Resumen:
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[EN] Air assisted atomizers are widely used for various purposes, for example coating processes, medical processes,
and sprinkler. However, the spray development processes, especially the breakup phenomena are not ...[+]
[EN] Air assisted atomizers are widely used for various purposes, for example coating processes, medical processes,
and sprinkler. However, the spray development processes, especially the breakup phenomena are not fully
understood yet. Generally, the main breakup of the air assisted atomizer depends on whether the mixing is
internal or external. The border between these processes is not clear. In order to study changes in the spray
configuration due to the way of mixing, the spray was investigated for the transition from internal to external
mixing. Therefore, an air assisted atomizer which allows adjusting the distance between injector to cover was
used. The atomizer consists of two components, which are a liquid injector and an injector cover with orifice. The
atomization air flows through the gap between the injector and the cover. The position of cover orifice is able to be
traversed from the position fully attached to the injector to several millimetre distances from the injector nozzle. In
this study, the water spray characteristics depending on the air and liquid mixture position were investigated
experimentally by two optical measurement techniques.
Imaging techniques were used for taking the spray structure as well as liquid core in near nozzle field. The water
mass flow, atomization air mass flow, and the cover position were changed and their effects on the spray were
investigated. Phase Doppler Anemometer (PDA) was applied for measurement of velocity and size of droplets in
water spray which injected into the atmosphere. The measurement positions were set at planes which located on
20 and 40mm downstream from the nozzle orifice. For each downstream position, radial profiles of the spray
pattern were measured on one air to water flow rate condition. The cover positions were changed and the
differences on the droplet velocity and diameter as a function of radial distance on each nozzle cover positions
were discussed. Also, high resolution direct imaging technique has been developed and applied for measurement
of size of droplets. The results from these measurement techniques were compared and they correspond well at
the high air to water flow rate conditions. At the low air to water flow rate condition, the agreement of the results of
these measurements became lower. It might be caused by the bouncing unspherical droplets.
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