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Effects of thermal denaturation on the longitudinal relaxation time (T1) of water protons in protein solutions: study of the factors determining the T1 of water protons.

The factors determining the longitudinal relaxation time (T1) of water protons in protein solutions were investigated by analyzing the effects of thermal denaturation on the T1 of the water protons. We treated the water protons and the protein protons "on a protein surface" as a dipole-dipole coupled two-spin system where relative translational diffusion is the dominant mechanism, and measured the change in the time development of the nuclear Overhauser effect (NOE) factors of the water protons. The T1 of the water protons was shortened markedly when the proteins were thermally denatured. Our analysis indicates that this relaxation enhancement is due to an increase in the value of the translational correlation time as well as the fraction of hydration water molecules, though the influence of "proton exchange" between the water protons and the labile protein protons cannot be completely neglected.

Animals↗

Control of the Stereochemistry of Kinetic Protonation: Intramolecular Proton Delivery(1)(,)(2).

Four decades ago, we noted that for delocalized carbanions and enols the protonation transition state is close to sp(2) hybridized and that, as a consequence, under kinetic control protonation takes place from the less hindered approach, most often with formation of the less stable of two possible stereoisomers. The initial report was followed by an extensive series of examples. Nevertheless, a major question remained, namely whether it was possible to deliver the proton to the more hindered face of such a species using intramolecular proton transfer. To this end, silyl ether precursors to the enols of 3-benzoyl-endo-6-phenyl-exo-6-pyridylbicyclo[3.1.0]hexane and its endo-6-pyridyl-exo-6-phenyl stereoisomer were synthesized. The corresponding enols were generated with fluoride anion. The endo-phenyl enol stereoisomers, on kinetic protonation, led stereoselectively to the endo-3-benzoyl product resulting from the less hindered protonation. In stark contrast, the endo-6-pyridyl enol isomer led stereoselectively to the exo-3-benzoyl ketone by intramolecular proton delivery. However, the kinetic orders of the stereochemistries differ; the intramolecular process requires additional proton donor molecules. The log of the ratio of the two stereochemistries is linear with the log of the proton donor concentration with the slope giving the difference in kinetic orders. An aromatic cyclic 14 electron Hückel transition state is proposed. Additionally, the roles of acyl, nitro and cyano delocalizing groups were analyzed with ab initio computations.

Journal Article↗

Mechanism of proton transport by plant plasma membrane proton ATPases.

The mechanism of proton translocation by P-type proton ATPases is poorly defined. Asp684 in transmembrane segment M6 of the Arabidopsis thaliana AHA2 plasma membrane P-type proton pump is suggested to act as an essential proton acceptor during proton translocation. Arg655 in transmembrane segment M5 seems to be involved in this proton translocation too, but in contrast to Asp684, is not essential for transport. Asp684 may participate in defining the E(1) proton-binding site, which could possibly exist as a hydronium ion coordination center. A model of proton translocation of AHA2 involving the side chains of amino acids Asp684 and Arg655 is discussed.

Arabidopsis↗

Light-induced proton slip and proton leak at the thylakoid membrane.

A treatment of leaves of Spinacia oleracea L. with light or with the thiol reagent dithiothreitol in the dark led to partly uncoupled thylakoids. After induction in intact leaves, the partial uncoupling was irreversible at the level of isolated thylakoids. We distinguish between uncoupling by proton slip, which means a decrease of the H+/e(-) -ratio due to less efficient proton pumping, and proton leak as defined by enhanced kinetics of proton efflux. Proton slip and proton leak made about equal contributions to the total uncoupling. The enhanced proton efflux kinetics corresponded to reduction of subunit CF1-gamma of the ATP synthase as shown by fluorescence labeling of thylakoid proteins with the sulfhydryl probe 5-iodoacetamido fluorescein. The maximum value of the fraction of reduced CF1-gamma was only 36%, which indicates that in vivo the reduction of CF1-gamma could be limited by fast reoxidation and/or restricted accessibility of CF1-gamma to thioredoxin. Measurements of the ratio ATP/2e indicated that only the uncoupling related to less efficient proton pumping led to a decrease in the ATP yield.

Chloroplast Proton-Translocating ATPases↗

Model for proton transport coupled to protein conformational change: application to proton pumping in the bacteriorhodopsin photocycle.

A modeling method is presented for protein systems in which proton transport is coupled to conformational change, as in proton pumps and in motors driven by the proton-motive force. Previously developed methods for calculating pKa values in proteins using a macroscopic dielectric model are extended beyond the equilibrium case to a master-equation model for the time evolution of the system through states defined by ionization microstate and a discrete set of conformers. The macroscopic dielectric model supplies free energy changes for changes of protonation microstate, while the method for obtaining the energetics of conformational change and the relaxation rates, the other ingredients needed for the master equation, are system dependent. The method is applied to the photoactivated proton pump, bacteriorhodopsin, using conformational free energy differences from experiment and treating relaxation rates through three adjustable parameters. The model is found to pump protons with an efficiency relatively insensitive to parameter choice over a wide range of parameter values, and most of the main features of the known photocycle from very early M to the return to the resting state are reproduced. The boundaries of these parameter ranges are such that short-range proton transfers are faster than longer-range ones, which in turn are faster than conformational changes. No relaxation rates depend on conformation. The results suggest that an "accessibility switch", while not ruled out, is not required and that vectorial proton transport can be achieved through the coupling of the energetics of ionization and conformational states.

Bacteriorhodopsins↗

Proton mobility in protonated glycylglycine and N-formylglycylglycinamide: a combined quantum chemical and RKKM study.

Theoretical model calculations were performed to investigate the degree of validity of the mobile proton model of protonated peptides. The structures and energies of the most important minima corresponding to different structural isomers of protonated diglycine and their conformers, as well as the barriers separating them, were determined by DFT calculations. The rate coefficients of the proton transfer reactions between the isomers were calculated using the RRKM method in order to obtain a quantitative measure of the time scale of these processes. The proton transfer reactions were found to be very fast already at and above the threshold to the lowest energy decomposition pathway. Two possible mechanisms of b2+-ion formation via water loss from the dipeptide are also discussed. The rate-determining step of the proton migration along a peptide chain is also investigated using the model compound N-formylglycylglycinamide. The investigations revealed that this process very possibly occurs via the protonation of the carbonyl oxygens of the amide bonds, and its rate-determining step is an internal rotation-type transition of the protonated C=O-H group between two adjacent C=O-HellipsisO=C bridges.

Chemical Phenomena↗

Inhibition of proton transfer in cytochrome c oxidase by zinc ions: delayed proton uptake during oxygen reduction.

We have investigated the effect of Zn ions on proton-transfer reactions in cytochrome c oxidase. In the absence of Zn(2+) the transition from the "peroxy" (P(R)) to the "ferryl" (F) intermediate has a time constant of approximately 100 micros and it is associated with proton transfer from the bulk solution with an intrinsic time constant of <<100 micros, but rate limited by the P(R)-->F transition. While in the presence of 100 microM Zn(2+) the P(R)-->F transition was slowed by a factor of approximately 2, proton uptake from the bulk solution was impaired to a much greater extent. Instead, about two protons (one proton in the absence of Zn(2+)) were taken up during the next reaction step, i.e. the decay of F to the oxidized (O) enzyme with a time constant of approximately 2.5 ms. Thus, the results show that there is one proton available within the enzyme that can be used for oxygen reduction and confirm our previous observation that F can be formed without proton uptake from the bulk solution. No effect of Zn(2+) was observed with a mutant enzyme in which Asp(I-132), at the entry point of the D-pathway, was replaced by its non-protonatable analogue Asn. In addition, no effect of Zn(2+) was observed on the F-->O transition rate when measured in D(2)O, because in D(2)O, the transition is internally slowed to approximately 10 ms, which is already slower than with bound Zn(2+). Together with earlier results showing that both the P(R)-->F and F-->O transitions are associated with proton uptake through the D-pathway, the results from this study indicate that Zn(2+) binds to and blocks the entrance of the D-pathway.

Binding Sites↗

Redesign of the proton-pumping machinery of cytochrome c oxidase: proton pumping does not require Glu(I-286).

One of the putative proton-transfer pathways leading from solution toward the binuclear center in many cytochrome c oxidases is the D-pathway, so-called because it starts with a highly conserved aspartate [D(I-132)] residue. Another highly conserved amino acid residue in this pathway, glutamate(I-286), has been indicated to play a central role in the proton-pumping machinery of mitochondrial-type enzymes, a role that requires a movement of the side chain between two distinct positions. In the present work we have relocated the glutamate to the opposite side of the proton-transfer pathway by constructing the double mutant EA(I-286)/IE(I-112). This places the side chain in about the same position in space as in the original enzyme, but does not allow for the same type of movement. The results show that the introduction of the second-site mutation, IE(I-112), in the EA(I-286) mutant enzyme results in an increase of the enzyme activity by a factor of >10. In addition, the double mutant enzyme pumps approximately 0.4 proton per electron. This observation restricts the number of possible mechanisms for the operation of the redox-driven proton pump. The proton-pumping machinery evidently does require the presence of a protonatable/polar residue at a specific location in space, presumably to stabilize an intact water chain. However, this residue does not necessarily have to be at a strictly conserved location in the amino acid sequence. In addition, the results indicate that E(I-286) is not the "proton gate" of cytochrome c oxidase controlling the flow of pumped protons from one to the other side of the membrane.

Catalysis↗

Catalytic function and local proton structure at the type 2 copper of nitrite reductase: the correlation of enzymatic pH dependence, conserved residues, and proton hyperfine structure.

Electron nuclear double resonance (ENDOR) of protons at Type 2 and Type 1 cupric active sites correlates with the enzymatic pH dependence, the mutation of nearby conserved, nonligating residues, and electron transfer in heterologously expressed Rhodobacter sphaeroides nitrite reductase. Wild-type enzyme showed a pH 6 activity maximum but no kinetic deuterium isotope effect, suggesting protons are not transferred in the rate-limiting step of nitrite reduction. However, protonatable Asp129 and His287, both located near the Type 2 center, modulated enzyme activity. ENDOR of the wild-type Type 2 center at pH 6.0 revealed an exchangeable proton with large hyperfine coupling. Dipolar distance estimates indicated that this proton was 2.50-2.75 or 2.25-2.45 A from Type 2 copper in the presence or absence of nitrite, respectively. This proton may provide a properly oriented hydrogen bond to enhance water formation upon nitrite reduction. This proton was eliminated at pH 5.0 and showed a diminished coupling at pH 7.5. Mutations of Asp129 and His287 reduced enzyme activity and altered the exchangeable proton hyperfine spectra. Mutation of Asp129 prevented a pH-dependent change at the Type 1 Cys167 ligand as observed by Cys C(beta) proton ENDOR, implying there is a Type 2 and pH-dependent alteration of the Type 1 center. Mutation of the Type 1 center ligand Met182 to Thr and mutation of Asp129 increased the activation energy for nitrite reduction. Involvement of both the Type 1 center and Asp129 in modulating activation energy shows that electron transfer from the Type 1 center to a nitrite-ligated Type 2 center is rate-limiting for nitrite reduction. Mutation of Ile289 to Ala and Val caused minor perturbation to enzyme activity, but as detected by ENDOR, allowed formate binding. Thus, bulky Ile289 may exclude non-nitrite ligands from the Type 2 active site.

Amino Acid Substitution↗

Pathway of proton transfer in bacterial reaction centers: second-site mutation Asn-M44-->Asp restores electron and proton transfer in reaction centers from the photosynthetically deficient Asp-L213-->Asn mutant of Rhodobacter sphaeroides.

Site-directed mutagenesis of the photosynthetic reaction center (RC) from Rhodobacter sphaeroides has shown Asp-213 of the L subunit (Asp-L213) to be important for photosynthetic viability. Replacement of Asp-L213 with Asn resulted in a photosynthetically deficient mutant, due to the 10(4)-fold slower rate for the proton-coupled electron transfer reaction QA-QB- + 2H+-->QAQBH2 (k(2)AB). The detrimental effect of Asn-L213 is surprising since RCs from Rhodopseudomonas viridis, Rhodospirillum rubrum, and Chloroflexus aurantiacus have Asn at the homologous position. However, RCs from these bacteria have an Asp located near QB (the secondary quinone acceptor) at the position homologous to Asn-M44 in Rb. sphaeroides which might function in place of Asp-L213. To test this conjecture a "viridis-like" structure was introduced into Rb. sphaeroides by replacing Asp-L213 with Asn and Asn-M44 with Asp. The RCs from this double mutant displayed near-native rates for the electron transfer reaction k(2)AB and restored photosynthetic competence. The rates for the first electron transfer reaction QA-QB-->QAQB- (k(1)AB) and charge recombination D+QAQB--->DQAQB (kBD) were also restored to near-native values. These results indicate that Asp at either the L213 or the M44 site near QB can provide a pathway for rapid proton transfer and explain why Asp-L213 need not be conserved in different photosynthetic bacteria. To test further the effect of Asp at M44 on electron and proton transfer to QB a mutant containing Asp at both L213 and M44 was constructed. The RCs from this mutant (Asn-M44-->Asp) exhibited faster proton-coupled electron transfer to QB-. The increased rate of proton-coupled electron transfer (k(2)AB) in the presence of negatively charged Asp residues near QB suggests the role of an Asp near QB as (i) a proton donor group in the proton transfer chain and/or (ii) a negatively charged residue stabilizing proton transfer to reduced QB.

Amino Acid Sequence↗

The roles of the two proton input channels in cytochrome c oxidase from Rhodobacter sphaeroides probed by the effects of site-directed mutations on time-resolved electrogenic intraprotein proton transfer.

The crystal structures of cytochrome c oxidase from both bovine and Paracoccus denitrificans reveal two putative proton input channels that connect the heme-copper center, where dioxygen is reduced, to the internal aqueous phase. In this work we have examined the role of these two channels, looking at the effects of site-directed mutations of residues observed in each of the channels of the cytochrome c oxidase from Rhodobacter sphaeroides. A photoelectric technique was used to monitor the time-resolved electrogenic proton transfer steps associated with the photo-induced reduction of the ferryl-oxo form of heme a3 (Fe4+ = O2-) to the oxidized form (Fe3+OH-). This redox step requires the delivery of a "chemical" H+ to protonate the reduced oxygen atom and is also coupled to proton pumping. It is found that mutations in the K channel (K362M and T359A) have virtually no effect on the ferryl-oxo-to-oxidized (F-to-Ox) transition, although steady-state turnover is severely limited. In contrast, electrogenic proton transfer at this step is strongly suppressed by mutations in the D channel. The results strongly suggest that the functional roles of the two channels are not the separate delivery of chemical or pumped protons, as proposed recently [Iwata, S., Ostermeier, C., Ludwig, B. & Michel, H. (1995) Nature (London) 376, 660-669]. The D channel is likely to be involved in the uptake of both "chemical" and "pumped" protons in the F-to-Ox transition, whereas the K channel is probably idle at this partial reaction and is likely to be used for loading the enzyme with protons at some earlier steps of the catalytic cycle. This conclusion agrees with different redox states of heme a3 in the K362M and E286Q mutants under aerobic steady-state turnover conditions.

Animals↗

Conserved Asp684 in transmembrane segment M6 of the plant plasma membrane P-type proton pump AHA2 is a molecular determinant of proton translocation.

The mechanism of proton pumping by P-type H(+)-ATPases is still unclear. In the plant P-type plasma membrane H(+)-ATPase AHA2, two charged residues, Arg(655) and Asp(684), are conserved in transmembrane segments M5 and M6, respectively, a region that has been shown be contribute to ion coordination in related P-type ATPases. Substitution of Arg(655) with either alanine or aspartate resulted in mutant enzymes exhibiting a significant shift in the P-type ATPase E(1)P-E(2)P conformational equilibrium. The mutant proteins accumulated in the E(1)P conformation, but were capable of conducting proton transport. This points to an important role of Arg(655) in the E(1)P-E(2)P conformational transition. The presence of a carboxylate moiety at position Asp(684) proved essential for coupling between initial proton binding and proton pumping. The finding that the carboxylate side chain of Asp(684) contributes to the proton-binding site and appears to function as an absolutely essential proton acceptor along the proton transport pathway is discussed in the context of a possible proton pumping mechanism of P-type H(+)-ATPases.

Adenosine Triphosphatases↗

Evaluation of proton density by magnetic resonance imaging: phantom experiments and analysis of multiple component proton transverse relaxation.

The quantitative evaluation of proton density by magnetic resonance imaging (MRI) is limited as a result of non-uniformities in the intensity distribution of the images and by the fact that only part of the protons of the tissue contribute to the image signal. This study was undertaken to estimate the accuracy of proton density measurements using a standard whole-body MR imager operating at 1.5 T. First, phantom experiments were performed to examine the possibility of an intensity correction. For the test phantom the systematical errors in the computed proton densities were reduced from 5 to 1% after correction. Secondly, proton transverse relaxation curves of biological tissues were measured in vitro on an MR spectrometer. A multi-exponential analysis of the data shows that for spin-echo times TE greater than 10 ms in total between 10 and 30% of the protons of the tissue do not contribute to the image signal. In all tissues a proton component with a free induction decay (FID) time T2* less than 32 microseconds was observed. In the time range TE greater than 10 ms two proton components can be distinguished in muscle and fatty tissue. Finally, it will be shown that a pixel-orientated two-exponential analysis of spin-echo images leads to a much more homogeneous density image than one-exponential computation, since tissue-specific biexponentiality and partial volume effects are taken into account. As a conclusion, the hydrogen density of biological tissues can be evaluated at best with an overall error of 10% from MR images for TE greater than 10 ms. This accuracy is insufficient for a pixel-orientated neutron therapy planning.

Adipose Tissue↗

Voltage-gated proton channels and other proton transfer pathways.

Proton channels exist in a wide variety of membrane proteins where they transport protons rapidly and efficiently. Usually the proton pathway is formed mainly by water molecules present in the protein, but its function is regulated by titratable groups on critical amino acid residues in the pathway. All proton channels conduct protons by a hydrogen-bonded chain mechanism in which the proton hops from one water or titratable group to the next. Voltage-gated proton channels represent a specific subset of proton channels that have voltage- and time-dependent gating like other ion channels. However, they differ from most ion channels in their extraordinarily high selectivity, tiny conductance, strong temperature and deuterium isotope effects on conductance and gating kinetics, and insensitivity to block by steric occlusion. Gating of H(+) channels is regulated tightly by pH and voltage, ensuring that they open only when the electrochemical gradient is outward. Thus they function to extrude acid from cells. H(+) channels are expressed in many cells. During the respiratory burst in phagocytes, H(+) current compensates for electron extrusion by NADPH oxidase. Most evidence indicates that the H(+) channel is not part of the NADPH oxidase complex, but rather is a distinct and as yet unidentified molecule.

Animals↗

Charge delocalization in proton channels, I: the aquaporin channels and proton blockage.

The explicit contribution to the free energy barrier and proton conductance from the delocalized nature of the excess proton is examined in aquaporin channels using an accurate all-atom molecular dynamics computer simulation model. In particular, the channel permeation free energy profiles are calculated and compared for both a delocalized (fully Grotthuss shuttling) proton and a classical (nonshuttling) hydronium ion along two aquaporin channels, Aqp1 and GlpF. To elucidate the effects of the bipolar field thought to arise from two alpha-helical macrodipoles on proton blockage, free energy profiles were also calculated for computational mutants of the two channels where the bipolar field was eliminated by artificially discharging the backbone atoms. Comparison of the free energy profiles between the proton and hydronium cases indicates that the magnitude of the free energy barrier and position of the barrier peak for the fully delocalized and shuttling proton are somewhat different from the case of the (localized) classical hydronium. The proton conductance through the two aquaporin channels is also estimated using Poisson-Nernst-Planck theory for both the Grotthuss shuttling excess proton and the classical hydronium cation.

Aquaporin 1↗

Purified proton conductor in proton translocating adenosine triphosphatase of a thermophilic bacterium.

1. The membrane-integrated portion (TF0) of the proton translocating ATPase complex (TF0-F1) of the thermophilic bacterium PS3 was highly purified. Its proton-conducting activity was investigated in vesicles reconstituted from TF0 and phospholipids (TF0 vesicles). 2. The rate of proton conduction through TF0 was proportional to the membrane potential imposed (6H+ uptake/s/TF0 molecule with 103 mV at pH 8.0). The pH profile of the rate revealed that a proton, not a hydroxy ion, was the true substrate conducted and that there was a monoprotic proton binding site in TF0 (pKa = 6.8). The temperature coefficient of proton conductance of TF0 showed a considerable variation depending on the phospholipids of the vesicles with respective transition temperatures. 3. Passive proton conduction through TF0 was inhibited stoichiometrically by addition of either the soluble ATPase portion (TF1) of TF0-F1, or an energy transfer inhibitor dicyclohexylcarbodiimide or an antibody against TF0. 4. The proton conductance of TF0 was concluded to represent its intrinsic activity in the original TF0-F1 complex.

Adenosine Triphosphatases↗

Isolation and reconstitution of the dicyclohexylcarbodiimide-sensitive proton pore of the clathrin-coated vesicle proton translocating complex.

The clathrin-coated vesicle proton translocating complex is composed of a maximum of eight polypeptides. The function of the components of this system have not been defined. Proton pumping catalyzed by the reconstituted, 200-fold purified proton translocating complex of clathrin-coated vesicles is inhibited 50% at a dicyclohexylcarbodiimide (DCCD)/protein ratio of 0.66 mumol of DCCD/mg of protein. At an identical DCCD/protein ratio, the 17-kDa component of the proton pump is labeled by [14C]DCCD. Through toluene extraction, the 17-kDa subunit has been isolated from the holoenzyme. The 17-kDa polypeptide diminished proteoliposome acidification when coreconstituted with either bacteriorhodopsin or the intact clathrin-coated vesicle proton translocating ATPase. In both instances, treatment of the 17-kDa polypeptide with DCCD restored proteoliposome acidification. Moreover, the proton-conducting activity of the 17-kDa polypeptide is abolished by trypsin digestion. These results demonstrate that the 17-kDa polypeptide present in the isolated proton ATPase of clathrin-coated vesicles is a subunit which functions as a transmembranous proton pore.

Animals↗