Supersonic molecular beam techniques were used to study the dynamics o
f direct C2H6 and C2D6 dissociation on Pt(111). The initial dissociati
on probabilities for both isotopes, SO(C2H6) and SO(C2D6), increased w
ith normal translational energy, E(n), over the entire range of E(n) s
tudied. A significant normal kinetic isotope effect was observed; the
ratio S0(C2H6)/S0(C2D6) decreased from 2.7 to 1.6 as E(n) was increase
d from 80 to 118 kJ/mol. A one-dimensional quantum mechanical tunnelin
g model based on an Eckart potential barrier quantitatively accounts f
or these observations. After correcting for translational energy dissi
pation to the lattice, the extracted barrier heights, V0, and widths,
L, are 123 kJ/mol, 1.1 angstrom and 130 kJ/mol, 1.1 angstrom for C2H6
and C2D6, respectively. The larger barrier height for the direct disso
ciation of C2D6 relative to C2H6 Can be attributed to differences in z
ero point energy for C-H(D) stretching motion. Neither S0(C2H6) nor SO
(C2D6) exhibited a dependence on nozzle temperature in these experimen
ts suggesting that excitation of the normal vibrational motions of met
hyl rocking and deformation, C-C stretching and torsion do not promote
direct ethane dissociation on Pt(111) under these experimental condit
ions.