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chemical physics of discharges - Argonne National Laboratory

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; it raised the question, still &?zesolved, as to whether the ions might<br />

’ not in some way be responsible for the chemistry. As a direct consequence there is<br />

a long-term quantitative spectroscopic study <strong>of</strong> plasma jets(9) currently in progress<br />

/(9) M. P. Freeman, “A Quantitative Examination <strong>of</strong> the LTE Condition in the Ef-<br />

1 fluent <strong>of</strong> an Atmospheric Pressure Argon Plasma Jet,“ CE-JILA-ONR Symposium<br />

on the “Interdisciplinary Aspects <strong>of</strong> Radiative Energy Transfer,”. Philadelphia,<br />

Penn., Feb. 24-26, 1966. In Press.<br />

/<br />

/<br />

J’<br />

that is expected to ultimately yield information on the nature and quantity <strong>of</strong> ions,<br />

atoms and high temperature molecular species flowing in jets <strong>of</strong> common plasma ma-<br />

terials.<br />

Although thermodynamic calculations had previously been performed for the nitro-<br />

gen-carbon-hydrogen system(l0) they were not in a form easy to compare with plasma<br />

/<br />

‘ (10) C. W. Marynmski, R. C. Phillips, J. C. Phillips, and N. K. Hiester, Ind.<br />

Eng. Chem. Fundamentals, 1, 52 (1962).<br />

/<br />

1 jet results obtained under normal operating constraints. The calculations were there-<br />

; ,fore reproduced(11) with the pertinent parameters varied to conform to the exigencies <strong>of</strong><br />

;I<br />

i<br />

1 (11) B. R. Bronfin, V. N. DiStefano, M. P: Freeman, and R. N. Hazlett, “Thermo-<br />

\<br />

1<br />

<strong>chemical</strong> Equilibrium in the Carbon-Hydrogen-Nitrogen System at Very High Tem-<br />

peratures,” Presented at the 15th CIC Chem. Engr. Conf., Q,uebec City, Quebec,<br />

Oct . 25-27, 1965.<br />

7<br />

j<br />

,/ plasma jet operation. Figures 3 and 4 show the results obtained when solid carbon<br />

is suppressed in the calculations to be consistent with its absence in the observed<br />

I/ products. An important fact immediately emerges. Neither at any experimentally<br />

/ attained average enthalpy, nor at any experimentally used ratio <strong>of</strong> methane to nitrogen,<br />

has the thermodynamically expected yield <strong>of</strong> HCN for a well-mixed system been<br />

(Note that the apparent fall-<strong>of</strong>f in calculated yield at high power levels<br />

/ ~ ~ ~ % methane w flow rates is due to the competitive formation <strong>of</strong> cyano, CN, which<br />

, may be presumed to be an HCN precursor.)<br />

7 The relationship between the observed and calculated equilibrium yield for the<br />

CHb-N2 System is strikingly similar to that recently reported for the F-C-N system by<br />

1 aronfin(l2) who thereupon advanced the plausible hypothesis that in either case the<br />

I<br />

r‘<br />

(12) B. R. Bronfin and R. N. H,azlett, Ind. Eng. Chem. F’undamentals, 5, 472 (1966).<br />

#<br />

i<br />

observed yield is in some way a consequence <strong>of</strong> equilibrium considerations. Now,<br />

from earlier work on the acetylene system(7) it would seem that the composition and

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