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. 2007 Feb;143(2):1055-67.
doi: 10.1104/pp.106.088302. Epub 2006 Dec 1.

Discrimination in the dark. Resolving the interplay between metabolic and physical constraints to phosphoenolpyruvate carboxylase activity during the crassulacean acid metabolism cycle

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Discrimination in the dark. Resolving the interplay between metabolic and physical constraints to phosphoenolpyruvate carboxylase activity during the crassulacean acid metabolism cycle

Howard Griffiths et al. Plant Physiol. 2007 Feb.

Abstract

A model defining carbon isotope discrimination (delta13C) for crassulacean acid metabolism (CAM) plants was experimentally validated using Kalanchoe daigremontiana. Simultaneous measurements of gas exchange and instantaneous CO2 discrimination (for 13C and 18O) were made from late photoperiod (phase IV of CAM), throughout the dark period (phase I), and into the light (phase II). Measurements of CO2 response curves throughout the dark period revealed changing phosphoenolpyruvate carboxylase (PEPC) capacity. These systematic changes in PEPC capacity were tracked by net CO2 uptake, stomatal conductance, and online delta13C signal; all declined at the start of the dark period, then increased to a maximum 2 h before dawn. Measurements of delta13C were higher than predicted from the ratio of intercellular to external CO2 (p(i)/p(a)) and fractionation associated with CO2 hydration and PEPC carboxylations alone, such that the dark period mesophyll conductance, g(i), was 0.044 mol m(-2) s(-1) bar(-1). A higher estimate of g(i) (0.085 mol m(-2) s(-1) bar(-1)) was needed to account for the modeled and measured delta18O discrimination throughout the dark period. The differences in estimates of g(i) from the two isotope measurements, and an offset of -5.5 per thousand between the 18O content of source and transpired water, suggest spatial variations in either CO2 diffusion path length and/or carbonic anhydrase activity, either within individual cells or across a succulent leaf. Our measurements support the model predictions to show that internal CO2 diffusion limitations within CAM leaves increase delta13C discrimination during nighttime CO2 fixation while reducing delta13C during phase IV. When evaluating the phylogenetic distribution of CAM, carbon isotope composition will reflect these diffusive limitations as well as relative contributions from C3 and C4 biochemistry.

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Figures

Figure 1.
Figure 1.
A diagram showing the major factors that determine Δ13C during CO2 exchange in CAM species during the four phases of the CAM cycle according to Equations 5 and 12. The terms pa, pi, and pm are the partial pressures of CO2 in the atmosphere, the intercellular airspace, and in the mesophyll cells. PCR and PCO refer to the photosynthetic carbon reduction and oxygenation cycles, respectively. The associated fractionation factors are shown by lowercase letters and are described in the “Theory” section.
Figure 2.
Figure 2.
Net CO2 uptake (A) and gs responses as a function of changing pCO2 measured from late afternoon (phase IV) and throughout the dark period (phase I) and into the light (phase II; B). Representative data are plotted as individual response curves for one leaf at selected intervals during the dark period. Gas exchange measurements were made at an irradiance of 300 μmol quanta m−2 s−1 in the light period, with day/night temperatures of 25°C/20°C and a pCO2 varied against a background gas mixture of 909 mbar nitrogen and 48 mbar of O2.
Figure 3.
Figure 3.
Initial slope of A/pi response (A) and variation in Amax measured every 2 h from late afternoon (phase IV) and throughout the dark period (phase I) and into the light (phase II; B). Data are plotted as mean ± SEM for three replicate leaves, with inset in A showing the relationship between initial slope and Amax, with experimental details in the Figure 1 legend. Different letters indicate significant differences between plants at P < 0.05.
Figure 4.
Figure 4.
A, Net A. B, gs. C, pi/pa measured from late afternoon (phase IV) and throughout the dark period (phase I) and into the light (phase II), with data (±SEM) for three replicate leaves from plants of K. daigremontiana maintained in a controlled-environment chamber on a reverse light/dark cycle. Gas exchange measurements were made at an irradiance of 300 μmol quanta m−2 s−1 in the light period, with day/night temperatures of 25°C/20°C and an inlet pCO2 of 531 μbar in 909 mbar of nitrogen and 48 mbar of O2 gas mixture.
Figure 5.
Figure 5.
Δ13C measured in association with gas exchange from late afternoon (phase IV) and throughout the dark period (phase I) and into the light period (phase II), with data (white circles, ±SEM) for three replicate leaves from plants of K. daigremontiana maintained in a controlled-environment chamber on a reverse light/dark cycle. Predicted Δ13C for the dark period (phase I) determined from the model developed in this article (see “Theory” section for details); dashed line is modeled Δ13C including correction for the draw down from substomatal cavity to cytoplasm calculated with gi = 0.044 mol m−2 s−1 bar−1 with Equation 8 and 14 b4 = 6.27‰ at a leaf temperature of 20°C; continuous line is modeled Δ13C using infinite gi (effectively using pi/pa) to parameterize the model.
Figure 6.
Figure 6.
A, Transpiration rate. B, Leaf to air VPD. C, The 18O isotopic composition of δt and at the δe calculated from the Craig-Gordon model (Eq. 18), measured from late afternoon (phase IV) and throughout the dark period (phase I) and into the light (phase II) with data (±SEM) for three replicate leaves from plants of K. daigremontiana that had been maintained in a controlled-environment chamber on a reverse light/dark cycle. The source water used for irrigation of plants had an isotopic composition of δ18OVSMOW = −5.5‰.
Figure 7.
Figure 7.
Δ18O measured in CO2 and in association with gas exchange, from late afternoon (phase IV) and throughout the dark period (phase I) and into the light period (phase II), with data (white circles, ± SEM) for three replicate leaves from plants of K. daigremontiana maintained in a controlled-environment chamber on a reverse light/dark cycle.
Figure 8.
Figure 8.
Δ18O as a function of pi/pa (A) and pm/pa (B and C). In A, no correction was made for gi, whereas in B and C, pm was derived by assuming a gi of 0.0.85 or 0.044 mol m−2 s−1 bar, respectively. The lines are not fitted to the data but represent the theoretical relationship of Δ18O and pi/pa or pm/pa at full isotopic equilibrium, where a = 7.7‰ and Δea = 45‰ or 51‰ using either the average δt or δs values, respectively, in Equation 24. The value of gi = 0.085 in B was estimated from minimizing the variance between measured and theoretical Δ18O calculated with the average δt. The CO2 supplied to the leaf had a Δ18O of 24‰ relative to VSMOW. Data points in each section represent the individual samples collected during light (white circles) and dark (black circles) from three replicate leaves of K. daigremontiana (for details, see Figs. 2 and 5, legends above).
Figure 9.
Figure 9.
Modeled predictions (Eqs. 8 and 14) of Δ13C for two contrasting assimilation rates and a pi/pa = 0.45 using b4 = 6.27‰ at a leaf temperature of 20°C plotted as a function of varying gi during phase I.

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