Dc. Tardy et al., IONIZATION-ENERGY OF TERT-BUTYL-D(9) ALCOHOL AND THE APPEARANCE ENERGY OF PROTONATED ACETONE - A NONEQUILIBRIUM DISSOCIATION, Journal of physical chemistry, 100(20), 1996, pp. 8144-8150
In the present photoionization study of tert-butyl alcohol, the parent
ion of the deuterated isotopomer [(CD3)(3)-COH] was observed and an i
onization energy (IE) of 9.82 +/- 0.02 eV was derived from a step-func
tion threshold at 126.25 nm. The appearance energies (AE's) of (CD3)(2
)COH+ and (CH3)(2)COH+ were also determined (at 298 K) to be 9.84 +/-
0.02 and 9.86 +/- 0.02 eV, respectively. From these results, the IE of
undeuterated tert-butyl alcohol (which was not observed) was estimate
d to be 9.84 +/- 0.03 eV. The difference between the IE and the derive
d AE(0) (AE = 10.01 +/- 0.03 eV at 0 K) implies an upper limit of 0.17
+/- 0.04 eV for the barrier to dissociation of (CH3)(3)COH+. A recent
evaluation of the proton affinity of acetone was employed to derive a
value of 5.40 +/- 0.10 eV for Delta(f)H degrees(0)[(CH3)(2)COH+] and,
thence, the enthalpy of reaction, Delta(f)H degrees(0) = 9.87 +/- 0.1
1 eV; and from this, an upper limit of 0.14 +/- 0.11 eV for the revers
e barrier of the dissociation was obtained. RRKM calculations were per
formed by using the energies derived from the experimental (and estima
ted) values. For excitation energies greater than or equal to 0.2 eV a
bove threshold, RRKM calculations yield large rate coefficients for di
ssociation. Also, the kinetic energy release (KER) was calculated for
various models of the dissociation complex. The calculated KER's are c
onsistent with experimental values when it is assumed that only 5 of t
he 38 vibrational modes of the transition state are active in the rand
omization of internal energy.