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chemical physics of discharges - Argonne National Laboratory

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202<br />

CONCLUSIONS<br />

Chemical reacticns can be initiated and sustained by a corona discharge. Boron has been<br />

deposited on a tungsten wire substrate in a corona discharge at relatively low temperatures.<br />

The deposition process is electro<strong>chemical</strong> in nature, the boron being deposited cathodically,<br />

and the mechanism for the reaction is indicated to be <strong>of</strong> the form:<br />

(a) Emission <strong>of</strong> electrons from the cathode<br />

(b) Ionization (or activation) <strong>of</strong> hydrogen, argon, or helium, and production <strong>of</strong><br />

secondary electrons which in turn ionize more hydrogen, etc.<br />

(c) Collision <strong>of</strong> ionized hydrogen, argon, or helium with boron tribromide and<br />

exchange <strong>of</strong> energy<br />

(d) Formation <strong>of</strong> positive boron radicals and hydrogen bromide or bromine<br />

(e) Transfer <strong>of</strong> the positive boron radical to the cathode<br />

(f) Electro<strong>chemical</strong> reaction <strong>of</strong> the boron radical to form an essentially amorphous<br />

deposit <strong>of</strong> boron<br />

The morphology <strong>of</strong> the deposit is essentially the same as the morphology <strong>of</strong> the substrate.<br />

There is no interaction <strong>of</strong> the boron with the tungsten and there is apparently some anisotropy<br />

<strong>of</strong> the deposit.<br />

The corona discharge during deposition is not essentially different from a corona discharge<br />

developed in an inert gas system, and the same criteria and properties are extant. Like a<br />

corona discharge in an inert gas, the coefficient <strong>of</strong> electron emission and the ability <strong>of</strong> the<br />

electrons to diffuse along the wire are most important in obtaining a uniform corona, and<br />

thus a uniform deposit, on the substrate. Furthermore, if the sheath <strong>of</strong> positively charged<br />

boron radicals becomes too dense. the corona is quenched and will not recover fast enough<br />

to prevent the breakup <strong>of</strong> the corona into points.<br />

ACKNOWLEDGEMENT<br />

This work was supported by the U. S. Air Force Contract AF 33(615)-2130, and was based<br />

upon an idea presented by J. B. Story. The filament cross-sections were prepared by<br />

W. C. Coons and the continuous system was operated by Barbara Traina. Grateful acknow-<br />

ledgement is also made to R. N. Varney, M. E. Sibert, and A. E. Hultquist for many help-<br />

ful discussions <strong>of</strong> gas <strong>discharges</strong> in general and <strong>of</strong> corona <strong>discharges</strong> in particular.<br />

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REFERENCES<br />

N. A. Kapzow, IIElelstrische Vorgange in Gasen und in Vakuum, Veb Deutscher<br />

Verlog der Wissenschaften, Berlin, 1955<br />

S. C. Brown, "Basic Data <strong>of</strong> Plasma Physics," The Technology Press <strong>of</strong> MIT and<br />

John Wiley and Sons, Inc., New York, 1959<br />

E. J. Helland, The Plasma State, Reinhold Publishing Corporation, New York, 1961<br />

L. B. Loeb, Electrical Coronas, Univ. <strong>of</strong> Calif. Press, 1965<br />

L. Ya. Markovskii, V. I. L'vova, Yu. D. Kondrashev, Bor. Trudy Konf. Khim, Bora;<br />

Ego Soedineii. 36-45 (1958) cf. FTD-MT-64-427, Foreign Technology Division,<br />

A. F. Systems Command, 1965<br />

W. V. Kotlensky andR. Schaeffer, J. Am. Chem. SOC. 80, 4517 (1958)<br />

R. T. Holzmann and W. F. Morris, J. Chem. Phys. 29, 677 (1958)<br />

N. R. Dibelius, J. C. Fraser, M. Kawahata, and C. D. Doyle, Chem. Engr.<br />

Progress, 60, No. 6, 41-44 (June 1964)<br />

S. J. Lawrence, Chem. Engr. Progress, 60, No. 6, 45-51 (June, 1964)<br />

J. A. C<strong>of</strong>fman and W. R. Browne, Scientific American, 212, No. 6, 90-98 (June 1965)<br />

N. A. Lange, Editor, Handbook <strong>of</strong> Chemistry, 10th Ed., 111, McCraw-Hill Book .<br />

Company, Inc., N. Y. 1961

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