The instability of viscous capillary jets subject to disturbances cons
isting of two superposed wavenumbers, and for large disturbance amplit
udes is investigated. Disturbances composed of the superposition of a
fundamental disturbance (first harmonic) with either its second or thi
rd harmonic are used. The influence of the wavenumber of the fundament
al disturbance on the jet breakup is studied for a disturbance compose
d of a first harmonic with an initial non-dimensional amplitude of eps
ilon(1) = 0.01 and a second harmonic with an initial non-dimensional a
mplitude of epsilon(2) = 0.05. The influence of the initial amplitudes
of the first and second harmonics on the jet breakup is studied for t
wo non-dimensional wavenumbers of the fundamental (first harmonic): k
= 0.45 and k = 0.7; the second harmonic is unstable in the former and
stable in the latter case. The effect of an added third harmonic is st
udied only for k = 0.45 but for a wide range of initial amplitudes. Al
l cases are studied for an in-phase and a 180 degrees out-of-phase sup
erposition of the two waves. The nonlinear interaction between the two
waves results in the formation of a variety of drop sizes and shapes.
The breakup times can be controlled within a wide range using this te
chnique.