1 2 Geophysical Research Letters 3 Supporting Information for 4 An analytical model for relating global terrestrial carbon assimilation with climate and 5 surface conditions using a rate-limitation framework Yuting Yang1,*, Randall J. Donohue1,2, Tim R. McVicar1,2 and Michael L. Roderick2,3 6 7 1 CSIRO Land and Water, Canberra, Australia 8 2 Australian Research Council Centre of Excellence for Climate System Science, Sydney, 9 Australia 10 3 11 University, Canberra, Australia 12 (Surnames are underlined) Research School of Biology and Research School of Earth Sciences, Australian National 13 14 Email: Yuting.yang@csiro.au; 15 Tel:+61 (2) 62183448 16 Address: CSIRO Land and Water, Black Mountain, Canberra, ACT 2602, Australia 17 Manuscript submitted to 18 19 Geophysical Research Letters Contents of this file 20 21 Figures S1 to S12 22 Tables S1 23 24 Additional Supporting Information 1 25 Supplementary Figure fs01 Relationship between mean annual incident solar radiation and 26 mean annual air temperature at the (a) catchment (32 global large catchments) and (b) grid- 27 cell (0.5o spatial resolution) scales over the period of 1982-2010. 28 29 Supplementary Figure fs02 Relationship between mean annual GPP_MTE and mean annual 30 P at the grid-cell scale (0.5o spatial resolution) over the period of 1982-2010. 31 Supplementary Figure fs03 Comparison between (a) observed mean annual GPP and GPP 32 estimated from the linear function (solid blue lines in Figure 3a) at the flux-site scale, and 33 between (b) mean annual GPP_MTE and GPP estimated from the linear function (solid blue 34 lines in Figure 3b) at the grid-cell scale. The red dash lines are 1:1 lines. 35 Supplementary Figure fs04 Relationship between A/Am(I) and Am(P)/Am(I) within the rate- 36 limitation framework using GPP estimates from 13 ecosystem models. (a) Multi-model 37 ensemble mean, (b) Biome-BGC, (c) CLASS, (d) CLM, (e) CLMVIC, (f) DLEM, (g) GTEC, 38 (h) ISAM, (i) ORCHIDEE, (J) LPJ, (k) SiBCASA, (l) TRIPLEX, (m) VEGAS and (m) 39 VISIT. The red ellipses highlight situations where the GPP estimation from some individual 40 models do not align with the rate-limitation framework. 41 Supplementary Figure fs05 Calibration of the model with solely fPAR at the flux-site level. (a) 42 Relationship between inverted α and fPAR and (b) comparison of GPP estimated by Eq. (6) in 43 combination with α estimated from the best-fit non-linear relationship between α and fPAR 44 2 shown in (a) (i.e., ๐ผ = 7.49๐PAR − 6.47๐PAR + 2.02) against site-level observations. The red 45 solid line in (a) indicate the best-fit function based on the least-square criteria, and the red 46 dashed line in (b) is 1:1 line. 47 Supplementary Figure fs06 Calibration of the model with solely fPAR at the grid-cell scale. (a) 48 Relationship between inverted α and fPAR and (b) comparison of GPP estimated by Eq. (6) in 49 combination with α estimated from the best-fit non-linear relationship between α and fPAR 50 0.5 shown in (a) (i.e., ๐ผ = 0.98๐PAR ) against GPP_MTE. The red solid line in (a) indicate the 51 best-fit function based on the least-square criteria, and the red dashed line in (b) is 1:1 line. 52 Supplementary Figure fs07 Comparison of estimated GPP and GPP_MTE at the grid-cell 53 scale. In part (a) α is estimated from the model calibrated at the flux-site scale (Eq. 8) and in 54 part (b) α is estimated from the model calibrated at the grid-cell scale (Eq. 9). Please note that 2 55 in (a) we only applied the model for grid-cells with fPAR larger than 0.3, as we do not have 56 low fPAR flux-sites (i.e., fPAR < 0.3) for calibrating the model (see Supplementary Table ts01). 57 In both parts the dashed red line is the 1:1 line. 58 Supplementary Figure fs08 Relationship between fPAR/I and P/I at the grid-cell scale across 59 the globe. 60 Supplementary Figure fs09 Location of the 32 catchments used in the supplementary 61 material. 62 Supplementary Figure fs10 Relationship between A/Am(I) and Am(P)/Am(I) within the rate- 63 limitation framework at the catchment (regression, y = 0.4295 x, R2 =0.97, blue line). The 64 dashed lines show the analytical solution for different parameter values. 65 Supplementary Figure fs11 Leave-one-out cross validation of estimated α from Eq. (7) 66 against inverted α at the catchment scale. The red dashed line is 1:1 line. 67 Supplementary Figure fs12 Comparison of mean annual GPP_MTE against mean annual 68 modelled GPP at the catchment scale (using α model calibrated at the catchment scale, i.e., 69 ๐ผcat = 1.587๐PAR + 0.006๐ฅ๐ − 0.084๐ง + 0.094). The red dash line is 1:1 lines. 70 Supplementary Table ts01 Summary of the flux site name (Site ID), mean annual GPP (g C 71 m-2 yr-1), fPAR, precipitation (P in mm yr-1), photosynthetic active radiation (I in MJ m-2 yr-1) 72 and references. 73 Introduction 74 Firstly, relationships between mean annual incident shortwave radiation and mean annual air 75 temperature at grid-cell scale is shown in Supplementary Figure fs01, to support our 76 statement that radiation and temperature is highly correlated at long-time scales in Section 2.1. 77 Secondly, to determine the maximum rain use efficiency (θmax), we plot the relationship 78 between mean annual GPP_MTE and mean annual P at the grid-cell scale (i.e., 0.5 degree 79 spatial resolution) over the years 1982 to 2010 (Supplementary Figure fs02). We found that at 80 low P, there is a distinct upper edge that represents the maximum GPP attainable for a given 81 P, and the slope of this upper edge is taken to be the maximum rain use efficiency. 3 82 Thirdly, we examined the performance of using the linear function in Figure 3(b) and (c) to 83 estimate GPP (Supplementary Figure fs03), and we found that it results in reasonable GPP 84 estimates. 85 Fourthly, we show the relationship between A/Am(I) and Am(P)/Am(I) within the rate- 86 limitation framework using GPP estimates from 13 ecosystem models during the Multi-scale 87 Synthesis and Terrestrial Model Intercomparison Project (MsTMIP) [Huntzinger et al. 2013] 88 (Supplementary Figure fs05). A similar result with Fig. 3b in the main text is found when 89 using the multi-model Ensemble mean (Supplementary Figure fs07 (a)), further reinforcing 90 the physical basis of the rate-limitation framework of the GPP model proposed herein. 91 However, GPP estimates from 5 of the 13 ecosystem models do not always satisfy the first- 92 order requirement (i.e., bounds between two GPP limits) based on visual examination, and 93 these models are Biome-BGC (b), CLASS (c), CLM (d), DLEM (f) and GTEC (g). 94 Fifthly, as fPAR plays a dominant role in determining α, we examined the relationship between 95 fPAR and α and used the best-fit non-linear function to estimate α based solely on fPAR. The 96 estimated α was then applied in Eq. (6) for estimating GPP at both the flux-site and grid-cell 97 scales (Supplementary Figures fs05 and fs06). 98 Sixthly, we also examined the difference and transferability of the two α models (i.e., Eq. (8) 99 calibrated at the flux-site scale and Eq. (9) calibrated at the grid-cell scale). Our results show 100 similar performances of Eq. (6) when applied with either Eq. (8) or Eq. (9) for predicting α at 101 the flux-site (Figures 5a and 5b in main text) and grid-cell scales (Supplementary Figure 102 fs07), suggesting that Eq. (8) and Eq. (9) are relatively conservative and transferable. 103 Seventhly, we tested the developed framework with fPAR, as there is a close relationship 104 between GPP and fPAR, and fPAR can be directly observed from satellite remote sensing. The 105 relationship between fPAR/I and P/I is shown in Supplementary Figure fs08, which shows that 106 fPAR also follows generally the Budyko-like framework. However, although fPAR is closely 107 related with GPP, the relationship is non-linear (e.g., fPAR tends to saturated in tropical 108 rainforest while GPP still shows large spatial variation due to variation in incoming solar 109 radiation). A more fundamental difference is that GPP is a flux variable that is suitable to be 110 analyzed with a rate-limitation framework, whereas fPAR is a state variable. 111 Finally, our results in the main text suggest that the model tends to perform better as the 112 spatial scale increases (i.e., better at the grid-cell scale than at the flux-site scale). This is not 4 113 surprising, because the spatial variability of local effects can be largely reduced at coarser 114 spatial scales. There have been similar findings regarding the Budyko hydroclimatological 115 model. To further demonstrate this point, we test our model at the catchment scale – a spatial 116 scale much larger than a 0.5o grid-cell. Another reason of testing the model at the catchment 117 scale is that catchments are independent hydrological units, which ensure the precipitated 118 water entirely consumed within the analysis unit. We chose here 32 global large catchments 119 (supplementary Figure fs09), and did the same analyses based on GPP_MTE as what we have 120 done for flux-sites and grid-cells. We found that the catchment-scale data also aligns with the 121 proposed Budyko-like GPP framework (supplementary Figure fs10). We also found that 122 calibration of the α model at the catchment scale results in the same three variables (i.e., fPAR, 123 ΔT and z, ๐ผcat = 1.587๐PAR + 0.006๐ฅ๐ − 0.084๐ง + 0.094) as for flux-sites and grid-cells, 124 and fPAR at the catchment scale play an even more important role in determining α (i.e., using 125 fPAR alone could explain 70% of the variance in αcat and adding ΔT explains a further 14%, 126 with z explaining a further 3%) (see Supplementary Figure fs11 for the validation of the α 127 model at the catchment scale using a leave-one-out cross validation approach). In addition, 128 combining the α model at the catchment scale, the proposed theoretical GPP model 129 performed well, and better than at the flux-site and grid-cell scales, in estimating GPP for the 130 catchments (i.e., R2=0.97, RMSE=110 g C m-2 yr-1) (Supplementary Figure fs12). 5 131 132 Supplementary Figure fs01 Relationship between mean annual incident solar radiation and 133 mean annual air temperature at the grid-cell (0.5o spatial resolution) scales over the period of 134 1982-2010. 135 136 137 Supplementary Figure fs02 Relationship between mean annual GPP_MTE and mean annual 138 P at the grid-cell scale (0.5o spatial resolution) over the period of 1982-2010. 139 6 140 141 Supplementary Figure fs03 Comparison between (a) observed mean annual GPP and GPP 142 estimated from the linear function (solid blue lines in Figure 3a) at the flux-site scale, and 143 between (b) mean annual GPP_MTE and GPP estimated from the linear function (solid blue 144 lines in Figure 3b) at the grid-cell scale. The red dash lines are 1:1 lines. 145 7 146 147 Supplementary Figure fs04 Relationship between A/Am(I) and Am(P)/Am(I) within the rate- 148 limitation framework using GPP estimates from 13 ecosystem models. (a) Multi-model 149 ensemble mean, (b) Biome-BGC, (c) CLASS, (d) CLM, (e) CLMVIC, (f) DLEM, (g) GTEC, 150 (h) ISAM, (i) ORCHIDEE, (J) LPJ, (k) SiBCASA, (l) TRIPLEX, (m) VEGAS and (m) 151 VISIT. The red ellipses highlight situations where the GPP estimation from some individual 152 models do not align with the rate-limitation framework. 8 153 154 Supplementary Figure fs05 Calibration of the model with solely fPAR at the flux-site level. (a) 155 Relationship between inverted α and fPAR and (b) comparison of GPP estimated by Eq. (6) in 156 combination with α estimated from the best-fit non-linear relationship between α and fPAR 157 2 shown in (a) (i.e., ๐ผ = 7.49๐PAR − 6.47๐PAR + 2.02) against site-level observations. The red 158 solid line in (a) indicate the best-fit function based on the least-square criteria, and the red 159 dashed line in (b) is 1:1 line. 9 160 161 Supplementary Figure fs06 Calibration of the model with solely fPAR at the grid-cell scale. (a) 162 Relationship between inverted α and fPAR and (b) comparison of GPP estimated by Eq. (6) in 163 combination with α estimated from the best-fit non-linear relationship between α and fPAR 164 0.5 shown in (a) (i.e., ๐ผ = 0.98๐PAR ) against GPP_MTE. The red solid line in (a) indicate the 165 best-fit function based on the least-square criteria, and the red dashed line in (b) is 1:1 line. 166 167 10 168 169 Supplementary Figure fs07 Comparison of estimated GPP and GPP_MTE at the grid-cell 170 scale. In part (a) α is estimated from the model calibrated at the flux-site scale (Eq. 8) and in 171 part (b) α is estimated from the model calibrated at the grid-cell scale (Eq. 9). Please note that 172 in (a) we only applied the model for grid-cells with fPAR larger than 0.3, as we do not have 173 low fPAR flux-sites (i.e., fPAR < 0.3) for calibrating the model (see Supplementary Table ts01). 174 In both parts the dashed red line is the 1:1 line. 175 176 Supplementary Figure fs08 Relationship between fPAR/I and P/I at the grid-cell scale across 177 the globe. 11 178 179 Supplementary Figure fs09 Location of the 32 catchments used in the supplementary 180 material. 181 182 Supplementary Figure fs10 Relationship between A/Am(I) and Am(P)/Am(I) within the rate- 183 limitation framework at the catchment scale (regression, y = 0.4295 x, R2 =0.97, blue line). 184 The dashed lines show the analytical solution for different parameter values. 12 185 186 Supplementary Figure fs11 Leave-one-out cross validation of estimated α from Eq. (7) 187 against inverted α at the catchment scale. The red dashed line is 1:1 line. 188 189 Supplementary Figure fs12 Comparison of mean annual GPP_MTE against mean annual 190 modelled GPP at the catchment scale (using α model calibrated at the catchment scale, i.e., 191 ๐ผcat = 1.587๐PAR + 0.006๐ฅ๐ − 0.084๐ง + 0.094). The red dash line is 1:1 lines. 13