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To examine the role of sulfoquinovosyl diacylglycerol (SQDG) in thylakoid membranes, we compared the structural and functional properties of photosystem II (PSII) between a mutant of Chlamydomonas reinhardtii defective in SQDG ( hf-2) and the wild type. The PSII core complex of hf-2, as compared with that of the wild type, showed structural fragility when solubilized with a detergent, dodecyl beta- d-maltoside, suggesting that the physical properties of the PSII complex were altered by the loss of SQDG. On the other hand, exposure of the cells to 41 degrees C for 120 min in the dark decreased the PSII activity to 70% and 50% of the initial levels in the wild type and hf-2, respectively, which implies that the PSII activity, in the absence of SQDG, becomes less stable under heat-stress conditions. PSII inactivated to 60% of the initial level by dark incubation at 41 degrees C was reactivated by following illumination even at 41 degrees C to more than 90% in the wild type, but only to 70% in hf-2. These results suggest that PSII inactivated by heat recovers through some mechanism dependent on light, and that SQDG participates in functioning of the mechanism. The conformational disorder of PSII caused by the defect in SQDG might be correlated with the increased susceptibility of its activity to heat-stress.

The recovery process after chilling-induced photoinhibition of photosystem I (PSI) was studied in leaves of a chilling-sensitive plant, cucumber (Cucumis sativus L. cv. Nanshin). Determination of chlorophyll content, photosystem (PS) activities in vivo and in vitro, and the amount of reaction-center subunits of PSI revealed that: (i) The content of chlorophyll decreased to 70% of the original level gradually from 1 to 3 days after exposure to a low temperature. (ii) The amount of functional PSI per unit leaf area was reduced to 30% of the initial level by the chilling treatment. The amount of functional PSI gradually increased during the next 6 days but only to 50% of the original level. (iii) When expressed on a chlorophyll basis, however, the amount of functional PSI recovered to 90% of the original level 6 days after the treatment. (iv) The residual amount of chlorophyll on the third day after the treatment closely correlated with the amount of functional PSI at that point. These results indicate that the decrease in chlorophyll content at a normal growth temperature after chilling treatment is a consequence of the degradation of irreversibly damaged PSI complexes. Immunoblot analysis confirmed that PsaAB protein, the reaction-center subunits of PSI, was degraded during the 3 days after chilling treatment. Some characteristics of the chilling injury frequently reported, i.e. irreversibility of the injury and development of visible symptoms at room temperature, can be explained as a consequence of the chilling-induced photoinhibition of PSI.

The morphology of the pyrenoid and the physiology of the CO2-concentrating mechanism (CCM) were investigated in Chlamydomonas (Cd.) mutabilis Gerloff UTEX 578, Cd. radiata Deason et Bold UTEX 966, Cd. augustae Skuja UTEX 1969, Cd. macrostellata Lund SAG 72.81, Cd. bipapillata Bourrelly SAG 11-47, and Chloromonas (Cr.) insignis Gerloff et Ettl NIES-447, all of which are closely related phylogenetically to the pyrenoid-less strains of Chloromonas. In the chloroplasts of Cd. mutabilis UTEX 578, Cd. radiata UTEX 966, Cd. augustae UTEX 1969, and Cd. macrostellata SAG 72.81, a typical, spheroidal, electron-dense pyrenoid matrix surrounded by starch granules was present, and ribulose-1,5-bisphosphate carboxylase/oxygenase (Rubisco; EC 4.1.1.39) molecules were highly concentrated in the pyrenoid matrix. On the other hand, while the pyrenoid matrix of Cr. insignis NIES-447 was electron-dense that of Cd. bipapillata SAG 11-47 was not, and neither was surrounded by starch granules. The pyrenoid matrices of these two species exhibited a higher concentration of Rubisco molecules than the thylakoid region (thylakoid and stroma) of the chloroplasts; however, the densities of Rubisco molecules in these pyrenoid matrices were low compared with those of the other four Chlamydomonas strains examined in this study and that of Cd. reinhardtii Dangeard. In all six strains examined, the presence of the CCM was indicated by relatively high photosynthetic affinities for CO2 (low values of K0.5(CO2)). However, differences in the inorganic carbon (Ci) pools were recognized in relation to the differences in pyrenoid morphology among the strains. In the typical pyrenoid-containing strains. Cd. mutabilis UTEX 578 and Cd. radiata UTEX 966, the ratio of internal to external inorganic carbon was about 20, while in Cr. insignis NIES-447 and Cd. bipapillata SAG 11-47 the ratio was only 2–3 similar to the two pyrenoid-less, CCM-containing strains of Chloromonas previously examined (E. Morita et al., 1998, Planta 204: 269–276). It is thus speculated that the presence of typical pyrenoids with a high concentration of Rubisco molecules is related to the formation of large Ci pools in the CCM. Detailed phylogenetic relationships among these Chlamydomonas/Chloromonas strains and the pyrenoid-less Chloromonas strains previously investigated were inferred based on the sequence of rbcL, the gene for the large subunit of Rubisco. Two monophyletic groups were resolved with high bootstrap values. Based on the tree topology resolved, it was inferred that loss of the typical pyrenoids accompanied by a decrease in intracellular Ci pools might have taken place independently in the two groups.

Physiological and morphological characteristics related to the CO2-concentrating mechanism (CCM) were examined in several species of the free-living, unicellular volvocalean genus Chloromonas (Chlorophyta), which differs morphologically from the genus Chlamydomonas only by lacking pyrenoids. The absence of pyrenoids in the chloroplasts of Chloromonas (Cr.) rosae UTEX 1337, Cr. serbinowii UTEX 492, Cr. clatharata UTEX 1970, Cr. rosae SAG 26.90, and Cr. palmelloides SAG 32.86 was confirmed by light and electron microscopy. In addition, immunogold electron microscopy demonstrated that ribulose-1,5-bisphosphate carboxylase/oxygenase (Rubisco; EC 4.1.1.39) molecules were distributed almost evently throughout the chloroplasts in all five Chloromonas strains. However, Chloromonas exhibited two types of physiological characteristics related to the CCM depending on the species or strains examined. Chloromonas rosae UTEX 1337 and Cr. serbinowii had high photosynthetic affinities for CO2 in cells grown in culture medium bubbled with air (low-CO2 cells), compared with those grown in medium bubbled with 5% CO2 (high-CO2 cells), indicating the presence of the low-CO2-inducible CCM. In addition, these two Chloromonas strains exhibited low-CO2-inducible carbonic anhydrase (CA; EC 4.2.1.1) activity and seemed to have small intracellular inorganic carbon pools. Therefore, it appears that Cr. rosae UTEX 1337 and Cr. serbinowii possess the CCM as in pyrenoid-containing microalgae such as Chlamydomonas reinhardtii. By contrast, Cr. clatharata, Cr. rosae SAG 26.90 and Cr. palmelloides showed low photosynthetic affinities for CO2 when grown under both CO2 conditions. Moreover, these three strains exhibited an apparent absence of intracellular inorganic carbon pools and lacked low-CO2-inducible CA activity. Thus, Cr. clatharata, Cr. rosae SAG 26.90 and Cr. palmelloides, like other pyrenoid-less algae (lichen photobionts) reported previously, seem to lack the CCM. The present study is the first demonstration of the CCM in pyrenoid-less algae, indicating that pyrenoids or accumulation of Rubisco in the chloroplasts are not always essential for the CCM in algae. Focusing on this type of CCM in pyrenoid-less algae, the physiological and evolutionary significance of pyrenoid absence is discussed.

It was recently shown that the site of photoinhibition in leaves ofCucumis sativus L. at low temperatures is Photosystem I (PSI), not PSII (I. Terashima et al. 1994, Planta193, 300–306). In the present study, the mechanisms of this PSI photoinhibition in vivo were examined. By lowering the photon flux density during the photoinhibitory treatment of leaves at 4°C for 5 h to less than 100 μmol·m−2s−1, we were able to separate the steps of the destruction of the electron-transfer components. Although P-700, the reaction-center chlorophyll, was almost intact in this low-light treatment, the quantum yield of the electron transfer through PSI and photochemically induced absorption change at 701 nm were markedly inhibited. This, along with the results from the measurements of the light-induced absorption changes in the presence of various concentrations of methyl viologen, an artificial electron acceptor, indicates that the component on the acceptor side of the PSI, A1 or Fx, is the first site of inactivation. When the photon flux density during the treatment was increased to 220 μmol·m−2s−1, the destruction of P-700 itself was also observed. Furthermore, the partial degradation of the chlorophyll-binding large subunits was observed in photoinhibited leaves. This degradation of the subunits was not detected when the treatment was carried out under nitrogen atmosphere, the condition in which the electron transfer is not inhibited. Thus, the photoinhibitory processes in the reaction center of PSI go through three steps, the inactivation of the acceptor side, the destruction of the reaction-center chlorophyll and the degradation of the reaction center subunit(s). The similarities and the differences between the mechanisms of PSI photoinhibition and those of PSII photoinhibition are discussed.

Maximum quantum yields (QY) of photosynthetic electron flows through PSI and PSII were separately assessed in thylakoid membranes isolated from leaves of Cucumis sativus L. (cucumber) that had been chilled in various ways. The QY(PSI) in the thylakoids prepared from the leaves treated at 4° C in moderate light at 220 μmol quanta·m−2·s−1 (400–700 nm) for 5 h, was about 20–30% of that in the thylakoids prepared from untreated leaves, while QY(PSII) decreased, at most, by 20% in response to the same treatment. The decrease in QY(PSI) was observed only when the leaves were chilled at temperatures below 10° C, while such a marked temperature dependency was not observed for the decrease in QY(PSII). In the chilling treatment at 4° C for 5 h, the quantum flux density that was required to induce 50% loss of QY (PSI) was ca. 50 umol quanta·m−2·s−1. When the chilling treatment at 4° C in the light was conducted in an atmosphere of N2, photoinhibition of PSI was largely suppressed, while the damage to PSII was somewhat enhanced. The ferricyanide-oxidised minus ascorbate-reduced difference spectra and the light-induced absorbance changes at 700 nm obtained with the thylakoid suspension, indicated the loss of P700 to extents that corresponded to the decreases in QY(PSI). Accordingly, the decreases in QY(PSI) can largely be attributed to destruction of the PSI reaction centre itself. These results clearly show that, at least in cucumber, a typical chillingsensitive plant, PSI is much more susceptible to aerobic photoinhibition than PSII.