Skip to main content
. 2018 Mar 9;218(3):986–998. doi: 10.1111/nph.15051

Figure 2.

Figure 2

Simulated values of (a) fraction of photosystem I (PSI) used for cyclic electron transport (CET) that is in BS cells (β), (b) the ratio of PSI used for CET to total PSII (C x : T), (c) fraction of mesophyll (M) cell‐absorbed light that is used for linear electron transport (LET) (u, descending curves) and fraction of bundle sheath (BS) cell‐absorbed light for LET (v, ascending curves), and (d) quantum yield (ΦCO2) and fraction of whole‐leaf CET (f CET), as a function of parameter α (the fraction of total PSII that is in the BS cells), using three values of f bsPSI, the fraction of PSI in BS cells (0.20, 0.35 and 0.50 for long‐dashed, solid and short‐dashed curves, respectively). Dashed curves are invisible in (d) as the same ΦCO2 and f CET were predicted with different values of f bsPSI.