A simple way to derive Bardeen's tunneling theory is introduced. With
a low rate of tunneling of, for example, electrons from one electrode
to another through a wide vacuum gap, the appearance of the second ele
ctrode can be regarded as a perturbation. Then Bardeen's formula for t
unneling follows exactly from Fermi's golden rule, supposing that this
perturbation appears suddenly at some instant of time. Bardeen's theo
ry is illustrated by assuming a smoothly variable barrier shape, inclu
ding the rectangular one as a limiting case. This exactly solvable exa
mple clarifies the sensitivity of the tunneling probability to the bar
rier shape and the energy of the tunneling particle. (C) 1995 American
Association of Physics Teachers.