The breaking of internal waves propagating in a stratified fluid of constan
t buoyancy frequency on a sloping boundary was investigated numerically. It
was found that at the boundary, nonlinear non-resonant interactions betwee
n the incident and reflected waves produced higher-mode waves. These modes
had frequencies greater than the local buoyancy frequency and so could not
radiate from the interaction region. The energy level of trapped waves incr
eased with time and subsequently led to overturning of the density field. A
t the critical frequency, when the reflected wave propagated in a direction
parallel to the slope, wave overturning occurred near the wall, but the po
int of overturning moved off the bottom as the propagation angle changed aw
ay from that of the bottom slope as the waves became increasingly supercrit
ical. The internal wave reflection coefficient generally increased as the e
ffects of nonlinearity and viscosity decreased, but depended strongly on th
e forcing frequency and the angle of the sloping boundary.