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Agapito et al.
molecules are in the ideal gas phase (isolated). It is related to
the thermodynamic stability of the corresponding carbon-
centered radical R•, as measured by its standard enthalpy of
formation ∆fH°(R•,g), through eq 2.
free reference molecule, regardless of the cause. To relate
BDEs to strain we need to consider it both in the parent
molecule and in its radical. However, evaluating strain in
the radicals is considerably more complex that in the parent
molecules. An important part of this work was therefore the
selection of a method that allows quantifying the strain in
the radicals studied.
RH(g) f R•(g) + H•(g)
(1)
DH°(C-H) ) ∆fH°(R•,g) + ∆fH°(H•,g) - ∆fH°(RH, g) (2)
Results
Most well-known BDEs for organic compounds have
been obtained in the gas phase from kinetics studies, ion cycles,
and photoionization mass spectrometry, but chemical accuracy
(i.e., values with errors smaller than ca. 4 kJ mol-1) was
achieved for only relatively few data.3–5 As the literature values
for the C-H BDEs in many small hydrocarbons have uncertain-
ties well above chemical accuracy, we investigated a number
of those molecules using a combined approach of theoretical
chemistry methods and time-resolved photoacoustic calorimetry
(TR-PAC).6,7
The strategy used to obtain BDEs from photoacoustic
calorimetry was based on the photochemical process below: di-
tert-butylperoxide (t-BuOOBu-t) is photolyzed, generating tert-
butoxyl radicals (reaction 3), each abstracting an hydrogen atom
from the organic molecule RH, reaction 4.
t-BuOOBu-t(sln)
9
hν8 2t-BuO•(sln)
(3)
2RH(sln) + 2t-BuO•(sln) f 2R•(sln) + 2t-BuOH(sln)
(4)
In a previous study we determined the C-H BDEs in a series
of open-chain hydrocarbons containing the allyl group.8We then
used the results to select the “best” values for the C-H BDEs
in these molecules, which allowed a quantitative discussion
of the factors that determine the stability of the corresponding
radicals, namely, hyperconjugation and resonance. Having
dealt with all relevant molecules from the simplest propene
to cyclohexadiene (viz., propane, propene, isobutene, 1-butene,
2-butene, 3-methyl-1-butene, 2-pentene, 1,3- and 1,4-penta-
diene, cyclohexene, and 1,3- and 1,4-cyclohexadiene), we
now turned our attention to the effect of ring strain on the
C-H BDEs. To this end we need to compare the five-
membered rings cyclopentane, cyclopentene, and 1,3-cyclo-
pentadiene, with the six-membered ones, cyclohexane, cy-
clohexene, and 1,4-cyclohexadiene, respectively. In this work
we report the TR-PAC determinations of C-H BDEs in
cyclopentane and cyclohexane. The TR-PAC experimental
results were complemented by quantum chemistry calcula-
tions for the same molecules and the corresponding radicals
(cyclopentyl and cyclohexyl), plus cyclopentene, cyclopenten-
3-yl, cyclopenten-4-yl, cyclohexen-4-yl, propane, and iso-
propyl. These and the previous results for the remaining
cyclic hydrocarbons, together with the simpler molecules
propene, 1-butene, (E)-2-pentene, 1,3- and 1,4-pentadiene,8
werethenusedtosystematicallyinvestigatethestructure-energetics
relationship in the five- and six-membered ring hydrocarbons
(see Supporting Information for the complete list of molecules
investigated).
Deconvolution of the resulting waveform (see Experimental
Section) first made it possible to confirm the reaction scheme
(reactions 3 and 4) and then afforded the observed fraction of
photon energy released as heat, φobs,i, for each process, and the
lifetime of the second, τ2. An estimate of the rate constant can
be obtained from this lifetime.10 The enthalpy of the hydrogen
abstraction reaction was derived from eq 5, where ∆obsH2
corresponds to the observed enthalpy change and is calculated
by multiplying φobs,2 (the observed heat fraction associated with
reaction 2) by Em ) NAhν (the molar photon energy). Φr is the
reaction quantum yield for the photolysis of di-tert-butylper-
oxide.11
-∆obsH2
∆rH2 )
(5)
Φr
As the enthalpy of reaction 4 is simply twice the difference
between the solution BDEs of the hydrocarbon C-H and tert-
butyl alcohol O-H, DH°sln(C-H) can be derived from eq 6,
where the subscript “sln” indicates that both BDEs are solution
values.
∆rH2
DH°sln(C-H) )
+ DH°sln(t-BuO-H)
(6)
2
In a previous work we determined DHosln(t-BuO-H) ) 455.2
( 5.2 kJ mol-1 in benzene.12 To derive the gas-phase value
DH°(C-H), the solvation terms illustrated in eq 7 must be
considered.13
Strain is the central concept in this discussion, used in the
conventional sense of Cox and Pilcher,9 i.e., including all
the stabilizing and destabilizing effects in relation to a strain-
DH°(C-H) ) DHs°ln(C-H) + ∆slnH°(RH,g) -
∆slnH°(R•,g) - ∆slnH°(H•,g) (7)
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