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PubMed2003

Redox potential of quinones in photosynthetic reaction centers from Rhodobacter sphaeroides: dependence on protonation of Glu-L212 and Asp-L213.

The absolute values of the one-electron redox potentials of the two quinones (Q(A) and Q(B)) in bacterial photosynthetic reaction centers from Rhodobacter sphaeroides were calculated by evaluating the electrostatic energies from the solution of the linearized Poisson-Boltzmann equation at pH 7.0. The redox potential for Q(A) was calculated to be between -173 and -160 mV, which is close to the lowest measured values that are assumed to refer to nonequilibrated protonation patterns in the redox state Q(A)(-). The redox potential of quinone Q(B) is found to be about 160-220 mV larger for the light-exposed than for the dark-adapted structure. These values of the redox potentials are obtained if Asp-L213 is nearly protonated (probability 0.75-1.0) before and after electron transfer from Q(A) to Q(B), while Glu-L212 is partially protonated (probability 0.6) in the initial state Q(A)(-)Q(B)(0) and fully protonated in the final state Q(A)(0)Q(B)(-). Conversely, if the charge state of the quinones is varied from Q(A)(-)Q(B)(0) to Q(A)(0)Q(B)(-) corresponding to the electron transfer from Q(A) to Q(B), Asp-L213 remains protonated, while Glu-L212 changes its protonation state from 0.15 H(+) to fully protonated. In agreement with results from FTIR spectra, there is proton uptake at Glu-L212 going along with the electron transfer, whereas Asp-L213 does not change its protonation state. However, in our simulations Asp-L213 is considered to be protonated rather than ionized as deduced from FTIR spectra. The calculated redox potential of Q(A) shows little dependence on the charge state of Asp-L213, which is due to a strong coupling with the protonation state of Asp-M17 but increases by 50 mV if Glu-L212 changes from the ionized to the protonated charge state. Both are in agreement with fluorescence measurements observing the decay of SP(+)Q(A)(-) in a wide pH regime. The computed difference in redox potential of Q(B) in the light-exposed and dark-adapted structure was traced back to the hydrogen bond of Q(B) with His-L190 that is lost in the dark-adapted structure and the charge of the non-heme iron atom, which is closer to Q(B) in the light-exposed than in the dark-adapted structure.

Amino Acid Substitution↗
PubMed2004

Proton release and uptake of pharaonis phoborhodopsin (sensory rhodopsin II) reconstituted into phospholipids.

pharaonis phoborhodopsin (ppR, also called pharaonis sensory rhodopsin II, psRII) is a photo-receptor for negative phototaxis in Natronobacterium pharaonis. During the photoreaction cycle (photocycle), ppR exhibits intraprotein proton movements, resulting in proton pumping from the cytoplasmic to the extracellular side, although it is weak. In this study, light-induced proton uptake and release of ppR reconstituted with phospholipid were analyzed using a SnO(2) electrode. The reconstituted ppR exhibited properties in proton uptake and release that are different from those of dodecyl maltoside solubilized samples. It showed fast proton release before the decay of ppR(M) (M-photointermediate) followed by proton uptake, which was similar to that of bacteriorhodopsin (BR), a light-driven proton pump. Mutant analysis assigned Asp193 to one (major) of the members of the proton-releasing group (PRG). Fast proton release was observed only when the pH was approximately 5-8 in the presence of Cl(-). When Cl(-) was replaced with SO(4)(2-), the reconstituted ppR did not exhibit fast proton release at any pH, suggesting Cl(-) binding around PRG. PRG in BR consists of Glu204 (Asp193 in ppR) and Glu194 (Pro183 in ppR). Replacement of Pro183 by Glu/Asp, a negatively charged residue, led to Cl(-)-independent fast proton release. The transducer binding affected the properties of PRG in ppR in the ground state and in the ppR(M) state, suggesting that interaction with the transducer extends to the extracellular surface of ppR. Differences and similarities in the molecular mechanism of the proton movement between ppR and BR are discussed.

Amino Acid Substitution↗
PubMed1998

Local-access model for proton transfer in bacteriorhodopsin.

The accessibility of the retinal Schiff base in bacteriorhodopsin was studied in the D85N/D96N mutant where the proton acceptor and donor are absent. Protonation and deprotonation of the Schiff base after pH jump without illumination and in the photocycle of the unprotonated Schiff base were measured in the visible and the infrared. Whether access is extracellular (EC) or cytoplasmic (CP) was decided from the effect of millimolar concentrations of azide on the rates of proton transfers. The results, together with earlier work on the wild-type protein, suggest a new hypothesis for the proton-transfer switch: (i) In the metastable 13-cis, 15-anti and all-trans, 15-syn photoproducts, but not in the stable isomeric states, access flickers between the EC and CP directions. (ii) The direction of proton transfer is decided both by this local access and by the presence of a suitable donor or acceptor group (in the wild type), or the proton conductivity in the EC and CP half-channels (in D85N/D96N). (iii) Thermal reisomerization of the retinal can occur only when the Schiff base is protonated, as is well-known. In the wild-type transport cycle, the concurrent local EC and CP access during the lifetime of the metastable 13-cis, 15-anti state enables the changing pKa's of the proton acceptor and donor to determine the direction of proton transfer. Proton transfer from the Schiff base to Asp-85 in the EC direction is followed by reprotonation by Asp-96 from the CP direction because proton release to the EC surface raises the pKa of Asp-85 and a large-scale protein conformation change lowers the pKa of Asp-96. The unexpected finding we report here for D85N/D96N, that when the retinal is in the stable all-trans, 15-anti and 13-cis, 15-syn isomeric forms access of the Schiff base is locked (in the EC and CP directions, respectively), suggests that in this protein reisomerization, rather than changes in the proton conductivities of the EC and CP half-channels, provides the switch function. With this mechanism, the various modes of transport reported for Asp-85 mutants (CP to EC direction with blue light, and EC to CP direction with blue plus green light) are understood also in terms of rules i-iii.

Amino Acid Substitution↗
PubMed2006

Implications of protonation and substituent effects for C-O and O-P bond cleavage in phosphate monoesters.

A recent study of phosphate monoesters that broke down exclusively through C-O bond cleavage and whose reactivity was unaffected by protonation of the nonbridging oxygens (Byczynski et al. J. Am. Chem. Soc. 2003, 125, 12541) raised several questions about the reactivity of phosphate monoesters, R-O-P(i). Potential catalytic strategies, particularly with regard to selectively promoting C-O or O-P bond cleavage, were investigated computationally through simple alkyl and aryl phosphate monoesters. Both C-O and O-P bonds lengthened upon protonating the bridging oxygen, R-O(H(+))-P(i), and heterolytic bond dissociation energies, DeltaH(C)(-)(O) and DeltaH(O)(-)(P), decreased. Which bond will break depends on the protonation state of the phosphoryl moiety, P(i), and the identity of the organosubstituent, R. Protonating the bridging oxygen when the nonbridging oxygens were already protonated favored C-O cleavage, while protonating the bridging oxygen of the dianion form, R-O-PO(3)(2)(-), favored O-P cleavage. Alkyl R groups capable of forming stable cations were more prone to C-O bond cleavage, with tBu > iPr > F(2)iPr > Me. The lack of effect on the C-O cleavage rate from protonating nonbridging oxygens could arise from two precisely offsetting effects: Protonating nonbridging oxygens lengthens the C-O bond, making it more reactive, but also decreases the bridging oxygen proton affinity, making it less likely to be protonated and, therefore, less reactive. The lack of effect could also arise without bridging oxygen protonation if the ratio of rate constants with different protonation states precisely matched the ratio of acidity constants, K(a). Calculations used hybrid density functional theory (B3PW91/6-31++G) methods with a conductor-like polarizable continuum model (CPCM) of solvation. Calculations on Me-phosphate using MP2/aug-cc-pVDZ and PBE0/aug-cc-pVDZ levels of theory, and variations on the solvation model, confirmed the reproducibility with different computational models.

Hydrogen-Ion Concentration↗
PubMed2005

Proton transfer of NH3-HCl catalyzed by only one molecule.

The proton transfer in NH(3)-HCl by only one molecule of catalyst was studied by using the MP2 method with the large 6-311++G(2d,2p) basis set. The 18 structures are obtained for the smallest units, NH(3)-HCl-A trimers, for which the proton transfer maybe occurred. The final results show that the proton transfers have occurred in the 15 cyclic shape structures for A = H(2)SO(4), H(2)SO(3), HCOOH (a), HF, H(2)O(2), HNO(3), HNO(2) (a), CH(3)OH, HCl, HNC, H(2)O, HNO(2) (b), NH(3), HCOOH (b), and HCHO, and not occurred in another 3 trimer structures for A = HCN, H(2)S, and PH(3). These results show that the proton transfer occurs from HCl to NH(3) when catalyst molecule A (acidic, neutral, or basic) not only as a proton donor strongly donates the proton to the Cl atom but as an acceptor strongly accepts the proton from the NH(3) molecule in the cyclic H-bond structure. In this work, a proton circumfluence model is proposed to explain the mechanism of the proton transfer. We find that, for the trimer, when the sum of two hydrogen bond lengths (R = R(1) + R(2)) is shorter than 5.0 A, molecule A has the ability to catalyze the proton transfer. In addition, we also find that the interaction energy E(int) between NH(3)-HCl and A is nearly related to the extent (R(H1)(-)(Cl)) of proton transfer, that is, the interaction energy E(int) increases with the proton transfer.

Ammonia↗
PubMed1996

Uptake characteristics of loracarbef and cephalexin in the Caco-2 cell culture model: effects of the proton gradient and possible presence of a distinctive second component.

The mechanisms of apical (AP) uptake of cephalexin (CEPH) and loracarbef (LOR) in the absence or presence of an (extemally imposed) proton gradient were determined using well-stirred diffusion chambers that minimize the effects of the unstirred water layer. The results indicated that, compared to AP uptake in the presence of an imposed proton gradient, AP uptake in the absence of an imposed proton gradient had higher K(m) values and lower Jmax values. Furthermore, when inhibition studies were performed in the absence of a proton gradient, only natural peptides were effective, whereas the peptide analogs (e.g., enalapril) were not. In addition to the effects of concentration and competitive inhibitors, the results also indicated that (1) the AP uptake of both drugs was decreased more than 60% by FCCP, regardless of whether the proton gradient was present or absent; (2) effects of protein kinase C promoter were dependent upon the presence of a proton gradient; and (3) AP uptake in the presence of an imposed proton gradient was not affected by feeding restriction, whereas AP uptake in the absence of an imposed proton gradient was. These results showed for the first time that two substrates with similar AP uptake characteristics in the presence of an imposed proton gradient may not share those characteristics in the absence of an imposed proton gradient. Taken together, these results suggest that the AP uptake component that functions in the absence of an imposed proton gradient is distinctly different from the one that functions in the presence of an imposed proton gradient. Data generated from the present study and those in the literature lend support to the hypothesis that this distinctive component represents the second binding site on the AP peptide transporter. However, an alternative hypothesis that there are two AP peptide transporters remains to be disapproved.

Caco-2 Cells↗
PubMed2001

A systematic comparison of triple therapies for treatment of Helicobacter pylori infection with proton pump inhibitor/ ranitidine bismuth citrate plus clarithromycin and either amoxicillin or a nitroimidazole.

BACKGROUND: Triple therapies with proton pump inhibitor/ranitidine bismuth citrate (RBC), clarithromycin (C) and either amoxicillin (A) or a nitroimidazole (I) are widely accepted as treatment for Helicobacter pylori infection. However, it is not clear which of these antibiotic combinations should be preferred. AIM: To evaluate whether there is a difference in efficacy between triple therapies with proton pump inhibitor/RBC, clarithromycin and either amoxicillin or a nitroimidazole. METHODS: The literature was examined for randomized trials comparing proton pump inhibitor/RBC-C-A and proton pump inhibitor/RBC-C-I. Studies were grouped according to the type of acid inhibitor used (proton pump inhibitor or RBC) and differences between pooled cure rates were calculated. RESULTS: Forty-seven studies were identified: seven using RBC, 39 using proton pump inhibitor, one using both. RBC-C-I was somewhat superior to RBC-C-A, although this difference only reached statistical significance in intention-to-treat analysis. Overall, proton pump inhibitor-C-I and proton pump inhibitor-C-A were equally effective, but in nitroimidazole-susceptible strains, proton pump inhibitor-C-I performed better, in nitroimidazole-resistant strains, proton pump inhibitor-C-A performed better. No serious side-effects were reported and pooled drop-out rates were equal. CONCLUSIONS: In general, proton pump inhibitor-C-I and proton pump inhibitor-C-A are equally effective and therefore other factors such as local prevalence of resistant strains, cost of therapy and options for second-line treatment should determine which regimen should be preferred. When using RBC, the RBC-C-I combination is somewhat superior to RBC-C-A.

Amoxicillin↗
PubMed2001

Does the widespread use of proton pump inhibitors mask, complicate and/or delay the diagnosis of Zollinger-Ellison syndrome?

BACKGROUND: Proton pump inhibitors are potent acid suppressants which, at normal doses, can result in hypergastrinaemia in patients with idiopathic oesophageal reflux disease and in the control of symptoms in most patients with gastrinomas. Therefore, their use could delay or mask the diagnosis of gastrinoma. AIM: To investigate whether the widespread use of proton pump inhibitors masks or complicates the diagnosis of gastrinoma. SUBJECTS AND METHODS: Data from two centres with different referral criteria for suspected gastrinomas were analysed (Gastroenterology Unit, Rome, Italy and National Institutes of Health, Bethesda, MD, USA). The number of referrals and the number of new patients with gastrinoma diagnosed in the years prior to the widespread use of proton pump inhibitors (1986-1992) were compared with the numbers since proton pump inhibitors became widely available (1993-1998). RESULTS: The decrease in referral rate (P=0.0009) and the decrease in the annual rate of gastrinoma diagnosis (P=0.0020) at both centres correlated with the increased use of proton pump inhibitors. At the Italian centre, there was a 62% decrease in annual referrals (P < 0.0001) in the post-proton pump inhibitor period, relative to the pre-proton pump inhibitor period, whereas there was an increase in the rate of referral of other gastrointestinal endocrine tumours. The number of new cases of gastrinoma diagnosed decreased by 40%. At the US centre, the referral rate decreased by 28% (P=0.024) in the post-proton pump inhibitor period. There was also a 43% decrease in the number of new cases diagnosed annually in the post-proton pump inhibitor period (P=0.0012). There was a 2.6-fold increase in the post-proton pump inhibitor period in the percentage of referrals with a false diagnosis of gastrinoma as the cause of hypergastrinaemia (P=0.0040). CONCLUSIONS: In both referral centres, less patients have been referred with a possible diagnosis of gastrinoma and fewer new patients with gastrinoma have been diagnosed since proton pump inhibitors became widely available. These data support the conclusion that, since proton pump inhibitors have been released, the diagnosis of gastrinoma has been masked and will probably be delayed, with the result that patients with gastrinoma will be diagnosed at more advanced stages in their disease course.

Anti-Ulcer Agents↗
PubMed1996

Protonation dynamics of the extracellular and cytoplasmic surface of bacteriorhodopsin in the purple membrane.

The dynamics of proton binding to the extracellular and the cytoplasmic surfaces of the purple membrane were measured by laser-induced proton pulses. Purple membranes, selectively labeled by fluorescein at Lys-129 of bacteriorhodopsin, were pulsed by protons released in the aqueous bulk from excited pyranine (8-hydroxy-1,3,6-pyrenetrisulfonate) and the reaction of protons with the indicators was measured. Kinetic analysis of the data imply that the two faces of the membrane differ in their buffer capacities and in their rates of interaction with bulk protons. The extracellular surface of the purple membrane contains one anionic proton binding site per protein molecule with pK = 5.1. This site is within a Coulomb cage radius (approximately 15 A) from Lys-129. The cytoplasmic surface of the purple membrane bears 4-5 protonable moieties (pK = 5.1) that, due to close proximity, function as a common proton binding site. The reaction of the proton with this cluster is at a very fast rate (3.10(10) M-1.s-1). The proximity between the elements is sufficiently high that even in 100 mM NaCl they still function as a cluster. Extraction of the chromophore retinal from the protein has a marked effect on the carboxylates of the cytoplasmic surface, and two to three of them assume positions that almost bar their reaction with bulk protons. The protonation dynamics determined at the surface of the purple membrane is of relevance both for the vectorial proton transport mechanism of bacteriorhodopsin and for energy coupling, not only in halobacteria, but also in complex chemiosmotic systems such as mitochondrial and thylakoid membranes.

Bacteriorhodopsins↗
PubMed1997

Monte Carlo calculated stopping-power ratios, water/air, for clinical proton dosimetry (50-250 MeV).

Calculations of stopping power ratios, water to air, for the determination of absorbed dose to water in clinical proton beams using ionization chamber measurements have been undertaken using the Monte Carlo method. A computer code to simulate the transport of protons in water (PETRA) has been used to calculate sw.air-data under different degrees of complexity, ranging from values based on primary protons only to data including secondary electrons and high-energy secondary protons produced in nonelastic nuclear collisions. All numerical data are based on ICRU 49 proton stopping powers. Calculations using primary protons have been compared to the simple continuous slowing-down approximation (c.s.d.a.) analytical technique used in proton dosimetry protocols, not finding significant differences that justify elaborate Monte Carlo simulations except beyond the mean range of the protons (the far side of the Bragg peak). The influence of nuclear nonelastic processes, through the detailed generation and transport of secondary protons, on the calculated stopping-power ratios has been found to be negligible. The effect of alpha particles has also been analysed, finding differences smaller than 0.1% from the results excluding them. Discrepancies of up to 0.6% in the plateau region have been found, however, when the production and transport of secondary electrons are taken into account. The large influence of nonelastic nuclear interactions on proton depth-dose distributions shows that the removal of primary protons from the incident beam decreases the peak-to-plateau ratio by a large factor, up to 40% at 250 MeV. It is therefore emphasized that nonelastic nuclear reactions should be included in Monte Carlo simulations of proton beam depth-dose distributions.

Air↗
PubMed2006

Review article: the clinical pharmacology of proton pump inhibitors.

Proton pump inhibitors inhibit the gastric H+/K+-ATPase via covalent binding to cysteine residues of the proton pump. All proton pump inhibitors must undergo acid accumulation in the parietal cell through protonation, followed by activation mediated by a second protonation at the active secretory canaliculus of the parietal cell. The relative ease with which these steps occur with different proton pump inhibitors underlies differences in their rates of activation, which in turn influence the location of covalent binding and the stability of inhibition. Slow activation is associated with binding to a cysteine residue involved in proton transport that is located deep in the membrane. However, this is inaccessible to the endogenous reducing agents responsible for restoring H+/K+-ATPase activity, favouring a longer duration of gastric acid inhibition. Pantoprazole and tenatoprazole, a novel proton pump inhibitor which has an imidazopyridine ring in place of the benzimidazole moiety found in other proton pump inhibitors, are activated more slowly than other proton pump inhibitors but their inhibition is resistant to reversal. In addition, tenatoprazole has a greatly extended plasma half-life in comparison with all other proton pump inhibitors. The chemical and pharmacological characteristics of tenatoprazole give it theoretical advantages over benzimidazole-based proton pump inhibitors that should translate into improved acid control, particularly during the night.

Antacids↗
PubMed1983

Kinetic analysis of the protonation of a surface group of a macromolecule.

The dynamics of proton transfer between a surface-attached acidic moiety and the bulk of the solution was measured using the laser-induced proton pulse technique. [Gutman, M., Huppert, D. and Pines, E. (1981) J. Am. Chem. Soc. 103, 3709-3713]. The model system for this study consists of pH indicators (either neutral red or bromcresol green) adsorbed on Brij 58 micelles, as defined targets for protonation and a non-adsorbed proton emitter (2-naphthol-3,6-disulfonate) for generation of protons in bulk. The reaction was measured with 50-ns time resolution over a time period of about 200 microseconds. The results were analyzed by a numerical solution of the coupled nonlinear differential equation corresponding with the reaction system. [Gutman, M., et al. (1983) J. Am. Chem. Soc. 105, 2210-2216]. Quantitative analysis reveals two independent reactions which govern the observed dynamics: (a) a diffusion-controlled reaction between the proton and the surface targets; (b) translocation of the protonated target between the hydration layer of the interface and a more hydrophobic one. The contribution of the translocation reaction to the dynamics of surface protonation is more pronounced for compounds like carboxylates or phenolates which increase their hydrophobicity upon protonation. Amines and azoaromatic structures are more hydrophilic in their protonated states, the dynamics of their protonation is less affected by post-protonation distribution within the microenvironments of the interface. The interrelation between the partial rate constants and the macroscopic time constants and equilibrium parameters is analyzed.

Bromcresol Green↗
PubMed1994

Pre-steady-state MgATP-dependent proton production and electron transfer by nitrogenase from Azotobacter vinelandii.

MgATP-dependent pre-steady-state proton production by nitrogenase from Azotobacter vinelandii was studied by monitoring the absorbance changes at 572 nm of the pH indicator o-cresolsulphonphtalein in a weakly buffered solution. The absorbance changes are characterized by a constant phase, a single exponential decrease and a linear decrease. The observed rate constant for the single exponential MgATP-dependent proton production by reduced nitrogenase proteins at 20.0 degrees C is 14 +/- 4 s-1. No proton production with a rate constant comparable to the observed rate constant of electron transfer (kobs approximately 100 s-1) was detected. The extent of the observed MgATP-dependent proton production is determined by the redox state of the nitrogenase proteins before mixing with MgATP; less protons are produced when more electrons are transferred from the Fe protein to the MoFe protein. Values of 2.7 +/- 0.3 mol H+produced/mol MoFe protein with oxidized Fe protein, and 1.1 +/- 0.1 mol H+produced/mol MoFe protein with reduced Fe protein, were found. The data are interpreted to mean that protons are taken up after electron transfer from the Fe protein to the MoFe protein; the ratio electrons(transferred)/H-uptake was calculated to be 1.2 +/- 0.2. After mixing the nitrogenase proteins with MgADP, proton production takes place as well. The proton-production curve did not have a constant phase and the observed rate constant of the single exponential reaction is higher, compared to MgATP-dependent proton production (kobs approximately 35 s-1). The amount of protons produced depends also on the redox state of the Fe protein; no proton production was observed with the oxidized Fe protein; with dithionite-reduced Fe protein a value of 3.1 +/- 0.4 mol H+produced/mol MoFe protein was found (or 0.5 +/- 0.1 mol H+/mol Fe protein). Similar results were obtained when only the Fe protein was mixed with MgADP, but the observed absorbance changes were smaller; mixing of dithionite-reduced Fe protein with MgADP resulted in the production of 0.17 +/- 0.05 mol H+/mol Fe protein. All reported absorbance changes were absent when the experiments were performed in a buffered solution. The series of events that occur after mixing of the nitrogenase proteins with MgATP will be presented and discussed. In the case of the reduced Fe protein, electron transfer takes place at a rate of 100 s-1, which is followed by H+ production (kobs approximately 14 s-1). When there is no electron transfer (oxidized Fe protein) the rate constant of the MgATP-induced proton production decreases.(ABSTRACT TRUNCATED AT 400 WORDS)

Adenosine Diphosphate↗
PubMed1984

Role of the electrochemical proton gradient in genetic transformation of Haemophilus influenzae.

The uptake of homologous DNA by Haemophilus influenzae was studied as a function of the proton motive force in completely competent cultures in the pH range of 6 to 8. The composition and magnitude of the proton motive force were varied by using the ionophores valinomycin and nigericin (in the presence of various potassium ion concentrations) and by using protonophores. No interaction of the ionophores with the DNA transformation system itself was observed. Either component of the proton motive force, the electrical potential or the pH gradient, can drive the uptake of DNA, and the extent of the uptake of DNA is ultimately determined by the total proton motive force. The transformation frequency increases with the proton motive force, which reaches a maximum value at around -130 mV. These results are consistent with an electrogenic proton-DNA symport mechanism, but direct evidence for such a system is not available. The proton motive force was followed during competence development of H. influenzae at pH 8. In the initial phase (up to 50 min), the proton motive force remained constant at about -90 mV, whereas the transformation frequency rose steeply. In the second phase, the proton motive force increased. The transformation frequency in this phase increased with the proton motive force, as in completely competent cultures. These observations and the observed inhibition by NAD of both the proton motive force and the transformation frequency indicate that structural components of the competent state are formed in the initial phase of competence development, whereas the second phase is characterized by an increase of the proton motive force.

Carbonyl Cyanide p-Trifluoromethoxyphenylhydrazone↗
PubMed2003

Differential response properties of IB(4)-positive and -negative unmyelinated sensory neurons to protons and capsaicin.

Activation of unmyelinated (C-fiber) nociceptors by noxious chemicals plays a critical role in the initiation and maintenance of injury-induced pain. C-fiber nociceptors can be divided into two groups in which one class depends on nerve growth factor during postnatal development and contains neuropeptides, and the second class depends on glial cell line-derived neurotrophic factor during postnatal development and contains few neuropeptides but binds isolectin B(4) (IB(4)). We determined the sensitivity of these two populations to protons and capsaicin using whole cell recordings of dorsal root ganglion neurons from adult mouse. IB(4)-negative unmyelinated neurons were significantly more responsive to protons than IB(4)-positive neurons in a concentration-dependent manner. Approximately 86% of IB(4)-negative neurons responded to pH 5.0 with an inward current compared with only 33% of IB(4)-positive neurons. The subtypes of proton-evoked currents in IB(4)-negative unmyelinated neurons were also more diverse. Many IB(4)-negative neurons exhibited transient, rapidly inactivating proton currents as well as sustained proton currents. In contrast, IB(4)-positive neurons never displayed transient proton currents and responded to protons only with sustained, slowly inactivating inward currents. The two classes of neurons also responded differently to capsaicin. Twice as many naïve IB(4)-negative unmyelinated neurons responded to 1 microM capsaicin as IB(4)-positive neurons, and the capsaicin-evoked currents in IB(4)-negative neurons were approximately fourfold larger than those in IB(4)-positive neurons. Interestingly, proton exposure altered the capsaicin responsiveness of the two classes of neurons in opposite ways. Brief preexposure to protons increased the number of capsaicin-responsive IB(4)-positive neurons by twofold and increased the capsaicin-evoked currents by threefold. Conversely, proton exposure decreased the number of capsaicin-responsive IB(4)-negative neurons by 50%. These data suggest that IB(4)-negative unmyelinated nociceptors are initially the primary responders to both protons and capsaicin, but IB(4)-positive nociceptors have a unique capacity to be sensitized by protons to capsaicin-receptor agonists.

Action Potentials↗
PubMed1994

Energizing porters by proton-motive force.

It is generally accepted that the chemistry of water was the most crucial determinant in shaping life on earth. Among the more important chemical features of water is its dissociation into protons and hydroxyl ions. The presence of relatively high proton concentrations in the ambient solution resulted in the evolution of proton pumps during the dawn of life on earth. These proton pumps maintained neutral pH inside the cells and generated electrochemical gradients of protons (proton-motive force) across their membranes. The existence of proton-motive force enabled the evolution of porters driven by it that are most probably among the more primitive porters in the world. The directionality of the substrate transport by the porters could be to both sides of the membranes because they can serve as proton symporters or antiporters. One of the most important subjects of this meeting is the mechanism by which proton-motive and other ion-motive forces drive the transport processes through porters. Is there a common mechanism of action for all proton-driven porters? Is there some common partial reaction by which we can identify the way that porters are energized by proton-motive force? Is there a common coupling between proton movement and uptake or secretion of certain molecules? Even a partial answer to one of these questions would advance our knowledge... or confusion. As my mentor Efraim Racker used to say: 'If you are not totally confused you do not understand the issue'.

Animals↗
PubMed2000

[Measurements of proton response of two lithium fluoride detectors with different thicknesses].

OBJECTIVE: To study the response characteristics of LiF detectors to proton fluence rate and energy, and to observe the thickness effect of the detector. METHOD: Protons were generated by an accelerator. Proton energy was changed in two ways, i.e. changing the accelerator energy directly, or using detector stacks to absorb the proton energy. The incident proton energy on each chip of detector stacks was calculated according to proton range in LiF. RESULT: The response of the detector to proton fluence rate was almost constant; when proton energy was above 9 MeV, the response of the detector to proton energy was constant (less than 10% errors). When proton energy was below 9 MeV, the response reduced gradually with the decrease of proton energy. Thickness effect for LiF thicknesses of 0.4mm and 0.8mm was not obvious. CONCLUSION: The homemade LiF detector is suitable for measurement of space radiation dose. When proton component (below 9 MeV) was abundant in radiation field, the decrease of the relative thermoluminescence efficiency should be taken into consideration.

Cosmic Radiation↗
PubMed1976

Relations between the electrical potential, pH gradient, proton flux and phosphorylation in the photosynthetic membrane.

The transmembrane electrical potential (deltaphi), the proton flux (H+), the rate of electron transport (e), the pH gradient (deltapH) and the rate of phosphorylation (ATP) were measured in chloroplasts of spinach. Photosynthesis was excited periodically with flashes of variable frequencies and intensities. A new method is described for determining the rate of electron transport and proton flux. Under conditions where the rate of electron transport and proton flux are not pH controlled the following correlations were found in the range 50 mV less than or equal to deltaphi less than or equal to 125 mV and 1.8 less than or equal to deltapH less than or equal to 2.7: (1) The pH gradient, deltapH, increases with H+ independently of Phout between 7-9. (2) The rate of phosphorylation, ATP, depends exponentially on deltapH (at constant deltaphi) and is independent of pHout between 7-9. (3) The rate of phosphorylation, ATP, depends also on deltaphi (at constant deltapH and at constant proton flux H+). (4) The proton flux via the ATPase pathway, Hp+, depends non-linearly on the ratio of the proton concentrations: Hp+ approximately (Hin+/Hout+)b, (b=2.3--2.6). The proton flux via the basal pathway, Hb+, depends linearly on the ratio of the proton concentrations: Hb+ approximately (Hin/Hout). (5) The ratio deltaH+/ATP (e/ATP, i.e. the ratio of the total proton flux, Hp+ + Hb+, and the rate of ATP formation, ATP, depends strongly on deltaphi and on deltapH. The ratio is deltaH+/ATP approximately 3 (e/ATP approximately 1.5) at deltapH 2.7 and deltaphi = 125 mV. (6) It is supposed that the reason for the dependence of deltaH+/ATP on deltaphi anddeltapH is the different functional dependence of the basal proton flux Hb+ and the phosphorylating proton flux Hp+ on deltapH and deltaphi. The calculation of deltaH+/ATP on the basis of this assumption is in fair agreement with the experimental values. Also the "threshold" effects can be explained in this way. (7) The ratio of deltaHp+/ATP, i.e. the ratio of the phosphorylating proton flux Hp+ and ATP, is deltaHp+/ATP APPROXIMATELY 2.4.

Adenosine Triphosphate↗