Effect of fluidic injections near the end of potential core for a Mach 0.5 subsonic jet
ORAL
Abstract
Although jets are known to be most receptive at the nozzle
exit, the most energetic sound sources are located a few jet
diameters downstream: near the end of the jet potential core.
Hence, fluctuations introduced at the nozzle exit of a turbulent jet
do not necessarily reach its intended target. In this work instead,
we introduce such disturbances via a fluidic injection system at
several locations downstream of the nozzle exit, including those
near the end of potenital core, to study their effect on the
radiated sound. In our experiments, the fluidic injection is
achieved via a newly-designed array of six equispaced minijets
acting on a core Mach 0.5 jet. A second injection system, located at
a fixed distance just upstream of the nozzle exit, with six
equispaced injectors is also used. Both the injection systems are
operated in our experiments steadily for different mass flow ratios. The latter
upstream injection system serves as the reference case and our goal
is to investigate how the downstream injections alter the radiated
sound over systems that perform fluidic injections near
the nozzle exit. For our analyzed downstream injection cases,
fluidic injection alter the centreline velocity decay and its
turbulent fluctuations via reducing the corresponding Reynolds
stresses of the core jet. This yields in a reduced peak sound at all the measured directivity
angles, but especially at the downstream shallow angles. In
contrast, when the jet is injected via the upstream system, the
radiated sound at all angles only show minor changes.
exit, the most energetic sound sources are located a few jet
diameters downstream: near the end of the jet potential core.
Hence, fluctuations introduced at the nozzle exit of a turbulent jet
do not necessarily reach its intended target. In this work instead,
we introduce such disturbances via a fluidic injection system at
several locations downstream of the nozzle exit, including those
near the end of potenital core, to study their effect on the
radiated sound. In our experiments, the fluidic injection is
achieved via a newly-designed array of six equispaced minijets
acting on a core Mach 0.5 jet. A second injection system, located at
a fixed distance just upstream of the nozzle exit, with six
equispaced injectors is also used. Both the injection systems are
operated in our experiments steadily for different mass flow ratios. The latter
upstream injection system serves as the reference case and our goal
is to investigate how the downstream injections alter the radiated
sound over systems that perform fluidic injections near
the nozzle exit. For our analyzed downstream injection cases,
fluidic injection alter the centreline velocity decay and its
turbulent fluctuations via reducing the corresponding Reynolds
stresses of the core jet. This yields in a reduced peak sound at all the measured directivity
angles, but especially at the downstream shallow angles. In
contrast, when the jet is injected via the upstream system, the
radiated sound at all angles only show minor changes.
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Presenters
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Arnab Samanta
Indian Institute of Technology Kanpur (IIT), Indian Institute of Technology, Kanpur, India
Authors
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Arnab Samanta
Indian Institute of Technology Kanpur (IIT), Indian Institute of Technology, Kanpur, India
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Ambica Singh
Indian Institute of Technology Kanpur
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Arun K Perumal
Indian Institute of Technology Kanpur