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Charged species

A large number of studies in the last decade have been concerned with primary processes in irradiated polymers. Unstable intermediates have been trapped and identified at low temperatures or detected by pulse radiolysis. In some cases, reactions of these intermediates have been identified and workers have attempted to correlate such reactions with the chemical effects of irradiation observed at room temperature. Some of the conclusions drawn will be summarized below. The elementary processes during irradiation at 77°K will be discussed first. The reactions of charged species, excited states and neutral radicals will be outlined successively. [Pg.316]

Electrons formed by ionization of the matrix by 7-photons or electrons according to [Pg.316]

A hydrogen atom or a fragment of side-group can be detached by a reaction similar to (74). Reaction of with the matrix can induce decomposition, e.g. [Pg.317]

If the parent cation is unstable, it can decompose into smaller fragments at 77°K before electron—cation recombination. Such a mechanism has been proposed for the formation of volatile products resulting from side-group scission in polymethylmethacrylate, viz. [Pg.317]

The fate of the electron can now be considered. If is stable and if the electron is physically trapped or forms stable anions according to [Pg.318]

With respect to ion-molecule reactions, the development of pulsed supersonic flows in Rennes (see Section 2.6.5) will also offer the possibility of achieving very low pressures in the supersonic flow and therefore will open the way to a revival of the ion-molecule CRESU apparatus by the use of a selective injection of ions which will be directly derived from expertise gained previously. Studies at temperatures close to 1K will be a decisive test in comparing present collision theories and are obviously of major importance. [Pg.110]


The chemical potential pi, has been generalized to the electrochemical potential Hj since we will be dealing with phases whose charge may be varied. The problem that now arises is that one desires to deal with individual ionic species and that these are not independently variable. In the present treatment, the difficulty is handled by regarding the electrons of the metallic phase as the dependent component whose amount varies with the addition or removal of charged components in such a way that electroneutrality is preserved. One then writes, for the ith charged species. [Pg.196]

One fascinating feature of the physical chemistry of surfaces is the direct influence of intermolecular forces on interfacial phenomena. The calculation of surface tension in section III-2B, for example, is based on the Lennard-Jones potential function illustrated in Fig. III-6. The wide use of this model potential is based in physical analysis of intermolecular forces that we summarize in this chapter. In this chapter, we briefly discuss the fundamental electromagnetic forces. The electrostatic forces between charged species are covered in Chapter V. [Pg.225]

Migration is the movement of ions due to a potential gradient. In an electrochemical cell the external electric field at the electrode/solution interface due to the drop in electrical potential between the two phases exerts an electrostatic force on the charged species present in the interfacial region, thus inducing movement of ions to or from the electrode. The magnitude is proportional to the concentration of the ion, the electric field and the ionic mobility. [Pg.1925]

Charged species are not a special case in RAMSES. As ean be seen from Figure 2-57, rr-electron systems can accommodate any number of electrons between zero and two times the number of atoms involved. [Pg.67]

Figure 2-57. Charged species and radicals are represented as T-systems,... Figure 2-57. Charged species and radicals are represented as T-systems,...
Atoms combine with one another to give compounds having properties different from the atoms they contain The attractive force between atoms m a compound is a chemical bond One type of chemical bond called an ionic bond, is the force of attraction between oppositely charged species (ions) (Figure 1 4) Ions that are positively charged are referred to as cations, those that are negatively charged are anions... [Pg.10]

Solvent Effects on the Rate of Substitution by the S l Mechanism Table 8 6 lists the relative rate of solvolysis of tert butyl chloride m several media m order of increasing dielectric constant (e) Dielectric constant is a measure of the ability of a material m this case the solvent to moderate the force of attraction between oppositely charged par tides compared with that of a standard The standard dielectric is a vacuum which is assigned a value e of exactly 1 The higher the dielectric constant e the better the medium is able to support separated positively and negatively charged species 8olvents... [Pg.345]

Electron distribution governs the electrostatic potential of molecules. The electrostatic potential describes the interaction of energy of the molecular system with a positive point charge. Electrostatic potential is useful for finding sites of reaction in a molecule positively charged species tend to attack where the electrostatic potential is strongly negative (electrophilic attack). [Pg.135]

Capillary zone electrophoresis provides effective separations of any charged species, including inorganic anions and cations, organic acids and amines, and large biomolecules such as proteins. For example, CZE has been used to separate a mixture of 36 inorganic and organic ions in less than 3 minutes.Neutral species, of course, cannot be separated. [Pg.606]

Thus two electrons exit the reaction zone, leaving a positively charged species (M ) called an ion (in this case, a molecular ion). Strictly, M" is a radical-cation. This electron/molecule interaction (or collision) was once called electron impact (also El), although no impact actually occurs. [Pg.13]

A further consequence of the high temperatures is that much of the sample is simply evaporated without producing isolated positive ions. There is a competition between formation of positive ions and the evaporation of neutral particles. Since the mass spectrometer examines only isolated charged species, it is important for maximum sensitivity that the ratio of positive ions to neutrals be as large as possible. Equation 7.1 governing this ratio is given here. [Pg.46]

The kinetic or translational energy of the ions is equal to the work done on moving the charged species through the potential, V, i.e., l/2mjVi = zV and l/2m2V2 = zV, where z is the charge on the ions and Vj, V2 are their final velocities. From this, we obtain Equations 33.1 and 33.2. [Pg.232]

Since a discharge is characterized by having a substantial population of charged species (electrons and ions), it responds to an applied electromagnetic field. The applied field moves electrons in one direction and positive ions in the opposite direction, in accordance with Maxwell s laws. [Pg.388]

Plasma consists of a gaseous mixture of neutral species, ions, and electrons. The charged species are in approximately equal concentrations. [Pg.394]

Magnetic/electric-sector instruments are used to manipulate ion beams by making use of the deflection of charged species (ions) in magnetic or electric fields. [Pg.401]

Positive or negative ions (electrically charged species) from a source are injected along the central axis of the quadrupole assembly. [Pg.405]

Ion/neutral reaction. Interaction of a charged species with a neutral reactant to produce either chemically different species or changes in the internal energy of one or both of the reactants. [Pg.444]


See other pages where Charged species is mentioned: [Pg.79]    [Pg.79]    [Pg.206]    [Pg.207]    [Pg.208]    [Pg.573]    [Pg.1944]    [Pg.2418]    [Pg.2724]    [Pg.27]    [Pg.67]    [Pg.252]    [Pg.135]    [Pg.205]    [Pg.220]    [Pg.254]    [Pg.348]    [Pg.173]    [Pg.199]    [Pg.71]    [Pg.40]    [Pg.87]    [Pg.88]    [Pg.151]    [Pg.151]    [Pg.175]    [Pg.183]    [Pg.399]    [Pg.438]    [Pg.61]    [Pg.152]   
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See also in sourсe #XX -- [ Pg.183 ]

See also in sourсe #XX -- [ Pg.115 ]

See also in sourсe #XX -- [ Pg.183 ]

See also in sourсe #XX -- [ Pg.32 ]

See also in sourсe #XX -- [ Pg.320 ]




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Atomic species electrical charge

Charge of the species

Charge transfer redox species

Charge-separated species

Charged Dioxygen Species

Charged Species Flow

Charged carotenoid species

Charged complex species

Charged species INDEX

Charged species electrostatic adsorption

Charged species thin-film model

Charged species transport

Charged species transport discrimination

Charged species, separation using

Charged species, transport, plasma

Charged species, transport, plasma processes

Crystal, charge-carrying species

Diffusion of charged species

Double charged species

ELECTRICAL METHODS FOR CHARGED SPECIES

Electrochemical recognition of charged and neutral guest species by redox-active

Electrochemical recognition of charged and neutral guest species by redox-active receptor

Electrochemical recognition of charged and neutral guest species by redox-active receptor molecules

Electrocyclic reactions of charged species

Formation and Stability of Charged Diatomic Species

From Charged to Well-Defined Species The Electrochemical Equilibrium

Hydrocarbon species, charged

Ion charged species

Irradiated charged species

Multi-charged cationic species

Multiply charged species

Nature of the Reagent Neutral or Charged Species

Negatively Charged Species with Metal Cations

Negatively charged species

Nitrogen positively-charged species

Oxides, Hydroxides, Hydrides, and Doubly Charged Species

Oxygen positively-charged species

Partially charged species

Partition coefficients charged-species partitioning

Plasma Species and Factors Active for Sterilization Direct Effect of Charged Particles

Polymers charged species

Positively charged species

Probability of Exit Boundary Charged Species

Reaction Kinetics Involving Charged Species

Reactions of Charged Species in Solution

Receptor molecules, redox-active, electrochemical recognition of charged and neutral guest species

Recognising multiply charged species

Recombination of Charged Species

SURFACE CHARGING IN ABSENCE OF STRONGLY ADSORBING SPECIES

Situation 1 Mean Exit Time for Charged Species

Stabilisation of charged species

Static electricity charged species concentration

Steady State Scavenging Rate for Charged Species

Surfactant interactions with oppositely charged species

The chemical potential of charged species

Thermodynamics charged species transport

Thermodynamics of charged species transport

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