The rate constants, k
q, for the exothermic
energy transfer from the triplet states of benzophenone
(3BZP*)
and triphenylene (3TPh*) to naphthalene (N), and also
from the singlet sate of triphenylene (1TPh*)
to
benzophenone (BZP), were measured in polar and nonpolar solvents as a
function of pressure at 25 °C. For
all the systems of the donor−acceptor pairs, the plots of
k
q against 1/η showed downward curvature.
For
3BZP*/N in acetonitrile, methanol, and
n-hexane, the plots of ln k
q against
ln η were linear with the slopes
larger than −1, while for 3BZP*/N in toluene and for
1TPh*/BZP in n-hexane they showed downward
curvature.
However, the plots of 1/k
q against η were
linear with positive intercepts for all the systems examined. It
was
also found that the plot of 1/k
q against
η/T, in which k
q was measured for
3BZP*/N as a function of temperature
and pressure in n-hexane, is linear. These results were
interpreted by the energy transfer mechanism via the
formation of an encounter complex between the donor and acceptor
molecules, and it was concluded that the
exothermic energy transfer examined in the present study is not fully
diffusion-controlled but competes with
a diffusion process that is expressed by a modified Debye equation.
The bimolecular rate constants for the
energy transfer, k
bim
(=k
diff
k
et/k
-
diff),
were in the range of (1−10) × 1010
M-1 s-1 depending
on solvent. The
pressure dependence of k
et is discussed from the
experimental fact that k
bim is independent of
solvent viscosity
changed by varying pressure and temperature in all the systems
examined.