of HP-136 reveals the formation of the radical of Figure 1,
where the UV band is virtually identical to that for diphen-
ylmethyl. The visible band (see 500-600 nm region) is more
would lead to an upper limit for its reacton with oxygen of
5
-1 -1
e10 M s , i.e., over 10 000 times less reactive than
4
1
typical free radicals. Careful comparison of nitrogen- and
oxygen-saturated samples, at either the 340 or 540 nm
maxima, shows that while neither the decay nor the growth
kinetics are significantly affected by oxygen (see Figure 2),
Figure 1. Transient spectra recorded following 308 nm laser
excitation of a sample containing 1% (w/v) HP-136 and 5% (v/v)
di-tert-butyl peroxide in acetonitrile under nitrogen. Monitored at
different times following the laser pulse, where the signal grows
and decays as indicated. The inset shows an expansion of the visible
region and facilitates visualizing the order of the traces.
Figure 2. Transient kinetic traces recorded at 340 nm following
3
1
08 nm laser excitation of a sample containing 2.5% (w/v) HP-
36 and 5% (v/v) di-tert-butyl peroxide in benzene under nitrogen
and oxygen.
•
intense than that in the case of Ph
2
C H, but enhancement of
the signal amplitude was 18% smaller in the presence of
oxygen. The true decrease is smaller than suggested by this
figure; it can be attributed to two origins, which we label
trivial and nontrivial. A trivial decrease of 11% is due to an
enhancement of the solution absorption at 308 nm (laser
excitation wavelength) in the presence of oxygen. Such
charge-transfer-mediated enhancements are common, al-
though they are frequently overlooked or believed to be
significantly smaller. The remaining 7% decrease in signal
intensity (thus contributing to the observed 18% decrease)
must have a different origin. We propose that this “nontrivial”
decrease should be attributed to a reversible reaction of the
HP-136 radical with oxygen, as illustrated in reaction 2. This
this band is common when heteroatoms are involved; the
•
best documented example is Ph
2
C OH, the ketyl radical from
4
-6
benzophenone.
presence of HP-136 shows that the formation of the HP-
36 radical (the same as in Figure 1) occurs concurrently
Photolysis of dicumyl peroxide in the
1
with the decay of cumyloxyl. We note that cumyloxyl
radicals are far more easily detectable than tert-butoxyl and
allow the easy corroboration of the precursor-derivative
relationship between cumyloxyl and the HP-136 radical.
C H was produced by laser irradiation
of di-tert-butyl peroxide in the presence of diphenylmethane.
7
•
In an experiment, Ph
2
When the sample was saturated with oxygen, the signal from
•
Ph
2
C H was totally quenched, with barely a fast spike
indicating its presence in the early stages following the laser
pulse. Remarkably, when the same experiment was repeated
with HP-136, oxygen did not cause any appreciable changes
in the rate of decay of the radical. Taking this lack of
quenching to reflect radical unreactivity toward oxygen
(
10) Janzen, E. G.; Johnston, F. J.; Avers, C. L. J. Am. Chem. Soc. 1967,
9, 1176.
11) Data were collected on a Bruker AX SMART 1K CCD diffracto-
8
(
type of reversibility is unprecedented for a diphenylmethyl-
type structure but is documented for triphenylmethyl radicals,
which are known to react with oxygen reversibly;
meter, Mo KR (λ ) 0.71073 Å), in the range 4.8° e 2θ e 45° using 0.3°
ω scans at 0, 90, and 180° in φ. No absorption corrections were required
-
1
8-10
(
µ ) 0.71 cm ). Systematic absences in the diffraction data [15943
collected, 2654 observed, unique (I > 2σI)] and unit-cell parameters [a )
however, in this case the equilibrium is extensively displaced
1
2
1
3.791(3) Å, b ) 10.797(2) Å, c ) 14.412(3) Å, â ) 108.174(3)°, V )
038.9(6), Z ) 4] were uniquely consistent with monoclinic, P21/c (No.
4). A tert-butyl group was found rotationally disordered in two positions
8
toward the peroxyl radical side. Howard and Ingold studied
this equilibrium as early as 1968 and determined an equi-
with a refined site occupancy distribution of 70/30. All non-hydrogen atoms
were refined with anisotropic displacement parameters. All hydrogen atoms
3
-1
librium constant of 8 × 10 M , or more conveniently
2
were treated as idealized contributions. RF(wRF ) ) 0.0492 (0.1287), GOF
expressed in terms of oxygen pressure above the solution,
)
1.040. All scattering factors and anomalous dispersion factors are
-
1
K ) 60 atm at 30 °C in hydrocarbon solvents. A similar
contained in the SHEXTL 5.10 program library (Sheldrick, G. M. Bruker
AXS, Madison, WI, 1997).
analysis for HP-136 would suggest an equilibrium constant
900
Org. Lett., Vol. 2, No. 7, 2000