The natural instability and breakup of electrified cone jets leads to the formation of chargeddroplets with size and charge distribution of the droplets governed by the physical properties
and electrospraying conditions under consideration. This thesis develops a leaky-dielectric
model to study the axisymmetric breakup of an electrified jet, using the phase field method
to treat interfacial phenomena. The model is used to analyze the breakup in a wide range
of the Taylor number (Γ), the Ohnesorge number (Oh) and the wavenumber relevant to
electrosprays operating in the cone-jet mode. The phase field technique accurately captures
the behavior of the jet after pinch-off and predicts the formation of primary and satellite
droplets. The numerical results are compared with existing experimental and numerical
studies, extending them to account for the formation of sub-satellite droplets. It is found that
for highly viscous jets, Oh ≫ 1, the number of sub-satellite droplets generated increases with
the Taylor number when compared to low viscous jets, hence widening the size distribution of
droplets. At fixed Γ and Oh the primary droplets are charged to an approximately constant
ratio of the Rayleigh charge limit, regardless of the wave number. Furthermore, the primary
droplets are charged below the Rayleigh limit for Γ ≲ 1.5, and charged above the Rayleigh
limit when Γ ≳ 1.5. Thus, most primary droplets are expected to be unstable at Taylor
numbers exceeding 1.5.