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chemical physics of discharges - Argonne National Laboratory

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35<br />

must be added to the Langevin cross section. Here is dipole moment and Etis the<br />

translational energy <strong>of</strong> the reacting system in center <strong>of</strong> mass coordinates.<br />

NO attempt will be made here to review all <strong>of</strong> the studies <strong>of</strong> the effect <strong>of</strong> energy<br />

upon the rates <strong>of</strong> ion-molecule reactions. However, several investigators who have<br />

made especially important contributions should be mentioned. In addition to the<br />

work <strong>of</strong> Hamill discussed above, important studies have been made by Futrell and<br />

Abramson (70), Giese and Maier (71), Friedman (72,73) and Light and Horrocks(74).<br />

- -- --<br />

(70) J. H. Futrell and F. P. Abramson, "Ion-Molecule Reactions in the Gas Phase,"<br />

Adv. in Chem. Series 58, Amer. Chem. SOC., 1966, p. 107.<br />

(71) C. F. Giese and W. B.xaier, J. Chem. Phys. 39, - 197, 739 (1963)<br />

(72) T. F. Moran and L. Friedman, J. Chem. Phys. 39, 2491 (1963); 62, 2391 (1965) - -<br />

(73) F. S. Klein and L. Friedman, J. Chem. Phys. 4l, 1789 (1964)<br />

(74) J. C. Light and J. Horrocks, Proc. Phys. 527 (1964)<br />

It should be pointed out that if the relative velocities <strong>of</strong> ions and neutrals<br />

become sufficiently high other reactions begin to OCCUL as a result <strong>of</strong> the different<br />

forces coming into play. Thus a fast moving ion passing a molecule with sufficient<br />

velocity may simply strip <strong>of</strong>f a peripheral atom, leaving the partially denuded entity<br />

behind. Such stripping reactions have been studied by Henglein (75) and Koski<br />

(76), who found that they obey quite different rules from those above. It thus<br />

(75) A. Henglein, "Ion Molecule Reactions in the Gas Phase," &. in Chem. Series<br />

- 58, Amer, Chem. SOC., Washington, D. C.,' p. 63<br />

-<br />

(76) M. A. Berta, B. Y. Ellis and W. S. Koski, ibid., p. 80<br />

appears that a complete theory <strong>of</strong> the rates <strong>of</strong> ion-molecule reactions has not been<br />

developed, but there is little doubt that to a first approximation the equation <strong>of</strong><br />

Gioumousis and Stevenson givsfairly good results. It is also true that the<br />

reactions tend to be quite fast, and this becomes a matter <strong>of</strong> overriding importance<br />

in many processes involving ions. Thus is has been shown by Lampe (77,78) and by<br />

Futrell (79) that ion-molecule reactions are the controlling factor in certain<br />

(77) F. W. Lampe, Radiation Research lo, 671 (1959)<br />

(78)<br />

(79) J. H. Futrell, J. &I. -m.<br />

82, 1551 (1960)<br />

=E<br />

*. 8l, 5921 (1959)<br />

-<br />

F. W. Lampe, 2. &. k m . z.,<br />

-<br />

radiation induced processes involving paraffin and olefin hydrocarbons.<br />

An electric discharge <strong>of</strong> course involves ions and electrons and the ions present<br />

can be sampled and analyzed by mass spectrometry. Such studies have been undertaken<br />

by a number <strong>of</strong> investigators and some progress is being made toward understanding<br />

the <strong>chemical</strong> behavior <strong>of</strong> ions in various <strong>discharges</strong>. The problem is complicated by<br />

the fact that there are several kinds <strong>of</strong> electric discharge, each <strong>of</strong> which has its<br />

own physical and <strong>chemical</strong> characteristics. Of these, the type most <strong>of</strong>ten studied is<br />

the direct current glow discharge, but corona and high frequency and micro-wave<br />

<strong>discharges</strong> have also received some attention.<br />

In order to analyze the ionic content <strong>of</strong> a discharge it is necessary to trans-<br />

fer the ions from the discharge into the mass analyzer. While this is not a par-<br />

ticularly serious problem at pressures below 10 microns, the difficulty becomes<br />

more acute as the pressure increases. This is attributable to the fact that elec-<br />

trons and ions diffuse to the walls at different rates, so that an electric gradient<br />

is established which alters the distribution <strong>of</strong> energy <strong>of</strong> the various charged species.<br />

Ordinarily a sheath <strong>of</strong> ions is formed at any surface, including that <strong>of</strong> a sampling<br />

probe and ions or electrons must have, or be given enough energy to pass through<br />

this sheath in order to be sampled. However, if the energy is sufficiently high<br />

some ions may be decomposed by collision. The result then is that there is <strong>of</strong>ten<br />

-

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