Daily Net Radiation
Net radiation requires the determination of both incoming and reflected short-wave radiation and net long-wave or thermal radiation. Expressing net radiation in terms of the net short-wave and long-wave components gives:
Hnet=Hday↓−α∗Hday↑+HL↓−HL↑ 1:1.2.11
or
Hnet=(1−α)∗Hday+Hb 1:1.2.12
where Hnet is the net radiation (MJm−2d−1), Hday is the short-wave solar radiation reaching the ground (MJm−2d−1), is the short-wave reflectance or albedo, HL is the long-wave radiation (MJm−2d−1), Hbis the net incoming long-wave radiation (MJm−2d−1) and the arrows indicate the direction of the radiation flux.
Net Short-Wave Radiation
Net short-wave radiation is defined as (1−α)∗Hday . SWAT+ calculates a daily value for albedo as a function of the soil type, plant cover, and snow cover. When the snow water equivalent is greater than 0.5 mm,
α=0.8 1:1.2.13
When the snow water equivalent is less than 0.5 mm and no plants are growing in the HRU,
α=αsoil 1:1.2.14
where soil is the soil albedo. When plants are growing and the snow water equivalent is less than 0.5 mm,
α=αplant∗(1−covsol)+αsoil∗covsol 1:1.2.15
where plant is the plant albedo (set at 0.23), and covsol is the soil cover index. The soil cover index is calculated
covsol=exp(−5.0X10−5∗CV) 1:1.2.16
where CV is the aboveground biomass and residue (kgha−1).
Net Long-Wave Radiation
Long-wave radiation is emitted from an object according to the radiation law:
HR=ε∗σ∗TK4 1:1.2.17
where HR is the radiant energy (MJm−2d−1), is the emissivity, is the Stefan-Boltzmann constant (4.90310−9MJm−2K−4d−1), and TK is the mean air temperature in Kelvin (273.15 + C). Net long-wave radiation is calculated using a modified form of equation 1:1.2.17 (Jensen et al., 1990):
Hb=fcld∗(εa−εvs)∗σ∗TK4 1:1.2.18
where Hb is the net long-wave radiation (MJm−2d−1), fcld is a factor to adjust for cloud cover, a is the atmospheric emittance, and vs is the vegetative or soil emittance.
Wright and Jensen (1972) developed the following expression for the cloud cover adjustment factor, fcld:
fcld=a∗HMXHday−b 1:1.2.19
where a and b are constants, Hday is the solar radiation reaching the ground surface on a given day (MJm−2d−1), and HMX is the maximum possible solar radiation to reach the ground surface on a given day (MJm−2d−1). The two emittances in equation 1:1.2.18 may be combined into a single term, the net emittance . The net emittance is calculated using an equation developed by Brunt (1932):
ε′=εa−εvs=−(a1+b1∗(e)) 1:1.2.20
where a1 and b1 are constants and e is the vapor pressure on a given day (kPa). The calculation of e is given in Chapter 1:2. Combining equations 1:1.2.18, 1:1.2.19, and 1:1.2.20 results in a general equation for net long-wave radiation:
Hb=−[a∗HMXHday−b]∗[a1+b1∗(e)]∗σ∗Tk4 1:1.2.21
Experimental values for the coefficients a,b,a1and b1 are presented in Table 1:1.3. The default equation in SWAT+ uses coefficient values proposed by Doorenbos and Pruitt (1977):
Hb=−[0.9∗HMXHday+0.1]∗[0.34−0.139(e)]∗σ∗Tk4 1:1.2.22
Table 1:1-3: Experimental coefficients for net long-wave radiation equations (from Jensen et al., 1990).
Davis, California
(1.35,
-0.35)
(0.35,
-0.145)
Southern Idaho
(1.22,
-0.18)
(0.325,
-0.139)
England
not available
not available
(0.47,
-0.206)
England
not available
not available
(0.44,
-0.253)
Australia
not available
not available
(0.35,
-0.133)
General
(1.2
-0.2)
(0.39,
-0.158)
General-humid areas
(1.0
0.0)
General-semihumid areas
(1.1
-0.1)
Table 1:1-4: SWAT+ input variables used in net radiation calculations.
SOL_ALB
soil: moist soil albedo
.sol
MAX TEMP
Tmx: Daily maximum temperature (C)
.tmp
MIN TEMP
Tmn: Daily minimum temperature (C)
.tmp
SOL_RAD
Hday: Daily solar radiation reaching the earth’s surface (MJ m-2 d-1)
.slr
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