Figure 5 Simulations with a coupled leaf gas exchange model (Duursma, 2015), demonstrating the effect of inclusion of the go parameter (Eqn 1) on leaf fluxes (a) Intrinsic water use efficiency (A,/g.) as a function of the photosynthetic photon flux density (PPFD), holding other environmental drivers constant, for thre¢ values of go. (b) The same simulations as in (a), but showing the intercellular CO2 concentration (C;). (c) Leaf transpiration (E_) simulations, where the vapo pressure deficit (VPD) and air temperature (T,i) were covaried based on an empirical relationship (Duursma et a/., 2014), reflecting typical covariation in fielc conditions. (d) The same simulations as in (c), but showing C;. Note how C; increases at high VPD and Tair, only when go > O. For all simulations, itis assumed tha Tieaf is equal to T,;,, and we ignore the differential permeability of the cuticle to COz and HzO (Hanson et al., 2016). When plants are sufficiently water stressed so that stomata are mostly closed, water loss still continues at a rate determined by the minimum conductance. Thus, models that aim to predict when plants desiccate and die must include a minimum conductance term. A classic study by Pisek & Winkler (1953) calculated the ength of time needed to desiccate leaves to some critical low water content, given the minimum transpiration rate and the saturated water content of the leaves. Based on that work, Burghardt & Riederer (2006) reported a direct correlation between gj,i, and the survival time of leaves. Sinclair (2000) presented the minimum conductance as a key drought tolerance trait, and used it as a basis for the prediction of crop mortality during severe drought. More recently, Gleason etal. (2014) and Blackman etal. (2016) have proposed that embolism resistance together with whole-plant capacitance and minimum transpiration rates all contribute to define the time to desiccation. Building on this work, Martin- StPaul etal. (2017) demonstrated, in a whole-plant model of hydraulic failure, that g,,i, was one of the key parameters to explain the drop in water potential below the cavitation threshold, because