Photosystem II energy coupling in chloroplasts with H2O2 as electron donor

NH₂OH-treated, non-water-splitting chloroplasts can oxidize H₂O₂ to O₂ through Photosystem II at substantial rates (100–250 μequiv · h^?1 · mg^?1 chlorophyll with 5 mM H₂O₂) using 2,5-dimethyl-p-benzoquinone as an electron acceptor in the presence of the plastoquinone antagonist dibromothymoquinone. This H₂O₂ → Photosystem II → dimethylquinone reaction supports phosphorylation with a $\text{P}\text{e}{}_2$ ratio of 0.25–0.35 and proton uptake with $\text{H}{}^{\mathrm{+}}\text{e}$ values of 0.67 (pH 8)–0.85 (pH 6). These are close to the $\text{P}\text{e}{}_2$ value of 0.3–0.38 and the $\text{H}{}^{\mathrm{+}}\text{e}$ values of 0.7–0.93 found in parallel experiments for the H₂O → Photosystem II → dimethylquinone reaction in untreated chloroplasts. Semi-quantitative data are also presented which show that the donor → Photosystem II → dibromothymoquinone (→O₂) reaction can support phosphorylation when the donor used is a proton-releasing reductant (benzidine, catechol) but not when it is a non-proton carrier (I^?, ferrocyanide).     

Reactions between primary and secondary acceptors of Photosystem II in Chlorella Pyrenoidosa under anaerobic conditions as studied by chlorophyll a fluorescence

The kinetics of the fluorescence yield Ф of chlorophyll a in Chlorella pyrenoidosa were studied under anaerobic conditions in the time range from 50 μs to several minutes after short ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 30}\text{ns}$ or 5 μs) saturating flashes. The fluorescence yield “in the dark” increased from $\text{Ф = 1}$ at the beginning to $\text{Ф ≈ 5}$ in about 3 h when single flashes separated by dark intervals of about 3 min were given.After one saturating flash, Ф increased to a maximum value (4–5) at 50 μs, then Ф decreased to about 3 with a half time of about 10 ms and to the initial value with a half time of about 2 s. When two flashes separated by 0.2 s were given, the first phase of the decrease after the second flash occurred within 2 ms. After one flash given at high initial fluorescence yield, the 10-ms decay was followed by a 10 s increase to the initial value. After the two flashes 0.2 s apart, the rapid decay was not follewed by a slow increase.These and other experiments provided additional evidence for and extend an earlier hypothesis concerning the acceptor complex of Photosystem II (Bouges-Bocquet, B. (1973) Biochim. Biophys. Acta 314, 250–256; Velthuys, B. R. and Amesz, J. (1974) Biochim. Biophys. Acta 333, 85–94): reaction center 2 contains an acceptor complex QR consisting of an electron-transferring primary acceptor molecule Q, and a secondary electron acceptor R, which can accept two electrons in succession, but transfers two electrons simultaneously to a molecule of the tertiary acceptor pool, containing plastoquinone (A). Furthermore, the kinetics indicate that 2 reactions centers of System I, excited by a short flash, cooperate directly or indirectly in oxidizing a plastohydroquinone molecule (A^2?). If initially all components between photoreaction 1 and 2 are in the reduced state the following sequence of reactions occurs after a flash has oxidised A^2? via System I: Q^?R^2? + A → Q^?R + A^2? → QR^? + A^2?. During anaerobiosis two slow reactions manifest themselves: the reduction of R (and A) within 1 s, presumably by an endogenous electron donor D₁, and the reduction of Q in about 10 s when R is in the state R^? and A in the state A^2?. An endogenous electron donor, D₂, and Q^? compete in reducing the photooxidized donor complex of System II in reactions with half times of the order of 1 s.     

Kinetics of reduction of the oxidized primary electron donor of Photosystem II in spinach chloroplasts and in Chlorella cells in the microsecond and nanosecond time ranges following flash excitation

Absorption changes (ΔA) at 820 nm, following laser flash excitation of spinach chloroplasts and Chlorella cells, were studied in order to obtain information on the reduction time of the photooxidized primary donor of Photosystem II at physiological temperatures.In the microsecond time range the difference spectrum of ΔA between 750 and 900 nm represents a peak at 820 nm, attributable to a radical-cation of chlorophyll a. In untreated dark-adapted material the signal can be attributed solely to P⁺?700; it decays in a polyphasic manner with half-times of 17 μs, 210 μs and over 1 ms. The oxidized primary donor of Photosystem II (P⁺_II) is not detected with a time resolution of 3 μs. After treatment with 3–10 mM hydroxylamine, which inhibits the donor side of Photosystem II, P⁺_II is observed and decays biphasically (a major phase with $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 20–40 μ}\text{s}$, and a minor phase with $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{? 200 μ}\text{s}$), probably by reduction by an accessory electron donor.In the nanosecond range, which was made accessible by a new fast-response flash photometer operating at 820 nm, it was found the P⁺_II is reduced with a half-time of 25–45 ns in untreated dark-adapted chloroplasts. It is assumed that the normal secondary electron donor is responsible for this fast reduction.     

Flash-induced photophosphorylation in Rhodospirillum rubrum chromatophores I. The relationship between cytochrome c-420 content and photophosphorylation

The content of cytochrome c-420 in Rhodospirillum rubrum chromatophores prepared by grinding with alumina is 5–10% of that in whole cells, and 20–40% in chromatophores by ‘French’ pressing.Flash-induced phosphorylation of various chromatophores which varied in cytochrome content from 7 to 40% is proportional to the cytochrome content. Extrapolating the cytochrome c-420 content to that observed in whole cells, a ratio $\text{ATP}\text{P}{}^{\mathrm{+}}\text{X}{}^{\mathrm{?}}$ near 1 is calculated. At low flash intensity the phosphorylation per flash is proportional to flash energy.Photophosphorylation in flashes given after a time of several minutes is only slightly dependent on the number of flashes. If the flashes are spaced from 0.1 to 10 s, relative phosphorylation in the first flash is about 70% and in the second 90% of that observed in the following flashes. Proton binding is not affected by the cytochrome c-420 content and a ratio of $\text{H}{}^{\mathrm{+}}\text{P}{}^{\mathrm{+}}\text{X}{}^{\mathrm{?}}$ of 2.3 was found.These results can be explained by a working hypothesis in which charge separation occurring at one reaction centre and the resulting electron transport mediated amongst others by c-420, results in the injection of two protons into an ATPase, this in contrast to a chemiosmotic mechanism, where the protons are released in the chromatophore inner space.     

Ligand-dependent reactivity of (Na+ + K+)-ATPase with showdomycin

Showdomycin inhibited pig brain ($\text{Na}{}^{\mathrm{+}}\text{+}\text{K}{}^{\mathrm{+}}\text{)-}\text{ATPase}$ with pseudo first-order kinetics. The rate of inhibition by showdomycin was examined in the presence of 16 combinations of four ligands, i.e., Na⁺, K⁺, Mg²⁺ and ATP, and was found to depend on the ligands added. Combinations of ligands were divided into five groups in terms of the magnitude of the rate constant; in the order of decreasing rate constants these were: (1)$\text{Na}{}^{\mathrm{+}}\text{+}\text{Mg}{}^{\mathrm{2+}}\text{+}\text{ATP}$, (2) $\text{Mg}{}^{\mathrm{2+}}$, $\text{Mg}{}^{\mathrm{2+}}\text{+}\text{K}{}^{\mathrm{+}}$, $\text{K}{}^{\mathrm{+}}$ and none, (3) $\text{Na}{}^{\mathrm{+}}\text{+}\text{Mg}{}^{\mathrm{2+}}\text{,}\text{Na}{}^{\mathrm{+}}$, $\text{K}{}^{\mathrm{+}}\text{+}\text{Na}{}^{\mathrm{+}}$ and $\text{Na}{}^{\mathrm{+}}\text{+}\text{K}{}^{\mathrm{+}}\text{+}\text{Mg}{}^{\mathrm{2+}}$, (4) $\text{Mg}{}^{\mathrm{2+}}\text{+}\text{K}{}^{\mathrm{+}}\text{+}\text{ATP}\text{,}\text{K}{}^{\mathrm{+}}\text{+}\text{ATP}$ and $\text{Mg}{}^{\mathrm{2+}}\text{+}\text{ATP}\text{, (5)}\text{K}{}^{\mathrm{+}}\text{+}\text{Na}{}^{\mathrm{+}}\text{+}\text{ATP}$, $\text{Na}{}^{\mathrm{+}}\text{+}\text{ATP}$, $\text{Na}{}^{\mathrm{+}}\text{+}\text{ATP}$, $\text{Na}{}^{\mathrm{+}}\text{+}\text{K}{}^{\mathrm{+}}\text{+}\text{Mg}{}^{\mathrm{2+}}\text{+}\text{ATP}$ and ATP. The highest rate was obtained in the presence of Na⁺, Mg²⁺ and ATP. The apparent concentrations of Na⁺, Mg²⁺ and ATP for half-maximum stimulation of inhibition ($\text{K}{}_{0.5}{}^{\mathrm{<mtext>s</mtext>}}$) were 3 mM, 0.13 mM and 4μM, respectively. The rate was unchanged upon further increase in Na⁺ concentration from 140 to 1000 mM. The rates of inhibition could be explained on the basis of the enzyme forms present, including E₁, E₂, ES, E₁-P and E₂-P, i.e., E₂ has higher reactivity with showdomycin than E₁, while E₂-P has almost the same reactivity as E₁-P. We conclude that the reaction of ($\text{Na}{}^{\mathrm{+}}\text{+}\text{K}{}^{\mathrm{+}}\text{)-}\text{ATPase}$ proceeds via at least four kinds of enzyme form (E₁, E₂, E₁ · nucleotide and EP), which all have different conformations.     

Thiophosphorylation of (Na + K+)-ATPase yields an ADP-sensitive phosphointermediate

(1) Treatment of $\text{(Na}{}^{\mathrm{+}}\text{+ K}{}^{\mathrm{+}}\text{)-ATPase}$ from rabbit kidney outer medulla with the $\text{γ-}{}^{35}\text{S}$ labeled thio-analogue of ATP in the presence of $\text{Na}{}^{\mathrm{+}}\text{+ Mg}{}^{\mathrm{2+}}$ and the absence of K⁺ leads to thiophosphorylation of the enzyme. The $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ value for [γ-S]ATP is 2.2 μM and for Na⁺ 4.2 mM at 22°C. Thiophosphorylation is a sigmoidal function of the Na⁺ concentration, yielding a Hill coefficient $\text{n}\text{H}\text{= 2.6}$. (2) The thio-analogue ($\text{K}{}_{\mathrm{<mtext>m</mtext><mtext>\; =\; 35\; \mu M</mtext>}}$) can also support overall $\text{(Na}{}^{\mathrm{+}}\text{+ K}{}^{\mathrm{+}}\text{)-ATPase}$ activity, but $\text{V}{}_{\mathrm{<mtext>max</mtext>}}$ at 37°C is only $\text{1.3 γ}\text{mol}\text{· (mg protein)}{}^{\mathrm{?}}\text{·}$ h^?1 or 0.09% of the specific activity for ATP ($\text{K}{}_{\mathrm{<mtext>m</mtext><mtext>\; =\; 0.43\; mM</mtext>}}$). (3) The thiophosphoenzyme intermediate, like the natural phosphoenzyme, is sensitive to hydroxylamine, indicating that it also is an acylphosphate. However, the thiophosphoenzyme, unlike the phosphoenzyme, is acid labile at temperatures as low as 0°C. The acid-denatured thiophosphoenzyme has optimal stability at pH 5–6. (4) The thiophosphorylation capacity of the enzyme is equal to its phosphorylation capacity, indicating the same number of sites. Phosphorylation by ATP excludes thiophosphorylation, suggesting that the two substrates compete for the same phosphorylation site. (5) The (apparent) rate constants of thiophosphorylation (0.4 s^?1 vs. 180 s^?1), spontaneous dethiophosphorylation (0.04 s^?1 vs. 0.5 s^?1) and K⁺-stimulated dethiophosphorylation (0.54 s^?1 vs. 230 s^?1) are much lower than those for the corresponding reactions based on ATP. (6) In contrast to the phosphoenzyme, the thiophosphoenzyme is ADP-sensitive (with an apparent rate constant in ADP-induced dethiophosphorylation of 0.35 s^?1, $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$$\text{ADP = 48 μM at 0.1 mM ATP}$) and is relatively K⁺-insensitve. The $\text{K}{}_{\mathrm{<mtext>m</mtext>}}$ for K⁺ in dethiophosphorylation is 0.9 mM and in dephosphorylation 0.09 mM. The thiophosphoenzyme appears to be for 75–90% in the ADP-sensitive E₁-conformation.     

Local measurement of lateral motion in erythrocyte membranes by photobleaching technique

The lateral diffusion coefficients ($\text{D}$) of the molecular fluorescence probe 3,3′-dioctadecylindocarbocyanine iodide (DII) in the membrane of discoid erythrocyte ghosts has been measured with the photobleaching technique between 7°C and 40°C. A fluorescence microscope which allows bleaching experiments within small local fields (approx. 1 μm²) at high magnification (X1600) has been used for these measurements. The diffusion coefficient increases from $\text{D = 9 · 10}{}^{\mathrm{?10}}\text{cm}{}^2\text{/s}$ to $\text{D = 7.5 · 10}{}^{\mathrm{?9}}\text{cm}{}^2\text{/s}$ from 7 to 40°C. An increase in membrane fluidity between 12°C and 17°C indicates a conformational change of the lipid bilayer moiety in this temperature region. The diffusion coefficient measured in the regions between the spicules of echinocytes is appreciably smaller than in the untransformed discoid ghosts. In the myelin tubes originating from cells, the lateral diffusion is somewhat larger (about a factor of 2) than in the non-transformed ghosts. With the fluorescence probe technique the rate of growth of myelin tubes of 0.3 μm diameter has been estimated.     

The study of the primary photoprocesses in Photosystem I of chloroplasts Recombination luminescence,chlorophyll triplet state and triplet-triplet annihilation

The dependence of the delayed luminescence of Photosystem I on the state of the reaction centers has been studied. Light flash induces a charge separation in the centers: $\text{P-700 · P-430}\textcolor{red}{}\text{P-700}{}^{\mathrm{+}}\text{· P-430}{}^{\mathrm{?}}$. Dark recombination of charges is accompanied by the recombination luminescence with $\text{τ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{? 20}\text{ms}$.If the centers are in the P-700 · P-430^? state or if P-430 is inactivated by heat, then flashing of Photosystem I generates the triplet state chlorophyll with $\text{τ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{? 0.5}\text{ms}$. The triplet state has been measured by the delayed fluorescence of chlorophyll at 20 °C and 77 °K and by the chlorophyll phosphorescence at 77 °K. The delayed fluorescence at 20 °C arises from the thermal activation of the triplet state up to the excited singlet level of chlorophyll and at 77 °K it is due to triplet-triplet annihilation. The quantum yield of the triplet formation, estimated by a comparison of the light saturation curves of delayed fluorescence at 20 °C and of P-700 photooxidation under the same experimental (optical) conditions, is ≈ 0.9 of the P-700⁺ yield. Only one triplet of chlorophyll can be generated per P-700. Under heat inactivation of P-430 the triplet formation is not observed when P-700 is oxidized.It is assumed that the triplet-triplet annihilation at 77 °K is related with the strong interaction between the chlorophyll molecules in the pigment complex of Photosystem I. The possibility of a triplet participation in the primary processes of photosynthesis is discussed.     

The dependence of reaction center and antenna triplets on the redox state of Photosystem I

The formation of chlorophyll triplet states during illumination of Photosystem I reaction center samples depends upon the redox state of P-700, X and ferredoxin Centers A and B. When the reaction centers are in the states P-700⁺A₁XFd_BFd^?_A and P-700 A₁XFd^?_BFd^?_A prior to illumination, we observe electron paramagnetic resonance (EPR) spectra from a triplet species which has zero-field splitting parameters (|D| and |E|) larger than those of either the chlorophyll a or chlorophyll b monomer triplet, and a polarization which results from population of the triplet spin sublevels by an intersystem crossing mechanism. We interpret this triplet as arising from photoexcited chlorophyll antenna species associated with reaction centers in the states P-700⁺Fd^?_A and P-700⁺X^?, respectively, which undergo de-excitation via intersystem crossing. When the reaction centers are in the states P-700A₁XFd^?_BFd^?_A and P-700A₁X^?Fd^?_BFd^?_A prior to illumination, we observe a triplet EPR signal with a polarization which results from population of the triplet spin sublevels by radical pair recombination, and which has a |D| value similar to that of chlorophyll a monomer. We interpret this triplet (the radical pair-polarized triplet) as arising from ³P-700 which has been populated by the process $\text{P-700}{}^{\mathrm{+}}\text{A}{}^{\mathrm{?}}{}_1\text{→}{}^3\text{P-700}\text{A}{}_1$. We observe both the radical pair-polarized triplet and the chlorophyll antenna triplet when the reaction centers are in the state P-700 A₁XFd^?_BFd^?_A, presumably because the processes P-700⁺A^?₁X → P-700⁺A₁X^? and $\text{P-700}{}^{\mathrm{+}}\text{A}{}^{\mathrm{?}}{}_1\text{X}\text{→}{}^3\text{P-700}\text{A}{}_1\text{X}$ have similar rate constants when Centers A and B are reduced, i.e., the forward electron transfer time from A^?₁ to X is apparently much slower in the redox state P-700 A₁XFd^?_BFd^?_A than it is in state P-700 A₁XFd_BFd_A. The amplitude of the radical pair-polarized triplet EPR signal does not decrease in the presence of a 13.5-G-wide EPR signal centered at g 2.0 which was recorded in the dark prior to triplet measurements in samples previously frozen under intense illumination. This g 2.0 signal, which has been attributed to phototrapped A^?₁ (Heathcote, P., Timofeev, K.N. and Evans, M.C.W. (1979) FEBS Lett. 101, 105–109), corresponds to as many as 12 spins per P-700 and can be photogenerated during freezing without causing any apparent attenuation of the radical pair-polarized triplet amplitude. We conclude that species other than A^?₁ contribute to the g 2.0 signal.     

The loss of the phoS periplasmic protein leads to a change in the specificity of a constitutive inorganic phosphate transport system in Escherichia coli

The phoS periplasmic protein, implicated in alkaline phosphatase regulation, is shown to be involved in inorganic phosphate (Pi) transport in $\text{E. coli}$. Although $\text{pho}\text{S}{}^{\mathrm{?}}$ cells dependent upon the PST system for Pi transport can grow in minimal medium with 1 mM Pi as source of phosphorus, the affinity of these cells for Pi is greatly reduced; Km = 18 μM compared with Km = 0.4 μM for $\text{phoS}{}^{\mathrm{+}}$ cells. $\text{pho}\text{S}{}^{\mathrm{?}}$ cells dependent upon the PST Pi transport system acquire the ability to accumulate Asi from the medium in contrast to $\text{pho}\text{S}{}^{\mathrm{+}}$ cells which exclude this toxic anion. It would appear that the periplasmic phoS protein is not essential for Pi accumulation but is involved in maintaining the specificity of the PST Pi transport system.     

Histamine,theophylline and tryptamine transport through lipid bilayer membranes

Diffusion of histamine, theophylline and tryptamine through planar lipid bilayer membranes was studied as a function of pH. Membranes were made of egg phosphatidylcholine plus cholesterol (1 : 1 mol ratio) in tetradecane. Tracer fluxes and electrical conductances were used to estimate the permeabilities to nonionic and ionic species. Only the nonionic forms crossed the membrane at a significant rate. The membrane permeabilities to the nonionic species were: histamine, $\text{3.5 · 10}{}^{\mathrm{?5}}\text{cm}\text{· s}{}^{\mathrm{?1}}$; theophylline, $\text{2.9 · 10}{}^{\mathrm{?4}}\text{cm}\text{· s}{}^{\mathrm{?1}}$; and tryptamine, $\text{1.8 · 10}{}^{\mathrm{?1}}\text{cm}\text{· s}{}^{\mathrm{?1}}$. Chemical reactions in the unstirred layers are important in the transport of tryptamine and theophylline, but not histamine. For example, as pH decreased from 10.0 to 7.5 the ratio of nonionic (B) to ionic (BH⁺) tryptamine decreased by 300-fold, but the total tryptamine permeability decreased only 3-fold. The relative insensitivity of the total tryptamine permeability to the ratio, [B]/[BH⁺], is due to the rapid interconversion of B and BH⁺ in the instirred layers. Our model describing diffusion and reaction in the unstirred layers can explain some ‘anomalous’ relationships between pH and weak acid/base transport through lipid bilayer and biological membranes.     

Delayed fluorescence from Rhodopseudomonas sphaeroides following single flashes

Delayed fluorescence from Rhodopseudomonas sphaeroides chromatophores was studied with the use of short flashes for excitation. Although the delayed fluorescence probably arises from a back-reaction between the oxidized reaction center bacteriochlorophyll complex (P⁺) and the reduced electron acceptor (X^?), the decay of delayed fluorescence after a flash is much faster ($\text{τ}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{≈ 120 μ}\text{s}$) than the decay of P⁺X^?. The rapid decay of delayed fluorescence is not due to the uptake of a proton from the solution, nor to a change in membrane potential. It correlates with small optical absorbance changes at 450 and 770 nm which could reflect a change in the state of X^?.The intensity of the delayed fluorescence is 11–18-fold greater if the excitation flashes are spaced 2 s apart than it is if they are 30 s apart. The enhancement of delayed fluorescence at high flash repetition rates occurs only at redox potentials which are low enough (< + 240 mV) so that electron donors are available to reduce P⁺X^? to PX^? in part of the reaction center population. The enhancement decays between flashes as PX^? is reoxidized to PX, as measured by the recovery of photochemical activity. Evidently, the reduction of P⁺X^? to PX^? leads to the storage of free energy that can be used on a subsequent flash to promote delayed fluorescence. The reduction of P⁺X^? also is associated with a carotenoid spectral shift which decays as PX^? is reoxidized to PX. Although this suggests that the free energy which supports the delayed fluorescence might be stored as a membrane potential, the ionophore gramicidin D only partially inhibits the enhancement of delayed fluorescence. With widely separated flashes, gramicidin has no effect on delayed fluorescence.At redox potentials low enough to keep X fully reduced, delayed fluorescence of the type described above does not occur, but one can detect weak luminescence which probably is due to phosphorescence of a protoporphyrin.     

Enthalpy and volume changes accompanying electron transfer from P-870 to quinones in Rhodopseudomonas sphaeroides reaction centers

A capacitor microphone was used to measure the enthalpy and volume changes that accompany the electron transfer reactions, $\text{PQ}{}_{\mathrm{A}}\text{→}\text{hv}\text{P}{}^{\mathrm{+}}\text{Q}{}^{\mathrm{?}}{}_{\mathrm{A}}\text{and PQ}{}_{\mathrm{A}}\text{Q}{}_{\mathrm{B}}\text{→}\text{hv}\text{P}{}^{\mathrm{+}}\text{Q}{}_{\mathrm{A}}\text{Q}{}^{\mathrm{?}}{}_{\mathrm{B}}$, following flash excitation of photosynthetic reaction centers isolated from Rhodopseudomonas sphaeroides. P is a bacteriochlorophyll dimer (P-870), and Q_A and Q_B are ubiquinones. In reaction centers containing only Q_A, the enthalpy of P⁺Q^?_A is very close to that of the PQ_A ground state (ΔH_r = 0.05 ± 0.03 eV). The free energy of about 0.65 eV that is captured in the photochemical reaction evidently takes the form of a substantial entropy decrease. In contrast, the formation of P⁺Q_AQ^?_B in reaction centers containing both quinones has a ΔH_r of 0.32 ± 0.02 eV. The entropy change must be near zero in this case. In the presence of o-phenanthroline, which blocks electron transfer between Q^?_A and Q_B, ΔH_r for forming P⁺Q^?_AQ_B is 0.13 ± 0.03 eV. The influence of flash-induced proton uptake on the results was investigated, and the ΔH_r values given above were measured under conditions that minimized this influence. Although the reductions of Q_A and Q_B involve very different changes in enthalpy and entropy, both reactions are accompanied by a similar volume decrease of about 20 ml/mol. The contraction probably reflects electrostriction caused by the charges on P⁺ and Q^?_A or Q^?_B.     

Reconstitution of b-type cytochrome oxidase from Rhodopseudomonas capsulata in liposomes and turnover studies of proton translocation

Purified b-type cytochrome oxidase from Rhodopseudomonas capsulata was incorporated into phospholipid vesicles to measure proton extrusion with pulses of ferrocytochrome c for one oxidase turnover. In accordance with the pH shift of its midpoint potential, the purified oxidase showed a proton extrusion of 0.24 $\text{H}{}^{\mathrm{+}}\text{e}{}^{\mathrm{?}}$ with uptake of 1 $\text{H}{}^{\mathrm{+}}\text{e}{}^{\mathrm{?}}$ from the liposomes for the reduction of oxygen to water. This proton translocation could only be observed in the presence of valinomycin +K⁺ and was not inhibited by DCCD. Oxidase preparations from the first purification step, which contain other protein compounds especially a membrane-bound cytochrome c but not the ubiquinol-cytochrome c₂-oxidoreductase showed a pumping activity of 0.9 $\text{H}{}^{\mathrm{+}}\text{e}{}^{\mathrm{?}}$, which was inhibited by DCCD for nearly 75%. Inhibition of the electron transfer was not observed, which could be explained by a ‘molecular slipping’ of proton extrusion and electron transfer. Proton extrusion from two oxidase-turnovers was only 80% of that from one turnover. The proton pumping of the b-type oxidase strongly depended on the enzyme/phospholipid ratio.     

Acid dissociation of cyclohexaamylose and cycloheptaamylose

Acid dissociation constants of aqueous cyclohexaamylose (6-Cy) and cycloheptaamylose (7-Cy) have been determined at 10–47 and 25–55°C, respectively, by pH potentiometry. Standard enthalpies and entropies of dissociation derived from the temperature dependences of these pK_a's are ΔH⁰ = 8.4 ± 0.3 kcal mol^?1, $\text{Δ}\text{S}{}^0\text{= ?28. ± 1}\text{cal mol}{}^{\mathrm{?1}}{}^0\text{K}{}^{\mathrm{?1}}$ for 6-Cy and ΔH⁰ = 10.0 ± 0.1 kcal mol^?1, $\text{Δ}\text{S}{}^0\text{= ?22.4 ±0.3}\text{cal mol}{}^{\mathrm{?1}}{}^0\text{K}{}^{\mathrm{?1}}$ for 7-Cy. Intrinsic ¹³C nmr resonance displacements of anionic 6- and 7-Cy were measured at 30°C in 5% D₂O ($\text{v}\text{v}$). These results indicate that the dissociation of 6- and 7-Cy involves both C2 and C3 2⁰-hydroxyl groups. The thermodynamic and nmr parameters are discussed in terms of interglucosyl hydrogen bonding.