The relationship between the free wave motion and the natural flexural
modes of beams is re-examined. The reflection of both propagating and
evanescent waves, incident upon a linearly constrained boundary, is f
irst analyzed. Boundary conditions are identified which cause no evane
scent wave to be reflected when a propagating wave is incident, and vi
ce versa. The phase differences between the incident and reflected wav
es are analyzed for the case in which two waves (one propagating and o
ne evanescent) are incident. The phase-closure principle is formally p
roved for single span uniform beams and is used to set up the exact fr
equency equation for a fully fixed beam. Whereas the principle has tra
ditionally been applied to the propagating wave motion, it is applied
in this paper also to the evanescent wave motion. Frequency equations
having quite different forms are thereby obtained, but they have ident
ical roots. A physical interpretation becomes obvious for the conventi
onal frequency equation for the fully fixed beam.