A comparison is made between the Bohm trajectory and Feynman path appr
oaches to the long-standing problem of determining the average time ta
ken for a particle described by the Schrodinger wave function psi to t
unnel through a potential barrier. The former approach follows simply
and uniquely from the basic postulates of Bohm's causal interpretation
of quantum mechanics; the latter is intimately related to the most fr
equently cited approaches based on conventional interpretations. Empha
sis is given to the fact the fundamentally different transmission (T)-
reflection (R) decompositions, particlelike and wavelike respectively,
are central to the two methods: \psi\(2) = [\psi\(2)](T) + [\psi\(2)]
(R) (Bohm trajectory approach); psi = psi(T) + psi(R) (Feynman path ap
proach).