo occurs. For 75% of locations, a b0 ≤ 0.98 was observed; consequently, an estimation bias higher than − 5% in 60% of locations was observed. The estimation errors are similar to those referred for ETo estimated with temperature only (0.48 to 0 73 mm day−1), however, slightly smaller, with RMSE < 0.70 for 90% of locations. The efficiency of modeling is good, ranging from 0.49 to 0.89 and with EF > 0.60 in 80% of the weather stations.

Fig. 6
figure 6

Frequency distribution of the accuracy indicators relative to the computation of ETo PMT with observed wind speed, actual vapor pressure estimated with e a Tdew and solar radiation R s estimated as R s TD using respectively ad and k Rs locally and seasonally calibrated

3.3 Accuracy of ETo estimation with the Hargreaves-Samani equation

The Hargreaves-Samani equation (HS, Eq. 11) is often used but not with very good results in humid climates as analyzed before. This fact may relate to the fact that authors do not calibrate the k Rs factor or perform such calibration using a less good approach. To overcome related problems, k Rs was calibrated locally without significant seasonal differences.

Accuracy indicators relative to the application of the HS equation for computing ETo using a calibrated k Rs factor are shown in Table 3 and Fig. 7. Results show a b0 ranging from 0.96 to 1.03, however with a slight underestimation tendency and, consequently, with 70% of cases showing an underestimation bias (PBIAS < − 2.5%). R 2 range 0.60 to 0.80 in 90% of cases. RMSE are relatively small, from 0.47 to 0.86 mm day−1, with 65% of the stations showing RMSE > 0.60 mm day−1. EF values are acceptable to good, with 45% of cases having EF < 0.60. Results analyzed above indicate that the HS equation may be used in Azores islands as alternative to the PMT method.

Table 3 Accuracy of ETo estimations using the Hargreaves-Samani equation after calibrating the kRs factor
Fig. 7
figure 7

Frequency distribution of the accuracy indicators relative to ETo-HS estimation

To better assess the relationships, ETo HS and PM-ETo scatter plots were used (Fig. 8). They show that those relationships are non-linear for the locations at high elevation but not exposed to strong winds (S. Caetano, S. Bárbara, and Lagoa do Fogo). For these conditions, overestimations of small ETo values and, particularly, underestimation of high ETo vales are greater than for other locations and when using the PMT method (Fig. 3). That non-linearity may be explained by the relatively small difference T max − T min (Fig. SI-2). Impacts of wind speed were not detected.

Fig. 8
figure 8

Comparing ETo HS with PM-ETo computed with full data sets for eight selected locations in various islands and having different environments. Included the FTO and the OLS regression equations and the OLS determination coefficient R 2

A tendency for the overestimation of ETo when using the original ETo-HS is reported in most studies performed in humid climates but studies relative to the use of HS after calibration of the k Rs coefficient report a decrease in the estimation errors relative to the use of a default value for the Hargreaves coefficient or k Rs. Estimation errors lower than those in the present study (0.47 to 0.86 mm day−1) were reported for several humid locations in the north-eastern Italy (Berti et al. 2014). Ren et al. (2016) for several locations in Mongolia, China indicated RMSE < 0.61 mm day−1 after appropriate calibration of k Rs. Aladenola and Madramootoo (2014) reported very high RMSE values for humid locations in Canada. Vanderlinden et al. (2004) calibrated the product 0.0135 k Rs for coastal areas and report RMSE ranging from 0.60 to 0.95 mm day−1. Mendicino and Senatore (2013) also calibrated the product 0.0135 k Rs and reported a mean absolute error ranging 0.32 to 1.24 mm day−1. This comparison with already published errors of estimate support the quite good results obtained in the current study.

3.4 Comparing the PMT and HS approaches

Comparing the application of PMT method with HS equation in the present study (Fig. 9), results show that indicators are not very different after proper calibration of k Rs. All regression coefficients relative to HS equation fall in the interval 0.95 to 1.05 while those for PMT are below 0.95 in 10% of cases. However, the PMT presents slightly lower bias of estimation. R 2 show a very similar distribution (Fig. 9). Lower RMSE, with only 20% of cases above 0.70 mm day−1 were observed for PMT while that frequency increases to 30% when HS is applied. Relative to PMT, 80% of cases have EF > 0.60 while this frequency is only 55% for HS. These results indicate that the use of PMT method is more appropriate than HS in humid island environments when only temperature data are available. Similar better accuracy results of the ETo-PMT relative to ETo-HS were obtained in a monsoon climate in Northern China (Liu and Pereira 2001; Pereira et al. 2003) and in sub-humid climates of Inner Mongolia (Ren et al. 2016). Todorovic et al. (2013) and Almorox et al. (2016) found a better performance of PMT relative to HS for monthly time-step within a wide variety of climates. Martínez and Thepadia (2010) also reported that PMT performed better than HS.

Fig. 9
figure 9

Frequency distribution of the “goodness-of-fit” indicators relative to the computation of ETo with the PMT approach with u 2 def () and the Hargreaves-Samani equation ()

For comparing HS with PMT approaches, linear FTO and OLS regressions between ETo HS and ETo PMT were developed (Fig. 10). They show a tendency for ETo HS to overestimate ETo PMT for locations at low elevation, near the sea (Santa Cruz das Flores, Horta and Santa Cruz da Graciosa). For the remaining locations, only a slight tendency for over-estimating the large ETo values and under-estimate the small ones was detected.

Fig. 10
figure 10

Comparing ETo HS with ETo PMT, for eight selected locations in various islands and having different environments. Included the FTO and the OLS regression equations and the OLS determination coefficient R 2

4 Conclusions

The spatial variability of climatic conditions that drive evapotranspiration is a matter of special importance for local agriculture and water management purposes in small volcanic islands, as it is the case of the Azores Islands. However, in these environments, the observation of surface meteorological data required for accurate PM-ETo computation is insufficient, with data not reflecting the high spatial variation of the climate as influenced by elevation, exposure to dominant winds and longitude. Therefore, it was of great importance to assess calculation approaches that provide for accurate ETo estimation using reduced data sets. Their application made it evident the influence of those factors on ETo estimation as well as the seasonality of its climatic drivers.

The approaches proposed by Allen et al. (1998) to estimate ETo using reduced data sets were tested considering recent developments for estimation of the actual vapor pressure (e a Tdew) and the short wave solar radiation (R s TD) after appropriate local and seasonal calibration of the respective adjustment factors, ad and k Rs, as discussed in the companion paper (Paredes et al. 2017). Tested approaches of the PM temperature method for humid island environments referred to the use of temperature data only and to cases when, in addition to temperature, some variables are observed, thus when estimates e a Tdew, R s TD or u 2 def are used together with observed variables. The PMT method yielded accurate results as analyzed using a set of accuracy indicators. Meanwhile, ETo results have shown to be influenced by the altitude and exposure to dominant winds.

Both temperature methods, the PMT approach and the Hargreaves-Samani equation, also using locally calibrated k Rs factors, were compared. Both approaches have shown good accuracy in representing the temporal behavior of ETo in all locations with relatively low estimation errors: RMSE ranging from 0.48 to 0.73 mm day−1 for PMT and from 0.47 to 0.86 mm day−1 for HS. However, PMT yielded better accuracy results for most locations, namely smaller RMSE and higher EF. In addition, ETo results of the HS equation have shown not to vary linearly with those of the PM-ETo equation for high elevation sites and, with a lesser extent, for windy locations. Moreover, contrarily to HS equation, PMT can be used combining data on observed variables with estimators of missing ones, which is helpful when using reduced data sets. Thus, for the Atlantic islands of Azores, accuracy results indicated the appropriateness of using PMT, including because this method approaches the Physics base of the original PM-ETo equation. Meanwhile, further and deep studies are desirable to better understand the variability of ETo in the humid climatic environments of Azores archipelago, as well as the role of related driving factors.