The modified phase‐space theory of reaction rates was coupled with Monte Carlo trajectory calculations to yield rate constants and energy distributions of reactants and products for the three‐atom dissociation and recombination reactions of hydrogen at 4000°K. Sample trajectories selected from those crossing a surface in phase space were calculated in forward and reverse directions to determine the classical rates of formation of bound and quasibound molecules from atoms. The probability of stabilization of quasibound molecules in successive collisions with hydrogen atoms was determined from additional trajectory calculations. The steady state correction factor for recombination, which accounts for dissociation of newly formed bound H2 molecules, was estimated from similar calculations. The computed rate constant for recombination is 3.1×1015 cm6 mole−2 sec−1. For equilibrium between free atoms and quasibound molecules established through tunneling, the over‐all rate constant is estimated to be 75% higher. In either case the process of termolecular recombination to produce bound molecules makes a substantial contribution to the over‐all rate.

1.
An extensive review of theory and experiment for three‐body dissociation and recombination reactions is given by
A. D.
Stepukhovich
and
V. M.
Umanskii
,
Russ. Chem. Rev.
38
,
590
(
1969
).
2.
H.
Eyring
,
H.
Gershinowitz
, and
C. E.
Sun
,
J. Chem. Phys.
3
,
786
(
1935
).
3.
R. E.
Roberts
,
R. B.
Bernstein
, and
C. F.
Curtiss
,
J. Chem. Phys.
50
,
5163
(
1969
);
R. E.
Roberts
,
R. B.
Bernstein
, and
C. F.
Curtiss
,
Chem. Phys. Lett.
2
,
236
(
1968
).
4.
R. T.
Pack
,
R. L.
Snow
, and
W. D.
Smith
,
J. Chem. Phys.
56
,
926
(
1972
).
5.
V. H.
Shui
and
John P.
Appleton
,
J. Chem. Phys.
55
,
3126
(
1971
).
6.
J. C.
Keck
,
Adv. Chem. Phys.
13
,
85
(
1967
).
7.
J. C.
Keck
,
Discussions Faraday Soc.
33
,
492
(
1960
).
8.
P. A.
Whitlock
,
J. T.
Muckermann
, and
R. E.
Roberts
,
Chem. Phys. Lett.
16
,
460
(
1972
).
9.
A. Jones and J. L. J. Rosenfeld, Abstracts of VII International Conference on the Physics of Electronic and Atomic Collisions, Amsterdam, 1971, p. 314.
10.
I. R.
Hurle
,
A.
Jones
, and
J. L. J.
Rosenfeld
,
Proc. R. Soc. A
310
,
253
(
1969
).
11.
V. H. Shui, J. P. Appleton, and J. C. Keck, Thirteenth Symposium (International) on Combustion, Salt Lake City, 1970 (Combustion Institute, Pittsburgh, 1971), p. 21.
12.
R. N.
Porter
and
M.
Karplus
,
J. Chem. Phys.
40
,
1105
(
1964
).
13.
W.
Kołos
and
L.
Wolniewicz
,
J. Chem. Phys.
43
,
2429
(
1965
);
W.
Kołos
and
L.
Wolniewicz
,
49
,
404
(
1968
).,
J. Chem. Phys.
14.
L.
Pederson
and
R. N.
Porter
,
J. Chem. Phys.
47
,
4751
(
1967
).
15.
R. L.
Jaffe
,
J. M.
Henry
, and
J. B.
Anderson
,
J. Chem. Phys.
59
,
1128
(
1973
).
16.
J. B.
Anderson
and
R. T. V.
Kung
,
J. Chem. Phys.
58
,
2477
(
1973
);
J. B.
Anderson
and
R. T. V.
Kung
,
60
,
2202
(
1974
).,
J. Chem. Phys.
17.
J. C.
Slater
,
Phys. Rev.
38
,
1109
(
1931
).
18.
H. C.
Conroy
and
B. L.
Bruner
,
J. Chem. Phys.
47
,
921
(
1967
).
19.
M.
Karplus
,
R. N.
Porter
, and
R. D.
Sharma
,
J. Chem. Phys.
43
,
3259
(
1965
).
20.
R. L.
Jaffe
and
J. B.
Anderson
,
J. Chem. Phys.
54
,
2224
(
1971
).
21.
Quantum partition functions for quasibound states have been estimated by
T. G.
Waech
and
R. B.
Bernstein
,
J. Chem. Phys.
46
,
4905
(
1967
).
22.
W. J. Dixon and F. J. Massey, Jr., Introduction to Statistical Analysis (McGraw‐Hill, New York, 1957), p. 62.
23.
W. Feller, An Introduction to Probability Theory and Its Applications (Wiley, New York, 1966), Vol. 1, p. 221.
24.
J. C.
Keck
and
G.
Carrier
,
J. Chem. Phys.
43
,
2284
(
1965
).
25.
B. J. McBride, S. Heimel, J. G. Ehlers, and S. Gordon, Thermodynamic Properties to 6000 °K for 210 Substances Involving the First 18 Elements. NASA SP‐3001, N63‐23715, Lewis Research Center, Cleveland, p. 185 (1963).
26.
The values of kij were obtained from weighted averages of kij and kijQj/Qi. For k21 and k12 results from the original phase‐space calculations were incorporated into the average. k15 and k35 are rough estimates.
27.
The discrepancy between ∑′kij and kc is largely due to the statistical errors in estimating kij’s. The effect of this uncertainty on δ is discussed in the text.
28.
(a)
R. W.
Patch
,
J. Chem. Phys.
36
,
1919
(
1962
).
(b)
E. A.
Sutton
,
J. Chem. Phys.
36
,
1923
(
1962
). ,
J. Chem. Phys.
(c)
T. A.
Jacobs
,
R. R.
Geidt
, and
N.
Cohen
,
J. Chem. Phys.
47
,
54
(
1967
). ,
J. Chem. Phys.
(d)
J. P.
Rink
,
J. Chem. Phys.
36
,
262
(
1962
).,
J. Chem. Phys.
29.
O. K.
Rice
,
J. Phys. Chem.
65
,
1972
(
1961
).
30.
B.
Widom
,
Science
148
,
1555
(
1965
).
31.
S. H. Bauer, in Abstracts of Papers, 133 Meeting, American Chemical Society (American Chemical Society, Washington, 1958), p. 8Q.
32.
A.
Gelb
,
R.
Kapral
, and
G.
Burns
,
J. Chem. Phys.
56
,
4631
(
1972
);
A. G.
Clarke
and
G.
Burns
,
J. Chem. Phys.
56
,
4626
(
1972
).,
J. Chem. Phys.
33.
B.
Widom
,
J. Chem. Phys.
55
,
44
(
1971
).
34.
J. E. Bennett and D. R. Blackmore, Thirteenth Symposium (International) on Combustion, Salt Lake City, 1970 (Combustion Institute, Pittsburgh, 1971).
35.
A review of potential surfaces is given by
C. A.
Parr
and
D. G.
Truhlar
,
J. Phys. Chem.
75
,
1844
(
1971
).
36.
L.
Shavitt
,
R. M.
Stevens
,
F. L.
Minn
, and
M.
Karplus
,
J. Chem. Phys.
48
,
2700
(
1968
).
This content is only available via PDF.
You do not currently have access to this content.