> For the complete documentation index, see [llms.txt](https://swatplus.gitbook.io/io-docs/llms.txt). Markdown versions of documentation pages are available by appending `.md` to page URLs; this page is available as [Markdown](https://swatplus.gitbook.io/io-docs/~/changes/GiVD5ID0WVyRIAumaMy2/optimal-growth/potential-growth/biomass-production/impact-of-climate-on-radiation-use-efficiency.md).

# Impact of Climate on Radiation-Use Efficiency

Radiation-use efficiency is sensitive to variations in atmospheric $$CO\_2$$ concentrations and equations have been incorporated into SWAT+ to modify the default radiation-use efficiency values in the plant database for climate change studies. The relationship used to adjust the radiation-use efficiency for effects of elevated $$CO\_2$$ is (Stockle et al., 1992):

             $$RUE=\frac{100*CO\_2}{CO\_2+exp(r\_1-r\_2*CO\_2)}$$                                                                  5:2.1.4

where $$RUE$$ is the radiation-use efficiency of the plant (kg/ha⋅(MJ/m$$^2$$)$$^{-1}$$ or 10$$^{-1}$$ g/MJ), $$CO\_2$$ is the concentration of carbon dioxide in the atmosphere (ppmv), and $$r\_1$$ and $$r\_2$$ are shape coefficients.

           The shape coefficients are calculated by solving equation 5:2.1.4 using two known points ($$RUE\_{amb}$$, $$CO\_{2amb}$$) and ($$RUE\_{hi}$$, $$CO\_{2hi}$$):

               $$r1=1n\[\frac{CO\_{2amb}}{(0.01*RUE\_{amb})}-CO\_{2amb}]+r\_2*CO\_{2amb}$$                              5:2.1.5

               $$r\_2=\frac{(1n\[\frac{CO\_{2amb}}{(0.01*RUE\_{amb})}-CO\_{2amb}]-1n\[\frac{CO\_{2hi}}{(0.01*RUE\_{hi})}-CO\_{2hi}])}{CO\_{2hi}-CO\_{2amb}}$$                                   5:2.1.6

where $$r1$$ is the first shape coefficient, $$r2$$ is the second shape coefficient, $$CO\_{2amb}$$ is the ambient atmospheric $$CO\_2$$ concentration (ppmv), $$RUE\_{amb}$$ is the radiation-use efficiency of the plant at ambient atmospheric $$CO\_2$$ concentration (kg/ha⋅(MJ/m$$^2$$)$$^{-1}$$ or 10$$^{-1}$$ g/MJ), $$CO\_{2hi}$$ is an elevated atmospheric $$CO\_2$$ concentration (ppmv), $$RUE\_{hi}$$ is the radiation-use efficiency of the plant at the elevated atmospheric $$CO\_2$$ concentration, $$CO\_{2hi}$$, (kg/ha⋅(MJ/m$$^2$$)$$^{-1}$$ or 10$$^{-1}$$ g/MJ). Equation 5:2.1.4 was developed when the ambient atmospheric $$CO\_2$$ concentration was 330 ppmv and is valid for carbon dioxide concentrations in the range 330-660 ppmv. Even though the ambient atmospheric concentration of carbon dioxide is now higher than 330 ppmv, this value is still used in the calculation. If the $$CO\_2$$ concentration used in the simulation is less than 330 ppmv, the model defines RUE = $$RUE\_{amb}$$.

     Stockle and Kiniry (1990) have shown that a plant’s radiation-use efficiency is affected by vapor pressure deficit. For a plant, a threshold vapor pressure deficit is defined at which the plant’s radiation-use efficiency begins to drop in response to the vapor pressure deficit. The adjusted radiation-use efficiency is calculated:

$$RUE=RUE\_{vpd=1}-\Delta rue\_{dcl}\*(vpd-vpd\_{thr})$$  if  $$vpd>vpd\_{thr}$$     5:2.1.7

$$RUE=RUE\_{vpd=1}$$                                                    if $$vpd \le vpd\_{thr}$$      5:2.1.8

where $$RUE$$ is the radiation-use efficiency adjusted for vapor pressure deficit (kg/ha⋅(MJ/m$$^2$$)$$^{-1}$$ or 10$$^{-1}$$ g/MJ), $$RUE\_{vpd=1}$$ is the radiation-use efficiency for the plant at a vapor pressure deficit of 1 kPa (kg/ha⋅(MJ/m$$^2$$)$$^{-1}$$ or 10$$^{-1}$$ g/MJ), $$\Delta rue\_{dcl}$$ is the rate of decline in radiation-use efficiency per unit increase in vapor pressure deficit (kg/ha⋅(MJ/m$$^2$$)$$^{-1}$$⋅kPa$$^{-1}$$ or (10$$^{-1}$$ g/MJ)⋅kPa$$^{-1}$$), $$vpd$$ is the vapor pressure deficit (kPa), and $$vpd\_{thr}$$ is the threshold vapor pressure deficit above which a plant will exhibit reduced radiation-use efficiency (kPa). The radiation-use efficiency value reported for the plant in the plant growth database, $$RUE\_{amb}$$, or adjusted for elevated carbon dioxide levels (equation 5:2.1.4) is the value used for $$RUE\_{vpd=1}$$. The threshold vapor pressure deficit for reduced radiation-use efficiency is assumed to be 1.0 kPa for all plants                ($$vpd\_{thr}=1.0$$). 

              The radiation-use efficiency is never allowed to fall below 27% of $$RUE\_{amb}$$. This minimum value was based on field observations (Kiniry, personal communication, 2001).