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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

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

Proton leakiness caused by cloned genes for the F0 sector of the proton-translocating ATPase of Escherichia coli: requirement for F1 genes.

To study expression of uncG, the gene coding for the gamma subunit of the Escherichia coli proton-translocating ATPase, deletions were made in the intergenic region between uncA, the gene coding for the alpha subunit, and uncG. Two deletions which fused uncA and uncG coded for alpha-gamma fusion polypeptides which were synthesized well both in vitro and in vivo, demonstrating that uncG expression is normally controlled by nucleotides in the intergenic region. Multicopy plasmids carrying these fusion genes and the genes for the other subunits of the ATPase had a harmful effect on the growth of E. coli. The effect was overcome by N,N'-dicyclohexylcarbodiimide, indicating that the cells probably leaked protons. The deleterious effect was eliminated by making a nonpolar deletion in the upstream F0 gene uncB, or by cloning each of the uncA-uncG fusion genes onto a separate plasmid, removed from the F0 genes, thus demonstrating that the fusion genes were not primarily responsible for the proton permeability. A plasmid which carried F0 genes and the gene for the delta subunit caused deleterious proton leakiness in unc+ cells but not in cells from which the unc operon was deleted. The proton leakiness caused by these different plasmids was therefore due to the production of a leaky F0 proton channel and required the presence of F1 genes. The results support a model for ATPase assembly in which F1 genes or polypeptides are involved in the formation or opening of the F0 proton channel.

Cell Membrane Permeability

Mechanism of respiration-driven proton translocation in the inner mitochondrial membrane. Analysis of proton translocation associated with oxidation of endogenous ubiquinol.

A study is presented of the kinetics and stoichiometry of fast proton translocation associated to aerobic oxidation of components of the mitochondrial respiratory chain. 1. Aerobic oxidation of ubiquinol and b cytochromes is accompanied in EDTA particles, obtained by sonication of beef-heart mitochondria, by synchronous proton uptake. 2. The rapid proton uptake associated to oxidation and b cytochromes is greatly stimulated by valinomycin plus K+, but is unaffected by carbonyl cyanide p-trifluoromethoxyphenylhydrazone. 3. 4 gion H+ are taken up per mol ubiquinol oxidized by oxygen. This H+/2e- ratio, measured in the rapid anaerobic-aerobic transition of the particles is unaffected by carbonyl cyanide p-trifluoromethoxyphenylhydrazone. 4. Intact mitochondria aerobic oxidation of oxygen-terminal electron carriers is accompanied by antimycin-insensitive synchronous proton release, oxidation of ubiquinol and reduction of b cytochromes. The amount of protons released is in excess with respect to the amount of ubiquinol oxidized. 5. It is concluded that electron flow along complex III, from ubiquinol to cytochrome c, is directly coupled to vectorial proton translocation. The present data suggest that there exist(s) between ubiquinol and cytochrome c one (or two) respiratory carrier(s), whose oxido-reduction is directly linked to effective transmembrane proton translocation.

Animals

Interactions of lithium and protons with the sodium-proton exchanger of dog red blood cells.

Passive movements of Li in dog red blood cells (RBC) ar like those of Na and protons in being stimulated by osmotic cell shrinkage and inhibited by amiloride. Li and protons have similar asymmetrical effects on Na-H exchange. When the intracellular fluid is made rich in Li or protons, Na-H exchange is stimulated. When the extracellular fluid is enriched in Li or protons, Na-H exchange is inhibited. In the case of protons, these effects can override alterations in driving force that are created by the experimental conditions. For example, acidification of the cytoplasm stimulates outward Na movements, while acidification of the medium inhibits Na efflux. Thus, protons (and, by analogy, Li) can interact with the Na-H exchanger not only as substrates but also as modulators. In previous experiments, the only way to activate the Na-H exchanger in dog RBC was to shrink the cells in hypertonic media. The influences of Li or protons, however, are so strong as to preempt the volume effects, so that the pathway can be activated even in swollen cells and deactivated in shrunken ones.

Amiloride

Interactions of protons with single open L-type calcium channels. pH dependence of proton-induced current fluctuations with Cs+, K+, and Na+ as permeant ions.

We studied the pH dependence of the proton-induced current fluctuations that appear in single open L-type Ca channels when monovalent ions are the charge carriers. We used different methods of analysis to obtain kinetic measurements even under conditions where the individual transitions were too fast to be resolved directly as discrete current steps between two conductance levels. The reciprocal of the dwell times at the high conductance level increased linearly with the pipette proton activity, with a slope that was similar for Cs, K, and Na as permeant ions. Contrary to the expectation for a simple model in which the high and low conductances represent the unprotonated and protonated states of the channel, respectively, the dwell times at the low conductance level were also pH dependent and lengthened with increasing proton activity. At all pH values the dwell times at the low conductance level were longest with Cs as permeant ion and shortened in the order Cs greater than K greater than Na. We introduce a more general model of the protonation cycle in which the channel is represented by four states and can be protonated and deprotonated both at the high and low conductance levels. The conductance change is represented by a conformational change of the channel protein. We discuss the validity of this model and its implications for the mechanism by which protons interact with ion permeation through L-type Ca channels.

Animals

Proton radiography as a tool for quality control in proton therapy.

Proton radiography is investigated for its use as a quality control tool in proton therapy. Images were produced both with range and range uncertainty information of protons passing through phantoms (Alderson phantom and a sheep's head). With the range images the correct positioning of the patient with respect to the beam could be verified. The range uncertainty images were used to quantitatively detect range variations of protons passing through inhomogeneities in the patient. These measurements can be used to indicate critical situations during proton therapy or to determine the safety margin around the tumor volume. With the range information the precision of different calibrations of computer tomography Hounsfield values to relative proton stopping power, used for proton treatment planning, was determined. It is found that the precision in range can be improved by a detailed analysis of the calibration data obtained from tissue-substitute measurements, by a factor of 2.5. The resulting range errors are in the order of the positioning precision (approximately 1 mm).

Animals

Analysis of difference spectra of protonated DNA: determination of degree of protonation of nitrogen bases and the fractions of disordered nucleotide pairs.

The titration curves of nitrogen bases and fractions of disordered nucleotide pairs are obtained during DNA protonation. It is shown that purine bases are the first sites of the DNA double helix protonation. The cytosine protonation is due to proton-induced conformational transition within GC pairs with the sequence proton transfer from (N-7) of guanine to (N-3) of cytosine. Within DNA with unwound regions the bases are protonated in the following order: cytosine, adenine, guanine. It is shown that GC pairs are the primary centres in which the unwinding of protonated DNAs occurs.

Animals

Proton conductance by the gramicidin water wire. Model for proton conductance in the F1F0 ATPases?

The gramicidin channel contains a single strand of water molecules associated through hydrogen bonds. Previous work has shown that channels of similar size are formed by association of transmembrane alpha helices of synthetic leucine-serine peptides. Both types of channels translocate protons with considerable selectivity relative to other cations, and it has been proposed that the selectivity arises by proton "hopping" along hydrogen-bonded chains of water, whereas other cations must cross by ordinary diffusion processes. It is possible that a similar mechanism underlies proton transport in the Fo subunit of the F1F0 ATP synthase. Using the gramicidin channel as a model, we have tested whether a single strand of water is kinetically competent to translocate protons at a rate sufficient to support known rates of ATP synthesis. We found that the gramicidin channel saturates at approximately 530 pS of protonic current in 4 M HCl, more than sufficient for typical ATP synthesis rates. It follows that proton diffusion to a putative channel in Fo, rather than the channel itself, may limit ATP synthesis rates.

Gramicidin

Mechanism of surface peptide proton exchange in bovine pancreatic trypsin inhibitor. Salt effects and O-protonation.

The acid-catalyzed hydrogen exchange rate constants kH, and the base-catalyzed rate constants kOH, have been determined (in the preceding paper) for the 25 most rapidly exchanging NH groups of bovine pancreatic trypsin inhibitor. Most of these NH groups are at the protein-solvent interface. The correlation of kH, but not kOH, with the static accessibility and hydrogen bonding of the peptide carbonyl O atom indicates that the mechanism of acid catalysis in proteins involves O-protonation. Agreement between the ionic strength dependence observed for kH and kOH and the ionic strength dependence calculated for an O-protonation mechanism supports this conclusion. N-protonation for acid catalysis, as well as N-deprotonation for base catalysis, have traditionally been assumed in the mechanism of the chemical step in peptide amide proton exchange. A preference for the alternative O-protonation mechanism has far-reaching implications in the interpretation of protein hydrogen exchange kinetics. With an O-protonation mechanism, acid-catalyzed rates of surface NH groups are primarily a function of the average solvent accessibility of the carbonyl O atoms in the dynamic solution structure, while base-catalyzed rates of surface NH groups measure solvent accessibility of the peptide N. The relative dynamic accessibilities of peptide O atoms, as measured by relative values of kH (corrected for electrostatic effects), correlate with O static accessibilities in the crystal structure. A lower correlation of static accessibility of N atoms with kOH is observed for surface NH groups in peptide groups in which the carbonyl O is not hydrogen bonded. For some surface NH groups, the observed pH of minimum rate, pHmin, deviates widely from the pHmin of model compounds. This is explained as the combined result of electrostatic effects and of the differences in accessibility of the carbonyl O and N atoms that result in a change in the relative values of kH and kOH as compared to those of model peptides. A mechanism whereby exchange of interior sites is catalyzed by interactions of catalysis ions with protein surface atoms via charge transfer is suggested.

Amides

Proton transfer in cytochrome bo3 ubiquinol oxidase of Escherichia coli: second-site mutations in subunit I that restore proton pumping in the mutant Asp135-->Asn.

The ubiquinol oxidase, cytochrome bo3, of Escherichia coli is a member of the respiratory heme-copper oxidase family and conserves energy from the reduction of dioxygen to water by translocation of protons across the bacterial membrane. Mutation of an aspartic acid residue (Asp135) to asparagine in subunit I of this enzyme was previously found to impair proton translocation [Thomas et al. (1993) Biochemistry 32, 10923-10928]. This residue is located in an interhelical "loop" between transmembranous helices II and III, which contains six well-conserved residues (Asn124, Pro128, Gly132, Asp135, Pro139, and Asn142). Site-directed mutagenesis was performed to study the function of this entire domain. Nonconservative mutations of Asn124 and Asn142 also resulted in a loss of proton translocation, whereas their conservative substitution to glutamine had no effect. Mutations in eight other positions within this domain did not affect proton translocation. Introduction of an acidic group at positions 139 or 142, but not at eight other tested positions, restored proton pumping in the Asp135-->Asn mutated protein. These results suggest that the C-terminal part of the domain may be alpha-helical and that the entire "loop" plays an important structural and functional role as part of an input channel of the proton translocation machinery.

Amino Acid Sequence

The mechanism of proton translocation by the cytochrome system of mitochondria. Characterization of proton-transfer reactions associated with oxidoreductions of terminal respiratory carriers.

A direct kinetic analysis is presented of rapid proton-releasing reactions at the outer or C-side of the membrane, in ox heart and rat liver mitochondria, associated with aerobic oxidation of reduced terminal respiratory carriers in the presence of antimycin. Valinomycin plus K+ enhances the rate of cytochrome c oxidation and the rate and extent of H+ release. In the presence of valinomycin the leads to H+/e- ratio, computed on the basis of total electron flow from respiratory carriers to oxygen, varies with pH, remaining always lower than 1, and is unaffected by N-ethylmaleimide. 2-Heptyl-4-hydroxyquinoline N-oxide and 5-(n-undecyl)-6-hydroxy-4,7-dioxobenzothiazole, at concentrations which inhibit in the presence of antimycin the oxygen-induced reduction of b cytochromes, cause also a marked depression of the H+ release associated with aerobic oxidation of terminal respiratory carriers. Aerobic oxidation of the cytochrome system in mitochondria and of isolated b-c1 complex and cytochrome c oxidase results in scalar proton release from ionizable groups (redox Bohr effects). In mitochondria and submitochondrial particles, about 70% of the oxidoreductions of the components of the cytochrome system are linked to scalar proton transfer by ionizable groups. In isolated b-c1 complex scalar proton transfer, resulting from redox Bohr effect, amounts to 0.9H+ per Fe-S protein (190 muT). In isolated cytochrome c oxidase, Bohr protons amount to 0.8 per haem a + a3. The results presented indicate that the H+ release from mitochondria during oxidation of terminal respiratory carriers derives from residual antimycin-insensitive electron flow in the quinone-cytochrome c span and from redox Bohr effects in the b-c1 complex and cytochrome c oxidase. There is no sign of proton pumping by cytochrome oxidase during its transition from the reduced to the active 'pulsed' state and the first one or two turnovers.

Animals

Sugar specificity and sugar-proton interaction for the hexose-proton-symport system of Chlorella.

The substrate specificity of the glucose-proton symport system was studied to gain information about the spatial relationship between the binding sites for glucose and proton. Charged glucose analogues such as amino sugars or sugar acids were not transported by the uptake system, with the exception of 2-amino-2-deoxy-D-glucose. This glucosamine was taken up in the charged form in uniport mechanism, i.e. without symport of proton. This result was interpreted to mean that the proton-binding site of the symport system is close to the hydroxyl at carbon 2 of glucose. This interpretation was strengthened by the following facts: The steric position of hydroxyl groups at carbons 1, 2 or 3 of glucose were especially important for efficient transport. O-Methylation was not tolerated at carbon 1, but it was tolerated at carbons 3, 4 or 6. The stoichiometric flow of proton and sugar could be disturbed by removal of hydroxyl group at carbon 1 of glucose. The pH-dependence of sugar transport is sugar-specific, e.g. the amino group at carbon 2 of glucose improves transport at higher pH. The configuration at carbon 2 of glucose influences the specificity for the symported ion. It is concluded that the coupled flow of proton and glucose occurs by simultaneous coordinate movement of both in a transmembrane channel.

Biological Transport

Proton-sulfate cotransport: external proton activation of sulfate influx into human red blood cells.

Sulfate influx into human red blood cells was measured at 0 and 22 degrees C at several fixed external pH values between 3 and 10. These cells had normal internal pH and chloride concentrations so that sulfate influx was not limited by the efflux half-cycle reactions. The flux was a Michaelis-Menten function of sulfate concentration at each pH with K1/2SO4 = 4-10 mM. External protons activated influx 100-fold at a single site with a pK = 5.9 at 22 degrees C and 5.5 at 0 degrees C. This pK is similar to the value 5.99 +/- 0.3 for external proton binding to the sulfate-loaded transporter at 0 degrees C (J. Gen. Physiol. 79: 87-114, 1982). The flux was stilbene sensitive even in valinomycin-treated cells and was independent of membrane potential. This proton-activated influx appears to be proton-sulfate cotransport. At high pH there was a proton-independent flux that was membrane potential and stilbene sensitive. This proton-insensitive flux appears to be SO4(2-)/Cl- exchange or net sulfate influx. The sulfate influx over the entire pH range may be described in terms of an equation for the sum of the influxes through these two pathways on band 3.

Anion Transport Proteins

Individual assignments of amide proton resonances in the proton NMR spectrum of the basic pancreatic trypsin inhibitor.

Studies of proton-proton nuclear Overhauser effects were used to obtain individual assignments of 17 amide proton resonances in the 360 MHz proton nuclear magnetic resonance spectrum of the basic pancreatic trypsin inhibitor. First, optimizing the conditions for obtaining selective nuclear Overhauser effects in the presence of spin diffusion in macromolecules is discussed. Truncated driven nuclear Overhauser experiments were used to assing the amide proton resonances of the beta-sheet in the inhibitor. It is suggested that these techniques could serve quite generally to obtain individual resonance assignments in beta-sheet secondary structures of proteins. Combination of nuclear Overhauser studies with spin decoupling further resulted in individual assignments of the gamma-methyl resonances of the two isoleucines and numerous Calpha and Cbeta protons.

Amides

Affinities of the protonated and non-protonated forms of hyoscine and hyoscine N-oxide for muscarinic receptors of the guinea-pig ileum and a comparison of their size in solution with that of atropine.

1. At 37 degrees C in 0.1 M NaCl the pKa of hyoscine (10 mM) is 7.53; the non-protonated form has about one-tenth of the affinity (log K = 8.58) of the protonated form (log K = 9.58) for muscarine-sensitive receptors of the guinea-pig ileum at 37 degrees C. 2. In the same conditions the pKa of hyoscine N-oxide is 5.78 and the non-protonated form is inactive on the ileum whereas the protonated form is highly active with log K estimated to be 9.9, at least as active as hyoscine methobromide (log K = 9.85). 3. Hyoscine methobromide appears to occupy less space in water than atropine methobromide; hyoscine hydrochloride occupies less space than hyoscyamine hydrochloride: the non-protonated forms are slightly bigger. Hyoscine N-oxide hydrobromide is slightly smaller than hyoscine methobromide but the removal of the proton is accompanied by a reduction in volume, such as is seen with other zwitterions. 4. These differences in volume indicated a reduction in entropy on solution which may allow a greater increase in entropy on binding to receptors and hence greater affinity. The higher activity of hyoscine itself could also be due to the presence of the N-methyl group in the axial position, rather than equatorial as in hyoscyamine or atropine. 5. The different position of the N-methyl group may partly explain why the pKa of hyoscine is 2 units lower than that of hyoscyamine or atropine. It is also probable that the unionized form of hyoscine is stabilized by hydration. 6. Although hyoscine N-oxide is only weakly active at pH 7.6, it is present in a highly active form in the acid environment of the stomach and so might be expected to act selectively at this site.

Animals

CF0, the proton channel of chloroplast ATP synthase. After removal of CF1 it appears in two forms with highly different proton conductance.

The discharge of the flash-induced transmembrane voltage through the exposed proton channel, CF0, of the chloroplast ATP synthase, CF0CF1 was investigated. EDTA treatment of thylakoid membranes exposed approximately 50% of total CF0 by removal of the CF1 counterparts. This greatly accelerated the decay of the transmembrane voltage, as was apparent from electrochromic-absorption changes of intrinsic pigments and by pH-indicating-absorption changes of added dyes. Two decay processes were discernible, one rapid with a typical half-decay time of 2 ms, and a slower one with a half-decay time variable between 20-100 ms. Both were sensitive to CF0 inhibitors, but only the rapid decay process was also inhibited by added CF1. CF1 was effective in surprisingly small amounts, which were significantly lower than those previously removed by EDTA treatment. This finding corroborated our previous conclusion that the rapid decay of the transmembrane voltage was attributable to only a few high-conductance channels among many CF0 molecules, typically in the order of one channel/CF1-depleted EDTA vesicle. Inhibition of photophosphorylation in control thylakoids was measured as function of the concentration of CF0 inhibitors. It was compared with the inhibition of proton conduction through exposed CF0 in EDTA vesicles. Photophosphorylation and proton conduction by the high-conductance form of CF0 were inhibited by the same low inhibitor concentrations. This suggested that the high-conducting form of CF0 with a time-averaged single-channel conductance of 1 pS [Lill, H., Althoff, G. & Junge, W. (1987) J. Membrane Biol. 98, 69-78] represented the proton channel in the integral enzyme, which acted as a low-impedance access from the thylakoid lumen to the coupling site in CF0CF1. The slow decay process was attributed to a majority of low-conductance CF0 channels, i.e. about 50 molecules/vesicle. The conductance of these channels was more than 100-fold lower and they did not compete with the very few highly conducting channels for rebinding of added CF1. The low proton conduction of the majority of exposed CF0 molecules, possibly due to a structural rearrangement, may be protecting the thylakoid membrane against rapid energy dissipation caused by accidental loss of CF1. It may also explain the low single-channel conductance of bacterial F0 reported in the literature.

Binding Sites