chemical physics of discharges - Argonne National Laboratory
chemical physics of discharges - Argonne National Laboratory chemical physics of discharges - Argonne National Laboratory
i 4 2 HYDROCARBON-NITROGEN REACTIONS IN A TRERMAL INDUCTION PLASMA Bary R. Bronfin United Aircraft Research Laboratories I East Hartford, ConneLticht 06108 I 4, Gas temperatures anove l5,OOO K have been observed in plasma generateddby radio-frequency induction coupling'. This high thermal erlergy regirre becon?es of iqcerest to the chemist for the investigation of highly endothermic reactions. I?. particular, this paper will report reactions between methane and nitrogen fed to a thermal induction plasma ar,d subsequently quenched to yield hydrogen cyanide, acetylene and hydrogen. / PREVIOUS STUDIES OF THE E-C-N SYSTEM Lar Pressure Discharges. Winkler and his co-workers2-5 have systematically studied the reactions of nitrogen, activated by passage through a high-voltage discharge, with various hydrocarbons. These studies were carried out at pressures near 1 torr with very low reagent flow rates. Gas temperatures were also low, typically 300 C. In this nonequilibrium system the reaction betw-een methane and "active" nitrogen yielded hydrogen cyanide, acetylene and hydrogen2. High Pressure Arcs. More recently high-power thermal arcs were used for the study of the H-C-N system near atmospheric pressure. Leutrer' operated 2 nitrogen plasma jet into which methane was mixed. In his briefly reported results, up to LO percent conversion of the nitrogen to HCN was found'. -At this symposium Freeman? has reported an extensive study of the synthesis of HCN, from EL nitrogen plasma jet intermixed with methane. Typically, a 7 percent conversion of N2 to HCN was observed. In both studies &, C2IJ2, and unreacted CHI, were also identified as major constituents in the cooled product stream. If the maximum mean temperature attainable in these previous studies is cal- cdated, one finds that enthalpy input was insufficient to generate mean tempern- f Caes greater than - 5000 K. \ J ,' B d P Dissociating Plasmas. Upon considering the various species possible in.the H-C-N system, the strongest bond found is N E N (226 kcal/g-mole). Thermal-dissociation of N2 is essentiaU.y complete at temperatures in excess of 8000 K". Orv. car. envision a high-pressure, stable plasma fed with any of e. variety of carbon, hydrogen, or nitrogen compounds and supplied with sufficient erthalpy to reach this high temperature range. The constituent species of srlch a plasma would be prinarily atomic nitrogen, atornic hydrogen, and atomic carbon near lo1-( cm-3 concentration. The result of rapidly quenching such! highly reactive atom mixture nas been generally Lnexplored. &ann and TimminsJ,lO, however, did study the rapid quenching of the simpler atonic-nitrogen/atormc-oxygen mixtures at 10,Oc)O K
348 and 1 atm, which were generated by a constricted d.c. arc. The study which is reported in this paper was undertaken to explore the chemical composition of mixtues formed. by the rapid . .quench . of atomic-nitragen/atomic-carbcn/atomichydrogen rnixtures. PLASMA REACTOR Radio-frequency Induction Plasma. One convenient approach to achieve the reqdred temperatures in excess of 10,000 K at atmospheric pressure is generation of a thermal plas,m by radio-frequency induction heating. The techniques for generating and containing a stable high-temperature induction plasma have been described in detail by Reedljll, Mironeru, Marynowski and Monroe'3, Freeman and ChaselL, and Thorpel?. Figure 1 presents a diagram of the plasma generator used, A few turns of copper tubing were wound around the outside of a water-cooled quartz reactor tube. This coil inductively coupled the supplied r.f. power into the gaseous reactants sent through the reactor. A water-cooled sampling tube with very small internal diameter which served to quench rapidly the reactive plasma species is shown. Efficient cooling allowed the entrance tip of the quench tube tc be placed directly into the plasma core. A cross-sectional diagram of the reactor is presented in Fig. 2. The iso- therms indicated are those determined spectroscopically by Reed' and' are repre- sentative of conditions in this study. No direct temperatwe measurements were attempted in the present study. The Induction Plasma as a Chemical Reactor. Several characteristics of this system can be exploited for chemical synthesis: 1. Average temperatures in excess of 10,000 K allar essentially complete molecular dissociation. (Lower power input can reduce the specific enthalpy to preserve desired free radicals.) 2. Plasma stability is maintained while operating at very low gas velocities (
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348<br />
and 1 atm, which were generated by a constricted d.c. arc. The study which is<br />
reported in this paper was undertaken to explore the <strong>chemical</strong> composition <strong>of</strong><br />
mixtues formed. by the rapid . .quench . <strong>of</strong> atomic-nitragen/atomic-carbcn/atomichydrogen<br />
rnixtures.<br />
PLASMA REACTOR<br />
Radio-frequency Induction Plasma. One convenient approach to achieve the<br />
reqdred temperatures in excess <strong>of</strong> 10,000 K at atmospheric pressure is generation<br />
<strong>of</strong> a thermal plas,m by radio-frequency induction heating. The techniques for<br />
generating and containing a stable high-temperature induction plasma have been<br />
described in detail by Reedljll, Mironeru, Marynowski and Monroe'3, Freeman and<br />
ChaselL, and Thorpel?. Figure 1 presents a diagram <strong>of</strong> the plasma generator used,<br />
A few turns <strong>of</strong> copper tubing were wound around the outside <strong>of</strong> a water-cooled<br />
quartz reactor tube. This coil inductively coupled the supplied r.f. power into<br />
the gaseous reactants sent through the reactor. A water-cooled sampling tube with<br />
very small internal diameter which served to quench rapidly the reactive plasma<br />
species is shown. Efficient cooling allowed the entrance tip <strong>of</strong> the quench tube<br />
tc be placed directly into the plasma core.<br />
A cross-sectional diagram <strong>of</strong> the reactor is presented in Fig. 2. The iso-<br />
therms indicated are those determined spectroscopically by Reed' and' are repre-<br />
sentative <strong>of</strong> conditions in this study. No direct temperatwe measurements were<br />
attempted in the present study.<br />
The Induction Plasma as a Chemical Reactor. Several characteristics <strong>of</strong> this<br />
system can be exploited for <strong>chemical</strong> synthesis:<br />
1. Average temperatures in excess <strong>of</strong> 10,000 K allar essentially complete molecular<br />
dissociation. (Lower power input can reduce the specific enthalpy to<br />
preserve desired free radicals.)<br />
2.<br />
Plasma stability is maintained while operating at very low gas velocities<br />
(