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The Proton

At a given velocity, these probabilities are uniquely determined from this equation subject to the normalization [Pg.44]


Figure Al.4.1. A PH molecule at equilibrium. The protons are labelled 1, 2 aud 3, respectively, aud the phosphorus uucleus is labelled 4. Figure Al.4.1. A PH molecule at equilibrium. The protons are labelled 1, 2 aud 3, respectively, aud the phosphorus uucleus is labelled 4.
The tliree protons in PH are identical aud indistinguishable. Therefore the molecular Hamiltonian will conmuite with any operation that pemuites them, where such a pemiutation interchanges the space and spin coordinates of the protons. Although this is a rather obvious syimnetry, and a proof is hardly necessary, it can be proved by fomial algebra as done in chapter 6 of [1]. [Pg.142]

Hj, H2 and H. The pemuitation (12) (where S denotes space-fixed position labels) is defined in this approach as pemuiting the nuclei that are in positions 1 and 2, and the pemuitation (123) as replacing the proton in position 1 by the proton in position 2 etc. With this definition the effect of first doing (12) and then doing (123) can be drawn as... [Pg.144]

If we were to define the operations of the point group as also rotating and reflecting the (p.q.r) axis system (in which case the axes would be tied to the positions of the nuclei), we would obtain a different multiplication table. We could call this the nuclear-fixed axis convention. To implement this the protons in the o, O2 and planes in figure Al.4.2 would be numbered H, H2 and respectively. With this convention the operation would move the a plane to the position in space originally occupied by the 02 plane. If we follow such a C3 operation by the reflection (in the plane containing Ft ) we find that, in the nuclear-fixed axis convention ... [Pg.146]

One anomaly inmrediately obvious from table A2.4.2 is the much higher mobilities of the proton and hydroxide ions than expected from even the most approximate estimates of their ionic radii. The origin of this behaviour lies in the way hr which these ions can be acconmrodated into the water structure described above. Free protons cannot exist as such in aqueous solution the very small radius of the proton would lead to an enomrous electric field that would polarize any molecule, and in an aqueous solution the proton inmrediately... [Pg.574]

The complete hydration shell of the proton consists of both the central FI O unit and fiirther associated water molecules mass spectrometric evidence would suggest that a total of four water molecules fomr the actual FIgOj unit, givmg a hydration number of four for the proton. Of course, the measurement of this number by... [Pg.574]

The enthalpy for this process is the proton affinity of the negative ion. [Pg.815]

After some straightforward manipulations of A3.8.22. the PI-QTST estimate of the proton transfer rate constant can be shown to be given by 48... [Pg.894]

Figure A3.8.3 Quantum activation free energy curves calculated for the model A-H-A proton transfer reaction described 45. The frill line is for the classical limit of the proton transfer solute in isolation, while the other curves are for different fully quantized cases. The rigid curves were calculated by keeping the A-A distance fixed. An important feature here is the direct effect of the solvent activation process on both the solvated rigid and flexible solute curves. Another feature is the effect of a fluctuating A-A distance which both lowers the activation free energy and reduces the influence of the solvent. The latter feature enliances the rate by a factor of 20 over the rigid case. Figure A3.8.3 Quantum activation free energy curves calculated for the model A-H-A proton transfer reaction described 45. The frill line is for the classical limit of the proton transfer solute in isolation, while the other curves are for different fully quantized cases. The rigid curves were calculated by keeping the A-A distance fixed. An important feature here is the direct effect of the solvent activation process on both the solvated rigid and flexible solute curves. Another feature is the effect of a fluctuating A-A distance which both lowers the activation free energy and reduces the influence of the solvent. The latter feature enliances the rate by a factor of 20 over the rigid case.
Collision-induced dissociation mass spectrum of tire proton-bound dimer of isopropanol [(CH2)2CHOH]2H. The mJz 121 ions were first isolated in the trap, followed by resonant excitation of their trajectories to produce CID. Fragment ions include water loss mJz 103), loss of isopropanol mJz 61) and loss of 42 anui mJz 79). (b) Ion-molecule reactions in an ion trap. In this example the mJz 103 ion was first isolated and then resonantly excited in the trap. Endothennic reaction with water inside the trap produces the proton-bound cluster at mJz 121, while CID produces the fragment with mJz 61. [Pg.1350]

In an earlier section, measurements were described in which the equilibrium constant, K, for bimolecular reactions involving gas-phase ions and neutral molecules were detennined. Another method for detemiining the proton or other affinity of a molecule is the bracketing method [ ]. The principle of this approach is quite straightforward. Let us again take the case of a proton affinity detemiination as an example. In a reaction... [Pg.1358]

For some experiments, the solar neutrino flux and the rate of decay of the proton being extreme examples, tire count rate is so small that observation times of months or even years are required to yield rates of sufficiently small relative uncertainty to be significant. For high count rate experiments, the limitation is the speed with which the electronics can process and record the incoming infomiation. [Pg.1422]

Figure B2.4.1 illustrates this type of behaviour. If there is no rotation about the bond joining the N, N -dimethyl group to the ring, the proton NMR signals of the two methyl groups will have different chemical shifts. If the rotation were very fast, then the two methyl enviromnents would be exchanged very quickly and only a single, average, methyl peak would appear in the proton NMR spectrum. Between these two extremes, spectra like those in figure B2.4.1 are observed. At low temperature, when the rate is slow, two... Figure B2.4.1 illustrates this type of behaviour. If there is no rotation about the bond joining the N, N -dimethyl group to the ring, the proton NMR signals of the two methyl groups will have different chemical shifts. If the rotation were very fast, then the two methyl enviromnents would be exchanged very quickly and only a single, average, methyl peak would appear in the proton NMR spectrum. Between these two extremes, spectra like those in figure B2.4.1 are observed. At low temperature, when the rate is slow, two...
Gutman M 1986 Application of the laser-induced proton pulse for measuring the protonation rate constants of specific sites on proteins and membranes Methods Enzymol. 127 522-38... [Pg.2969]

We further make the following tentative conjecture (probably valid only under restricted circumstances, e.g., minimal coupling between degrees of freedom) In quantum field theories, too, the YM residual fields, A and F, arise because the particle states are truncated (e.g., the proton-neutron multiplet is an isotopic doublet, without consideration of excited states). Then, it is within the truncated set that the residual fields reinstate the neglected part of the interaction. If all states were considered, then eigenstates of the form shown in Eq. (90) would be exact and there would be no need for the residual interaction negotiated by A and F. [Pg.158]

H at m energy of 1.2 eV in the center-of-mass frame. By using an atomic orbital basis and a representation of the electronic state of the system in terms of a Thouless determinant and the protons as classical particles, the leading term of the electronic state of the reactants is... [Pg.231]

The strongly electronegative (p. 49) chlorine atom becomes a chloride ion, the proton accepting the electron pair donated by the nitrogen atom. A similar reaction occurs when ammonia is passed into water, but to a much lesser extent as oxygen in water is a poorer donor of the electron pair ... [Pg.43]

This is an exothermic process, due largely to the large hydration enthalpy of the proton. However, unlike the metallic elements, non-metallic elements do not usually form hydrated cations when their compounds dissolve in water the process of hydrolysis occurs instead. The reason is probably to be found in the difference in ionisation energies. Compare boron and aluminium in Group III ... [Pg.80]

Towards a simple Lewis base, for example the proton, phosphine is a poorer electron donor than ammonia, the larger phosphorus atom being less able to form a stable covalent bond with the acceptor atom or molecule. Phosphine is, therefore, a much weaker base than ammonia and there is no series of phosphonium salts corresponding to the ammonium salts but phosphonium halides. PH4X (X = Cl, Br, I) can be prepared by the direct combination of phosphine with the appropriate hydrogen halide. These compounds are much more easily dissociated than ammonium halides, the most stable being the iodide, but even this dissociates at 333 K PH4I = PH3 -t- HI... [Pg.226]

The other halides dissociate at lower temperatures and, if put into water, all are decomposed, the proton transferring to water which is a better electron pair donor ... [Pg.226]

Pure sulphuric acid is a true acid. In dilute aqueous solution, sulphuric acid is an acid because the solvent water has an affinity for the proton ... [Pg.302]

Thus water is available to take the proton, and HjSjO, to lose it, even in the pure ... [Pg.302]


See other pages where The Proton is mentioned: [Pg.90]    [Pg.207]    [Pg.295]    [Pg.314]    [Pg.332]    [Pg.26]    [Pg.126]    [Pg.141]    [Pg.156]    [Pg.156]    [Pg.574]    [Pg.574]    [Pg.814]    [Pg.818]    [Pg.895]    [Pg.1359]    [Pg.1479]    [Pg.1507]    [Pg.1508]    [Pg.1509]    [Pg.1515]    [Pg.1569]    [Pg.2091]    [Pg.232]    [Pg.78]    [Pg.116]    [Pg.145]    [Pg.240]    [Pg.328]   


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A Equilibria between Isomeric Ions Differing in the Site of Proton Attachment

Anhydrase Shuttling the Protons

Carbocation Generation The Role of Protonation

Complications Caused by Protonation at the Wrong Site

Conjugate acid The species formed when proton is added to a base

Conjugate acid-base pair Two species related to each other by the donating and accepting of a single proton

Current, Poor Proton Transport in the CCL

Electron Transport Creates an Electrochemical Potential Gradient for Protons across the Inner Membrane

Excited State Proton Transfer (ESPT) from the Neutral Chromophore

Experiments for the Direct Observation of Proton Spin-Diffusion

Formation of the Boundary Layer Enriched in Protons

Ground State Protonation Equilibria of the AvGFP Chromophore

Hypothesis on the Mechanism of Proton Transport in Biological Membranes

Incoherent neutron scattering studies of proton conductors from the anhydrous solid state to aqueous solutions

Measuring the true proton conductivity

NMR of water protons (the enhancement factor)

Nuclei other than the proton

On the mechanism of proton translocation

One More Step in Understanding Proton Mobility The Conway, Bockris, and Linton (CBL) Theory

Oxyacid An acid in which the acidic proton

PROTON TRANSFER AND THE PRINCIPLES OF STABILITY

Physical nature of the solvent induced proton transfer

Proton Abstraction Monosubstitution of the Aryne

Proton Binding The Simplest Cation

Proton Donors on the Cationic Polymerization of Epoxides

Proton NMR Spectrum of the Model Compound

Proton Transfer Reactions and the EVB Model

Proton Transfer The ESIPT Mechanism

Proton Transfer as the Rate-Determining Step

Proton Transfer in Systems with the Intramolecular Hydrogen Bonding

Proton Transfer in the Solid State

Proton Transfer to a Hydridic Hydrogen in the Solid State

Proton Transfers in the Electronic Excited State

Proton Transport Near the Polymer-Water Interface

Proton tautomerism in the solid state

Proton the methylene

Proton transfer in condensed phases beyond the quantum

Proton transfer in the ground state

Proton transfer reactions in the excited state

Proton transfers in the transition state

Proton translocation models directly involving the Schiff base nitrogen

Protonation of the

Protonation of the Coordinated Dinitrogen

Protonation of the coordinated

Protonation of the heteroatom

Protonation reactions (and the formation of adducts)

Protonation states of the ASP 25, 125 dyad

Protonation-induced Intramolecular Electron Transfer in the Ferrocene-Quinone Conjugated System

Protonic and Electronic Conductivity in the Catalyst Layer

Regions of the proton NMR spectrum

Reversal electron current against the proton motion

Solvent and Concentration Dependence of the 7-Proton Resonance

Synthetic applications of the aqueous aza Diels-Alder reaction involving simple protonated iminium ions

Synthetic applications of the aqueous aza Diels-Alder reaction with protonated C-acyl iminium ions

Synthetic applications of the asymmetric aqueous aza Diels-Alder reaction with simple protonated iminium ions

THE ATOMIC NUCLEUS IS MADE OF PROTONS AND NEUTRONS

The Atom Protons, Electrons, and Neutrons

The Attached Proton Test (APT)

The Bronsted Acidity of Protonic Zeolites

The Choice of Dielectric Constant Proton Binding as a Paradigm

The Dynamics of Proton Transfers

The Effect of Fluorine Substituents on Proton Chemical Shifts

The Effect of Proton (Cation) Exchange Level

The First 2-Electron-2-Proton Transfer

The NOE Through-Space Interactions between Protons

The Properties of Protons, Neutrons, and Electrons

The Proton Condition

The Proton Crystal Model

The Proton Exchange Membrane

The Proton Exchange Membrane Fuel Cell (PEMFC)

The Proton Transfer Concept

The Proton as a Different Sort of Ion

The Proton-Promoted Dissolution Reaction

The Protonation Mechanism of Ferric-Dioxygen (5) to Cpd

The Protonic Concept

The Quantum Character of Proton Transfer

The Search for a Protonated Cyclopropyl Ring

The Stability of a Nucleus Is Determined Primarily by Its Neutron-to-Proton Ratio

The Tunnelling Mechanism in Proton Transfer Reactions

The differences between carbon and proton NMR

The energy-transducing membrane is topologically closed and has a low proton permeability

The extent of protonation and deprotonation

The free proton

The hydrogen ion (proton)

The ipso protonation

The isotropic proton

The lone proton migration mechanism (translocation)

The p-process (proton capture)

The partial-proton-transfer concept

The proton circuit

The proton donor-acceptor concept of acids and bases

The proton pump

The proton-ATPase complex

The protonated species of water

The protonation of anthracene anion radical by phenol

The structures of protonated carboxylic acids and esters

Trace Element Analysis is Possible with the Proton Probes

Two views on the protonation regioselectivity

Using NMR Spectra to Analyze Molecular Structure The Proton Chemical Shift

Validity of the WKB Tunneling Probability Expression for Proton Transfer

Via rate-limiting proton transfer to give the phenolate

Weathering and the Environmental Proton Balance

Who Gets the Proton

Zero proton condition at the surface

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