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chemical physics of discharges - Argonne National Laboratory

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360<br />

The phenomena ir. t:te pias::.& ::et experiments which convert less nitrogen than<br />

the ,;axinurn pred3ct.Yd 6). the ?'re:czilig rnuuel my well be l.ir,ked to a [nixing or diff'L;sian<br />

rate (CHq a:. i 32 were !~dt prcfliixta) or' tc temperatures 4nsur'ficient to reach<br />

Thi;.qsesticn is ~ i ~ sub,).:et l : 12 a separ-te theoretical analysis now in progress<br />

Tf .<br />

by the author .<br />

THE REACTION SEQUENCE<br />

The experimental data support the fallowing description <strong>of</strong> the overall reac-<br />

tion seqdence:<br />

i. Plasma Reactic;;w. ' Feed reagerits. are dissociated to their atomic constitu-<br />

ents in a therim, plasma. Some Tthermai ioiiizatiQn accurs at sufficiently<br />

high ternperatu.-s.<br />

CF& i 92 - c + H + N + C+ + H+ + N+ + e-<br />

2. Initial Coohnt Plasma taken inco a small-diameter cold tube rapidly<br />

cools witn <strong>chemical</strong> reactio:is following equlibriwn.<br />

C + H + N + ions - H + CIV + C2H + N2 - HCN + @ + N2 + C2w<br />

3. Frozen Reaction Emetics. Rapid cooling continues, but at a rate much<br />

greater than the progress <strong>of</strong> the apparently complex reaction sequence<br />

necessary to des%roy trle species HCN, C2H2, and %. Hence the composi-<br />

tion <strong>of</strong> the cooiliig gas is frozen at the end <strong>of</strong> Step.2.<br />

Evidence fyr the Freezing llbdel in Other Reacting Systems. The freezing model ,<br />

likely is applicable to a wide variety <strong>of</strong> reacting thermal plasma systems which '<br />

emplcy a rapid quench. hmnann and. Timiinsl5 found a mechanism involving the freezin&<br />

<strong>of</strong> equilibratiag reactiuns 'ta be applicable to their study <strong>of</strong> the quenching <strong>of</strong> \<br />

nitrogen-oxygetl plasmc. Ahed by a wealth <strong>of</strong> published rate data on <strong>chemical</strong> reactiotis<br />

in air, they were ~ble to model thc time-temperature-composition history <strong>of</strong><br />

M-0 plasma cooling within mail-diameter tubes. A quite similar freezing tempera- 1<br />

ture, Tf , was found at 35Oi;'K 1'c.r that system. The equilibrium composition <strong>of</strong> nitric<br />

uxi?e, NO, at Tf was preserved during continued rapid coolfng.<br />

\<br />

CONCLUSIONS ' . , . . \<br />

Mixtures <strong>of</strong> mechane and nitrogen can be fed continuously to a thermal argon<br />

indluctiori plasma maintaified abcve 13,300 K. .A rapid quer.ch <strong>of</strong> the heated plasma<br />

kxture produces HCN, C2@, anc &.<br />

the nitrogen converted, range between 3 and 70 percent, a function <strong>of</strong> the input<br />

,<br />

Final yields <strong>of</strong> HCN, expressed'as a fraction Of I<br />

stoicbiometry . i<br />

1<br />

I<br />

'';<br />

<<br />

ti<br />

c

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