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A cascade atomization
and drop breakup model in STAR-CD
Ossi Kaario, Technical
Research Centre of Finland, Martti Larmi, Helsinki
University of Technology, Finland,
Franz Tanner, Michigan Technological University, USA
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The
breakup of liquid fuel jets in diesel combustion engines
plays a decisive role in the
evolution of the spray and its subsequent processes;
it has a direct influence on an efficient and clean
engine operation. Recent investigations conducted by
various researchers, utilizing different experimental
techniques, show that transient, high-pressure-driven
fuel jets are broken into liquid fragments of various
shapes and sizes at the time they exit the injector
nozzle or shortly thereafter. Subsequently, these liquid
fragments are subject to aerodynamic forces, which
lead to further breakups until the droplets reach a
stable state. The fundamental mechanisms responsible
for the aerodynamic breakup are either the Rayleigh-Taylor
or Kelvin-Helmholtz instability on the liquid/gas interface.
The Enhanced Taylor Analogy Breakup
(ETAB) model simulates this liquid jet disintegration
process as a cascade of drop breakups. The breakup
criterion is determined by Taylor's linear drop deformation
dynamics and the associated drop breakup condition.
Breakup occurs when the normalized drop distortion
exceeds a critical value. The breakup into product
droplets is modeled after the experimentally observed
bag or stripping breakup mechanisms and the radial
velocities of the product droplets are derived from
an energy conservation consideration.
At the nozzle
exit, the liquid jet is simulated as a sequence of
large, high velocity drops which are very unstable.
In order to avoid an immediate breakup, they are
assigned a deformation velocity such that their lifetime
is extended to match experimentally observed jet
breakup lengths. This computational artifice leads
to the simulation of a fragmented liquid core, as
reported by various research groups. An additional
benefit of this initial breakup delay is the radial
velocity of the product droplets at first breakup,
which results in an automatic adjustment of the spray
cone angle to changes in the gas density. On the
other hand, the model requires an initial drop size
distribution in order to compensate for the neglect
of the surface stripping near the nozzle exit. This
phenomenon determines the fuel-air mixing near the
nozzle exit, and has a strong influence on the ignition
location. The performance of the ETAB model has been
compared with the WAVE model, as implemented in STAR-CD,
and with measurements obtained under controlled conditions
from a constant volume bomb. The simulations showed
good overall agreement with experimental data, especially
the drop sizes were well predicted. In addition,
the amount of model tuning for a particular injection
condition is considerably reduced due to the automatic
adjustment of the spray cone angle to the changes
in the gas density.
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Top: Spray penetrations for the ETAB and WAVE
computations compared with experimental data
Bottom: Drop
sizes expressed as Sauter mean diameter (SMD) for
the ETAB and WAVE computations compared with experimental
data
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