chemical physics of discharges - Argonne National Laboratory
chemical physics of discharges - Argonne National Laboratory chemical physics of discharges - Argonne National Laboratory
10; He: + N2 -. 2He + h': (8) whi!? Sholette and Muschlitz' iive values of 5-x 1013 and 11 x 1013 cc mole--' sec for the reactions (1) and (10) He(23S) + N2 - He + N+ + e- 2 He(Z3S) + O2 -.. He + 06 + e- (9) ( 10) Our preliminary results are in quite reasonable agreement. 1 References 1. C. 8. Collins and W. W. Robertson, J. Chem. Phys. 2, 701 (1964); 40, 202 (1964); lo, 2208 (1964). 2. A. L. Schmcltekopf and H. P. Broida, J. Chem. Phys. 2, 1261 (1963). 3. 4. 5. E. E. Ferguson, F. C. Fehsenfeld, P. D. Goldan, A. L. Schmeltekopf, and H. I. Schiff, Planetary Space Sci. 2, 823 (1965). J. W. Andersen and R. Friedman, Rev. Sci. Just. 2, 61 (1949). F. C. Fehsenfeld, K. M. Evenson, and H. P. Broida, Rev. Sci. Just. 96, 294 (19651. 6. E. W. HcDaniel, Collision Processes in Ionized Gases (John Wiley & Sons, Inc., New York, 1964), p. 503. 7. Ibid, p. 516. 8. F. C. Fehsenfeld, A. L. Schmeltekopf, P. D. Goldan, H. I. Schiff, and E. E. Ferguson, J. Chem. Phys. 5, 4087 (1966). 9. W. P. Sholette and E. E. Huschlitz, J. Chem. Phys. 2, 3368 (1965). a. Run 0 Table I Titration with N2 at 3915 A 4 x 10 FHc moles/sec P mm Hg T OK k x cc mole-lsec-l 2 (cm scc )(mm Hg) 1 6.93 2.70 363 2.1 374 2 9-30 3.46 376 2.0 480 3 16.1 ' 5.41 413 2.8 696 4 30.6 9.64 480 4.2 2140 5 39.6 12.1 508 4.4 3310 b. Titration with O2 at 5587 (First negative system of 0') 2 6 7.94 2-99 370 6.7 40 3 7 16.1 5-36 409 8.4 543 8 30.8 9.58 475 9.0 1660 9 45.6 13.8 515 8.3 4030 c. Titration with O2 at 4118 (Second negative system of O*) 2 10 11 12 13 8.00 16.1 30.5 45.5 3.11 5.40 9.58 14.0 3 66 418 488 5 26 5.7 5.3 6.4 5.1 33 1 643 1020 2140 f
THE MATHEMATICS OF STEADY-STATE DIFFUSION AND FLOW TUBE SYSTEMS 11. Measurement of Discharge-Zone Rate Parameters Peter R. Rony Central Research Department Monsanto Company St. Louis, Missouri ' I. INTRODUCTION The techniques used to measure the rate of a chemical reaction or to determine the physical characteristics of a chemical compound are dictated by the physical and chemical properties of the compound, particularly by its lifetime and reactivity in relation to its chemical environment. This environment can be chosen to maximize the interactions between the compound and other materials (a reaction environment) or else to minimize such interactions (an isolation environment). Progress in chemistry has been dependent upon the skill chemists have shown in selecting the appropriate reaction or isolation environments. The problem of developing suitable isolation environments has been a difficult one in the study of flames, shock waves, explosions, and electrical discharges, where the chemical intermediates -- ions, electrons, atoms, free radicals, excited atoms, excited molecules, excited ions, and metastable mole- cules -- are highly reactive and have extremely short lifetimes. Notable advances along these lines have been the matrix isolation technique developed by Pimentel and co-workers, contacting the intermediates with a very cold surface, and the use of materials that deactivate surfaces against the recom- bination of atoms and free None of these techniques have yet been successful in significantly prolonging the lifetime of an ion. This problem can be circumvented by the expedient of placing a source of the chemical intermediates in close proximity to a sink and optimizing the rates of loss and transport of the highly reactive species between these two regions. The most popular source-sink system for the study of gas-phase kinetics of neutral molecules is the diffusion or flow tube, which usually employs an electrodeless discharge as the source.s,io Such systems have also been used with considerable success in the fieId of plasma chemistry for the experimental measurement of associative detachment and ion-neutral reaction rates.11,12 The simplicity of these systems is deceptive -- they are usually quite complex. To illustrate this point, Table I gives a non-exhaustive list of rate processes occurring within the system shown in Fig. l.24 It is clear that a comprehensive mathematical description of such systems is desirable not only to aid in the choice of experimental conditions and assessment of experimental data, but also to guide those who use diffusion or flow tubes or the measured rate parameters. Most theoretical descriptions of a diffusion or flow tube have ignored the source of reactive species -- the electrical discharge -- by the assumption of 'a specified value for the reactive specie concentration at the discharge-zone boundary.13-17 Tsu and Boudart were the first to incofporate the discharge zone in the derivation and the author has elaborated upon this type of theoretical I ,
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THE MATHEMATICS OF STEADY-STATE DIFFUSION AND FLOW TUBE SYSTEMS<br />
11. Measurement <strong>of</strong> Discharge-Zone Rate Parameters<br />
Peter R. Rony<br />
Central Research Department<br />
Monsanto Company<br />
St. Louis, Missouri '<br />
I. INTRODUCTION<br />
The techniques used to measure the rate <strong>of</strong> a <strong>chemical</strong> reaction or to<br />
determine the physical characteristics <strong>of</strong> a <strong>chemical</strong> compound are dictated by<br />
the physical and <strong>chemical</strong> properties <strong>of</strong> the compound, particularly by its lifetime<br />
and reactivity in relation to its <strong>chemical</strong> environment. This environment<br />
can be chosen to maximize the interactions between the compound and other<br />
materials (a reaction environment) or else to minimize such interactions (an<br />
isolation environment). Progress in chemistry has been dependent upon the<br />
skill chemists have shown in selecting the appropriate reaction or isolation<br />
environments.<br />
The problem <strong>of</strong> developing suitable isolation environments has been a<br />
difficult one in the study <strong>of</strong> flames, shock waves, explosions, and electrical<br />
<strong>discharges</strong>, where the <strong>chemical</strong> intermediates -- ions, electrons, atoms, free<br />
radicals, excited atoms, excited molecules, excited ions, and metastable mole-<br />
cules -- are highly reactive and have extremely short lifetimes. Notable<br />
advances along these lines have been the matrix isolation technique developed<br />
by Pimentel and co-workers, contacting the intermediates with a very cold<br />
surface, and the use <strong>of</strong> materials that deactivate surfaces against the recom-<br />
bination <strong>of</strong> atoms and free None <strong>of</strong> these techniques have yet<br />
been successful in significantly prolonging the lifetime <strong>of</strong> an ion.<br />
This problem can be circumvented by the expedient <strong>of</strong> placing a source <strong>of</strong><br />
the <strong>chemical</strong> intermediates in close proximity to a sink and optimizing the rates<br />
<strong>of</strong> loss and transport <strong>of</strong> the highly reactive species between these two regions.<br />
The most popular source-sink system for the study <strong>of</strong> gas-phase kinetics <strong>of</strong> neutral<br />
molecules is the diffusion or flow tube, which usually employs an electrodeless<br />
discharge as the source.s,io<br />
Such systems have also been used with considerable<br />
success in the fieId <strong>of</strong> plasma chemistry for the experimental measurement <strong>of</strong><br />
associative detachment and ion-neutral reaction rates.11,12<br />
The simplicity <strong>of</strong> these systems is deceptive -- they are usually quite<br />
complex. To illustrate this point, Table I gives a non-exhaustive list <strong>of</strong><br />
rate processes occurring within the system shown in Fig. l.24 It is clear that<br />
a comprehensive mathematical description <strong>of</strong> such systems is desirable not only<br />
to aid in the choice <strong>of</strong> experimental conditions and assessment <strong>of</strong> experimental<br />
data, but also to guide those who use diffusion or flow tubes or the measured<br />
rate parameters.<br />
Most theoretical descriptions <strong>of</strong> a diffusion or flow tube have ignored<br />
the source <strong>of</strong> reactive species -- the electrical discharge -- by the assumption<br />
<strong>of</strong> 'a specified value for the reactive specie concentration at the discharge-zone<br />
boundary.13-17 Tsu and Boudart were the first to inc<strong>of</strong>porate the discharge zone<br />
in the derivation and the author has elaborated upon this type <strong>of</strong> theoretical<br />
I<br />
,