Radical Yields in Branched Hydrocarbon Radiolysis
J. Phys. Chem. A, Vol. 107, No. 43, 2003 9247
on the structure of the molecules under consideration and the
eluent being used. We note here that the detailed spectroscopic
information available from the 3-D recordings is essential to
identify the chromatographic peaks properly. Without this
information, it is likely, because tertiary iodides usually elute
before their isomers, that one would assume the first peak in
the radiochromatogram of Figure 9 to be the tertiary iodide.
C-C bonds adjacent to the tertiary site.19,20 Because C-C
rupture occurs only as the result of primary processes, the high
yields of the radicals produced radiolytically by the rupture of
the C-C bonds adjacent to the tertiary site demonstrate that
the energy deposited by ionizing radiation is similarly localized
at tertiary sites.
We especially note here that 2,4-dimethylpentane is a special
case in that the yield of the isobutyl radical is 12% higher than
that of its complement, the isopropyl radical (cf. Figure 6). This
contrasts with the similar yields of ethyl and 3-pentyl radicals
observed in the case of 3-ethylpentane and the relatively low
yield of the complement to the methyl radical produced from
2,3-dimethylbutane. For the normal alkanes, the smaller frag-
ments are observed in slightly greater abundance than their
complements.1 Although one expects the yields of complemen-
tary fragments to be similar factors, other than simple bond
rupture, such as secondary reactions of the ions initially
produced, they play some role in determining the yields of
radicals that can be scavenged at microsecond times.
In summary, this study shows that in the radiolysis of
branched alkanes the loss of H from tertiary positions occurs
an order of magnitude more frequently than from primary
positions but that competitive effects play a role when there
are several tertiary H atoms present. The relative frequency for
the loss from secondary and primary positions (3.2) is similar
to that observed for normal alkanes. These observations provide
the basis for a general understanding of bond rupture in the
radiolysis of saturated branched hydrocarbons.
Discussion and Summary
It has previously been shown1 that in the radiolysis of the
normal alkanes the relative yields the for production of
secondary and primary radicals are proportional to the number
of secondary H atoms in the alkane (i.e., that the relative
frequency for the loss of H from a secondary position is
independent of the size of the alkane and a factor of 3.24 greater
than for loss from a primary position). The yields given in Tables
2 and 3 correspond to similar relative frequencies of 3.6 and
3.1 for the cases of 2,4-dimethylpentane and 3-ethylpentane,
respectively. The relative frequency for the production of
secondary and primary radicals is clearly not strongly dependent
on the structure of the alkane.
The yields of tertiary radicals from the three hydrocarbons
studied are high, as expected from the relatively low energy of
a tertiary C-H bond.17 For 3-ethylpentane, the yields of the
tertiary and primary radicals are in the ratio of 1.65 so that,
taking into account the 9-fold greater number of primary H
atoms, the relative frequency for the loss of a tertiary H is 14.9
times that for the loss of a primary H. For 2,3-dimethylbutane
and 2,4-dimethylpentane, this relative frequency is somewhat
lowers10.2 for each of the two tertiary H atomssindicating
competition between the tertiary positions. Hydrogen atoms
should, of course, mainly abstract at the tertiary position and
will contribute to the observed selectively. However, because
the H-atom yield is estimated to be only ∼1.5,18 H abstraction
alone cannot explain the observed selectivity in the yields of
C-H rupture. It is clear that there is considerable selectivity in
the initial bond rupture processes.
Acknowledgment. The research described herein was sup-
ported by the Office of Basic Energy Sciences of the U.S.
Department of Energy. This is contribution NDRL-4452 from
the Notre Dame Radiation Laboratory. We also acknowledge
the support of the Hungarian Research Fund (OTKA T 037294).
References and Notes
(1) Wojnarovits, L.; Schuler, R. H. J. Phys. Chem. A. 2000, 104, 1346.
(2) Holroyd, R. A. J. Phys. Chem. 1966, 70, 1341.
The yields for radicals produced by the rupture of the central
C-C bonds are similar: 1.74 for 2,3-dimethylbutane, 1.61 for
2,4-dimethylpentane, 1.58 for 3-ethylpentane, and somewhat
higher than the total yield of 1.3 for C-C scission in the normal
alkanes.1 The rupture of a central C-C bond is only marginally
affected by groups that are remote from that bond. For 2,3-
dimethylbutane and 2,4-dimethylpentane, the yields for the
rupture of a terminal C-C bond are high, as expected from the
previous study that showed that methyl radical production was
strongly enhanced by the presence of adjacent methyl groups.5
As a result, fragmentation accounts for 40% of the radicals as
compared to 25% in the case of the normal alkanes. For
3-ethylpentane, the methyl radical production is low, as expected
from the previous study. In this case, the yield of ethyl radicals
is 60% greater than the yield of 0.5 expected from its yield
from n-heptane.1 There appears to be a modest effect of the
adjacent ethyl groups analogous to the effect of methyl
substitution noted in ref 7.
(3) Holroyd, R. A. J. Am. Chem. Soc. 1966, 88, 5381.
(4) All ratios of bond rupture given here have been normalized for the
number of equivalent bonds in the hydrocarbon.
(5) Schuler, R. H. J. Phys. Chem. 1958, 62, 37.
(6) Schuler, R. H.; Foldiak, G. J. Phys. Chem. 1978, 82, 2756.
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(12) Ref 1, Supporting Information.
(13) Kimura, K.; Nagakura, S. Spectrochim. Acta 1961, 17, 166.
(14) Scoggins, M. W.; Miller, J. W. Anal. Chem. 1966, 38, 612.
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(16) Wojnarovits, L.; Schuler, R. H. To be submitted for publication.
(17) The primary, secondary, and tertiary bond energies are ap-
proximately 98, 94, and 92 kcal mol-1. Benson, S. W. Thermochemical
Kinetics; John Wiley and Sons: New York, 1976.
(18) Radiolysis of Hydrocarbons; Foldiak, G., Ed.; Elsevier: Amsterdam,
1981.
(19) Ausloos, P.; Lias, S. G. Far Ultraviolet Photochemistry of Organic
Compounds. In Chemical Spectroscopy and Photochemistry in the Vacuum
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1300.
In general, photochemical studies have shown that that excess
energy in excited alkanes is highly localized around tertiary
carbon atoms and leads to the preferential rupture of C-H and