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Rapid calcium release and proton uptake at the disk membrane of isolated cattle rod outer segments. 1. Stoichiometry of light-stimulated calcium release and proton uptake.

We reported a rapid, light-stimulated release of calcium from isolated rod outer segments that is apparent only when both the disk membrane and the plasma membrane are made permeable to calcium by adding the ionophore A23187 [Kaupp, U. B., Schnetkamp, P. P. M., & Junge, W. (1979) Biochim. Biophys. Acta 552, 390-403]. In this paper, we have investigated the light-sensitive diskal binding sites and the calcium release mechanism in their dependence on the pH and the presence of mono- and divalent cations, including calcium itself. We have observed now that several different rod outer segment preparations (i.e., rod outer segments with an intact plasma membrane, broken cells, and sonicated material) possess a similar dependence of their calcium release on the ionic conditions, however, only if manipulated in a way that gives access to the outer conditions of sites within disks (namely, ionophore added in the case of intact rod outer segments). Monovalent cations, at concentrations between 20 and 40 mM, suppress light-induced calcium release. Divalent and trivalent cations are more efficient inhibitors by 1-2 and 2-3 orders of magnitude, respectively. These results suggest that calcium release is controlled by an interfacial potential. The optimum pH for calcium release is pH 6.3, and virtually no release occurs beyond pH 4.5 and 9. The drop for acidic pH is attributed to the pH dependence of calcium binding to disk membranes, and the drop for alkaline pH is attributed to the pH dependence of the metarhodopsin I/metarhodopsin II transition and the light-stimulated proton uptake. In general, calcium release parallels calcium binding as a function of pH and calcium concentrations, although the release saturates at lower calcium concentrations ((KDapp = 5 microM) than would be expected from the amount of calcium bound (KD = 30-60 microM). The maximum stoichiometry is approximately 1 mol of calcium release per mol of rhodopsin bleached. Concomitant measurements of the light-stimulated uptake of protons by the disk membrane revealed a maximal stoichiometry of 2.8 mol of protons taken up per mol of rhodopsin bleached. We present an integrated description of light-stimulated calcium release, proton uptake, and changes of the interfacial potential at the disk membrane.

Animals↗

Conformation and interaction of short nucleic acid double-stranded helices. I. Proton magnetic resonance studies on the nonexchangeable protons of ribosyl ApApGpCpUpU.

1H nuclear magnetic resonance (NMR) spectra of a self-complementary ribosyl hexanucleotide, A2GCU2, are investigated as a function of temperature and ionic strength in D2O. Seventeen nonexchangeable base and ribose-H1' resonances are resolved, and unequivocally assigned by a systematic comparison with the spectra of a series of oligonucleotide fragments of the A2GCU2 sequence varying in chain length from 2 to 5. Changes in the chemical shifts of the 17 protons from the hexamer as well as the six H1'-H2' coupling constants are followed throughout a thermally induced helix-coil transition. These sigma vs. T and J vs. T (degrees C) profiles indicate that the transition is not totally cooperative and that substantial populations of partially bonded structures must exist at intermediate temperatures, with the central G-C region being most stable. Transitions in chemical shift for protons in the same base pair exhibit considerable differences in their Tm values as the data reflect both thermodynamic and local magnetic field effects in the structural transition, which are not readily separable. However, an average of the Tm values agrees well with the value predicted from studies of the thermally induced transition made by optical methods. The values of J1'-2' for all six residues become very small (less than 1.5 Hz) at low temperatures indicating that C3'-endo is the most heavily populated furanose conformation in the helix. The sigma values of protons in the duplex were compared with those calculated from the ring current magnetic anisotropies of nearest and next-nearest neighboring bases using the geometrical parameters of the A'-RNA and B-DNA models. The sigma values of the base protons in the duplex calculated assuming the A'-RNA geometry agree (+/- approximately 0.1 ppm) with the observed values much more accurately than those calculated on the basis of B-DNA geometry. The measured sigma values of the H1' are not accurately predicted from either model. The synthesis of 35 mg of A2GCU2 using primer-dependent polynucleotide phosphorylase is described in detail with extensive discussion in the microfilm edition.

Binding Sites↗

Conformation and interaction of short nucleic acid double-stranded helices. II. Proton magnetic resonance studies on the hydrogen-bonded NH-N protons of ribosyl ApApGpCpUpU helix.

A self-complementary ribohexanucleotide, ApApGpCpUpU, was synthesized and its NH-N hydrogen-bonded protons were studied by proton magnetic resonance. At 1 degree C, 0.17 M Na+, pH 7.6 with 10 mM phosphate-0.1 mM EDTA in H2O, three proton resonances are found in the low-field region with the following chemical shifts and line widths at half-height: 13.2 ppm (80 Hz), 13.5 ppm (30 Hz), and 14.2 ppm (44 Hz). The existence of these resonances indicates the formation of a self-complementary, hydrogen-bonded duplex under these conditions. Upon elevation of temperature, these three resonances sequentially broaden and finally all disappear near 35 degrees C. Unambiguous assignments of these three resonances can be made to the terminal A(1)-U(6) pairs, interior A(2)-U(5) pairs, and to the middle G(3)-C(4) pairs. The assignments were based on (i) the differential sensitivities of the line widths of these resonances to thermal variation, as well as on (ii) a comparison of the computed chemical shifts with the observed chemical shifts. The quantitative aspects of the NH proton transfer between helix, coil, and water are discussed in relationship to the line widths of these resonances and the lifetime of the helix state. The computed chemical shifts of the NH-N resonances based on the A-RNA (or A'-RNA) model agree more closely with the observed chemical shifts than the computed values based on the B-DNA model. These results suggest that the helical duplex of A2GCU2 assumes a conformation similar to A-RNA (or A'-RNA) in aqueous solution. The results on both the NH-N resonances and the C-H resonances are summarized and discussed in terms of the helical conformation of (A2GCU2)2.

Hydrogen Bonding↗

Proton transfer to nickel-thiolate complexes. 1. Protonation of [Ni(SC(6)H(4)R-4)(2)(Ph(2)PCH(2)CH(2)PPh(2))] (R = Me, MeO, H, Cl, or NO(2)).

The kinetics of the equilibrium reaction between [Ni(SC(6)H(4)R-4)(2)(dppe)] (R= MeO, Me, H, Cl, or NO(2); dppe = Ph(2)PCH(2)CH(2)PPh(2)) and mixtures of [lutH](+) and lut (lut = 2,6-dimethylpyridine) in MeCN to form [Ni(SHC(6)H(4)R-4)(SC(6)H(4)R-4)(dppe)](+) have been studied using stopped-flow spectrophotometry. The kinetics for the reactions with R = MeO, Me, H, or Cl are consistent with a single-step equilibrium reaction. Investigation of the temperature dependence of the reactions shows that DeltaG = 13.6 +/- 0.3 kcal mol(-)(1) for all the derivatives but the values of DeltaH and DeltaS vary with R (R = MeO, DeltaH() = 8.5 kcal mol(-)(1), DeltaS = -16 cal K(-)(1) mol(-)(1); R = Me, DeltaH() = 10.8 kcal mol(-)(1), DeltaS = -9.5 cal K(-)(1) mol(-)(1); R = Cl, DeltaH = 23.7 kcal mol(-)(1), DeltaS = +33 cal K(-)(1) mol(-)(1)). With [Ni(SC(6)H(4)NO(2)-4)(2)(dppe)] a more complicated rate law is observed consistent with a mechanism in which initial hydrogen-bonding of [lutH](+) to the complex precedes intramolecular proton transfer. It seems likely that all the derivatives operate by this mechanism, but only with R = NO(2) (the most electron-withdrawing substituent) does the intramolecular proton transfer step become sufficiently slow to result in the change in kinetics. Studies with [lutD](+) show that the rates of proton transfer to [Ni(SC(6)H(4)R-4)(2)(dppe)] (R = Me or Cl) are associated with negligible kinetic isotope effect. The possible reasons for this are discussed. The rates of proton transfer to [Ni(SC(6)H(4)R-4)(2)(dppe)] vary with the 4-R-substituent, and the Hammett plot is markedly nonlinear. This unusual behavior is attributable to the electronic influence of R which affects the electron density at the sulfur.

Journal Article↗

Weak intramolecular proton-hydride and proton-fluoride interactions: experimental (NMR, X-ray) and DFT studies of the bis(NBH(3)) and bis(NBF(3)) adducts of 1,3-dimethyl-1,3-diazolidine.

Bis(NBH(3)), bis(NBF(3)), and NBF(3)/NBH(3) adducts 1-3 were prepared from 1,3-dimethyl-1,3-diazolidine and characterized by the (1)H, (13)C, (11)B, (19)F, 2D (1)H(-13)C HETCOR and NOESY NMR spectra. The structures and conformations of the adducts were established by the variable-temperature (1)H NMR spectra, the X-ray diffraction method (adduct 2A), and density functional calculations at different theoretical levels. The experimental and theoretical data have revealed that bis adducts 1-3 prefer trans orientations of the borane groups (1A, 2A, 3A) in solution, the solid state, and the gas phase. The studies have shown that the energetic preference of trans adducts with respect to cis compounds, decreasing as 2A (2.9 kcal/mol) > 3A (2.7 kcal/mol) > 1A (1.4 kcal/mol), is dictated by spatially repulsive interactions between the CH(3), BH(3), and BF(3) groups. The results of DFT calculations agree well with an experimental trans/cis isomeric ratio of 9:1 determined in solutions of adduct 1. The calculated geometry and energy, as well as the topological analysis of electronic densities, show that trans adducts 1-3 should exist in gas phase as twist conformations T-2 stabilized by the intramolecular C-H(delta+)...(-delta)H-B or C-H(delta+)...(-delta)F-B interactions. These interactions are characterized as closed-shell. The energy of one proton-hydride and proton-fluoride intramolecular contact, estimated as 1.9 (1A-T-2) and 0.7 (2A-T-2) kcal/mol, respectively, classifies the "elongated" intramolecular interactions CH(delta+)...(-delta)HB and CH(delta+)...(-delta)FB as weak ones. It has been established that, on going from gas phase to a condensed phase (solution and solid), the twist-conformations T-2 transform to conformations T-1, probably by intermolecular dipole-dipole interactions. The data presented in this work show that despite a weakness of the "elongated" proton-hydride and proton-fluoride interactions, they can play a significant role in the stabilization of conformational molecular states, especially when cooperativity is in action.

Journal Article↗

Extreme projection of a proton into the pi-cloud of an aromatic ring: record shielding of an aromatic proton in trans-10b-methyl-10c-(1-naphthyl)-10b,10c-dihydropyrene.

A synthetic sequence involving dithiametacyclophane --> metacyclophanediene --> dihydropyrene was employed to prepare trans-10b-methyl-10c-(2-naphthyl)- and trans-10b-methyl-10c-(1-naphthyl)-10b,10c-dihydropyrene 5 and 6, respectively. Both exhibit a strong diamagnetic ring current despite the introduction of an internal bulky substituent within the pi-electron cloud. Their electronic spectra suggest interaction between the two near-perpendicular naphthyl and dihydropyrenyl pi systems, resulting in red shift and band broadening. All naphthyl protons are well resolved in their 1H NMR spectra due to a strong shielding effect of the dihydropyrene ring. The most shielded protons in 5 and 6 are H1' and H2' at delta 2.47 and 1.42, respectively, being 5.25 and 5.95 ppm shifted from those of reference protons. There is evidence for free rotation on the NMR time scale of the 2-naphthyl ring in 5 with a preference for a particular conformer, whereas the 1-naphthyl ring in 6 is conformationally rigid with its H2' projecting deeply into the pi-cloud, thus accounting for the most shielded aromatic proton (H2' in 6) reported to date.

Journal Article↗

Protons colliding with crystalline ice: proton reflection and collision induced water desorption at low incidence energies.

We present results of classical trajectory (CT) calculations on the sticking of protons to the basal plane (0001) face of crystalline ice, for normal incidence at a surface temperature (Ts) of 80 K. The calculations were performed for moderately low incidence energies (Ei) ranging from 0.05 to 4.0 eV. Surprisingly, significant reflection is predicted at low values of Ei (< or = 0.2 eV) due to repulsive electrostatic interactions between the incident proton and the surface water molecules with one of their H-atoms pointing upward toward the gas phase. The sticking probability increases with Ei and converges to unity for Ei > or = 0.8 eV. In the case of sticking, the proton is trapped in the ice forming a Zundel complex (H5O2+), with an average binding energy of 9.9 eV with a standard deviation of 0.5 eV, independent of the value of Ei. In nearly all sticking trajectories, the proton is implanted into the ice surface, with a penetration depth that increases with Ei. The strong interaction with the neighboring water molecules leads to a local rupture of the hydrogen bonding network, resulting in collision induced desorption of water (puffing), a process that occurs with significant probability even at the lowest Ei considered. The probability of water desorption increases with Ei. In nearly all trajectories in which water desorption occurs, a single three-coordinated water molecule is desorbed from the topmost monolayer.

Journal Article↗

IR spectrum and structure of protonated ethanol dimer: implications for the mobility of excess protons in solution.

This Communication reports IR spectra and density functional calculations for the isolated protonated ethanol dimer and its N2-microsolvated complexes, (EtOH)2H+-(N2)n (n = 0-2) to investigate the degree of delocalization of the excess proton in this fundamental building block of an alcohol proton wire. The first spectroscopic characterization of isolated and microsolvated (EtOH)2H+ suggests that the excess proton is (nearly) equally shared between both EtOH units under symmetric solvation conditions (Zundel-type ion, n = 0 and 2), whereas it is largely localized on a single EtOH molecule for asymmetric solvation (Eigen-type ion, n = 1).

Journal Article↗

Electrochemical and homogeneous proton-coupled electron transfers: concerted pathways in the one-electron oxidation of a phenol coupled with an intramolecular amine-driven proton transfer.

Proton-coupled electron transfers currently attract considerable attention in view of their likely involvement in many natural processes. Electrochemistry, through techniques such as cyclic voltammetry, is an efficient way of investigating the reaction mechanism of these reactions, and deciding whether proton and electron transfers are concerted or occur in a stepwise manner. The oxidation of an ortho-substituted 4,6-di (tert-butyl)-phenol in which the phenolic hydrogen atom is transferred during the reaction to the nitrogen atom of a nearby amine is taken as illustrative example. A careful analysis of the cyclic voltammetric responses obtained with this compound and its OD derivative allows, after estimation of the various thermodynamic parameters, ruling out the occurrence of the square scheme mechanism involving the proton-electron and electron-proton sequences. Simulation and comparison of the rate constant and H/D kinetic isotope effect with theoretical predictions show that the experimental value of the preexponential factor is ca. 1 order of magnitude larger than the theoretical value. Detailed calculations suggest that an electric field effect is responsible for this discrepancy.

Journal Article↗

Phase II feasibility study of high-dose radiotherapy for prostate cancer using proton boost therapy: first clinical trial of proton beam therapy for prostate cancer in Japan.

OBJECTIVE: To assess the feasibility of high-dose radiotherapy for prostate cancer using proton boost therapy following photon radiotherapy. METHODS: The primary endpoint was acute grade 3 or greater genitourinary (GU) and gastrointestinal (GI) toxicities. The study included patients with clinical stage T1-3N0M0 prostate cancer. Radiotherapy consisted of 50 Gy/25 fx photon irradiation to the prostate and the bilateral seminal vesicles followed by proton boost of 26 Gy(E)/13 fx to the prostate alone. Hormonal therapy was allowed before and during the radiation therapy. RESULTS: Between January 2001 and January 2003, 30 patients were enrolled in this study. Acute grade 1/2 GU and GI toxicities were observed in 20/4 and 17/0 patients, respectively. With the median follow-up period of 30 months (range 20-45), late grade 1/2 GU and GI toxicities occurred in 2/3 and 8/3 patients, respectively. No grade 3 or greater acute or late toxicities were observed. All patients were alive, but six patients relapsed biochemically after 7-24 months. CONCLUSIONS: Proton boost therapy following photon radiotherapy for prostate cancer is feasible. To evaluate the efficacy and safety of proton beam therapy, a multi-institutional phase II trial is in progress in Japan.

Adenocarcinoma↗

[1H-NMR study of the OR1 operon in bacteriophage lambda. I. Assignment of signals from imino protons and adenine C2 protons].

An oligodeoxyribonucleotide composed of 17 residues, d(TATCACCGCCAGAGGTA), and a complementary chain were synthesized. Their duplex was identical with the operator OR1, the binding site for bacteriophage lambda cro and c1 repressors. The 1H NMR spectra (500 MHz) of the duplex imino and aromatic protons were studied at 10, 20 and 25 degrees C. Signals from the imino protons of complementary base pairs and from the C2 protons of adenine (with the exception of the duplex terminal nucleotides) were assigned using the NOE technique and the known characteristics of short DNA fragment melting. No signals from the imino protons of the terminal base pairs were detected even at 10 degrees C due to fraying which increased as the temperature was raised. The assignment of signals can be used to identify centers of interaction between the operator OR1 and repressors, as well as to study possible local changes in DNA geometry.

Adenine↗

[Nature of endogenous proton conductance of the inner mitochondrial membrane. Role of Ca2+ transport system in proton transfer].

In order to elucidate the nature of endogenous proton conductance of rat liver inner mitochondrial membrane, the dependence of the rate of Ca2+ transport on pH was studied. It was found that the inhibiting effect of H+ is independent of protonation of functional groups of hypothetical Ca2+ carrier, but results from electrogenic transfer of H+ across the membrane, which is highly permeable for the proton. The adsorption of H+ by mitochondria is inhibited by ruthenium red and other specific inhibitors of Ca2+ transport. It is concluded that endogenous proton conductance of the inner mitochondrial membrane depends on the functioning of the same transport system essential for membrane permeability for Ca2+ and other bivalent cations. The correlation observed between the rates of H+ and Ca2+ transport in mitochondria and the ratio of cation mobilities in aqueous solutions is in favour of a "porous" mechanism of cation transport across the mitochondrial membrane.

Animals↗

Proton beam radiotherapy for uveal melanoma: results of Curie Institut-Orsay proton therapy center (ICPO).

PURPOSE: This study reports the results of proton beam radiotherapy based on a retrospective series of patients treated for uveal melanoma at the Orsay Center. METHODS AND MATERIALS: Between September 1991 and September 2001, 1,406 patients with uveal melanoma were treated by proton beam radiotherapy. A total dose of 60 cobalt Gray equivalent (CGE) was delivered in 4 fractions on 4 days. Survival rates were determined using Kaplan-Meier estimates. Prognostic factors were determined by multivariate analysis using the Cox model. RESULTS: The median follow-up was 73 months (range, 24-142 months). The 5-year overall survival and metastasis-free survival rates were 79% and 80.6%, respectively. The 5-year local control rate was 96%. The 5-year enucleation for complications rate was 7.7%. Independent prognostic factors for overall survival were age (p < 0.0001), gender (p < 0.0003), tumor site (p < 0.0001), tumor thickness (p = 0.02), tumor diameter (p < 0.0001), and retinal area receiving at least 30 CGE (p = 0.003). Independent prognostic factors for metastasis-free survival were age (p = 0.0042), retinal detachment (p = 0.01), tumor site (p < 0.0001), tumor volume (p < 0.0001), local recurrence (p < 0.0001), and retinal area receiving at least 30 CGE (p = 0.002). Independent prognostic factors for local control were tumor diameter (p = 0.003) and macular area receiving at least 30 CGE (p = 0.01). Independent prognostic factors for enucleation for complications were tumor thickness (p < 0.0001) and lens volume receiving at least 30 CGE (p = 0.0002). CONCLUSION: This retrospective study confirms that proton beam radiotherapy ensures an excellent local control rate. Further clinical studies are required to decrease the incidence of postirradiation ocular complications.

Adolescent↗

Conformal proton radiation therapy of the posterior fossa: a study comparing protons with three-dimensional planned photons in limiting dose to auditory structures.

PURPOSE: Conventional radiation therapy for pediatric posterior fossa tumors can cause sequelae such as hearing loss and impairments in language and learning. Modern three-dimensional (3D) treatment techniques have improved dose conformity to the posterior fossa. This report compares the normal tissue dose-sparing capabilities of proton radiation therapy (PRT) with 3D conformal photon plans. METHODS AND MATERIALS: Nine children underwent previous PRT for primary CNS malignancies. Using original planning CT scans, the posterior fossa, inner and middle ear, and temporal lobes were delineated. Three-dimensional treatment plans were generated for protons and photons. Normal tissue exposures were calculated by averaging mean doses received and by analysis of dose-volume histogram. RESULTS: The 95% isodose encompassed the posterior fossa in all plans. Normal structures received markedly less radiation from PRT plans than from 3D photon plans. The cochlea received an average mean of 25 +/- 4% of the prescribed dose from PRT, and 75 +/- 6% from photons. Forty percent of temporal lobe volume was completely excluded using protons; with photons 90% of the temporal lobe received 31% of the dose. CONCLUSION: PRT resulted in increased dose sparing of normal structures analyzed. Posterior fossa conformity of 3D photons came at the expense of increasing amounts of normal tissue receiving low to moderate doses.

Child↗

A simple energy-conserving system: proton reduction coupled to proton translocation.

Oxidative phosphorylation involves the coupling of ATP synthesis to the proton-motive force that is generated typically by a series of membrane-bound electron transfer complexes, which ultimately reduce an exogenous terminal electron acceptor. This is not the case with Pyrococcus furiosus, an archaeon that grows optimally near 100 degrees C. It has an anaerobic respiratory system that consists of a single enzyme, a membrane-bound hydrogenase. Moreover, it does not require an added electron acceptor as the enzyme reduces protons, the simplest of acceptors, to hydrogen gas by using electrons from the cytoplasmic redox protein ferredoxin. It is demonstrated that the production of hydrogen gas by membrane vesicles of P. furiosus is directly coupled to the synthesis of ATP by means of a proton-motive force that has both electrochemical and pH components. Such a respiratory system enables rationalization in this organism of an unusual glycolytic pathway that was previously thought not to conserve energy. It is now clear that the use of ferredoxin in place of the expected NAD as the electron acceptor for glyceraldehyde 3-phosphate oxidation enables energy to be conserved by hydrogen production. In addition, this simple respiratory mechanism readily explains why the growth yields of P. furiosus are much higher than could be accounted for if ATP synthesis occurred only by substrate-level phosphorylation. The ability of microorganisms such as P. furiosus to couple hydrogen production to energy conservation has important ramifications not only in the evolution of respiratory systems but also in the origin of life itself.

Biochemical Phenomena↗

The amino-terminal domain of the vacuolar proton-translocating ATPase a subunit controls targeting and in vivo dissociation, and the carboxyl-terminal domain affects coupling of proton transport and ATP hydrolysis.

The 100-kDa "a" subunit of the vacuolar proton-translocating ATPase (V-ATPase) is encoded by two genes in yeast, VPH1 and STV1. The Vph1p-containing complex localizes to the vacuole, whereas the Stv1p-containing complex resides in some other intracellular compartment, suggesting that the a subunit contains information necessary for the correct targeting of the V-ATPase. We show that Stv1p localizes to a late Golgi compartment at steady state and cycles continuously via a prevacuolar endosome back to the Golgi. V-ATPase complexes containing Vph1p and Stv1p also differ in their assembly properties, coupling of proton transport to ATP hydrolysis, and dissociation in response to glucose depletion. To identify the regions of the a subunit that specify these different properties, chimeras were constructed containing the cytosolic amino-terminal domain of one isoform and the integral membrane, carboxyl-terminal domain from the other isoform. Like the Stv1p-containing complex, the V-ATPase complex containing the chimera with the amino-terminal domain of Stv1p localized to the Golgi and the complex did not dissociate in response to glucose depletion. Like the Vph1p-containing complex, the V-ATPase complex containing the chimera with the amino-terminal domain of Vph1p localized to the vacuole and the complex exhibited normal dissociation upon glucose withdrawal. Interestingly, the V-ATPase complex containing the chimera with the carboxyl-terminal domain of Vph1p exhibited a higher coupling of proton transport to ATP hydrolysis than the chimera containing the carboxyl-terminal domain of Stv1p. Our results suggest that whereas targeting and in vivo dissociation are controlled by sequences located in the amino-terminal domains of the subunit a isoforms, coupling efficiency is controlled by the carboxyl-terminal region.

Adenosine Triphosphatases↗

Phloem-localized, proton-coupled sucrose carrier ZmSUT1 mediates sucrose efflux under the control of the sucrose gradient and the proton motive force.

The phloem network is as essential for plants as the vascular system is for humans. This network, assembled by nucleus- and vacuole-free interconnected living cells, represents a long distance transport pathway for nutrients and information. According to the Münch hypothesis, osmolytes such as sucrose generate the hydrostatic pressure that drives nutrient and water flow between the source and the sink phloem (Münch, E. (1930) Die Stoffbewegungen in der Pflanze, Gustav Fischer, Jena, Germany). Although proton-coupled sucrose carriers have been localized to the sieve tube and the companion cell plasma membrane of both source and sink tissues, knowledge of the molecular representatives and the mechanism of the sucrose phloem efflux is still scant. We expressed ZmSUT1, a maize sucrose/proton symporter, in Xenopus oocytes and studied the transport characteristics of the carrier by electrophysiological methods. Using the patch clamp techniques in the giant inside-out patch mode, we altered the chemical and electrochemical gradient across the sucrose carrier and analyzed the currents generated by the proton flux. Thereby we could show that ZmSUT1 is capable of mediating both the sucrose uptake into the phloem in mature leaves (source) as well as the desorption of sugar from the phloem vessels into heterotrophic tissues (sink). As predicted from a perfect molecular machine, the ZmSUT1-mediated sucrose-coupled proton current was reversible and depended on the direction of the sucrose and pH gradient as well as the membrane potential across the transporter.

Animals↗

The protonation-deprotonation kinetics of the protonated Schiff base in bicelle bacteriorhodopsin crystals.

In the recently published x-ray crystal structure of the "bicelle" bacteriorhodopsin (bbR) crystal, the protein has quite a different structure from the native and the in cubo bacteriorhodopsin (cbR) crystal. Instead of packing in parallel trimers as do the native membrane and the cbR crystals, in the bbR crystal the protein packs as antiparallel monomers. To date, no functional studies have been performed, to our knowledge, to investigate if the photocycle is observed in this novel protein packing structure. In this study, both Raman and time-resolved transient absorption spectroscopy are used to both confirm the presence of the photocycle and investigate the deprotonation-reprotonation kinetics of the Schiff base proton in the bbR crystal. The observed rates of deprotonation and reprotonation processes of its Schiff base have been compared to those observed for native bR under the same conditions. Unlike the previously observed similarity of the rates of these processes for cbR crystals and those for native bacteriorhodopsin (bR), in bbR crystals the rate of deprotonation has increased by 300%, and the rate of reprotonation has decreased by nearly 700%. These results are discussed in light of the changes observed when native bR is delipidated or monomerized by detergents. Both the change of the hydrophobicity of the environment around the protonated Schiff base and Asp85 and Asp96 (which could change the pKa values of proton donor-acceptor pairs) and the water structure in the bbR crystal are offered as possible explanations for the different observations.

Aspartic Acid↗