2.1.1. General Equations
The physical process, whereby water flows from evaporating surfaces into the atmosphere, is referred to as actual evapotranspiration (ET). This water flux occurs via canopies through stomata as actual transpiration and directly from the soil surface as actual evaporation. Stomata are small openings on the plant leaf through which gases and water vapor pass. The vaporization occurs within the leaf, in the intercellular spaces, and the vapor exchange with the atmosphere is controlled by the stomatal aperture, which can be open and closed, depending on the pressure of the guard cell. Nearly all soil water taken up by roots is lost by transpiration and a negligible fraction is used within the plant. Not only the type of crop, but also the crop development, environment, cultural management and irrigation system should be considered when assessing transpiration.
For modeling ET, distinctions are made between reference crop evapotranspiration (ET
0) and actual evapotranspiration (ET). ET
0 is the evapotranspiration rate from a reference surface, not short of water, which can be a hypothetical grass surface with specific characteristics, while ET involves all conditions of any vegetated surface. Agro-meteorological parameters, vegetation characteristics, management and environmental aspects affect ET. Other factors to be considered are ground cover, plant density, plant architecture, microclimate and soil moisture. Considering irrigated crops, cultivation practices and the type of irrigation system, can alter the microclimate, affecting the canopy characteristics and the moisture content of the soil and the plants. The effect of soil moisture on water fluxes is primarily conditioned by the magnitude of the water deficit and the type of soil. On the other hand, too much water will result in water logging, which might damage the root and limit root water uptake by inhibiting respiration [
61].
Evapotranspiration is an energy consuming process, referred to as the latent heat flux (λE). ET can be derived from the latent heat of vaporization (λ), density of water and λE. As a first approximation, an ET of 1 mm d
−1 is equivalent to a λE of 28 W m
−2, being therefore the chain between the water and energy balances. All energy fluxes should be considered when deriving the energy balance equation, which for a given surface can be written as:
where R
n is the net radiation, H is the sensible heat flux and G is the soil heat flux. All terms in Equation 1 can be expressed in W m
−2 or MJ m
−2 d
−1, being either positive or negative. Positive R
n means energy flux to the surface and positive G, λE and H indicate fluxes of energy from the surface. Equation 1 states that the R
n is redistributed over H, λE and G, considering only vertical fluxes and ignoring the net rate at which energy is being transferred horizontally, by advection; however, this term can be significant near the edges of crops or natural vegetation [
62]. Therefore it is accurate only when applied to large, extensive surfaces. Other energy terms, such as heat stored or released in the canopies, or the energy used in metabolic activities, are not considered. These last terms account only for a small fraction of the daily R
n and can be neglected in hydrological studies.
The atmosphere warms up when R
n is positive. Heating of the atmosphere occurs from the land surface, thus the surface temperature (T
0) during daylight hours exceeds the air temperature (T
a). H is the rate of heat loss to the air by convection and conduction, due to a temperature difference, being expressed by the following equation for heat transport [
63]:
where ρ
a is air density (kg m
−3), c
p is air specific heat at constant pressure (J kg
−1 K
−1), T
0 and T
a are in K; and r
ah is the aerodynamic resistance to heat transport in the boundary above the land surface (s m
−1) applicable to the same two heights.
λE can be determined as:
where γ is the psychrometric constant (kPa °C
−1); e
a is the actual water vapor pressure of the air (kPa) at the reference height above the surface (z); r
s and r
av are respectively the surface and aerodynamic resistances (s m
−1) to the latent heat flux; and e
s(T
0) is the saturated water vapor pressure (kPa) at T
0.
These fundamental equations constitute the base for regional ET modeling approaches, which use remotely-sensed radiances. The transfer equations for H (Equation 2) and for λE (Equation 3) were combined [
64] into the surface energy balance (Equation 1), and the world wide accepted combination equation for open water evaporation was developed. The combination equation was modified into a version that can be applied to the vegetated surfaces by inserting a canopy resistance [
65], eliminating T
0 from Equations 1–3.
Considering r
ah and r
av nearly equal in practice, and replaced by r
a for both heat and vapor flux transports, the PM equation to predict ET from vegetated surfaces [
61] became:
where Δ (kPa °C
−1) is the slope of the saturated vapor pressure curve and D (kPa) is the vapor pressure deficit in the air near the vegetated surfaces.
The difficulties of using Equation 4, especially at the regional scale, are considered to be the estimations of r
a and r
s [
66]. Differences in crop height and leaf area index (LAI) determine crop roughness and thereby r
a. Crop rooting characteristics, root water uptake and LAI influence the value of r
s. With the availability of the evapotranspiration resistances, ET can be derived from agro-meteorological data by means of Equation 4, providing a good approach because it combines the main drivers of water fluxes; provides an energy constraint on the water fluxes; and modeled ET are not overly sensitive to any of the inputs [
23]. The magnitude of r
s is mainly governed by environmental entities and soil moisture status [
67,
68]. Where the vegetation does not completely cover the soil, r
s includes the effects of the soil evaporation. With field values of λE, R
n, G, r
a and microclimatic data, r
s can be estimated inverting Equation 4 [
5,
13,
14], and together with remote sensing parameters, the ET at the regional scale can be obtained. On the other hand, Equation 4 applied to the reference crop allows the modeling of the ratio ET/ET
0 with satellite variables. The next section describes the steps for modeling by using the PM equation in these two ways.
2.1.2. Penman-Monteith models
Table 1 summarizes the steps for modeling the regional ET by the two models based on the PM equation. For the first model (PM1), the radiation balance was done with locally calibrated equations and satellite values of R
n, G and the evapotranspiration resistances together with weather data, while for the second one (PM2), the only remote sensing parameters are the surface albedo (α
0), the surface temperature (T
0) and the Normalized Difference Vegetation Index (NDVI). For both models, the ratio ET/ET
0 is applied to grids of ET
0 at instantaneous and daily time scales.
Table 1.
Summary of the regression analyses.
Table 1.
Summary of the regression analyses.
Parameter | Equation | a | b | R2 |
---|
α0 | α0 = aαp + b | 0.70 | 0.06 | 0.96 |
T0 | T0 = aTsat + b | 1.11 | −31.89 | 0.95 |
εa | εa = a(−lnsw)b | 0.94 | 0.10 | 0.75 |
ε0 | ε0 = alnNDVI + b | 0.06 | 1.00 | 0.90 |
G/Rn | G/Rn = aexp(bα0) | 3.98 | −25.47 | 0.90 |
z0m | z0m = exp [(aNDVI/α0) + b] | 0.24 | −2.12 | 0.92 |
rs | rs = exp[a(T0/α0)(1 − NDVI) + b] | 0.04 | 2.72 | 0.93 |
ra | ra = azoh−1 + b | 0.22 | 29.5 | 0.78 |
ET/ET0 | ET/ET0 = exp{a + b[T0/( α0NDVI)]} | 1.90 | −0.008 | 0.91 |
Figure 1 shows the radiation balance for obtaining R
n with the parameterizations of
Table 1, necessary for the PM1 model.
Figure 1.
Schematic flowchart for the regional radiation balance for PM1 model.
Figure 1.
Schematic flowchart for the regional radiation balance for PM1 model.
Simple regression equations were used for atmospheric correction to obtain the regional values of α
0 and T
0 by using field and satellite measurements. The satellite measured radiances are affected by the atmospheric interaction in the radiative transfer path, being part of the incident global solar radiation (R
G) scattered back before it reaches the earth surface. A simplified linear relationship between α
0 measured by pyranometers in the field and the planetary albedo by Landsat satellite (α
p) has been applied [
69]. From the field energy balance experiments, the aerodynamic surface temperature (T
0) was calculated from Equation 2 while the radiometric surface temperature was obtained from the Landsat band 6 (T
sat). Other than for a thin surface, a difference arises between radiometric and aerodynamic surface temperatures [
70]. Excellent agreement was found between aerodynamic surface and canopy radiometric temperatures for a dense, fully closed wheat crop [
71], however, for sparse or composite vegetation, the differences increase [
72]. The satellite thermal radiation was therefore corrected for both atmospheric emission and the difference between radiometric and surface temperature by applying a regression equation with field and satellite values (
Table 1).
Considering that the field measurements involved contrasting hydrological surfaces with different values for α
0; for the use of the Equation 2 for estimating T
0, microclimatic measurements with stability corrections were applied to r
a in flux profile relationships. Since EC systems directly provide u
*, with good agreements of H when comparing field and satellite values [
27], it is assumed that the two key first regressions from
Table 1 have good accuracy in the semi-arid region of the Low-Middle São Francisco river basin.
In the regional radiation balance (
Figure 1), the net short wave radiation available at the earth surface depends on R
G and α
0.
Measured R
L↓ over natural vegetation (caatinga)—in combination with microclimatic data of air temperature (T
a)—accorded the inspection of the apparent emissivity of the atmosphere (ε
a). The regional values of R
L↓ were then estimated from the Stefan Boltzman equation by using the relation of ε
a with the atmospheric transmissivity (τ
sw) together with grids of T
a from the net of agro-meteorological stations. τ
sw was, in turn, calculated by the ratio of the grid of R
G measured by the net of pyrometers and the solar radiation at the top of the atmosphere (R
a) [
27]. For R
L↑, the Stefan Boltzman equation was applied using images of T
0 and the correlation of field values of surface emissivity (ε
0) and satellite measurements of NDVI [
73], this last parameter being obtained from the infrared and red regions of the Landsat images.
The regional values of R
n resulted from the balance of all short and long wave radiations (
Figure 1). The term G in large scale was acquired by an exponential relation of field values of the ratio G/R
n and α
0, assuming that both ratios are dependent on the type and architecture of the vegetation and soil moisture conditions and that the exponential relation was the best found for comparing the two ratios involving natural vegetation and irrigated crops (R
2 = 0.96) under several hydrological conditions in semi-arid region of Brazil (
Table 1).
The behavior of z
0m in natural vegetation and irrigated crops was described for the semi-arid conditions of the Low-Middle São Francisco river basin [
14]. To estimate this roughness parameter at the regional scale from remote sensing measurements, a simplified expression based on α
0 from field measurements and NDVI from satellite images, with locally calibrated regression coefficients shown in
Table 1 was used. The inclusion of α
0 helps to distinguish between vegetation having different architecture but similar values of NDVI [
48]. For example table grape may present the same NDVI values as mango orchard, but substantially lower LAI. The coefficient of determination is rather encouraging for describing a difficult land surface parameter by some simplified remote sensing variables.
For the PM1 model, r
a was estimated from the roughness length for heat transport (z
0h), which in turn was considered as a function of z
0m (z
0h = 0.1 z
0m) [
61]. This relation is very useful, as there is no unique relationship between surface roughness characteristics such as the geometry of the roughness elements and z
0h [
74,
75]. The low determination coefficient in
Table 1 is not a problem, because Equation 4 is insensitive to r
a, especially when r
a << r
s and at daily timescales [
23]. Finally, to complete the resistance terms in the PM equation, the field values of r
s were correlated with the field values of T
0, α
0 and satellite measurements of NDVI. For PM2 model, the instantaneous ET/ET
0 field values were also modeled with field values of T
0 and α
0 together with satellite data of NDVI (
Table 1).
Figure 2 presents the schematic overview to convert spectral radiance into ET by using the satellite parameters and the grids of daily ET
0 when applying the PM2 model.
Figure 2.
Schematic flowchart for calculating the actual evapotranspiration when applying the PM2 model.
Figure 2.
Schematic flowchart for calculating the actual evapotranspiration when applying the PM2 model.
After converting the spectral radiances and the atmospheric corrections, the images of NDVI, α
0 and T
0 are the only input parameters for estimating the instantaneous values of the ratio ET/ET
0 without the need of the regional radiation balance shown in
Figure 1. The instantaneous values of this ratio are multiplied by the daily grids of ET
0 to estimate the regional ET for 24 hours.
Both, r
s and ET/ET
0 values are related to the soil moisture conditions and so are the remote sensing vegetation indicators such as NDVI, α
0 and T
0. Based on this principle, two models were proposed. The relationship between vegetation indices with soil moisture and ET rates have been reported in the semi-arid region of Brazil [
14,
27]. The relations for modeling the regional ET in a mixture of natural vegetation and irrigated crops are depicted in
Figure 3.
For the first model based on direct application of Equation 4 (PM1), the images of R
n, G, r
s and r
a, are used together with the interpolated weather data from the net of agro-meteorological stations (
Table 1;
Figure 1,
Figure 3a and
Figure 3b). The regional values of λE are acquired and transformed into millimeters of water (ET). After the determination of ET at the regional scale, the instantaneous ratio of ET/ET
0 is calculated with grids of ET
0 for these same spatial and time scales. The second model (PM2) is based on the modeling of ET/ET
0 at the satellite overpass time (subscript sat) at the regional scale (
Table 1 and
Figure 3c). The instantaneous images of ET/ET
0 obtained by both models are then multiplied by the grids of ET
0 for 24 hours.
The satellite overpass time values of ET/ET
0 and those for 24 hours in irrigated mango orchard and caatinga were compared (
Figure 3d). The slope is close to one, supporting the assumption that instantaneous and daily ratios can be considered equal. A factor of 1.18 for the evaporative fraction [EF = λE/(R
n − G)] was necessary to extrapolate the latent heat fluxes from satellite overpass to daily time scale based on field and satellite measurements in the semi-arid conditions of the Low-Middle São Francisco river basin, Brazil [
14,
37].
Figure 3.
Relations for the evapotranspiration resistances and ET/ET0 ratio. (a) Surface resistance (rs); (b) aerodynamic resistance (ra); (c) satellite overpass time value of ET/ET0 (subscript sat). (d) daily values of ET/ET0 (subscript 24). T0: surface temperature; α0: surface albedo; NDVI: Normalized Difference Vegetation Index; z0h: roughness length for heat transport.
Figure 3.
Relations for the evapotranspiration resistances and ET/ET0 ratio. (a) Surface resistance (rs); (b) aerodynamic resistance (ra); (c) satellite overpass time value of ET/ET0 (subscript sat). (d) daily values of ET/ET0 (subscript 24). T0: surface temperature; α0: surface albedo; NDVI: Normalized Difference Vegetation Index; z0h: roughness length for heat transport.
The coefficients of determination in
Figure 3a and
Figure 3c are very good (R
2 > 0.90). The lower value for r
a (
Figure 3b) is not a big problem since, according to some sensitivity analysis errors in λE estimations, changes in the magnitudes of this resistance do not cause large errors, because it appears in both the numerator and the denominator of the PM equation [
23,
76].