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PubMed2001

Proton motion and proton transfer in the formamidine-formic acid complex: an Ab initio projector augmented wave molecular dynamics study.

An ab initio molecular dynamics study performed with the projector augmented wave method (PAW) on proton motion and (double) proton transfer in the formamidine-formic acid complex is reported. The PAW trajectories were calculated with a time interval of 0.12 fs, for a total evolution time period of 36ps, and for temperatures in the range 500-600 K. All proton-transfer processes start with a proton transition at the O-H...N group, and are followed by a second proton transition, either at the same group ("single crossing-recrossing transitions") or at the other group, namely the N-H...O group ("double proton transfers"). According to the delay between the two transitions (more or less than 15 fs), one may distinguish between "concerted" (42%) or "successive" (16%) single crossing-recrossing transitions, and between "simultaneous" (7%) or "successive" (35%) double proton transfers. Successive processes take place via a zwitterionic intermediate, which remains stable for up to approximately 120 fs ("ionic regions"). The findings are in excellent agreement with the results of ab initio (HF, MP2) and density functional theory (DFT; B3LYP, B3P86) calculations, according to which the zwitterionic intermediate that results from the first proton transition is a true local minimum. Furthermore, it is shown that the optimized geometries of stationary points (ground state, transition state, and zwitterion) comply well with corresponding average data obtained from the PAW trajectories for normal periods, crossover points, and ionic regions.

Journal Article↗

PubMed2001

Light-induced proton release and proton uptake reactions in the cyanobacterial phytochrome Cph1.

The P(r) to P(fr) transition of recombinant Synechocystis PCC 6803 phytochrome Cph1 and its N-terminal sensor domain Cph1Delta2 is accompanied by net acidification in unbuffered solution. The extent of this net photoreversible proton release was measured with a conventional pH electrode and increased from less than 0.1 proton released per P(fr) formed at pH 9 to between 0.6 (Cph1) and 1.1 (Cph1Delta2) H(+)/P(fr) at pH 6. The kinetics of the proton release were monitored at pH 7 and pH 8 using flash-induced transient absorption measurements with the pH indicator dye fluorescein. Proton release occurs with time constants of approximately 4 and approximately 20 ms that were also observed in parallel measurements of the photocycle (tau(3) and tau(4)). The number of transiently released protons per P(fr) formed is about one. This H(+) release phase is followed by a proton uptake phase of a smaller amplitude that has a time constant of approximately 270 ms (tau(5)) and is synchronous with the formation of P(fr). The acidification observed in the P(r) to P(fr) transition with pH electrodes is the net effect of these two sequential protonation changes. Flash-induced transient absorption measurements were carried out with Cph1 and Cph1Delta2 at pH 7 and pH 8. Global analysis indicated the presence of five kinetic components (tau(1)-tau(5): 5 and 300 micros and 3, 30, and 300 ms). Whereas the time constants were approximately pH independent, the corresponding amplitude spectra (B(1), B(3), and B(5)) showed significant pH dependence. Measurements of the P(r)/P(fr) photoequilibrium indicated that it is pH independent in the range of 6.5-9.0. Analysis of the pH dependence of the absorption spectra from 6.5 to 9.0 suggested that the phycocyanobilin chromophore deprotonates at alkaline pH in both P(r) and P(fr) with an approximate pK(a) of 9.5. The protonation state of the chromophore at neutral pH is therefore the same in both P(r) and P(fr). The light-induced deprotonation and reprotonation of Cph1 at neutral pH are thus due to pK(a) changes in the protein moiety, which are linked to conformational transitions occurring around 4 and 270 ms after photoexcitation. These transient structural changes may be relevant for signal transduction by this cyanobacterial phytochrome.

Bacterial Proteins↗

PubMed2004

Proton transfer to nickel-thiolate complexes. 2. Rate-limiting intramolecular proton transfer in the reactions of [Ni(SC(6)H(4)R-4)(PhP[CH(2)CH(2)PPh(2)](2))](+) (R = NO(2), Cl, H, Me, or MeO).

The protonation of [Ni(SC(6)H(4)R-4)(triphos)](+) (triphos = PhP[CH(2)CH(2)PPh(2)](2); R = NO(2), Cl, H, Me, or MeO) by [lutH](+) (lut = 2,6-dimethylpyridine) to form [Ni(S(H)C(6)H(4)R-4)(triphos)](2+) is an equilibrium reaction in MeCN. Kinetic studies, using stopped-flow spectrophotometry, reveal that the reactions occur by a two-step mechanism. Initially, [lutH](+) rapidly binds to the complex (K(2)(R)) in an interaction which probably involves hydrogen-bonding of the acid to the sulfur. Subsequent intramolecular proton transfer from [lutH](+) to sulfur (k(3)(R)) is slow because of both electronic and steric factors. The X-ray crystal structures of [Ni(SC(6)H(4)R-4)(triphos)](+) (R = NO(2), H, Me, or MeO) show that all are best described as square-planar complexes, with the phenyl substituents of the triphos ligand presenting an appreciable barrier to the approach of the sterically demanding [lutH](+) to the sulfur. The kinetic characteristics of the intramolecular proton transfer from [lutH](+) to sulfur have been investigated. The rate of intramolecular proton transfer exhibits a nonlinear dependence on Hammett sigma(+), with both electron-releasing and electron-withdrawing 4-R-substituents on the coordinated thiolate facilitating the rate of proton transfer (NO(2) > Cl > H > Me < MeO). The rate constants for intramolecular proton transfer correlate well with the calculated electron density of the sulfur. The temperature dependence of the rate of the intramolecular proton transfer reactions shows that deltaH() is small but increases as the 4-R-substituent becomes more electron-withdrawing [deltaH = 4.1 (MeO), 6.9 (Me), 11.4 kcal mol(-)(1) (NO(2))], while DeltaS() becomes progressively less negative [deltaS = -50.1 (MeO), -41.2 (Me), -16.4 (NO(2)) cal K(-)(1) mol(-)(1)]. Studies with [lutD](+) show that the rate of intramolecular proton transfer varies with the 4-R-substituent [(k(3)(NO)2)(H)/(k(3)(NO)2)(D) = 0.39; (k(3)(Cl))(H)/(k(3)(Cl))(D) = 0.88; (k(3)(Me))(H)/(k(3)(Me))(D) = 1.3; (k(3)(MeO))(H)/(k(3)(MeO))(D) = 1.2].

Journal Article↗

PubMed1999

Identification of the proton pathway in bacterial reaction centers: inhibition of proton transfer by binding of Zn2+ or Cd2+.

The reaction center (RC) from Rhodobacter sphaeroides converts light into chemical energy through the light induced two-electron, two-proton reduction of a bound quinone molecule QB (the secondary quinone acceptor). A unique pathway for proton transfer to the QB site had so far not been determined. To study the molecular basis for proton transfer, we investigated the effects of exogenous metal ion binding on the kinetics of the proton-assisted electron transfer kAB(2) (QA-*QB-* + H+ --> QA(QBH)-, where QA is the primary quinone acceptor). Zn2+ and Cd2+ bound stoichiometrically to the RC (KD </= 0.5 microM) and reduced the observed value of kAB(2) 10-fold and 20-fold (pH 8.0), respectively. The bound metal changed the mechanism of the kAB(2) reaction. In native RCs, kAB(2) was previously shown to be rate-limited by electron transfer based on the dependence of kAB(2) on the driving force for electron transfer. Upon addition of Zn2+ or Cd2+, kAB(2) became approximately independent of the electron driving force, implying that the rate of proton transfer was reduced (>/= 10(2)-fold) and has become the rate-limiting step. The lack of an effect of the metal binding on the charge recombination reaction D+*QAQB-* --> DQAQB suggests that the binding site is located far (>10 A) from QB. This hypothesis is confirmed by preliminary x-ray structure analysis. The large change in the rate of proton transfer caused by the stoichiometric binding of the metal ion shows that there is one dominant site of proton entry into the RC from which proton transfer to QB-* occurs.

Amino Acid Sequence↗

PubMed2003

A computer simulation study of the hydrated proton in a synthetic proton channel.

Classical molecular dynamics simulations using the multistate empirical valence bond model for aqueous proton transport were performed to characterize the hydration structure of an excess proton inside a leucine-serine synthetic ion channel, LS2. For such a nonuniform pore size ion channel, it is found that the Zundel ion (H(5)O(2)(+)) solvation structure is generally more stable in narrow channel regions than in wider channel regions, which is in agreement with a recent study on idealized hydrophobic proton channels. However, considerable diversity in the relative stability of the Zundel to Eigen cation (H(9)O(4)(+)) was observed. Three of the five wide channel regions, one located at the channel's center and the other two located near the channel mouths, are found to show extraordinary preference for the Eigen solvation structure. This implies that proton hopping is inhibited in these regions and therefore suggests that these regions may behave as barriers in the proton conducting pathway inside the channel. The proton solvation is also greatly influenced by the local molecular environment of the protein. In particular, the polar side chains of the Ser residues, which are intimately involved in the solvation structure, can greatly influence proton solvation. However, no preference of the influence by the various Ser side chains was found; they can either promote or prevent the formation of certain solvation structures.

Computer Simulation↗

PubMed1987

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↗

PubMed1975

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↗

PubMed2004

Theory and simulation of proton-coupled electron transfer, hydrogen-atom transfer, and proton translocation in proteins.

A theory of proton coupled electron transfer (PCET) is reviewed with application to charge transfer steps in the photosystem II oxygen-evolving complex (PSII/OEC). The relation between PCET when it is a concerted electron proton transfer (ETPT) process and hydrogen-atom transfer (HAT) reactions is discussed. Signatures expected for HAT reactions in terms of the size of the kinetic isotope effect and overall magnitude of the rate constant are discussed in the context of PSII/OEC. The formal similarity of ETPT to proton transfer and translocation is used to introduce a combined quantum mechanical (for the transferring protons) and molecular dynamics for the heavy-atom degrees of freedom approach. The method is used to examine double proton transfer in cytochrome c oxidase where two waters and a glutamate (Glu286) that is implicated in the proton translocation mechanism form a cyclic hydrogen bonded structure. Protonation of the glutamate is found to occur in agreement with experimental results.

Electron Transport↗

PubMed1993

Gaugement of the inner space of the apomyoglobin's heme binding site by a single free diffusing proton. I. Proton in the cavity.

Time resolved fluorimetry was employed to monitor the geminate recombination between proton and excited pyranine anion locked, together with less than 30 water molecules, inside the heme binding site of Apomyoglobin (sperm whale). The results were analyzed by a numerical reconstruction of the differential rate equation for time-dependent diffusion controlled reaction with radiating boundaries using N. Agmon's procedure (Huppert, Pines, and Agmon, 1990, J. Opt. Soc. Am. B., 7:1541-1550). The analysis of the curve provided the effective dielectric constant of the proton permeable space in the cavity and the diffusion coefficient of the proton. The electrostatic potential within the cavity was investigated by the equations given by Gilson et al. (1985, J. Mol. Biol., 183:503-516). According to this analysis the dielectric constant of the protein surrounding the site is epsilon prot < or = 6.5. The diffusion coefficient of the proton in the heme binding site of Apomyoglobin-pyranine complex is D = 4 x 10(-5) cm2/s. This value is approximately 50% of the diffusion coefficient of proton in water. The lower value indicates enhanced ordering of water in the cavity, a finding which is corroborated by a large negative enthropy of binding delta S0 = -46.6 cal.mole-1 deg-1. The capacity of a small cavity in a protein to retain a proton had been investigated through the mathematical reconstruction of the dynamics. It has been demonstrated that Coulombic attraction, as large as delta psi of energy coupling membrane, is insufficient to delay a free proton for a time frame comparable to the turnover time of protogenic sites.

Animals↗

PubMed1993

Gaugement of the inner space of the apomyoglobin's heme binding site by a single free diffusing proton. II. Interaction with a bulk proton.

The reaction mechanism and the dynamic aspects of protonation of a defined moiety located inside an aqueous cavity in a protein were monitored by time resolved spectroscopy using the pyranine apomyoglobin complex as a model (Shimoni, Tsfadia, Nachliel, and Gutman, 1993, Biophys. J. 64:472-479). The reaction was synchronized by a short laser pulse and the reprotonation of the ground state pyranine anion (phi O-) was monitored, in the microsecond time scale, by its transient absorption at 457 nm. The observed signal was reconstructed by a numeric solution of nonlinear, coupled differential equations which account for the direct reaction of phi O- with bulk proton and by proton transfer from the nearby amino acids: His 64, Asp 44, Asp 60, and Glu 59. A unique combination of rate constant was obtained which quantitates the contribution of each pathway to the overall relaxation process. In the first phase of the dynamics phi O- abstracts a proton from the nearby protonated histidine. The bulk proton interacts preferentially with the cluster of three carboxylates and immediately shuttled to the deprotonated histidine. The high proximity of the reactive groups and the strong electrostatic forces operating inside the heme binding cavity render the rate of proton transfer in the site ultrafast.

Animals↗

PubMed2002

Pulsed EPR studies of nonexchangeable protons near the Mo(V) center of sulfite oxidase: direct detection of the alpha-proton of the coordinated cysteinyl residue and structural implications for the active site.

Pulsed electron nuclear double resonance (ENDOR) spectra of nonexchangeable protons in the vicinity of the Mo(V) center of the high pH (hpH) and low pH (lpH) forms of native chicken liver sulfite oxidase (SO) and recombinant human SO have been obtained and analyzed for the first time. The close similarity of the spectra for the chicken and human enzymes indicates that the structures of their molybdenum centers are essentially identical. For lpH SO, the closest nonexchangeable proton is found to be approximately 2.8 A from the Mo atom. To more accurately determine the distance to this proton and facilitate its assignment, the C-band electron spin-echo envelope modulation (ESEEM) spectra of lpH SO were also analyzed. From the obtained distance and comparison with the X-ray structure, this closest nonexchangeable proton is assigned to the alpha-proton of the coordinated conserved cysteinyl residue (Cys185 in chicken, Cys207 in human). The closest Mo...H distance for the nonexchangeable protons of hpH SO is found to be approximately 3.3 A. For the cysteinyl alpha-proton, such an increase in the Mo...H distance only requires a very small change in torsional angles. This study demonstrates that details of the enzyme structural rearrangements with pH can be monitored by ENDOR spectroscopy and suggests that a similar approach may be routinely used to probe the orientation of the coordinated cysteinyl residue in mutant forms of SO that are catalytically compromised.

Animals↗

PubMed2006

Monte Carlo simulations of proton pumps: on the working principles of the biological valve that controls proton pumping in cytochrome c oxidase.

Gaining a detailed understanding of the proton-pumping process in cytochrome c oxidase (COX) is one of the challenges of modern biophysics. Recent mutation experiments have highlighted this challenge by showing that a single mutation (the N139D mutation) blocks the overall pumping while continuing to channel protons to the binuclear center without inhibiting the oxidase activity. Rationalizing this result has been a major problem because the mutation is quite far from E286, which is believed to serve as the branching point for the proton transport in the pumping process. In the absence of a reasonable explanation for this important observation, we have developed a Monte Carlo simulation method that can convert mutation and structural information to pathways for proton translocation and simulate the pumping process in COX on a millisecond and even subsecond time scale. This tool allows us to reproduce and propose a possible explanation to the effect of the N139D mutation and to offer a consistent model for the origin of the "valve effect" in COX, which is crucial for maintaining uphill proton pumping. Furthermore, obtaining the first structure-based simulation of proton pumping in COX, or in any other protein, indicates that our approach should provide a powerful tool for verification of mechanistic hypotheses about the action of proton transport proteins.

Biophysical Phenomena↗

PubMed2003

Redox-coupled proton translocation in biological systems: proton shuttling in cytochrome c oxidase.

In the respiratory chain free energy is conserved by linking the chemical reduction of dioxygen to the electrogenic translocation of protons across a membrane. Cytochrome c oxidase (CcO) is one of the sites where this linkage occurs. Although intensively studied, the molecular mechanism of proton pumping by this enzyme remains unknown. Here, we present data from an investigation of a mutant CcO from Rhodobacter sphaeroides [Asn-139 --> Asp, ND(I-139)] in which proton pumping is completely uncoupled from the catalytic turnover (i.e., reduction of O2). However, in this mutant CcO, the rate by which O2 is reduced to H2O is even slightly higher than that of the wild-type CcO. The data indicate that the disabling of the proton pump is a result of a perturbation of E(I-286), which is located 20 A from N(I-139) and is an internal proton donor to the catalytic site, located in the membrane-spanning part of CcO. The mutation results in raising the effective pKa of E(I-286) by 1.6 pH units. An explanation of how the mutation uncouples catalytic turnover from proton pumping is offered, which suggests a mechanism by which CcO pumps protons.

Amino Acid Substitution↗

PubMed1986

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↗

PubMed1989

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↗

PubMed1994

The differences in the T2 relaxation rates of the protons in the partially-deuteriated and fully protonated sugar residues in a large oligo-DNA ('NMR-window') gives complementary structural information.

Selective incorporation of the stereospecifically deuteriated sugar moieties (> 97 atom % 2H enhancements at H2', H2'', H3' and H5'/5'' sites, approximately 85 atom % 2H enhancement at H4' and approximately 20 atom % 2H enhancement at H1') in DNA and RNA by the 'NMR-window' approach has been shown to solve the problem of the resonance overlap [refs. 1, 2 & 3]. Such specific deuterium labelling gives much improved resolution and sensitivity of the residual sugar proton (i.e. H1' or H4') vicinal to the deuteriated centers (ref. 3). The T2 relaxation time of the residual protons also increases considerably in the partially-deuteriated (shown by underline) sugar residues in dinucleotides [d(CpG), d(GpC), d(ApT), d(TpA)], trinucleotide r(A2'p5'A2'p5'A) and 20-mer DNA duplex 5'd(C1G2C3-G4C5G6C7G8A9A10T11T12C13G14C15G16C17G18C19G20)(2) 3'. The protons with shorter T2 can be filtered away using a number of different NMR experiments such as ROESY, MINSY or HAL. The NOE intensity of the cross-peaks in these experiments includes only straight pathway from H1' to aromatic proton (i-i and i-i + 1) without any spin-diffusion. The volumes of these NOE cross-peaks could be measured with high accuracy as their intensity is 3 to 4 times larger than the corresponding peaks in the fully protonated residues in the normal NOESY spectra. The structural informations thus obtainable from the residual protons in the partially-deuteriated part of the duplex and the fully protonated part in the 'NMR window' can indeed complement each other.

Base Composition↗

PubMed1995

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↗

PubMed1999

Intramolecular proton transfers in stereoisomeric gas-phase ions and the kinetic nature of the protonation process upon chemical ionization

The isobutane chemical ionization (CI) mass spectra of cis- and trans-1-butyl-3- and -4-dimethylaminocyclohexanols and of their methyl ethers exhibit abundant [MH - H(2)O](+) and [MH - MeOH](+) ions respectively. On the other hand, only the MH(+) ions of the cis-isomers exhibit significant [MH - H(2)O](+) and [MH - MeOH](+) ions under collision-induced dissociation (CID) conditions. The non-occurrence of water and methanol elimination in the CID spectra of the trans-isomers indicates retention of the external proton at the dimethylamino group in the MH(+) ions that survive after leaving the ion source and the first quadrupole of the triple-stage quadrupole ion separating system, and the trans-orientation of the two basic sites does not allow proton transfer from the dimethylamino group to the hydroxyl or methoxyl. Such transfer is allowed in the cis-amino alcohols and amino ethers via internal hydrogen-bonded (proton-bridged) structures, resulting in the elimination of water and methanol from the surviving MH(+) ions of these particular stereoisomers upon CID. The abundant [MH - ROH](+) ions in the isobutane-CI mass spectra of the trans-isomers indicates protonation at both basic sites, affording two isomeric MH(+) ions in each case, one protonated at the dimethylamino group and the other at the less basic oxygen function. These results show that the isobutane-CI protonation of the amino ethers and amino alcohols is a kinetically controlled process, occurring competitively at both basic sites of the molecules, despite the large difference between their proton affinities ( approximately 25 and approximately 35 kcal mol(-1); 1 kcal = 4.184 kJ). Copyright 1999 John Wiley & Sons, Ltd.

Journal Article↗