Initial formation of ATP in photophosphorylation does not require a proton gradient

Mitochondrial energetics with transmembrane electrostatically localized protons: do we have a thermotrophic feature?

Transmembrane electrostatically localized protons (TELP) theory has been recently recognized as an important addition over the classic Mitchell's chemiosmosis; thus, the proton motive force (pmf) is largely contributed from TELP near the membrane. As an extension to this theory, a novel phenomenon of mitochondrial thermotrophic function is now characterized by biophysical analyses of pmf in relation to the TELP concentrations at the liquid-membrane interface. This leads to the conclusion that the oxidative phosphorylation also utilizes environmental heat energy associated with the thermal kinetic energy (kBT) of TELP in mitochondria. The local pmf is now calculated to be in a range from 300 to 340 mV while the classic pmf (which underestimates the total pmf) is in a range from 60 to 210 mV in relation to a range of membrane potentials from 50 to 200 mV. Depending on TELP concentrations in mitochondria, this thermotrophic function raises pmf significantly by a factor of 2.6 to sixfold over the classic pmf. Therefore, mitochondria are capable of effectively utilizing the environmental heat energy with TELP for the synthesis of ATP, i.e., it can lock heat energy into the chemical form of energy for cellular functions.

Isothermal Environmental Heat Energy Utilization by Transmembrane Electrostatically Localized Protons at the Liquid-Membrane Interface

This study employing the latest theory on transmembrane electrostatic proton localization has now, for the first time, consistently elucidated a decades-longstanding bioenergetic conundrum in alkalophilic bacteria and more importantly discovered an entirely new feature: isothermal environmental heat utilization by electrostatically localized protons at the liquid-membrane interface. It was surprisingly revealed that the protonic motive force (equivalent to Gibbs free energy) from the isothermal environmental heat energy utilization through the electrostatically localized protons is not constrained by the overall energetics of the redox-driven proton pump system because of the following: (a) the transmembrane electrostatically localized protons are not free to move away from the membrane surface as a protonic capacitor feature; (b) the proton pumps embedded in the cell membrane extend beyond the localized proton layer apparently as an asymmetric property of the biological membrane; and (c) the protonic inlet mouth of the ATP synthase that accepts protons is located within this layer as another natural property of the asymmetric biological membrane. This work has now, for the first time, shown a novel thermotrophic feature where biological systems can isothermally utilize environmental heat energy through transmembrane electrostatically localized protons to help drive ATP synthesis.

Electrostatically localized proton bioenergetics: better understanding membrane potential

In Mitchell's chemiosmotic theory, membrane potential Δ ψ was given as the electric potential difference across the membrane. However, its physical origin for membrane potential Δ ψ was not well explained. Using the Lee proton electrostatic localization model with a newly formulated equation for protonic motive force (pmf) that takes electrostatically localized protons into account, membrane potential has now been better understood as the voltage difference contributed by the localized surface charge density ( [ H L + ] + ∑ i = 1 n [ M L i + ] ) at the liquid-membrane interface as in an electrostatically localized protons/cations-membrane-anions capacitor. That is, the origin of membrane potential Δ ψ is now better understood as the electrostatic formation of the localized surface charge density that is the sum of the electrostatically localized proton concentration [ H L + ] and the localized non-proton cations density ∑ i = 1 n [ M L i + ] at the liquid membrane interface. The total localized surface charge density equals to the ideal localized proton population density [ H L + ] 0 before the cation-proton exchange process; since the cation-proton exchange process does not change the total localized charges density, neither does it change to the membrane potential Δ ψ . The localized proton concentration [ H L + ] represents the dominant component, which accounts about 78% of the total localized surface charge density at the cation-proton exchange equilibrium state in animal mitochondria. Liquid water as a protonic conductor may play a significant role in the biological activities of membrane potential formation and utilization.

Cooperation among electron-transfer complexes in ATP synthesis in chloroplasts

We have investigated the extent to which redox reactions of thylakoid membranes cooperate in ATP synthesis. This was done by measuring the onset of ATP synthesis following a series of single-turnover light-flashes at various levels of electron transport inhibition. In the presence of antibiotics that prevent the formation of a membrane potential, the onset of ATP synthesis seems to depend entirely on the formation of an adequately large delta pH. Under our conditions, the accumulation of about 60 mmol H+ X mol chlorophyll-1 is then necessary to form the requisite delta pH, which in turn requires about 15 saturating flashes in uninhibited thylakoid samples. Inhibition of some of the electron transfer centers by limiting the light intensity of the flashes, by dichlorophenyldimethylurea, by heat treatment, or by NH2OH-treatment caused an increase in the number of flashes required for the onset of ATP synthesis. The increase in the requisite number of flashes reflected the decreased number of electrons transferred in each flash, almost exactly the same number of electrons being transferred before ATP synthesis could begin. This effect of inhibitors was true when the two photosystems were operating in unison and when either of the two photosystems was acting alone. However, when either photosystem acted alone, there was an increase in the number of flashes required for the onset of ATP synthesis, an increase which was consistent with the observed lower flash-induced proton accumulation. A mathematical analysis of the onset of flash-induced ATP synthesis shows that at least several hundred proton-translocating electron transport complexes must be cooperating to form the threshold delta pH. In spite of this evidence for extensive cooperation among different electron transport complexes in ATP formation, the implied pooling of H+ ions does not seem to involve inner vesicle regions accessible to exogenous buffers. Thus, even when the number of H+ ions accumulated per flash was reduced by 70% through attenuation of the intensity of the flashes, exogenous hydrogen ion buffers present within the lumen of the thylakoid vesicle had no effect on the number of flashes required for the onset of ATP synthesis.

A time lag in the onset of ATP-Pi exchange catalyzed by purified ATP-synthase (CF0-CF1) proteoliposomes and by chloroplasts

The time course of ATP-Pi exchange which is catalyzed by the isolated chloroplast ATP synthase in phospholipid vesicles was studied. The following observations were made. (i) The onset of 32Pi incorporation into ATP lags behind ATP hydrolysis. The lag lasts for about 2 min at 37 degrees C and is followed by a steady-state rate which is constant for more than 30 min. Under the same experimental conditions, ATP hydrolysis shows an initial burst followed by a constant, slower rate. (ii) The initial lag is independent of Mg-ATP concentration in the range 0.2-5 mM and of the presence of ADP. In contrast, the steady-state rate of ATP-Pi exchange has an apparent Km of 0.3 mM for Mg-ATP and is stimulated by ADP. (iii) Increasing the temperature from 30 to 45 degrees C decreases the lag from 6 min to zero. The steady-state rate of ATP-Pi exchange is affected to a much smaller extent by the temperature in this range. (iv) The lag is insensitive to valinomycin or tetraphenylboron, while the steady-state rate is partially inhibited. Nigericin and protonophores affect both the lag and steady-state rate. (v) ATP-induced membrane potential formation, as followed by oxonol VI, does not correlate with the lag in its kinetics and temperature dependence. ATP-induced pH gradient formation could not be detected in the proteoliposome system. (vi) Light-triggered ATP-Pi exchange in chloroplasts shows essentially the same time course as the proteoliposome system, but the lag lasts for only about 20 s at room temperature and is unaffected by a preexisting proton gradient. These results suggest that the initial lag in ATP-Pi exchange does not reflect the time required for the buildup of a protomotive force (delta - mu H+) nor the time required to produce ADP. It is suggested, therefore, that the lag reflects an internal autocatalytic conformational change in the ATP-synthase complex which is initiated by ATP hydrolysis and which converts the enzyme from an "exclusive ATPase state" to a "reversible ATP-synthase state". This slow transition is not directly coupled to a trans-membrane pH or potential gradient.

Effect of pyridine homologues on proton flux through the CF0 . CF1 complex and photophosphorylation in chloroplasts

At concentrations below 1 mM, hydrophobic pyridine homologues decrease the rate of photophosphorylation and light-stimulated hydrolysis of ATP and light-activated exchange of the tightly bound nucleotides in chloroplasts, but increase the rate of the Hill reaction. Unlike uncoupling agents, the presence of the organic base at such low concentrations decreases the rate of light-dependent leakage and has no effect on the efficiency of two-stage photophosphorylation in broken chloroplasts. By assuming that the organic base is bound to independent equivalent sites in the thylakoid membrane, a simple expression can be derived which relates the observed rates of photophosphorylation and light-stimulated hydrolysis of ATP quantitatively to the concentration of the organic base in solution and gives dissociation equilibrium constants which are on the order of the relative hydrophobicities of the pyridine homologues. A possible mechanistic model for the CF0 . CF1 complex is proposed which could serve as the basis for a unified interpretation of the kinetics of proton translocation in illuminated chloroplasts, the steady-state rate of photophosphorylation, the light-stimulated ATPase activity, and the light-activated exchange of tightly bound adenine nucleotides.

The induction kinetics of bacterial photophosphorylation. Threshold effects by the phosphate potential and correlation with the amplitude of the carotenoid absorption band shift

1. ATP synthesis (monitored by luciferin-luciferase) can be elicited by a single turnover flash of saturating intensity in chromatophores from Rhodopseudomonas capsulata, Kb1. The ATP yield from the first to the fourth turnover is strongly influenced by the phosphate potential: at high phosphate potential (-11.5 kcal/mol) no ATP is formed in the first three turnovers while at lower phosphate potential (-8.2 kcal/mol) and the yield in the first flash is already one half of the maximum, which is reached after 2-3 turnovers. 2. The response to ionophores indicates that the driving force for ATP synthesis in the first 20 turnovers is mainly given by a membrane potential. The amplitude of the carotenoid band shift shows that during a train of flashes an increasing delta psi is built up, which reaches a stationary level after a few turnovers; at high phosphate potential, therefore, more turnovers of the same photosynthetic unit are required to overcome an energetic threshold. 3. After several (six to seven) flashes the ATP yield becomes constant, independently from the phosphate potential; the yield varies, however, as a function of dark time (td) between flashes, with an optimum for td = 160-320 ms. 4. The decay kinetics of the high energy state generated by a long (125 ms) flash have been studied directly measuring the ATP yield produced in post-illumination by one single turnover flash, under conditions of phosphate potential (-10 kcal/mol), which will not allow ATP formation by one single turnover. The high energy state decays within 20 s after the illumination. The decay rate is strongly accelerated by 10(-8) M valinomycin. 5. Under all the experimental conditions described, the amplitude of the carotenoid signal correlates univocally with the ATP yield per flash, demonstrating that this signal monitores accurately an energetic state of the membrane directly involved in ATP synthesis. 6. Although values of the carotenoid signal much larger than the minimal threshold are present, relax slowly, and contribute to the energy input for phosphorylation, no ATP is formed unless electron flow is induced by a single turnover flash. 7. The conclusions drawn are independent from the assumption that a delta psi between bulk phases is evaluable from the carotenoid signal.

The onset of photophosphorylation correlates with the rise in transmembrane electrochemical proton gradients

The onset of photophosphorylation was determined by exposing chloroplast thylakoids to either single or multiple light flashes of varying duration. In aggreement with the results of Ort et al. (Ort, D.R., Dilley, R.A. and Good, N.E. (1976) Biochim. Biophys. Acta 449, 108--124), the permeant buffer imidazole in the presence of valinomycin and K+ did not greatly delay the onset of phosphorylation driven by multiple activation. In single flashes, however, the lag in the development of phosphorylation was much longer and imidazole caused a further delay. A significant delta pH was generated by the multiple flash regime. The onset of photophosphorylation is, therefore, consistent with the rise in transmembrane delta pH.

Kinetic factors limiting the synthesis of ATP by chromatophores exposed to short flash excitation

ATP synthesis was measured after chromatophores from Rhodopseudomonas capsulata had been subjected to illumination by single turnover flashes fired at variable frequencies. Three processes were examined, which under different conditions can limit the net yield of ATP. (1) A process with an apparent relaxation time of 10-20 ms. This reaction probably limits the rate of ATP synthesis in continuous illumination. It has similar time dependence to the stimulation of the carotenoid shift decay by ADP after a single flash. (2) An active state of the ATPase only persists when the chromatophores are excited more often than once in 10 s. This state decays with similar kinetics to the entire carotenoid shift decay. Full activation is achieved after two flashes. (1) and (2) are not significantly affected by concentrations of antimycin A sufficient to block electron flow through the cytochrome b/c2 oxidoreductase and abolish phase III in the generation of the carotenoid shift. (3) In the presence of antimycin A, after the third, fourth and subsequent flashes ATP synthesis is limited by the quantity of reducing equivalents transported through the reaction centre rather than by the level of the electrochemical proton gradient.