Excitation spectra for Photosystem I and Photosystem II in chloroplasts and the spectral characteristics of the distribution of quanta between the two photosystems

The parameters listed in the title were determined within the context of a model for the photochemical apparatus of photosynthesis.

The fluorescence of variable yield at 750 nm at −196 °C is due to energy transfer from Photosystem II to Photosystem I. Fluorescence excitation spectra were measured at −196 °C at the minimum, F_O, level and the maximum, F_M, level of the emission at 750 nm. The difference spectrum, F_M–F_O, which represents the excitation spectrum for F_V is presented as a pure Photosystem II excitation spectrum. This spectrum shows a maximum at 677 nm, attributable to the antenna chlorophyll a of Photosystem II units, with a shoulder at 670 nm and a smaller maximum at 650 nm, presumably due to chlorophyll a and chlorophyll b of the light-harvesting chlorophyll complex.

Fluorescence at the F_O level at 750 nm can be considered in two parts; one part due to the fraction of absorbed quanta, , which excites Photosystem I more-or-less directly and another part due to energy transfer from Photosystem II to Photosystem I. The latter contribution can be estimated from the ratio of F_O/F_V measured at 692 nm and the extent of F_V at 750 nm. According to this procedure the excitation spectrum of Photosystem I at −196 °C was determined by subtracting 1/3 of the excitation spectrum of F_V at 750 nm from the excitation spectrum of F_O at 750 nm. The spectrum shows a relatively sharp maximum at 681 nm due to the antenna chlorophyll a of Photosystem I units with probably some energy transfer from the light-harvesting chlorophyll complex.

The wavelength dependence of was determined from fluorescence measurements at 692 and 750 nm at −196 °C. is constant to within a few percent from 400 to 680 nm, the maximum deviation being at 515 nm where shows a broad maximum increasing from 0.30 to 0.34. At wavelengths between 680 and 700 nm, increases to unity as Photosystem I becomes the dominant absorber in the photochemical apparatus.     

Light-induced absorbance changes in chloroplasts mediated by Photosystem I and Photosystem II at low temperature

Stable light-induced absorbance changes in chloroplasts at −196 °C were measured across the visible spectrum from 370 to 730 nm in an effort to find previously undiscovered absorbance changes that could be related to the primary photochemical activity of Photosystem I or Photosystem II. A Photosystem I mediated absorbance increase of a band at 690 nm and a Photosystem II mediated absorbance increase of a band at 683 nm were found. The 690-nm change accompanied the oxidation of P₇₀₀ and the 683-nm increase accompanied the reduction of C-550. No Soret band was detected for P₇₀₀.

A specific effort was made to measure the difference spectrum for the photooxidation of P₆₈₀ under conditions (chloroplasts frozen to −196 °C in the presence of ferricyanide) where a stable, Photosystem II mediated EPR signal, attributed to P₆₈₀⁺ has been reported. The difference spectra, however, did not show that P₆₈₀⁺ was stable at −196 °C under any conditions tested. Absorbance measurements induced by saturating flashes at −196 °C (in the presence or absence of ferricyanide) indicated that all of the P₆₈₀⁺ formed by the flash was reduced in the dark either by a secondary electron donor or by a backreaction with the primary electron acceptor. We conclude that P₆₈₀⁺ is not stable in the dark at −196 °C: if the normal secondary donor at −196 °C is oxidized by ferricyanide prior to freezing, P₆₈₀⁺ will oxidize other substances.     

Photooxidation of cytochrome b559 and the electron donors in chloroplast Photosystem II

The effect of light on the reaction center of Photosystem II was studied by differential absorption spectroscopy in spinach chloroplasts.

At − 196 °C, continuous illumination results in a parallel reduction of C-550 and oxidation of cytochrome b₅₅₉ high potential. With flash excitation, C-550 is reduced, but only a small fraction of cytochrome b₅₅₉ is oxidized. The specific effect of flash illumination is suppressed if the chloroplasts are preilluminated by one flash at 0 °C.

At − 50 °C, continuous illumination results in the reduction of C-550 but little oxidation of cytochrome b₅₅₉. However, complete oxidation is obtained if the chloroplasts have been preilluminated by one flash at 0 °C. The effect of preillumination is not observed in the presence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea.

A model is discussed for the reaction center, with two electron donors, cytochrome b₅₅₉ and Z, acting in competition. Their respective efficiency is dependent on temperature and on their states of oxidation. The specific effect of flash excitation is attributed to a two-photon reaction, possibly based on energy-trapping properties of the oxidized trap chlorophyll.     

The back reaction in the primary electron transfer couple of photosystem II of photosynthesis

Changes of C-550, cytochrome b₅₅₉ and fluorescence yield induced in chloroplasts by single saturating flashes were studied at low temperature. A single saturating flash at −196°C was quite ineffective in reducing C-550, oxidizing cytochrome b₅₅₉ or increasing the fluorescence yield, presumably because most of the charge separation induced by the flash was dissipated by a direct back reaction in the primary electron transfer couple. The back reaction, which competes with the dark reduction of the oxidized primary electron donor by a secondary electron donor, becomes increasingly important as the temperature is lowered because of the temperature coefficient of the reaction with the secondary donor. The effect of the back reaction is to lower the quantum yield for the production of stable photochemical products by steady irradiation. Assuming a quantum yield of unity for the photoreduction of C-550 at room temperature, the quantum yield for the reaction is about 0.40 at −100°C and 0.27 at −196°C.     

Effect of low temperature (−30 to −60°C) on the reoxidation of the Photosystem II primary electron acceptor in the presence and absence of 3(3,4-dichlorophenyl)-1,1-dimethylurea

The fluorescence yield has been measured on spinach chloroplasts at low temperature (−30 to −60°C) for various dark times following a short saturating flash. A decrease in the fluorescence yield linked to the reoxidation of the Photosystem II electron acceptor Q is still observed at −60°C. Two reactions participate in this reoxidation: a back reaction or charge recombination and the transfer of an electron from Q⁻ to Pool A. The relative competition between these two reactions at low temperature depends upon the oxidation state of the donor side of the Photosystem II center:

1. (1) In dark-adapted chloroplasts (i.e. in States S₀+S₁ according to Kok, B., Forbush, B. and McGloin, M. (1970) Photochem. Photobiol. 11, 457–475), Q, reduced by a flash at low temperature, is reoxidized by a secondary acceptor and the positive charge is stabilized on the Photosystem II donor Z. Although this reaction is strongly temperature dependent, it still occurs very slowly at −60°C.

2. (2) When chloroplasts are placed in the S₂+S₃ states by a two-flash preillumination at room temperature, the reoxidation of Q⁻ after a flash at low temperature is mainly due to a temperature-independent back reaction which occurs with non-exponential kinetics.

3. (3) Long continuous illumination of a frozen sample at −30°C causes 6–7 reducing equivalents to be transferred to the pool. Thus, a sufficient number of oxidizing equivalents should have been generated to produce at least one O₂ molecule.

4. (4) A study of the back reaction in the presence of 3(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) shows the superposition of two distinct non-exponential reactions one temperature dependent, the other temperature independent.

The effect of temperature on the primary reaction of chloroplast Photosystem II Evidence for a temperature-dependent back reaction

The primary reaction of Photosystem II has been studied over the temperature range from −196 to −20 °C. The photooxidation of the reaction-center chlorophyll (P680) was followed by the free-radical electron paramagnetic resonance signal of P680⁺, and the photoreduction of the Photosystem II primary electron acceptor was monitored by the C-550 absorbance change.

At temperatures below −100 °C, the primary reaction of Photosystem II is irreversible. However, at temperatures between −100 and −20 °C a back reaction that is insensitive to 3-(3′,4′-dichlorophenyl)-1,1′-dimethylurea (DCMU) occurs between P680⁺ and the reduced acceptor.

The amount of reduced acceptor and P680⁺ present under steady-state illumination at temperatures between −100 and −20 °C is small unless high light intensity is used to overcome the competing back reaction. The amount of reduced acceptor present at low light intensity can be increased by adjusting the oxidation-reduction potential so that P680⁺ is reduced by a secondary electron donor (cytochrome b₅₅₉) before P680⁺ can reoxidize the reduced primary acceptor. The photooxidation of cytochrome b₅₅₉ and the accompanying photoreduction of C-550 are inhibited by DCMU. The inhibition of C-550 photoreduction by DCMU, the dependence of P680 photooxidation and C-550 photoreduction on light intensity, and the effect of the availability of reduced cytochrome b₅₅₉ on C-550 photoreduction are unique to the temperature range where the Photosystem II primary reaction is reversible and are not observed at lower temperatures.     

Redox titration of the primary electron acceptor of Photosystem I in spinach chloroplasts

The midpoint potential of the primary electron acceptor of Photosystem I in spinach chloroplasts was titrated using the photooxidation of P₇₀₀ at −196 °C as an index of the amount of primary acceptor present in the oxidized state. The redox potential of the chloroplast suspension was established by the reducing power of hydrogen gas (mediated by clostridial hydrogenase and 1,1′-trimethylene-2,2′-dipyridylium dibromide) at specific pH values at 25 °C. Samples were frozen to −196 °C and the extent of the photooxidation of P₇₀₀ was determined from light-minus-dark difference spectra. This titration indicated a midpoint potential of −0.53 V for the primary electron acceptor of Photosystem I.     

Probing fluorescence induction in chloroplasts on a nanosecond time scale utilizing picosecond laser pulse pairs

The fluorescence induction and other fluorescence properties of spinach chloroplasts at room temperature were probed utilizing two 30-ps wide laser pulses (530 nm) spaced Δt (s) apart in time (Δt = 5–110 ns). The energy of the first pulse (P₁) was varied (10¹²–10¹⁶ photons · cm⁻²), while the energy of the second (probe) pulse (P₂) was held constant (5 · 10¹³ photons · cm⁻²). A gated (10 ns) optical multichannel analyzer-spectrograph system allowed for the detection of the fluorescence generated either by P₁ alone, or by P₂ alone (preceded by P₁). The dominant effect observed for the fluorescence yield generated by P₁ alone is the usual singlet-singlet exciton annihilation which gives rise to a decrease in the yield at high energies. However, when the fluorescence yield of dark-adapted chloroplasts is measured utilizing P₂ (preceded by pulse P₁) an increase in this yield is observed. The magnitude of this increase depends on Δt, and is characterized by a time constant of 28 ± 4 ns. This rise in the fluorescence yield is attributed to a reduction of the oxidized (by P₁) reaction center P-680⁺ by a primary donor. At high pulse energies (P₁ = 4 · 10¹⁴ photons · cm⁻²) the magnitude of this fluorescence induction is diminished by another quenching effect which is attributed to triplet excited states generated by intense P₁ pulses. Assuming that the P₁ pulse energy dependence of the fluorescence yield rise reflects the closing of the reaction centers, it is estimated that about 3–4 photon hits per reaction center are required to close completely the reaction centers, and that there are 185–210 chlorophyll molecules per Photosystem II reaction center.     

Energy transfer in the photochemical apparatus of flashed bean leaves

Fluorescence and energy transfer properties of bean leaves greened by brief, repetitive xenon flashes were studied at −196 °C. The bleaching of P-700 has no influence on the yield of fluorescence at any wavelength of emission. The light-induced fluorescence yield changes which are observed in both the 690 and 730 nm emission bands in the low temperature fluorescence spectra are due to changes in the state of the Photosystem II reaction centers. The fluorescence yield changes in the 730 nm band are attributed to energy transfer from Photosystem II to Photosystem I. Such energy transfer was also confirmed by measurements of the rate of photooxidation of P-700 at −196 °C in leaves in which the Photosystem II reaction centers were either all open or all closed. It is concluded that energy transfer from Photosystem II to Photosystem I occurs in the flashed bean leaves which lack the light-harvesting chlorophyll a/b protein.     

The relationship between Q, C-550 and cytochrome b 559 in photoreactions at −196° in chloroplasts

Absorbance changes and fluorescence yield changes induced by irradiating spinach chloroplasts with red light at −196° were measured as a function of the redox potential of the chloroplast suspension. Absorbance changes at 546 nm indicate the photoreduction of C-550 and changes at 556 nm indicate the photooxidation of cytochrome b 559. The changes of fluorescence yield indicate the photoreduction of Q, the fluorescence quencher of chlorophylla a in Photosystem II. The titration curves for all three changes were essentially the same and showed the same midpoint potential. In other experiments as well, it was found that when C-550 is in the reduced state the fluorescence yield of the chloroplasts is high and the low-temperature photooxidation of cytochrome b 559 is blocked. These data indicate that C-550 may be equivalent to Q and that cytochrome b 559 serves as the electron donor for the photoreduction of C-550 at low temperature.     

Cadmium effect on the growth, photosynthesis, ultrastructure and phytochelatin content of green microalga Scenedesmus armatus: A study at low and elevated CO2 concentration

Short-term experiments were carried out to examine the toxicity of cadmium chloride (CdCl₂) at a concentration of 93 μM (EC_50/24) to green microalga Scenedesmus armatus, cultured at low (0.1%) and elevated (2%) concentration of CO₂. Cadmium did not affect the viability of cells cultured for 24 h in both CO₂ variants but markedly inhibited the growth of algae. This inhibition was more pronounced in cultures aerated with 0.1% (about 50% of control) than with 2% CO₂ (about 75% of control) and did not change during 72 h of culture. Cadmium inhibited the rate of oxygen evolution (P_oxy.) (70% of control) of cells cultured at 0.1% CO₂ and had no effect on P_oxy. of cells cultured at 2% CO₂. The values of the chlorophyll fluorescence parameters, i.e. F_M (maximum fluorescence yield), F_V (variable fluorescence), F_V/F_M (maximum quantum yield of PSII), Φ_PSII (effective quantum yield of PSII) and qP (photochemical quenching) were reduced by cadmium treatment in algae grown at 0.1% CO₂ concentration, whereas F₀ (initial fluorescence yield) remained unaffected. In high-CO₂ grown cells only F_V was significantly reduced. Cd-treated cells synthesized several thiol-containing peptides identified by HPLC as a dimer (PC₂), a trimer (PC₃) and a tetramer (PC₄) of phytochelatins (PC_S). High-CO₂ grown cells produced significantly more PCs than low-CO₂ grown cells and their individual appearance depended on the time of exposure and CO₂ level. The ultrastructural analysis of low-CO₂ grown cells showed in chloroplasts an increased number of small starch grains visible around the pyrenoid. In the enhanced vacuome compartment, various types of vacuoles were clearly seen in Cd-treated cells. Vacuoles containing non-membranous, electron-opaque deposits of an undefined structure and myelin-like figures were especially observed. The results suggest that algae living in conditions of elevated CO₂ are better protected against cadmium than those at ordinary CO₂ level, and productive processes are less affected than the growth ones.     

Light-induced changes of fluorescence and absorbance in spinach chloroplasts at −40 °C

1. 1. Spinach chloroplasts were stored in the dark for at least 1 h, rapidly cooled to −40 °C, and illuminated with continuous light or short saturating flashes. In agreement with the measurements of Joliot and Joliot, chloroplasts that had been preilluminated with one or two flashes just before cooling showed a less efficient increase in the yield of chlorophyll a fluorescence upon illumination at −40 °C than dark-adapted chloroplasts. The effect disappeared below −150 °C, but reappeared again upon warming to −40 °C. Little effect was seen at room temperature in the presence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU), added after the preillumination.

2. 2. Light-induced absorbance difference spectra at −40 °C in the region 500–560 nm indicated the participation of two components, the socalled 518-nm change (P518) and C-550. After preillumination with two flashes the absorbance change at 518 nm was smaller, and almost no C-550 was observed. After four flashes, the bands of C-550 were clearly visible again.

3. 3. The fluorescence increase and the absorbance change at 518 nm showed the same type of flash pattern with a minimum after the second and a maximum at the fourth flash. In the presence of 100 μM hydroxylamine, the fluorescence response was low after the fourth and high again after the sixth flash, which confirmed the hypothesis that the flash effect was related to the so-called S-state of the electron transport pathway from water to Photosystem 2.

4. 4. The kinetics of the light-induced absorbance changes were the same at each wavelength, and, apart from the size of the deflection, they were independent of preillumination. Flash experiments indicated that the absorbance changes were a one-quantum reaction. This was also true for the fluorescence increase in dark-adapted chloroplasts, but with preilluminated chloroplasts several flashes were needed to approximately saturate the fluorescence yield.

5. 5. The results are discussed in terms of a mechanism involving two electron donors and two electron acceptors for System 2 of photosynthesis.

Photochemical properties of a Photosystem II subchloroplast fragment

1. The Photosystem II fraction (D-10) obtained by incubation of spinach chloroplasts with digitonin was further purified by incubation with Triton X-100. The resulting Photosystem II subchloroplast fragment (DT-10) contained 1 mole of cytochrome b-559 per 170 moles of chlorophyll. It lacked cytochrome f and cytochrome b₆ and its content of P700 was low.

2. The DT-10 fragment showed only traces of photochemical activity with water as electron donor, but it was active in a Photosystem II reaction with 2,6-dichlorophenolindophenol as electron acceptor and diphenyl carbazide as donor. Photoreduction of NADP⁺ with diphenyl carbazide as donor was negligible. There was some photoreduction of NADP⁺ with ascorbate plus 2,6 dichlorophenolindophenol as donor but this activity could be accounted for by contamination with Photosystem I. These results are consistent with the Z-scheme of photosynthesis with Photosystems I and II operating in series for the reduction of NADP⁺ from water. DT-10 subchloroplast fragments showed a light-induced rise in fluorescence yield at 20 °C in the presence of diphenyl carbazide. A light-induced fluorescence increase also was observed at 77 °K.

3. During the preparation of the DT-10 fragment, the high potential form of cytochrome b-559 was largely converted to a form of lower potential and C-550 was converted to the reduced state. A photoreduction of C-550 was observed at liquidnitrogen temperature, provided the C-550 was oxidised with ferricyanide prior to cooling. Some photooxidation of cytochrome b-559 was obtained at 77 °K if the preparation was reduced prior to cooling, but the degree of photooxidation was variable with different preparations. C-550 does not appear to be identical with the primary fluorescence quencher, Q.

4. Photosystem I subchloroplast fragments (D-144) released by the action of digitonin were compared with Photosystem I fragments (DT-144) released from D-10 fragments by Triton X-100. There were no significant differences between D-144 and DT-144 fragments either in chlorophyll a/b ratio or in P700 content.     

Chlorophyll a fluorescence and photochemical activities of chloroplast fragments

1. Comparative studies were made on the fluorescence characteristics of chlorophyll a at 20° and −193°, and quantum efficiencies for P 700 oxidation and NADP⁺ reduction were measured in chloroplasts and chloroplast fragments obtained after incubation with 0.5% digitonin.

2. Differences in the flurescence yield of chlorophyll a in flowing and stationary suspensions of untreated chloroplasts and of the large fragments are indicative of light-induced photoreduction of the quencher Q of chlorophyll a, associated with pigment System 2 (chlorophyll a₂). The relatively low constant fluorescence yield of chlorophyll a in the small fragments indicates the absence of fluorescent chlorophyll a₂ from these fragments and suggests that the low fluorescence is due to chlorophyll a, associated with pigmen System 1 (chlorophyll a₁). The ratio of the fluorescence yields of chlorophyll a₁ and chlorophyll a₂ is 0.45:1. In the large particles the concentration ratio of pigment System 1 and System 2 is 1:3.

3. The efficiencies of quanta absorbed at 673, 683 and 705 nm for NADP⁺ reduction and P 700 oxidation in untreated chloroplasts and chloroplast fragments indicate that digitonin treatment results in a separation of System 2 from System 1 in the small fragments. Sonication does not cause such a separation. Under the conditions used P 700 oxidation and NADP⁺ reduction in the small fragments separated after digitonin treatment, occurred with maximal efficiency of 0.7 to 1.0 and 0.7, respectively.

4. The constancy of the fluorescence yield of chlorophyll a₁ in the small fragments, under conditions at which P 700 is oxidized and NADP⁺ is reduced, is interpreted as evidence either for the hypothesis that the fluorescence of chlorophyll a₁ is controlled by the redox state of the primary photoreductant XH, or alternatively for the hypothesis that energy transfer from fluorescent chlorophyll a₁ to P 700 goes via an intrinsically weak fluorescent, still unknown, chlorophyll-like pigment.

5. The low-temperature emission band around 730 nm is argued not to be due to excitation by System 1 only; the relatively large half width of the band, as compared to the emission bands at 683 and 696 nm, suggests that it is possibly due to overlapping emission bands of different pigments.     

Energy transduction in photosynthetic bacteria. XI. Further resolution of cytochromes of b type and the nature of the CO-sensitive oxidase present in the respiratory chain of Rhodopseudomonas capsulata

1. In membranes prepared from dark grown cells of Rhodopseudomonas capsulata, five cytochromes of b type (E′₀ at pH 7.0 +413±5, +270±5, +148±5, +56±5 and −32±5 mV) can be detected by redox titrations at different pH values. The midpoint potentials of only three of these cytochromes (b₁₄₈, b₅₆, and b₋₃₂) vary as a function of pH with a slope of 30 mV per pH unit.

2. In the presence of a Co/N₂ mixture, the apparent E′₀ of cytochrome b₂₇₀ shifts markedly towards higher potentials (+355 mV); a similar but less pronounced shift is apparent also for cytochrome b₁₅₀. The effect of CO on the midpoint potential of cytochrome b₂₇₀ is absent in the respiration deficient mutant M6 which possesses a specific lesion in the CO-sensitive segment of the branched respiratory chain present in the wild type strain.

3. Preparations of spheroplasts with lysozyme digestion lead to the release of a large amount of cytochrome c₂ and of virtually all cytochrome cc′. These preparations show a respiratory chain impaired in the electron pathway sensitive to low KCN concentration, in agreement with the proposed role of cytochrome c₂ in this branch; on the contrary, the activity of the CO-sensitive branch remains unaffected, indicating that neither cytochrome c₂ nor the CO-binding cytochrome cc′ are involved in this pathway.

4. Membranes prepared from spheroplasts still possess a CO-binding pigment characterized by maxima at 420.5, 543 and 574 nm and minima at 431, 560 nm in CO-difference spectra and with an band at 562.5 nm in reduced minus oxidized difference spectra. This membrane-bound cytochrome, which is coincident with cytochrome b₂₇₀, can be classified as a typical cytochrome “o” and considered the alternative CO-sensitive oxidase.     

Temperature dependence of delayed light emission in spinach chloroplasts

1. Delayed light of chlorophyll emitted at 0.1–3.9 ms after cessation of repetitive flash light was studied at temperatures between +40 and −196 °C in isolated spinach chloroplasts.

2. Induction kinetics of delayed light varied depending on temperature. It was found to be composed of two phases; one was an initial rapid rise followed by a rather fast decline to a low steady state level (fast phase), and the other was a slow increase after the initial rapid rise to the maximum followed by an insignificant slow decrease to a high steady state level (slow phase). The fast phase existed between −175 and 40 °C with the maximum at −40 °C, while the slow phase, between 0 and 40 °C with the maximum at 25 °C.

3. The intensity of delayed light at −175 °C was found to be less than one fiftieth that at 0 °C, and no delayed light emission was observed at −196 °C within experimental accuracy. This is in contrast to the results reported by Tollin, G., Fujimori, E. and Calvin, M. ((1958) Proc. Natl. Acad. Sci. U.S. 44, 1035–1047) in which the intensity of delayed light measured at −170 °C was about a half that at 0 °C.

4. The induction of delayed light measured at −96 °C was found to be significantly suppressed by the preillumination at −196 °C. This finding suggests that the primary photochemical event still survives at −196 °C without emission of delayed light.

5. Decay kinetics of delayed light after the flash excitation revealed the presence of at least two decay components. A slow decay component with a half decay time of several tens of milliseconds was observed at temperatures higher than 0 °C. A fast decay component with a half decay time of about 0.2 ms was observed at temperatures between −120 and 25 °C. The decay rate of this component was slightly retarded on cooling.

6. The System II particles derived from spinach chloroplasts with digitonin treatment showed a temperature dependence of delayed light similar to that of the chloroplasts. System I particles, on the other hand, scarcely emitted the delayed light at any temperature between 40 and −196 °C.     

Fluorescence yield kinetics in the microsecond-range in Chlorella pyrenoidosa and spinach chloroplasts in the presence of hydroxylamine

The kinetics of fluorescence yield inChlorella pyrenoidosa and spinach chloroplasts were studied in the time range of 0.5 μs to several hundreds of microseconds in the presence of hydroxylamine. Fluorescence was excited with a just-saturating xenon flash with a halfwidth of 13 μs (λ = 420 nm). The fast rise of the fluorescence yield which was limited by the rate of light influx, was, in the presence of 10⁻³–10⁻² M hydroxylamine, replaced by a slow component which had a half risetime of 25 μs in essence independent of light intensity. This slow fluorescence yield increase reflects a dark reaction on the watersplitting side of Photosystem II. Simultaneous oxygen evolution measurements suggested that a fast fluorescence component is only present in organisms with intact O₂-evolving system, whereas a slow rise predominantly occurs in organisms with the watersplitting system irreversibly inhibited by hydroxylamine.

The results can be explained by the following hypotheses: (a) The primary donor of Photosystem II in its oxidized state, P⁺, is a fluorescence quencher. (b) Hydroxylamine prevents the secondary electron donor Z from reducing the oxidized reaction center pigment P⁺ rapidly. This inhibition is dependent on hydroxylamine concentration and is complete at a concentration of 10⁻² M. (c) A second donor (not transporting electrons from water) transfers electrons to P⁺ with a half time of roughly 25 μs.     

A negative resistance region underlies the triggering property of membrane potential in human T-lymphocytes

Steady-state current-voltage relationships (SSCVRs) of the plasma membrane of human T-lymphocytes were studied at the physiological temperature of 37°C by using the whole-cell patch-clamp technique. SSCVRs displayed a characteristic N-like shape with a negative resistance region (NRR) in a voltage range of −45 to −35 mV. The majority of cells assayed revealed SSCVR patterns crossing the V-axis at three points (in mV): V₁ = −55 to −45, V₂ = −40 to −35, V₃ = −30 to −10. SSCVRs of T-cells activated by phytohaemagglutinin (48–96 h) also displayed NRR, but crossed the V-axis at one point only (V₁ = −55 to −60 mV). It implies the possibility of two stable levels of membrane potential (V₁ and V₃) for the resting T-cells, but only one (V₁) for activated T-cells. These data thus account for the triggering property of T-cell membrane potential previously reported. The NRR can be explained on the basis of the Hodgkin-Huxley type n⁴j model of K⁺ channel kinetics. According to the model the possibility for a membrane to have on or two stable levels of membrane potential depends on the ratio of selective K⁺ conductance to non-selective leaky conductance (G_k/G_leak). The steady-state level of K⁺ conductance in resting T-lymphocytes proved to be sensitive to Ca²⁺. Buffering Ca²⁺ ions from either external or internal solution resulted in an appreciable increase in K⁺ conductance. The possibility for membrane potential have two stable levels of membrane potential in connection with the Ca²⁺ dependence of K⁺ conductance was supposed to be important for Ca²⁺-signalling during T-cell activation.     

Characteristics of thermoluminescence bands of intact leaves and isolated chloroplasts in relation to the watersplitting activity in photosynthesis

Plant materials (intact leaves, chloroplasts or subchloroplast particles) preilluminated at a low temperature (e.g. −60°C) were rapidly cooled to −196°C and then the luminescence emitted from the sample on raising the temperature was measured as a function of temperature, by means of a sensitive photo-electron counting technique. Mature spinach leaves showed five luminescence bands at different temperatures which were denoted as Z_v, A, B₁, B₂ and C bands. The A, B₁, B₂ and C bands appeared at constant temperatures, −10, +25, +40 and +55°C, respectively, being independent of the illumination temperature, but the Z_v band appeared at a variable temperature slightly higher than the illumination temperature. The B₁ and B₂ bands were absent in the thermoluminescence profiles of samples devoid of the oxygenevolving activity, such as heat-treated spinach leaves, wheat leaves greened under intermittent illumination and photosystem-II particles prepared with Triton X-100. It was deduced that these luminescence bands arise from the energy stored by the electron flow in photosystem II to evolve oxygen, and other bands were ascribed to charge-separation in some other sites not related to the oxygen evolving system.     

Kinetic characterization of chiral biocatalysis of cycloarenes by the camphor 5-monooxygenase enzyme system

Redox enzyme mediated biocatalysis has the potential to regio- and stereo-specifically oxidize hydrocarbons producing valuable products with minimal by-product formation. In vitro reactions of the camphor (cytochrome P-450) 5-monooxygenase enzyme system with naphthalene-like substrates yield stereospecifically hydroxylated products from nonactivated hydrocarbons. Specifically, the enzyme system catalyzes the essentially stereospecific conversion of the cycloarene, tetralin (1,2,3,4-tetrahydronaphthalene) to (R)-1-tetralol ((R)-(−)-1,2,3,4-tetrahydro-1-naphthol). It is shown that this reaction obeys Michaelis–Menten kinetics and that interactions between the enzyme subunits are not affected by the identity of the substrate. This subunit independence extends to the efficiency of NADH usage by the enzyme system—subunit ratios do not effect efficiency, but substrate identity does. Tetralin is converted at an efficiency of 13±3%, whereas (R)-1-tetralol is converted at 7.8±0.7%. A model of this system based on Michaelis–Menten parameters for one subunit (Pdx: K_M=10.2±2 μM) and both substrates (tetralin: K_M=66±26 μM, ν_max=0.11±0.04 s⁻¹, and (R)-1-tetralol: K_M=2800±1300 μM, ν_max=0.83±0.22 s⁻¹) is presented and used to predict the consumption and production of all substrates, products and cofactors.