To follow stomatal responses to ozone (O3) in different Arabidopsis lines, we constructed a rapid‐response O3 exposure/gas‐exchange measurement device consisting of eight through‐flow whole‐rosette cuvettes. To separate rosette from roots and growth substrate, plant is grown through an agar‐filled hole in a polished glass plate fixed on the pot. Following insertion of the plant, the plate forms air‐tight bottom surface of the cuvette; thus the rosette is enclosed without touching it during any phase of the insertion of the plant to the cuvette. The device allows monitoring rapid responses in the stomatal function. For example, an acute exposure to 150 ppb O3 decreased stomatal conductance to 60–70% of its initial value within 9–12 min. Thereafter, the conductance regained its preexposure value within further 30–40 min in spite of the continuing O3 exposure. The transient decrease was absent in the abscisic acid‐insensitive mutant abi2 defective in a class 2C protein phosphatase. This provides an in vivo confirmation that the early transient decrease in stomatal conductance is not a result of physical damage by the reactive oxygen species (ROS) formed from O3 breakdown but reflects the biological action of ROS, transduced through a signalling cascade. Thus, the apparatus will be helpful in specifying complex molecular and genetic interactions in rapid responses in guard cells in vivo.
Photosynthesis is a complex process whose rate is affected by many biochemical and biophysical factors. Fortunately, it is possible to determine, or at least estimate, many of the most important parameters using a combination of optical methods and gas transient analyses. We describe here a computer-operated routine that has been developed to make detailed assessments of photosynthesis at a comprehensive level. The routine comprised the following measurements: steady-state light and CO 2 response curves of net CO 2 assimilation at 21 and 2 kPa O 2 ; transients from limiting to different saturating CO 2 concentrations at 2 kPa O 2 ; post-illumination CO 2 fixation transient; dark-light induction of O 2 evolution; O 2 yield from one saturating single-turnover flash; chlorophyll fluorescence F 0 , F s and F m during the light and CO 2 response curves; leaf transmission at 820 nm (P700 + ) during the light and CO 2 response curves; post-illumination re-reduction time of P700 + . The routine was executed on a two-channel fast-response gas exchange measurement system (A. Laisk and V. Oja: Dynamic Gas Exchange of Leaf Photosynthesis. CSIRO, Canberra, Australia). Thirty-six intrinsic characteristics of the photosynthetic machinery were derived, including quantum yield of CO 2 fixation ( Y CO2 Key-words : Betula pendula Roth; leaf; methods; photosynthesis.)Abbreviations : A , net CO 2 assimilation rate; AC, assimilatory charge; a II , a I , a 0 , relative optical cross-sections of PSII and PSI antenna and of non-photosynthetic absorption; C a , C i , C w , C c , CO 2 concentrations: ambient, intercellular space, cell wall liquid and carboxylation site, respectively; CRC, carbon reduction cycle; Cyt, b 6 f, cytochrome b 6 f; DCMU, dichlorophenol-dimethyl urea; ETR, and J , electron transport rate; F 0 , F s , F m , F md , fluorescence yields, minimum, steady state, maximum (all in the light) and maximum F m in the dark, respectively; FRL, far-red light; Γ , CO 2 compensation point; K s , Rubisco CO 2 /O 2 specificity; k N , relative rate constant for regulatory non-photochemical excitation quenching; k P0 , relative rate constant for photochemical excitation quenching at open PSII centres; P s , P m , P o , 820 nm signal difference from the dark level, steady state, maximum and corresponding to oxidizable P700; PAD, ( I in equations), PFD, photon flux density, absorbed and incident, respectively; PC, plastocyanin; PGA, 3-phosphoglyceric acid; P i , inorganic phosphate; PSI, PSII, photosystems I and II; PQ, plastoquinone; P700, donor pigment of PSI; q E , q I , non-photochemical quenching, energy dependent and inhibitory; R d , R K , Krebs cycle CO 2 evolution rate in the dark and in the light, respectively; r gw , r m , r md , leaf diffusion resistances, in gas phase, mesophyll total and mesophyll diffusional; RuBP, ribulose 1,5-bisphosphate; Rubisco, ribulose 1,5-bisphosphate carboxylase-oxygenase; SCE, specific carboxylation efficiency; VPD, water
Sunflower (Helianthus annuus L.) and tobacco (Nicotiana tabacum L.) were grown in the laboratory and leaves were taken from field-grown birch trees (Betula pendula Roth). Chlorophyll fluorescence, CO2 uptake and O2 evolution were measured and electron transport rates were calculated, J(C) from the CO2 uptake rate considering ribulose-1,5-bisphosphate (RuBP) carboxylation and oxygenation, J(O) from the O2 evolution rate, and J(F) from Chl fluorescence parameters. Mesophyll diffusion resistance, r(md), used for the calculation of J(C), was determined such that the in vivo Rubisco kinetic curve with respect to the carboxylation site CO2 concentration became a rectangular hyperbola with Km(CO2) of 10 microM at 22.5 degrees C. In sunflower, in the absence of external O2, J(O) = 1.07 J(C) when absorbed photon flux density (PAD) was varied, showing that the O2-independent components of the alternative electron flow to acceptors other than CO2 made up 7% of J(C). Under saturating light, J(F), however, was 20-30% faster than J(C), and J(F)-J(C) depended little on CO2 and O2 concentrations. The inter-relationship between J(F)-J(C) and non-photochemical quenching (NPQ) was variable, dependent on the CO2 concentration. We conclude that the relatively fast electron flow J(F)-J(C) appearing at light saturation of photosynthesis contains a minor component coupled with proton translocation, serving for nitrite, oxaloacetate and oxygen reduction, and a major component that is mostly cyclic electron transport around PSII. The rate of the PSII cycle is sufficient to release the excess excitation pressure on PSII significantly. Although the O2-dependent Mehler-type alternative electron flow appeared to be under the detection threshold, its importance is discussed considering the documented enhancement of photosynthesis by oxygen.
The oxidation kinetics under far-red light (FRL) of photosystem I (PSI) high potential donors P700, plastocyanin (PC), and cytochrome f (Cyt f) were investigated in sunflower leaves with the help of a new high-sensitivity photometer at 810 nm. The slopes of the 810 nm signal were measured immediately before and after FRL was turned on or off. The same derivatives (slopes) were calculated from a mathematical model based on redox equilibrium between P700, PC and Cyt f and the parameters of the model were varied to fit the model to the measurements. Typical best-fit pool sizes were 1.0-1.5 micromol m(-2) of P700, 3 PC/P700 and 1 Cyt f/P700, apparent equilibrium constants were 15 between P700 and PC and 3 between PC and Cyt f. Cyclic electron flow (CET) was calculated from the slope of the signal after FRL was turned off. CET activated as soon as electrons accumulated on the PSI acceptor side. The quantum yield of CET was close to unity. Consequently, all PSI in the leaf were able to perform in cycle, questioning the model of compartmentation of photosynthetic functions between the stroma and grana thylakoids. The induction of CET was very fast, showing that it was directly redox-controlled. After longer dark exposures CET dominated, because linear e- transport was temporarily hindered by the dark inactivation of ferredoxin-NADP reductase.
Oxidation of photosystem I (PSI) donors under far-red light (FRL), slow re-reduction by stromal reductants and fast re-reduction in the dark subsequent to illumination by white light (WL) were recorded in leaves of several C(3) plants at 810 and 950 nm. During the re-reduction from stromal reductants the mutual interdependence of the two signals followed the theoretical relationship calculated assuming redox equilibrium between plastocyanin (PC) and P700, with the equilibrium constant of 40 +/- 10 (Delta E (m) = 86-99 mV) in most of the measured 24 leaves of nine plant species. The presence of non-oxidizable PC of up to 13% of the whole pool, indicating partial control of electron transport by PC diffusion, was transiently detected during a saturation pulse of white light superimposed on FRL or on low WL. Nevertheless, non-oxidizable PC was absent in the steady state during fast light-saturated photosynthesis. It is concluded that in leaves during steady state photosynthesis the electron transport rate is not critically limited by PC diffusion, but the high-potential electron carriers PC and P700 remain close to the redox equilibrium.
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