Isolation of chestnut chloroplasts: membrane potentials of chestnut and spinach thylakoids

Typical chestnut thylakoid extracts isolated by mechanical disruption of leaf tissues had an equivalent of 0.28 kg m⁻³ chlorophyll (Chl) which is six times less than in thylakoids obtained from spinach, although Chl content in leaves was only half as small. According to optical microscopy, the vesicles showed a good integrity, exhibiting at 21 °C a high capacity of photon-induced potential membrane generation, which was demonstrated by the almost full 9-amino-6-chloro-2-methoxyacridine fluorescence quenching in a hyper-saline medium containing 150 mM KCl and having osmotic potential of −1.5 MPa. The half-time of the thylakoid potential generation was 11.7 s with the time of dissipation around 8.9 s. In such conditions, spinach thylakoids showed an increased swelling and also differences in the half-time generation which was almost four times faster than was observed in chestnut. However, when spinach thylakoids were incubated in a typical hypo-saline medium without KCl with osmotic potential −0.8 MPa, no additional swelling was observed. Consequently the half-time of potential dissipation was 35 s. Studies with nigericin suggested a chestnut thylakoid ΔpH significantly smaller than that observed in spinach, which was confirmed by the measurements of the ATP driven pumping activity.     

Significance of structural variation in thylakoid membranes in maintaining functional photosystems during reproductive growth

Structural variation in the stroma‐grana (SG) arrangement of the thylakoid membranes, such as changes in the thickness of the grana stacks and in the ratio between grana and inter‐grana thylakoid, is often observed. Broadly, such alterations are considered acclimation to changes in growth and the environment. However, the relation of thylakoid morphology to plant growth and photosynthesis remains obscure. Here, we report changes in the thylakoid during leaf development under a fixed light condition. Histological studies on the chloroplasts of fresh green Arabidopsis leaves have shown that characteristically shaped thylakoid membranes lacking the inter‐grana region, referred to hereafter as isolated‐grana (IG), occurred adjacent to highly ordered, large grana layers. This morphology was restored to conventional SG thylakoid membranes with the removal of bolting stems from reproductive plants. Statistical analysis showed a negative correlation between the incidences of IG‐type chloroplasts in mesophyll cells and the rates of leaf growth. Fluorescence parameters calculated from pulse‐amplitude modulated fluorometry measurements and CO₂ assimilation data showed that the IG thylakoids had a photosynthetic ability that was equivalent to that of the SG thylakoids under moderate light. However, clear differences were observed in the chlorophyll a/b ratio. The IG thylakoids were apparently an acclimated phenotype to the internal condition of source leaves. The idea is supported by the fact that the life span of the IG thylakoids increased significantly in the later developing leaves. In conclusion, the heterogeneous state of thylakoid membranes is likely important in maintaining photosynthesis during the reproductive phase of growth.     

Exposure to low levels of photosynthetically active radiation induces rapid increases in palisade cell chloroplast volume and thylakoid surface area in sunflower (Helianthus annuus L.)

Summary Sudden changes in photoactive radiation (PAR) (wavelength, 400–700 nm) induces rapid surface area changes in chloroplast thylakoid membranes. Although this response may have important photo-acclimative functions for the plant, little is known about the mechanisms by which changes in irradiance are detected or how thylakoid membranes actually increase or decrease surface area. Knowledge of the time required for significant changes in thylakoid area would help eliminate or support several possible mechanisms that may be involved in this aspect of photo-acclimation in plants. Leaf tissues were acclimated to a PAR of 500 mol quanta per m² per s then exposed to low irradiance (PAR, 50 mol quanta per m² per s) and sampled at 5, 15, 30, and 60 min post exposure. Tissue and cell structure were quantified and results showed a significant increase in the surface-to-volume ratio and surface area per unit of standard leaf volume for both appressed and nonappressed thylakoids within 5 min of exposure to low irradiance. On the basis of the ratios of appressed to nonappressed thylakoids, the surface area of the nonappressed thylakoids was found to increase faster than that of the appressed thylakoids throughout the sample period. The portion of the appressed thylakoids in contact with the stroma was defined as margin thylakoids. Margin thylakoid surface-to-volume ratio did not change relative to the high-irradiance control during the sample period but did remain significantly lower than the low-irradiance control during the sample period. The ratio of appressed to margin thylakoids indicated a broadening and shortening of the appressed thylakoid stack within the first 5 min of low-irradiance exposure. The rapidity of the shade response indicates that the early events in this response probably do not directly involve gene activation pathways.Abbreviations PAR photosynthetically active radiation - Sv surface to volume density - Vv volume density - UV-B ultraviolet B radiation     

Acclimation of leaves to low light produces large grana: the origin of the predominant attractive force at work

Photosynthetic membrane sacs (thylakoids) of plants form granal stacks interconnected by non-stacked thylakoids, thereby being able to fine-tune (i) photosynthesis, (ii) photoprotection and (iii) acclimation to the environment. Growth in low light leads to the formation of large grana, which sometimes contain as many as 160 thylakoids. The net surface charge of thylakoid membranes is negative, even in low-light-grown plants; so an attractive force is required to overcome the electrostatic repulsion. The theoretical van der Waals attraction is, however, at least 20-fold too small to play the role. We determined the enthalpy change, in the spontaneous stacking of previously unstacked thylakoids in the dark on addition of Mg²⁺, to be zero or marginally positive (endothermic). The Gibbs free-energy change for the spontaneous process is necessarily negative, a requirement that can be met only by an increase in entropy for an endothermic process. We conclude that the dominant attractive force in thylakoid stacking is entropy-driven. Several mechanisms for increasing entropy upon stacking of thylakoid membranes in the dark, particularly in low-light plants, are discussed. In the light, which drives the chloroplast far away from equilibrium, granal stacking accelerates non-cyclic photophosphorylation, possibly enhancing the rate at which entropy is produced.     

ATP formation onset lag and post-illumination phosphorylation initiated with single-turnover flashes. III. Characterization of the ATP formation onset lag and post-illumination phosphorylation for thylakoids exhibiting localized or bulk-phase delocalized energy coupling

When 100 mM KCl replaced sucrose in a chloroplast thylakoid stock suspension buffer, the membranes were converted from a localized proton gradient to a delocalized proton gradient energy coupling mode. The KCl-suspended but not the sucrose-suspended thylakoids showed pyridine-dependent extensions of the ATP onset lag and pyridine effects on post-illumination phosphorylation. The ATP formation assays were performed in a medium of identical composition, using about a 200-fold dilution of the stock thylakoid suspension; hence the different responses were due to the pretreatment, and not the conditions present in the phosphorylation assay. Such permeable buffer effects on ATP formation provide a clear indicator of delocalized proton gradients as the driving force for phosphorylation. The pyridine-dependent increases in the onset lags (and effects on post-illumination phosphorylation) were not due to different ionic conductivities of the membranes (measured by the 515 nm electrochromic absorption change), H⁺/e ^– ratios, or electron transport capacities for the two thylakoid preparations. Thylakoid volumes and [ 14C]pyridine equilibration were similar with both preparations. The KCl-induced shift toward a bulk-phase delocalized energy coupling mode was reversed when the thylakoids were placed back in a low-salt medium.Proton uptake, at the ATP-formation energization threshold flash number, was much larger in the KCl-treated thylakoids and they also had a longer ATP formation onset lag, when no pyridine was present. These results are consistent with the salt treatment exposing additional endogenous buffering groups for interaction with the proton gradient. The concomitant appearance of the pyridine buffer effects implies that the additional endogenous buffering groups must be located on proteins directly exposed in the aqueous lumen phase.Kinetic analysis of the decay of the post-illumination phosphorylation in the two thylakoid preparations showed different apparent first-order rate constants, consistent with there being two different compartments contributing to the proton reservoirs that energize ATP formation. We suggest that the two compartments are a membrane-phase localized compartment operative in the sucrose-treated thylakoids and the bulk lumen phase into which protons readily equilibrate in the KCl-treated thylakoids.     

Growth and development of winter rye at cold-hardening temperatures results in thylakoid membranes with increased sensitivity to low concentrations of osmoticum

Chloroplasts developed at cold-hardening (5°C) and non-hardening temperatures (20°C) were compared with respect to the stability of photosynthetic electron transport activities, the capacity to produce and maintain a H⁺ gradient and the capacity fat photophosphorylation as a function of resuspension in the presence or absence of osmoticum. The results for electron transport indicate that whole chain, photosystem I and pfaotosystem II activities in non-hardened chloroplast thyalkoids were unaffected by resuspension in the presence of high or low osmoticum. In contrast, the same electron transport activities in cold-hardened chloroplast thylakoids exhibited a 3- to 4-fold decrease in activity when resuspended in the presence of low osmoticum. Impairment of electron transport through photosystem II of cold-hardened thylakoids resuspended in the presence of low osmoticum was supported by room temperature fluorescence induction kinetics. Since the presence of Mn²⁺ partially overcame this inhibition, it is concluded that this osmotically-induced inhibition of PSII activity in cold-hardened chloroplast thylakoids may, in part, be due to damage to the H₂O-splitting side of photosystem II. Both the initial rate and the maximum capacity for cyclic photophosphorylation were significantly inhibited in cold-hardened as compared to non-hardened thylakoids upon resuspension in the presence of low concentrations of osmoticum. This was correlated with an inability of the cold-hardened chloroplast thylakoids to maintain a significant transrnembrane H⁺ gradient. The results indicate that cold-hardened thylakoid membranes required an osmotic concentration (0.8 M) twice as high as non-hardened thylakoids (0.4 M) to produce the same initial rate of H⁺ uptake. In addition, the capacity to produce a proton gradient in cold-hardened thylakoids was less stable than that in non-hardened thylakoids regardless of the osmotic concentration tested. It is concluded that development of rye thylakoid membranes at low temperature results in a differential sensitivity to low osmoticum and thus extreme caution should be exercised when comparing the structure and function of isolated thylakoids developed under contrasting thermal regimes.     

Oxygen reduction in chloroplast thylakoids results in production of hydrogen peroxide inside the membrane

Hydrogen peroxide production in isolated pea thylakoids was studied in the presence of cytochrome c to prevent disproportionation of superoxide radicals outside of the thylakoid membranes. The comparison of cytochrome c reduction with accompanying oxygen uptake revealed that hydrogen peroxide was produced within the thylakoid. The proportion of electrons from water oxidation participating in this hydrogen peroxide production increased with increasing light intensity, and at a light intensity of 630 μmol quanta m^− 2 s^− 1 it reached 60% of all electrons entering the electron transport chain. Neither the presence of a superoxide dismutase inhibitor, potassium cyanide or sodium azide, in the thylakoid suspension, nor unstacking of the thylakoids appreciably affected the partitioning of electrons to hydrogen peroxide production. Also, osmolarity-induced changes in the thylakoid lumen volume, as well as variation of the lumen pH induced by the presence of Gramicidin D, had negligible effects on such partitioning. The flow of electrons participating in lumen hydrogen peroxide production was found to be near 10% of the total electron flow from water. It is concluded that a considerable amount of hydrogen peroxide is generated inside thylakoid membranes, and a possible mechanism, as well as the significance, of this process are discussed.     

Cation-mediated regulation of excitation energy distribution in chloroplasts lacking organized Photosystem II complexes

Despite the total loss of Photosystem II activity, thylakoids isolated from the green nuclear maize mutant hcf1-3 contain normal amounts of the light-harvesting chlorophyll $\text{a}\text{b}$ pigment-protein complex (LHC). We interpret the spectroscopic and ultrastructural characteristics of these thylakoids to indicate that the LHC present in these membranes is not associated with Photosystem II reaction centers and thus exists in a ‘free’ state within the thylakoid membrane. In contrast, the LHC found in wild-type maize thylakoids shows the usual functional association with Photosystem II reaction centers. Several lines of evidence suggest that the free LHC found in thylakoids isolated from hcf1-3 is able to mediate cation-dependent changes in both thylakoid appression and energy distribution between the photosystems: (1) Thylakoids isolated from hcf1-3 and wild-type seedlings exhibit a similar Mg²⁺-dependent increase in the short/long wavelength fluorescence emission peak ratio at 77 K. This Mg²⁺ effect is lost following incubation of thylakoids isolated from either source with low concentrations of trypsin. Such treatment results in the partial proteolysis of the LHC in both membrane types. (2) Thylakoids isolated from both hcf1-3 and wild-type seedlings show a similar Mg²⁺ dependence for the enhancement of the maximal yield of room temperature fluorescence and light scattering; both Mg²⁺ effects are abolished by brief incubation of the thylakoids with low concentrations of trypsin (3) Mg²⁺ acts to reduce the relative quantum efficiency of Photosystem I-dependent electron transport at limiting 650 nm light in thylakoids isolated from hcf1-3. (4) The pattern of digitonin fractionation of thylakoid membranes, which is dependent upon structural membrane interactions and upon LHC in the thylakoids, is similar in thylakoids isolated from both hcf1-3 and wild-type seedlings. We conclude that the surface-exposed segment of the LHC, but not the LHC-Photosystem II core association, is necessary for the cation-dependent changes in both thylakoid appression and energy distribution between the two photosystems, and that the LHC itself is able to transfer excitation energy directly to Photosystem I in a Mg²⁺-dependent fashion in the absence of Photosystem II reaction centers. The latter phenomenon is equivalent to a cation-induced change in the absorptive cross-section of Photosystem I.     

Distribution of the early light-inducible protein in the thylakoids of developing pea chloroplasts

The distribution of the early light-inducible protein (ELIP) of pea (Pisum sativum) between grana and stroma thylakoids was studied. An antibody raised against a bacterial-expressed fusion protein containing ELIP sequences was used. Illumination of dark-grown pea seedlings causes an accumulation of the ELIP in the thylakoid membranes with a maximum level at 16 h. During continuous illumination exceeding 16 h the level decreases again. The fractionation of thylakoid membranes of 48-h-illuminated pea seedlings in grana and stroma thylakoids reveals that there is no uniform distribution of ELIP in the thylakoids. Rather 60-70% of ELIP was found in the stroma thylakoids and 30-40% in the grana thylakoids. This distribution is in accordance with that of photosystem I but not with that of photosystem II. After Triton-X-100 solubilization almost all ELIP is found in the photosystem-I-containing fraction. This also supports an association of ELIP with photosystem I.     

Lateral heterogeneity of plant thylakoid protein complexes: early reminiscences

The concept that the two photosystems of photosynthesis cooperate in series, immortalized in Hill and Bendall''s Z scheme, was still a black box that defined neither the structural nor the molecular organization of the thylakoid membrane network into grana and stroma thylakoids. The differentiation of the continuous thylakoid membrane into stacked grana thylakoids interconnected by single stroma thylakoids is a morphological reflection of the non-random distribution of photosystem II/light-harvesting complex of photosystem II, photosystem I and ATP synthase, which became known as lateral heterogeneity.     

Metastable proton pools in thylakoids and their importance for the stability of Photosystem II

After isolated chloroplast thylakoids have been transferred to a medium which is more alkaline than their storage medium, they retain considerable amounts of unequilibrated protons for often longer than 10 min. Essentially all of these protons are released upon uncoupler addition when the thylakoids are osmotically swollen, but only a portion of them when they are in a shrunken state. Osmotic swelling also greatly accelerates the inactivation of the water-oxidizing system enzyme of Photosystem II, and its depletion of functional Cl^?, at alkaline pH. Analyses of the mestable proton gradient in terms of stoichiometry, temperature dependence, and effect on fluorescent amine probes, suggest that most of the protons involved are bound and exchange readily with the bulk phases only when the thylakoids are swollen. It is concluded that, in shrunken thylakoids, the water-oxidizing enzymes are buried in special H⁺-sequestering domains which probably are formed by cavities in the inner surface of the thylakoid membrane. An observed cooperative action of alkaline pH and divalent cations during Cl^?-extraction from Photosystem II is interpreted as revealing an involvement of both a negatively charged surface region and positively charged groups in maintaining the functional integrity of the site of water oxidization.     

Photosynthetic Membranes of Synechocystis or Plants Convert Sunlight to Photocurrent through Different Pathways due to Different Architectures

Thylakoid membranes contain the redox active complexes catalyzing the light-dependent reactions of photosynthesis in cyanobacteria, algae and plants. Crude thylakoid membranes or purified photosystems from different organisms have previously been utilized for generation of electrical power and/or fuels. Here we investigate the electron transferability from thylakoid preparations from plants or the cyanobacterium Synechocystis. We show that upon illumination, crude Synechocystis thylakoids can reduce cytochrome c. In addition, this crude preparation can transfer electrons to a graphite electrode, producing an unmediated photocurrent of 15 μA/cm². Photocurrent could be obtained in the presence of the PSII inhibitor DCMU, indicating that the source of electrons is Q_A, the primary Photosystem II acceptor. In contrast, thylakoids purified from plants could not reduce cyt c, nor produced a photocurrent in the photocell in the presence of DCMU. The production of significant photocurrent (100 μA/cm²) from plant thylakoids required the addition of the soluble electron mediator DCBQ. Furthermore, we demonstrate that use of crude thylakoids from the D1-K238E mutant in Synechocystis resulted in improved electron transferability, increasing the direct photocurrent to 35 μA/cm². Applying the analogous mutation to tobacco plants did not achieve an equivalent effect. While electron abstraction from crude thylakoids of cyanobacteria or plants is feasible, we conclude that the site of the abstraction of the electrons from the thylakoids, the architecture of the thylakoid preparations influence the site of the electron abstraction, as well as the transfer pathway to the electrode. This dictates the use of different strategies for production of sustainable electrical current from photosynthetic thylakoid membranes of cyanobacteria or higher plants.     

Quantitative separation of spinach thylakoids into Photosystem II-enriched inside-out vesicles and Photosystem I-enriched right-side-out vesicles

Yeda press disruption of thylakoids in the presence of magnesium followed by aqueous polymer two-phase partitioning fractionated the total thylakoid membrane material into two distinctly different fractions. One fraction comprised approx. 60% of the material on a chlorophyll basis and contained inside-out vesicles while the other fraction (40%) contained right-side-out vesicles. The sidedness of the vesicles was determined from the direction of their light-induced proton translocation. The inside-out vesicles showed a pronounced Photosystem (PS) II enrichment as judged by their high PS II and low PS I activities. Moreover, they showed a high ratio between the PS II reaction centre chlorophyll-protein complex and the PS I reaction centre chlorophyll-protein complex (CP I). The chlorophyll $\text{a}\text{b}$ ratio was as low as 2.3 compared to 3.2 for the starting material. In contrast, the right-side-out vesicles showed a pronounced PS I enrichment. Their chlorophyll $\text{a}\text{b}$ ratio was 4.3–4.9. The tight stacking induced by Mg²⁺ allows a quantitative formation of inside-out vesicles from the appressed thylakoid regions while mainly non-appressed thylakoids turn right-side-out. The possibility of fractionating all of the thylakoid material into two sub-populations with markedly different composition with respect to PS I and PS II argues against a close physical association between the two photosystems and in favour of their spatial separation in the plane of the membrane. This fractionation procedure, which can be completed within 1 h and gives high yields of both PS II inside-out thylakoids and PS I right-side-out thylakoids, should be very useful for facilitating and improving studies on both the transverse and lateral organization of the thylakoid membrane.     

Direct measurement of k channels in thylakoid membranes by incorporation of vesicles into planar lipid bilayers

Light-driven electron transfer reactions cause the active accumulation of protons inside thylakoids, yet at steady state the electrical potential difference across the thylakoid membrane is very small; therefore, there must be a flux of other ions to balance the charge that would otherwise be built up by the net movement of H⁺. This paper presents direct measurements of ion movements through channels in the thylakoid membrane. These were made possible by fusing thylakoid vesicles from spinach (Spinacia oleracea L.) into planar lipid bilayers, using techniques developed originally to study sarcoplasmic reticulum. No Mg²⁺ current was found, but voltage-dependent channels have been characterized, these being somewhat selective for K⁺ over Cl⁻. The data are consistent with a role for these channels in charge balance during light-driven H⁺ movements.     

Changes in the Cationic Regulation of Structure and Function in Thylakoids Isolated from Wheat Seedlings Treated with BASF 13.338

When wheat seedlings (Triticum vulgare cf HD 2189) were grown in the presence of BASF 13.338 (4-chloro-5-[dimethylamino]-2-phenyl-3[2H]-pyridazinone), there was a decrease in the ratio of linolenic acid to linoleic acid in the thylakoid membrane lipids (JB St John 1976 Plant Physiol 57: 38) and an increase in the ratio of photosystem II to photosystem I (RM Mannan, S Bose 1984 Photochem Photobiol 41: 63). Accompanying these gross structural changes were alterations in the cationic regulation of structure and functioning of the thylakoid membranes: (a) Mg²⁺-induced increase in the room temperature fluorescence was totally absent; (b) Mg²⁺-induced increase in absorbance at 560 nm, indicative of granal stacking, was slightly higher in thylakoids isolated from the BASF 13.338 treated plants suggesting an increased degree of stacking; and (c) absorption changes in the red and Soret regions of the absorption spectrum, normally resulting from the addition of divalent cation or alkyl anion, or from osmotic shrinkage were almost totally absent in thylakoid membranes isolated from BASF 13.338 treated plants. These observations have been interpreted in terms of: (a) significant alterations in the lipid matrix of the thylakoids from treated plants, (b) absence of cation-induced reorganization of the pigment-protein complexes in the horizontal plane of the treated thylakoid membranes suspended in low salt medium, and (c) absence of dynamic changes even within the individual pigment-protein complexes of treated thylakoids.     

Loss of the SPHF homologue Slr1768 leads to a catastrophic failure in the maintenance of thylakoid membranes in Synechocystis sp. PCC 6803

Background

In cyanobacteria the photosystems are localised to, and maintained in, specialist membranes called the thylakoids. The mechanism driving the biogenesis of the thylakoid membranes is still an open question, with only two potential biogenesis factors, Vipp1 and Alb3 currently identified.

Methodology/Principal Findings

We generated a slr1768 knockout using the pGEM T-easy vector and REDIRECT. By comparing growth and pigment content (chlorophyll a fluoresence) of the Δslr1768 mutant with the wild-type, we found that Δslr1768 has a conditional phenotype; specifically under high light conditions (130 µmol m⁻² s⁻¹) thylakoid biogenesis is disrupted leading to cell death on a scale of days. The thylakoids show considerable disruption, with loss of both structure and density, while chlorophyll a density decreases with the loss of thylakoids, although photosynthetic efficiency is unaffected. Under low light (30 µmol m⁻² s⁻¹) the phenotype is significantly reduced, with a growth rate similar to the wild-type and only a low frequency of cells with evident thylakoid disruption.

Conclusions/Significance

This is the first example of a gene that affects the maintenance of the thylakoid membranes specifically under high light, and which displays a phenotype dependent on light intensity. Our results demonstrate that Slr1768 has a leading role in acclimatisation, linking light damage with maintenance of the thylakoids.     

Chloroplast thylakoid protein phosphatase is a membrane surface-associated activity

Chloroplast thylakoid protein phosphatase activity was measured using ³²P-labeled histone as an exogenous substrate and an assay of the ³²Pi released involving formation of a phosphomolybdate complex and organic extraction. The activity was liberated from wheat (Triticum aestivum) thylakoids by washing the membranes in NaCl-containing solutions followed by centrifugation. The liberated phosphatase activity had a pH optimum of approximately 6.75, was inhibited by addition of 10 millimolar EDTA or EGTA, and was stimulated by addition of millimolar amounts of dithiothreitol, magnesium, manganese, or calcium ions. The rate of thylakoid protein dephosphorylation was decreased following liberation of a portion of the protein phosphatase activity and was increased by addition of salt-liberated phosphatase fraction. These results suggest that at least a portion of wheat thylakoid protein phosphatase is a peripheral, rather than an integral, membrane protein.     

Surface-charge related actions of polylysine on thylakoid membranes

Polycation binding to the negatively charged surface of chloroplast thylakoid membranes is known to cause an inhibition of photosystem I activity. It also interferes with the cation-dependent rearrangement of chlorophyll proteins in the thylakoid membrane. It was shown that added anions prevented or reversed the inhibition of photosystem I by polylysine without decreasing its binding to the membranes. Anions also caused a change in the interaction of the chlorophyll proteins in polylysine-treated thylakoids as indicated by an increase in the relative fluorescence intensity from photosystem II. In both cases, the relative effectiveness of the anions tested depended on their valence; for example, the tetravalent species Fe(CN)₆^4t- was effective at a concentration at least 2 orders of magnitude lower than the divalent species SO₄^2?. These results suggest that anions act by screening the positive charge of the polylysine-coated membrane surface. Measurements of the response of the anionic fluorescent probe 1-anilinonapthalene-8-sulfonate to an addition of anions to polylysine-treated thylakoids supported this contention. It was concluded that the action of polylysine on photosystem I and on the chlorophyll proteins is mediated by changes of the electrical properties of the thylakoid membrane and may not involve a direct binding of the polycation to the affected membrane proteins.     

High salt stress in coupled and uncoupled thylakoid membranes: A comparative study

The effect of high salt concentration on photosystem II (PS II) electron transport rates and chlorophyll a fluorescence induction kinetics was investigated in coupled and uncoupled spinach thylakoid membranes. With increase in salt concentration, the rates of electron transport mediated by PS II and the F _v/F _m ratio were affected more in uncoupled thylakoids as compared to coupled thylakoid membranes. The uncoupled thylakoid membranes seemed to behave like coupled thylakoid membranes at high NaCl concentration (∼1 M). On increasing the salt concentration, the uncoupler was found to be less effective and Na⁺ probably worked as a coupling enhancer or uncoupling suppressor. We suggest that positive charge of Na⁺ mimics the function of positive charge of H⁺ in the thylakoid lumen in causing coupled state. The function of NaCl (monovalent cation) could be carried out by even lower concentration of Ca²⁺ (divalent cation) or Al³⁺ (trivalent cation). We conclude that this function of NaCl as coupling enhancer is not specific, and in general a positive charge is required for causing coupling in uncoupled thylakoid membranes. Published in Russian in Biokhimiya, 2009, Vol. 74, No. 6, pp. 761–767.     

Millisecond Delayed Light as an Indicator of Electrical Gradients across Chloroplast Thylakoids

DELAYED light emission from photosynthetic organisms was discovered by Strehler and Arnold¹. The emitted light has a spectrum similar to that of chlorophyll a fluorescence and can often persist for minutes after terminating the illumination. In recent years it has been found that the intensity of emission during the first few milliseconds of the decay is sensitive to the high energy state of the chloroplasts². Wraight and Crofts³ have suggested that this sensitivity is due to the establishment of electrical and pH gradients across the thylakoids during the illumination stage. The linking of the high energy state with these gradients is an essential feature of Mitchell's chemiosmotic hypothesis⁴. Wraight and Crofts³ have argued that the light-induced pH and electrical gradients act in such a way as to decrease the activation energy necessary to lift electrons from the metastable state, created during the preillumination, to the first singlet of chlorophyll. If this hypothesis is correct, the establishment of an electrical gradient across the thylakoid membranes by some means other than light-induced electron transport should change the intensity of millisecond delayed light emission. One possible way to create membrane potentials is to subject chloroplasts to salt gradients. The magnitude of the potentials developed will be a function of the concentration gradients and the relative rates of penetration of the ions across the thylakoid membranes^5,6.