# 1:1.2.5 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:

$$H\_{net}=H\_{day}\downarrow-\alpha\*H\_{day}\uparrow+H\_L\downarrow-H\_L\uparrow$$                                                                                            1:1.2.11

or

$$H\_{net} = (1-\alpha) H\_{day} + H\_b$$                                                                                                                              1:1.2.12

where $$H\_{net}$$ is the net radiation ($$MJ  m^{-2}   d^{-1}$$), $$H\_{day}$$ is the short-wave solar radiation reaching the ground ($$MJ m^{-2} d^{-1}$$), is the short-wave reflectance or albedo, $$H\_L$$ is the long-wave radiation ($$MJ m^{-2} d^{-1}$$), $$H\_b$$ is the net incoming long-wave radiation ($$MJ m^{-2} d^{-1}$$) and the arrows indicate the direction of the radiation flux. &#x20;

### 1:1.2.5.1 Net Short-Wave Radiation

Net short-wave radiation is defined as $$(1-\alpha) H\_{day}$$. 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,

$$\alpha=0.8$$                                                                                                                                                                   1:1.2.13      &#x20;

When the snow water equivalent is less than 0.5 mm and no plants are growing in the HRU,

$$\alpha=\alpha\_{soil}$$                                                                                                                                                                1:1.2.14

where $$\alpha\_{soil}$$ is the soil albedo. When plants are growing and the snow water equivalent is less than 0.5 mm,  &#x20;

&#x20;$$\alpha=\alpha\_{plant} (1-cov\_{sol})+\alpha\_{soil} cov\_{sol}$$                                                                                                           1:1.2.15

where $$\alpha\_{plant}$$ is the plant albedo (set at 0.23), and $$cov\_{sol}$$ is the soil cover index. The soil cover index is calculated

$$cov\_{sol}=exp(-5.0X10^{-5}\*CV)$$                                                                                                                 1:1.2.16

where $$CV$$ is the aboveground biomass and residue ($$kg  ha^{-1}$$).

### 1:1.2.5.2 Net Long-Wave Radiation

Long-wave radiation is emitted from an object according to the radiation law:

$$H\_R=\varepsilon \sigma T\_K^{4}$$                                                                                                                                                          1:1.2.17

where $$H\_R$$ is the radiant energy ($$MJ m^{-2} d^{-1})$$, $$\varepsilon$$ is the emissivity, $$\sigma$$ is the Stefan-Boltzmann constant  ($$4.903    10^{-9} MJ m^{-2} K^{-4} d^{-1})$$, and $$T\_K$$ is the mean air temperature in Kelvin (273.15 + $$\degree C$$). Net long-wave radiation is calculated using a modified form of equation 1:1.2.17 (Jensen et al., 1990):

&#x20;$$H\_b=f\_{cld} (\varepsilon\_a -\varepsilon\_{vs}) \sigma T\_K^{4}$$                                                                                                                                 1:1.2.18

where $$H\_b$$ is the net long-wave radiation ($$MJ m^{-2} d^{-1}$$), $$f\_{cld}$$ is a factor to adjust for cloud cover, $$\varepsilon\_a$$ is the atmospheric emittance, and $$\varepsilon\_{vs}$$ is the vegetative or soil emittance.&#x20;

Wright and Jensen (1972) developed the following expression for the cloud cover adjustment factor, $$f\_{cld}$$: &#x20;

$$f\_{cld}=a \frac{H\_{day}}{H\_{MX}}-b$$                                                                                                                                                  1:1.2.19

where $$a$$ and $$b$$ are constants, $$H\_{day}$$ is the solar radiation reaching the ground surface on a given day        ($$MJ m^{-2}d^{-1}$$), and $$H\_{MX}$$ is the maximum possible solar radiation to reach the ground surface on a given day ($$MJ m^{-2}d^{-1}$$).&#x20;

The two emittances in equation 1:1.2.18 may be combined into a single term, the net emittance $$\varepsilon'$$. The net emittance is calculated using an equation developed by Brunt (1932):        &#x20;

$$\varepsilon'=\varepsilon\_a-\varepsilon\_{vs}=-(a\_1+b\_1 \sqrt{(e)})$$                                                                                                                 1:1.2.20

where $$a\_1$$ and $$b\_1$$ 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: &#x20;

$$H\_b=-\[a \frac{H\_{day}}{H\_{MX}}-b] \[a\_1+b\_1 \sqrt{(e)}] \sigma T\_k^4$$                                                                                                        1:1.2.21

Experimental values for the coefficients $$a,b,a\_1$$, and $$b\_1$$ are presented in Table 1:1.3. The default equation in SWAT+ uses coefficient values proposed by Doorenbos and Pruitt (1977):&#x20;

$$H\_b=-\[0.9 \frac{H\_{day}}{H\_{MX}}+0.1] \[0.34-0.139\sqrt{(e)}] \sigma T\_k^4$$                                                                                     1:1.2.22

Table 1:1-3: Experimental coefficients for net long-wave radiation equations (from Jensen et al., 1990).

<table><thead><tr><th width="183">Region</th><th>(a,</th><th>b)</th><th>(a1,</th><th>b1)</th></tr></thead><tbody><tr><td>Davis, California</td><td>(1.35,</td><td>-0.35)</td><td>(0.35,</td><td>-0.145)</td></tr><tr><td>Southern Idaho</td><td>(1.22,</td><td>-0.18)</td><td>(0.325,</td><td>-0.139)</td></tr><tr><td>England</td><td>not available</td><td>not available</td><td>(0.47,</td><td>-0.206)</td></tr><tr><td>England</td><td>not available</td><td>not available</td><td>(0.44,</td><td>-0.253)</td></tr><tr><td>Australia</td><td>not available</td><td>not available</td><td>(0.35,</td><td>-0.133)</td></tr><tr><td>General</td><td>(1.2</td><td>-0.2)</td><td>(0.39,</td><td>-0.158)</td></tr><tr><td>General-humid areas</td><td>(1.0</td><td>0.0)</td><td></td><td></td></tr><tr><td>General-semihumid areas</td><td>(1.1</td><td>-0.1)</td><td></td><td></td></tr></tbody></table>

Table 1:1-4: SWAT+ input variables used in net radiation calculations.

| Definition                                                                             | Source Name | Input Name | Input File                                                                                                |
| -------------------------------------------------------------------------------------- | ----------- | ---------- | --------------------------------------------------------------------------------------------------------- |
| $$\alpha\_{soil}$$: moist soil albedo                                                  | alb         | alb        | [soils.sol](https://swatplus.gitbook.io/io-docs/introduction-1/soils/soils.sol)                           |
| $$T\_{mx}$$: Daily maximum temperature ($$\degree C$$)                                 | max temp    | tmpmax     | [.tmp](https://swatplus.gitbook.io/io-docs/introduction-1/climate/tmp.cli-and-temperature-data-files)     |
| $$T\_{mn}$$: Daily minimum temperature ($$\degree C$$)                                 | min temp    | tmpmin     | [.tmp](https://swatplus.gitbook.io/io-docs/introduction-1/climate/tmp.cli-and-temperature-data-files)     |
| $$H\_{day}$$: Daily solar radiation reaching the earth’s surface ($$MJ m^{-2}d^{-1}$$) | solrad      | slr        | [.slr](https://swatplus.gitbook.io/io-docs/introduction-1/climate/slr.cli-and-solar-radiation-data-files) |
