The protonmotive force in bovine heart submitochondrial particles. Magnitude, sites of generation and comparison with the phosphorylation potential.

1. The magnitude of the protonmotive force in respiring bovine heart submitochondrial particles was estimated. The membrane-potential component was determined from the uptake of S14CN-ions, and the pH-gradient component from the uptake of [14C]methylamine. In each case a flow-dialysis technique was used to monitor uptake. 2. With NADH as substrate the membrane potential was approx. 145mV and the pH gradient was between 0 and 0.5 unit when the particles were suspended in a Pi/Tris reaction medium. The addition of the permeant NO3-ion decreased the membrane potential with a corresponding increase in the pH gradient. In a medium containing 200mM-sucrose, 50mM-KCl and Hepes as buffer, the total protonmotive force was 185mV, comprising a membrane potential of 90mV and a pH gradient of 1.6 units. Thus the protonmotive force was slightly larger in the high-osmolarity medium. 3. The phosphorylation potential (= deltaG0' + RT ln[ATP]/[ADP][Pi]) was approx. 43.1 kJ/mol (10.3kcal/mol) in all the reaction media tested. Comparison of this value with the protonmotive force indicates that more than 2 and up to 3 protons must be moved across the membrane for each molecule of ATP synthesized by a chemiosmotic mechanism. 4. Succinate generated both a protonmotive force and a phosphorylation potential that were of similar magnitude to those observed with NADH as substrate. 5. Although oxidation of NADH supports a rate of ATP synthesis that is approximately twice that observed with succinate, respiration with either of these substrates generated a very similar protonmotive force. Thus there seemed to be no strict relation between the size of the protonmotive force and the phosphorylation rate. 6. In the presence of antimycin and/or 2-n-heptyl-4-hydroxyquinoline N-oxide, ascorbate oxidation with either NNN'N'-tetramethyl-p-phenylenediamine or 2,3,5,6-tetramethyl-p-phenylenediamine as electron mediator generated a membrane potential of approx. 90mV, but no pH gradient was detected, even in the presence of NO3-. These data are discussed with reference to the proposal that cytochrome oxidase contains a proton pump.     

Isotope and thermal effects in chemiosmotic coupling to the membrane ATPase of Streptococcus

We measured rates of ATP synthesis by the proton-translocating ATPase of the motile Streptococcus strain V4051. Starved cells were energized artificially by exposing their membranes to a variable electrical potential difference (internal medium negative) and a fixed pH difference (internal medium alkaline). The initial rates of ATP synthesis increased exponentially with protonmotive force. The results were the same in D2O and H2O; there was no solvent isotope effect. At a fixed protonmotive force, the rates were strongly dependent on temperature, as expected for a reaction with a large enthalpy of activation. At a different protonmotive force, the rates varied with temperature in an identical fashion; there was no change in the enthalpy of activation. We conclude that protonation-deprotonation steps are not rate limiting and that the protons that cross the membrane drive ATP synthesis by mass action. The transmembrane electric field acts by changing the concentrations of the reactants, not by changing the configuration of the enzyme-substrate complex.     

Protonmotive force as the source of energy for adenosine 5''-triphosphate synthesis in Escherichia coli.

Net synthesis of adenosine 5'-triphosphate (ATP) in energy-depleted cells of Escherichia coli was observed when an inwardly directed protonmotive force was artificially imposed. In wild-type cells, ATP synthesis occurred whether the protonmotive force was dominated by the membrane potential (negative inside) or the pH gradient (alkaline inside). Formation of ATP did not occur unless the protonmotive force exceeded a value of 200 mV. Under these conditions, no ATP synthesis was found when cells were exposed to an inhibitor of the membrane-bound Ca2+- and Mg2+- stimulated adenosine triphosphatase (EC 3.6.1.3), dicyclohexylcarbodiimide, or to a proton conductor, carbonylcyanide-p-trifluoromethoxyphenyl-hydrazone. Adenosine triphosphatase-negative mutants failed to show ATP synthesis in response to either a membrane potential or a pH gradient. ATP synthesis driven by a protonmotive force was observed in a cytochrome-deficient mutant. These observations are consistent with the chemiosmotic hypothesis of Mitchell (1961, 1966, 1974).     

Control of the protonmotive force in Rhodopseudomonas sphaeroides in the light and dark and its effect on the initiation of flagellar rotation

The addition of low concentrations of the uncoupler of CCP (0.01−0.1 μM) to actinically illuminated, photosynthetically grown Rhodopseudomonas sphaeroides did not inhibit motility. When CCCP addition was followed by a period of dark, anaerobic incubation the bacteria became nonmotile, and motility was not regained immediately on actinic re-illumination. The length of the delay before the onset of motility on re-illumination was proportional to the concentration of uncoupler added, until at higher concentrations (0.5−5 μM) maximum motility was not regained. Flagellar rotation depends on the protonmotive force, therefore the total pmf and the electrical and chemical components were measured under a variety of environmental conditions. The addition of the uncoupler to dark-incubated bacteria caused the collapse of the respiratory protonmotive force, but had no effect on the rapid reformation of the full protonmotive force on re-illumination. The time-course of protonmotive force generation was very similar to that measured in untreated bacteria and showed little change with increasing concentrations of uncoupler, although the size of the induced protonmotive force was eventually reduced. The ΔpH component of the protonmotive force developed more slowly than the Δψ component, but the time taken for the development of the ΔpH did not increase as the CCCP concentration increased. The delay in motility was longer under conditions where ΔpH was the sole or major component of the protonmotive force. ATP is required for taxis but not motility in bacteria. The addition of CCCP to dark-incubated bacteria caused a rapid fall in intracellular ATP which recovered rapidly on re-illumination. At high uncoupler concentrations the ATP content fell as the protonmotive force was reduced. However, the delay in resumption of motility was observed at CCCP concentrations which did not affect either the protonmotive force or the ATP concentration reached on illumination. There was no delay in recovery of motility when protonmotive force was increased but ATP levels reduced by the addition of the ATPase inhibitor venturicidin. In its proposed that initiation of flagellar rotation involves a protonmotive force dependent modification of the motor and that this modification acts as the on-off switch for the motor.     

Constraints on models for the flagellar rotary motor

Most bacteria that swim are propelled by flagellar filaments, each driven at its base by a rotary motor embedded in the cell wall and cytoplasmic membrane. A motor is about 45 nm in diameter and made up of about 20 different kinds of parts. It is assembled from the inside out. It is powered by a proton (or in some species, a sodium-ion) flux. It steps at least 400 times per revolution. At low speeds and high torques, about 1000 protons are required per revolution, speed is proportional to protonmotive force, and torque varies little with temperature or hydrogen isotope. At high speeds and low torques, torque increases with temperature and is sensitive to hydrogen isotope. At room temperature, torque varies remarkably little with speed from about -100 Hz (the present limit of measurement) to about 200 Hz, and then it declines rapidly reaching zero at about 300 Hz. These are facts that motor models should explain. None of the existing models for the flagellar rotary motor completely do so.     

The requirement for energy during export of beta-lactamase in Escherichia coli is fulfilled by the total protonmotive force.

The energy requirement for the maturation and export of the plasmid-encoded TEM beta-lactamase in Escherichia coli K12 was shown to be fulfilled by the total protonmotive force. This was demonstrated by assessing the inhibition of proteolytic processing of the precursor form of beta-lactamase caused by perturbation of the energized state of the membrane in cells treated with valinomycin. The magnitude of the membrane potential was manipulated by varying the concentration of KCl in the medium and the pH gradient was manipulated by varying the external pH. Both components were simultaneously affected by addition of the protonophore carbonylcyanide-p- trifluoromethoxy phenylhydrazone (FCCP). Inhibition of processing was demonstrated in a mutant strain having a defective ATP synthase where protonmotive force could be dissipated without altering the intracellular level of ATP, indicating that the observed inhibition was not the result of decreased ATP concentration. Half-maximal accumulation of precursor of beta-lactamase was observed in all cases when the level of protonmotive force was decreased to approximately 150 mV. Under those conditions the membrane potential varied from 65 to 140 mV (internally negative) and the pH gradient from 95 to 25 mV (internally alkaline). Thus, the energy requirement is satisfied by the total protonmotive force, with no specificity for either the membrane potential or the pH gradient.     

Constraints on flagellar rotation

The motion of tethered cells of Streptococcus was analyzed at low values of protonmotive force (delta p). Cells repeatedly energized and de-energized stopped at discrete angular positions, indicating a rotational symmetry of barriers to rotation of order 5 or 6. At values of delta p smaller than -30 mV, constraints imposed by these barriers were evident when cells were starved and gradually energized, but not when they were energized first and then gradually de-energized. At values of delta p larger than about -30 mV, the cells behaved as if there were no barriers. Cells spinning in this regime also executed rotational Brownian movement. At energy levels above threshold, the motor determines torque; it does not fix the position of the rotor relative to the stator.     

The effect of beta-galactosides on the protonmotive force and growth of Escherichia coli

The effect of three beta-galactosides on the components membrane potential (delta psi) and pH gradient (delta pH) of protonmotive force and growth of Escherichia coli has been examined. A good correlation between the reduction of the protonmotive force and growth inhibition was observed. Thus some galactosides had little effect on either the protonmotive force or growth while lactose diminished the protonmotive force and caused growth inhibition. This effect of lactose was dependent on the ionic composition of the growth media. In Medium A (77 mM-Na+, 85 mM-K+) lactose diminished delta psi but had no effect on delta pH. Growth inhibition was transient at an external pH 6.0 but complete at pH 7.5. In medium KA (approximately 1 mM-Na+, 162 mM-K+) delta pH was diminished and delta psi was not affected and consequently growth inhibition was complete at pH 6.0. In medium NA (163 mM-Na+, 20 mM-K+) lactose had little effect on delta psi, delta pH or growth. These data support Skulachev's hypothesis of buffering of the protonmotive force by K+ and Na+ gradients.     

Dynamics of a tightly coupled mechanism for flagellar rotation. Bacterial motility, chemiosmotic coupling, protonmotive force.

The bacterial flagellar motor is a molecular engine that couples the flow of protons across the cytoplasmic membrane to rotation of the flagellar filament. We analyze the steady-state behavior of an explicit mechanical model in which a fixed number of protons carries the filament through one revolution. Predictions of this model are compared with experimentally determined relationships between protonmotive force, proton flux, torque, and speed. All such tightly coupled mechanisms produce the same torque when the motor is stalled but vary greatly in their behavior at high speed. The speed at zero load predicted by our model is limited by the rates of association and dissociation of protons at binding sites on the rotor and by the mobility of force generators containing transmembrane channels that interact with these sites. Our analysis suggests that more could be learned about the motor if it were driven by an externally applied torque backwards (at negative speed) or forwards at speeds greater than the zero-load speed.     

Solvent-isotope and pH effects on flagellar rotation in Escherichia coli

We studied changes in speed of the flagellar rotary motor of Escherichia coli when tethered cells or cells carrying small latex spheres on flagellar stubs were shifted from H(2)O to D(2)O or subjected to changes in external pH. In the high-torque, low-speed regime, solvent isotope effects were found to be small; in the low-torque, high-speed regime, they were large. The boundaries between these regimes were close to those found earlier in measurements of the torque-speed relationship of the flagellar rotary motor (, Biophys. J. 65:2201-2216;, Biophys. J., 78:1036-1041). This observation provides direct evidence that the decline in torque at high speed is due primarily to limits in rates of proton transfer. However, variations of speed (and torque) with shifts of external pH (from 4.7 to 8.8) were small for both regimes. Therefore, rates of proton transfer are not very dependent on external pH.     

The stall torque of the bacterial flagellar motor.

The bacterial flagellar motor couples the flow of protons across the cytoplasmic membrane to the rotation of a helical flagellar filament. Using tethered cells, we have measured the stall torque required to block this rotation and compared it with the torque of the running motor over a wide range of values of proton-motive force and pH. The stall torque and the running torque vary identically: both appear to saturate at large values of the proton-motive force and both decrease at low or high pH. This suggests that up to speeds of approximately 5 Hz the operation of the motor is not limited by the mobility of its internal components or the rates of proton transfer reactions coupled to flagellar rotation.     

Magnitude of the protonmotive force in respiring Staphylococcus aureus and Escherichia coli.

The membrane potential and pH gradient developed across the plasma membranes of whole cells of Staphylococcus aureus and spheroplasts of Escherichia coli were estimated. The distributions of potassium ions in the presence of valinomycin and the pH gradient across the membrane were determined from the changes in pK and pH observed in the external medium during transition from the energized respiring state to the de-engerized resting condition. The protonmotive force in respiring cells was estimated at 211 mV for S. aureus and 230 mV for E. coli at external pH values of approximately 6.5. The adequacy of these protonmotive forces as a driving force for substrate accumulation or adenosine 5'-triphosphate synthesis is discussed.     

A model for bacterial flagellar motor: free energy transduction and self-organization of rotational motion

A bacterial flagellar motor is an energy transducing molecular machine which shows some attractive characteristics. First, this motor is driven by a protonmotive force (PMF) across the membrane, two components of which, electric potential delta psi and chemical potential -(2.3RT/F)delta pH, are equivalently transduced to the mechanical work of the motor rotation. Second, a PMF threshold for rotation is observed. Third, this motor can rotate reversibly either counterclockwise (CCW) or clockwise (CW) at almost the same speed. To clarify the osmomechanical coupling of this motor, these characteristics must be explained consistently at the molecular level. In this paper, in order to allow quantitative analyses of the above characteristics, a theoretical model of a bacterial flagellar motor is constructed assuming that the torque generating sites are electrodes which can be charged by protons and that the electrostatic interaction between the electrodes generates the rotation torque. Electrode reaction reasonably derives the equivalence of delta psi and -(2.3RT/F)delta pH. In this model, rates of charging and discharging of protons are influenced by the motor rotation rate, so that the torque generating sites co-operatively work through the motor rotation. We named this kind of co-operativity among them "dynamic co-operativity" in torque generation. This co-operativity causes autocatalytic generation of motor torque and the existence of the rotation threshold. In this model, the appearance of the stable rotational states can be described by phase transition caused by the dynamic co-operativity among torque generating sites. According to this model, the flagellar motor has two stable rotational states corresponding to CCW and CW, which show the same torques. The motor selects one direction from them to rotate, and that is self-organization of rotational motion. Interpretation of the transition between the two stable rotational states as the chemotactic reversals of the flagellar motor is also discussed.     

Torque generated by the bacterial flagellar motor close to stall.

In earlier work in which electrorotation was used to apply external torque to tethered cells of the bacterium Escherichia coli, it was found that the torque required to force flagellar motors backward was considerably larger than the torque required to stop them. That is, there appeared to be substantial barrier to backward rotation. Here, we show that in most, possibly all, cases this barrier is an artifact due to angular variation of the torque applied by electrorotation, of the motor torque, or both; the motor torque appears to be independent to speed or to vary linearly with speed up to speeds of tens of Hertz, in either direction. However, motors often break catastrophically when driven backward, so backward rotation is not equivalent to forward rotation. Also, cells can rotate backward while stalled, either in randomly timed jumps of 180 degrees or very slowly and smoothly. When cells rotate slowly and smoothly backward, the motor takes several seconds to recover after electrorotation is stopped, suggesting that some form of reversible damage has occurred. These findings do not affect the interpretation of electrorotation experiments in which motors are driven rapidly forward.     

Adenosine 5''-triphosphate synthesis driven by a protonmotive force in membrane vesicles of Escherichia coli.

Adenosine 5'-triphosphate (ATP) synthesis energized by an artificially imposed protonmotive force (delta p) in adenosine 5'-diphosphate-loaded membrane vesicles of Escherichia coli was investigated. The protonmotive force is composed of an artificially imposed pH gradient (delta pH) or membrane potential (deltapsi), or both. A delta pH was established by a rapid alteration of the pH of the assay medium. A delta psi was created by the establishment of diffusion potential of K+ in the presence of valinomycin. The maximal amount of ATP synthesized was 0.4 to 0.5 nmol/mg of membrane protein when energized by a delta pH and 0.2 to 0.3 nmol/mg of membrane protein when a delta psi was imposed. Simultaneous imposition of both a delta pH and delta psi resulted in the formation of greater amounts of ATP (0.8 nmol/mg of membrane protein) than with either alone. The amount of ATP synthesized was roughly proportional to the magnitude of the artificially imposed delta p. Although p-chloromercuribenzoate, 2-heptyl-4-hydroxyquinoline-N-oxide, or NaCN each inhibits oxidation of D-lactate, and thus oxidative phosphorylation, none inhibited ATP synthesis driven by an artificially imposed delta p. Membrane vesicles prepared from uncA or uncB strains, which are defective in oxidative phosphorylation, likewise were unable to catalyze ATP synthesis when energy was supplied by an artificially imposed delta p.     

Evidence for an electrogenic 3-deoxy-2-oxo-D-gluconate--proton co-transport driven by the protonmotive force in Escherichia coli K12.

Evidence is presented indicating that the carrier-mediated uptake of 3-deoxy-2-oxo-D-gluconate and D-glucuronate in Escherichia coli K12 is driven by the deltapH and deltapsi components of the protonmotive force. 1. Approximately two protons enter the cells with each sugar molecule, independent of the sugar and the strain used. 2. In respiring cells, the magnitude of the pH gradient alone, as measured by distribution of [3H]acetate, appears to be insufficient to account for the chemical gradient of 3-deoxy-2-oxo-D-gluconate that is developed between pH 6.0 and 8.0. 3. If the external pH is varied between 5.5 and 8.0, 3-deoxy-2-oxo-D-gluconate uptake is gradually inhibited by valinomycin plus K+ ions, whereas the inhibition caused by nigericin is concomitantly relieved, thus reflecting the relative contribution of deltapH and deltapsi to the total protonmotive force at each external pH. 4. 3-Deoxy-2-oxo-D-gluconate can be transiently accumulated into isolated membrane vesicles in response to an artificially induced pH gradient. The process is stimulated when the membrane potential is collapsed by valinomycin in the presence of K+ ions.     

Characterization of Escherichia coli lactose carrier mutants that transport protons without a cosubstrate. Probes for the energy barrier to uncoupled transport

The Escherichia coli lactose carrier is an energy-transducing H+/galactoside cotransport protein which strictly couples sugar and proton transport in 1:1 stoichiometry. Here we describe five lactose carrier mutants which catalyze "uncoupled" sugar-independent H+ transport. Symptoms similar to uncoupling by a proton ionophore have been observed in cells expressing these mutant carriers. The mutations occur at two separate loci, encoding substitutions either for alanine 177 (valine) or tyrosine 236 (histidine, asparagine, phenylalanine, or serine). Compared to the parent, cells expressing the valine 177 carrier grew slowly on minimal media with glucose as carbon source. When washed cells were incubated in the absence of added sugars the mutant showed a reduced protonmotive force compared with the parent. Addition of either thiodigalactoside or alpha-p-nitrophenylgalactoside reduced the defect in protonmotive force. Sugar-independent H+ entry rate into cells expressing either the normal carrier or the Val-177 mutant were measured directly using the pH electrode. Following sudden acidification of the external medium (by either oxygen-pulse or acid-pulse) protons entered more rapidly into cells expressing the Val-177 carrier. This novel sugar-independent mode of H+ transport probably depends on an acquired capacity of the Val-177 carrier to bind the transported proton with higher than normal affinity in a transition state involving the binary carrier/H+ complex.     

A requirement for ATP for beta-galactoside transport by Bacillus alcalophilus.

Lactose-grown cells of Bacillus alcalophilus actively transported methylthio-beta, D-galactoside (TMG) in a range of pH values from 7.5 to 10.5 with a pH optimum at 8.5. The TMG was accumulated in a chemically unmodified form, and cell extracts failed to catalyze either ATP or P-enolpyruvate-dependent phosphorylation of TMG. At pH 8.5, the lactose-grown cells exhibited a transmembrane proton gradient (deltapH) of 1.38 units, interior acid, and a transmembrane electrical potential (delta psi) of -132 mV. Accordingly, the total protonmotive force at this pH was very low, -51mV. Several lines of evidence indicate that the protonmotive force or delta psi did not directly energize TMG transport but, rather, that ATP was directly required: (a) in cells treated with arsenate so that the delta psi was unaffected and cellular ATP levels were markedly lowered, TMG transport was inhibited in proportion to the reduction of cellular ATP, while electrogenic alpha-aminoisobutyric acid transport was not; (b) when a valinomycin-induced potassium diffusion potential was established in starved cells, alpha-aminoisobutyric acid transport, but not TMG transport, was stimulated; and (c) in a series of experiments in which the delta psi was rapidly abolished by treatment with gramicidin, ATP levels declined slowly and the rate of TMG transport correlated directly with ATP levels rather than with the delta psi. Consumption of cellular ATP concomitant with TMG transport could be demonstrated.     

Coupling between the sodium and proton gradients in respiring Escherichia coli cells measured by 23Na and 31P nuclear magnetic resonance

The relationship between the steady-state sodium gradient (delta pNa) and the protonmotive force developed by endogenously respiring Escherichia coli cells has been studied quantitatively, using 23Na NMR for measurement of intracellular and extracellular sodium concentrations, 31P NMR for measurement of intracellular and extracellular pH, and tetraphenylphosphonium distribution for measurement of membrane potential. At constant protonmotive force, the sodium concentration gradient was independent of extracellular concentrations over the measured range of 4-285 mM, indicating that intracellular sodium concentration is not regulated. The magnitude of delta pNa was measured as a function of the composition and magnitude of the protonmotive force. At external pH values below 7.2, delta pNa was parallel to delta pH but showed no simple relationship to the membrane potential; above pH 7.2 the parallel relationship began to diverge, with delta pH continuing to decrease but delta pNa starting to level off or increase. Although plots of delta pNa versus delta pH had slopes of close to 1, the value of delta pNa consistently exceeded that of delta pH by approximately 0.4 units, indicating a partially electrogenic character to the putative H+/Na+ antiport. The apparent stoichiometry was 1.13 +/- 0.01 at external pH below 7.2. The possible significance of this nonintegral stoichiometry is discussed according to a model in which two distinct integral stoichiometries (possibly 1H+/1Na+ and 2H+/1Na+) are available with some relative probability; the model predicts futile cycling of sodium ions and a dissipative proton current. In the course of this study, we discovered that the magnitude of the pH gradient developed by the cells was osmolarity-dependent, yielding steady-state intracellular pH values that varied from 7.1 at 100 mosm to 7.7 at 800 mosm.     

Colony formations in a halotolerantBrevibacterium sp. JCM 6894 on solid medium with different pH values

Viable cells of a halotolerantBrevibacterium sp. JCM 6894 grown in a liquid medium with pH 7.1 were enumerated as the colony-forming cells on three kinds of agar media with different pH values. Unexpectedly they were lower at neutral pH rather than acidic or alkaline pH. This tendency was invariable regardless of the changes in the concentrations of nutrients in the agar medium as well as in the growth phases of the cells. From the comparison of cell growth between liquid and solid media with different pHs, we notified the importance of the pH changes in liquid medium accompanied with growth. Effects of salts and pH of the liquid medium on protonmotive force (Δp) was estimated from membrane potentials (ΔΨ) and proton gradients (ΔpH) of the strain JCM 6894. In the absence of salts, Δp of the strain JCM 6894 was the largest at neutral pH, which was conflicting with the result of cell viability. The addition of NaCl led to the reduction of Δp at acidic pH, mainly due to the dissipation of ΔΨ, which seems to be consistent with the lower numbers of colony formed at acidic pH in the presence of NaCl.