The modulational instability development of Langmuir and electromagnet
ic waves is reviewed in highly collisional plasmas where the character
istic frequency OMEGA of the modulated perturbations is much less than
nu(eff), the effective electron collision frequency. All calculations
are based on Braginskii's system of hydrodynamic equations in collisi
on-dominated plasmas and use a simple and universal formalism includin
g new methods developed for description of the modulational effects in
arbitrary media. It is demonstrated that the modulational instability
for the situation considered is mostly determined by collisional effe
cts (differential Joule heating nonlinearity), in contrast to the well
known modulational instability in collisionless plasmas (where pondero
motive force nonlinearity dominates). Rates and thresholds of the inst
abilities are found in various limits. Coupled nonlinear Langmuir and
sound waves are presented. Theory taking into account combined effect
of the differential Joule heating, ponderomotive force and relativisti
c electron mass variation on the instability of electromagnetic waves
is presented. Effects of magnetic fields are briefly discussed.