26.03.2013 Views

chemical physics of discharges - Argonne National Laboratory

chemical physics of discharges - Argonne National Laboratory

chemical physics of discharges - Argonne National Laboratory

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

100<br />

The existence <strong>of</strong> the 6 bands and emission from higher vibrational levels <strong>of</strong> the<br />

NO(A2Z+) state indicate that this rate is a lower bound to the rate <strong>of</strong> energy transfer<br />

from N2(A3Z$) to NO(X2JI). There are several states <strong>of</strong> NO<br />

energy exchange involving N2(A3C+) -- the a4n, b4n, b4Z-,<br />

accessible in an<br />

as well as the A2Z+<br />

and B2n which are revealed by deir emission.<br />

The total rate <strong>of</strong> de-excitation <strong>of</strong><br />

3+<br />

N2(A Zu) can be estimated, since we know,<br />

in the absence <strong>of</strong> NO, its deactivation rate is 1/~ = 50/sec, and the intensit<br />

<strong>of</strong> the Vegard-Kaplan bands is reduced by half when [NO] % 7 x 10l1 &olecules/ cm 3 ,<br />

i.e., 50 = ki6(7 x 1011); in other words<br />

ki6 = 7 x cm3/sec<br />

3+<br />

or essentiallya quarter <strong>of</strong> all the N2(A 1 )<br />

U<br />

v' = 0 level <strong>of</strong> the NO(A2Z+).<br />

deactivated leads to excitation <strong>of</strong> the<br />

2<br />

It is apparent from the spectra that excitation <strong>of</strong> the A Z state <strong>of</strong> NO by<br />

Nz(A3Z:) decreases in efficiency as v' increases in the NO molecule, becoming<br />

very small for v' = 3 which is the highest level observed. This level can only be<br />

excited by Nz(A3Zt v = l), while the v' = 2, 1, and 0 levels <strong>of</strong> the NO(A2C+)<br />

state can be excited by<br />

the rate coefficient <strong>of</strong><br />

N2(A3C$ v = 0,l). Using the data in Fig. 14, we can obtain<br />

as<br />

1.<br />

2.<br />

3.<br />

4.<br />

5.<br />

6.<br />

7.<br />

1 2 +<br />

N2(A31: v' = 1) + NO(X2n) -+ N2(X Z) + NO(A Z v = 3)<br />

k (1,3) = 10-l~ cm3/sec. .<br />

16<br />

REFERENCES<br />

R. A. Young, Canad. J. Chem. 46, 1171 (1966). This paper contains additional<br />

references. K. Wray independently arrived at similar conclusions in J. Chem.<br />

Phys. 44, 623 (1966).<br />

Enhancetron Nuclear Data Inc.<br />

R. A. Young and G. Black, J. Chem. Phys. 44, 3741 (1966). This paper has references<br />

leading back to the description <strong>of</strong> most <strong>of</strong> the phenomenon associated with dis-<br />

charged nitrogen.<br />

R. A. Young and R. L. Sharpless, Discussions Faraday SOC. 33, 228 (1962).<br />

A. B. Collear and I. W. M. Smith, Trans. Faraday SO~. 6l, 2383 (1965). .,-<br />

W. R. Brennan, Studies in active nitrogen, Ph. D. Thesis, Dept. <strong>of</strong> Chemistry,<br />

Harvard University, Sept. 1964, and references quoted here; R. W. Nicholls,<br />

J. Res. Natl. Bureau Std. (U.S.) m, 451 (1961); R. A. Young and R. L. Sharpless,<br />

I<br />

J. Chem. Phys. 39, 1071 (1963); R. A. Young and R. L. Sharpless, J. Chem. Phys.<br />

- 39, 1971 (1963); R. A. Young and G. Black, J. Chem. Phys. (in press). These<br />

references contain an extensive review <strong>of</strong> the pertinent chemiluminescent reactions. !<br />

C. H. Dugan, An experimental study <strong>of</strong> metastable atoms and molecules, Thesis,<br />

Division <strong>of</strong> Engineering and Applied Physics, Harvard University, June 1963;<br />

C. H. Dugan and N. P. Carleton (in press).<br />

(33)<br />

I<br />

1

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!