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. 2019 Feb 22;70(10):2839–2855. doi: 10.1093/jxb/erz068

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© The Author(s) 2019. Published by Oxford University Press on behalf of the Society for Experimental Biology.

This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted reuse, distribution, and reproduction in any medium, provided the original work is properly cited.

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Fig. 8. — Parameter values (A–J) derived from the leaf energy balance model using Bayesian inference. Steady-state target for the stomatal conductance to water vapour (g_sw) (A) during the initial dark period (g₁), (B) the light period (g₂), and (C) the final dark period (g₃). (D) The slow increase or decrease in g_sw over time (s_l), with the dotted line representing 0. (E) The leaf shortwave absorbance (α_l). The time lag and the time constant for (F and G) an increase (ϕ_i and τ_i) and (H and I) a decrease (ϕ_d and τ_d) in g_sw. (J) The amount of energy per unit area required to change the temperature of the material by 1 °K (k). The model was fitted on observations from five leaves. Error bars represent the 95% credible interval. Colours represent the different leaf areas.