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Rotorcraft Aeroacoustics
An Introduction
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Preliminary Remarks
Rotorcraft Noise is becoming an area of
considerable concern to the community.
United States and most European
countries have stringent limitations of
acceptable noise levels.
Any new design must be done with these
limitations, to avoid unpleasant surprises
during certification time.
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Some Definitions
Sound Pressure Level is measured in
Decibels.
PressureSquareMean
102
,
log10log20
2
2
5
Re
2
Re
2
10
Re
10
p
m
Np
where
p
p
p
pSPL
f
ff
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Overall Sound Pressure Level, OASPL
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Weighting
A Weighting: Emphasizes sound
frequencies that people here best.
Perceived Noise Level (PNL) weighting:
The most annoying frequencies are
weighted more than others.
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Typical dB Levels
Hearing Threshold: 0 dBA
Whisper : 20 dBA
Quite Neighborhood: 40 dBA Normal Speech: 60 dBA
Busy Office: 80 dBA
Heavy Traffic: 100 dBA Discotheque 120 dBA
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Flight Tests
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Why Flight Tests? Why Flight Test?Wind-tunnel tests provide precise, repeatable control of rotor
operating conditions, but accurate noise measurements are difficult for several
reasons: Wall effects prevent the rotor wake from developing exactly as it does in free
flight. This is crucial because an important contributor to rotor noise is theinteraction between the rotor and its own wake (such as blade-vortexinteraction).
In many wind-tunnel tests, the rotor test stand is not the same shape as the
helicopter fuselage, hence aerodynamic interference between the test stand androtor is different than in flight.
The wind-tunnel walls cause reflections that may corrupt the acoustic signals.
The wind tunnel has its own background noise, caused by the wind-tunnel driveand by the rotor test stand. (The YO-3A aircraft is actually quieter than many
wind tunnels.)
The wind tunnel turbulence level is rarely the same as in flight.
The rotor is frequently trimmed differently in a wind-tunnel test than in flight.
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Wind Tunnel Tests
http://halfdome.arc.nasa.gov/research/IRAP-intro.html
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Flight Test vs. Wind Tunnel Tests
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Noise Abatement: Quite Approach
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Cabin Noise Reduction with
Actuators
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Kirchoff Formulation
f(x,y,z,t):Rotor Surface
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Ffowcs Williams-Hawkings Formulation
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FWH Formulation (Continued)
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FWH Formulation (Continued)
Stress Tensor that includes pressure,
Comes from a CFD analysis
Integration is over rotor surface
Mr is Mach number of a source on the blade along r
R: distance between point on the blade and observer
Ret: Retarded time, that is time at which noise left the rotor
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BVI Noise Predictions with
Computed Loads
Surface pressure input
From RFS2BVIa code
Jointly developed at Ga Tech
And Boeing Mesa.
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Coupling of Acoustics Solver to CFD Codes
and Comprehensive Codes
Provides trim,
Blade dynamics,
Elastic deformations
Provides surface Pressures
As a function of time all
Over the blade surface
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Concluding Remarks
Outputs from CFD codes (or even lifting
line/blade element theory) can be input
into aeroacoustic codes, that solve the
wave equation in integral form.
Satisfactory agreement is obtained for
thickness, lift, and shock noise sources
with these approaches.