Penn State Center for Acoustics and Vibration · TBL model: Modified Chase-Howe Corcos Flow...
Transcript of Penn State Center for Acoustics and Vibration · TBL model: Modified Chase-Howe Corcos Flow...
Penn State
Center for Acoustics and Vibration
Structural Vibration and Acoustics Group
Presented as part of the 2012 CAV Spring workshop
Stephen Hambric, Group Leader
15 May 2012
Marty Trethewey Sabih Hayek
Stephen Conlon John Fahnline
Andrew Barnard Robert Campbell
Tim McDevitt Kevin Koudela
Tony Jun Huang Dan Linzell
Micah Shepherd
2/31 15 May 2012
CAV Overview
• Some project highlights – Quiet rotorcraft roof panel study with NASA
• Student Research – Effects of cabin pressurization on TBL-excited panel response
– Parallel acoustic boundary element procedures
– Recharacterization of the CAV hemi-anechoic room
– Fluid-structure interaction of flow-excited cylinder (a precursor to
propeller crashback)
– Static effects on vibration-based structural health monitoring
• Future Projects
• Important upcoming conference
3/31 15 May 2012
CAV
Development of Acoustically Tailored
Composite Rotorcraft Fuselage Panels
Principal Investigators: S.A. Hambric and K.L. Koudela
[email protected], [email protected]
Sponsor:
Collaborators:
4/31 15 May 2012
CAV NASA NRA Project
• Development of
Acoustically
Tailored Composite
Rotorcraft Fuselage
Panels
– Joint with Bell
Helicopter and
Kansas State
University
– Combine treatments:
• Embedded
viscoelastomers
• Band-gap systems
• Tailored composites
5/31 15 May 2012
CAV Assess Baseline Panel
• Beam roof
frame
• Honeycomb
core sandwich
panel center
6/31 15 May 2012
CAV Baseline Panel in NASA SALT
7/31 15 May 2012
CAV Baseline Panel FE and BE Model
• Virtual Transmission Loss analysis with diffuse acoustic
field excitation cross-spectral densities
8/31 15 May 2012
CAV Baseline Panel Transmission Loss
9/31 15 May 2012
CAV Next Steps
• Design and build optimized quiet roof panel
• Test in NASA SALT and compare performance to that
of baseline panel
10/31 15 May 2012
CAV
Optimization of Aircraft Panels Excited by
Turbulent Boundary Layer (TBL) Flow
Advisor: S.A. Hambric
Student: Micah Shepherd (PhD, Acoustics)
Sponsor:
11/31 15 May 2012
CAV Initial Study – Effects of Ribs and
Pressurization on Panel Response
Acoustic radiation
Aircraft panel
1 1
M M
P mnrad m nn m
G r G
HffG h G h
Tff FFG G
{ }
FF p
kk y c y jkx c x c x
G
e e e
12/31 15 May 2012
CAV NASA Designed Test Panel
Stringer thickness: 1 mm
Ring frames thickness: 1.27 mmPanel thickness: 1.27 mm
Critical frequency: 9.5 kHz
Clamped boundary conditions
13/31 15 May 2012
CAV FE Model
15568 linear quad elements
Stringer thickness: 1 mm
Ring frames thickness: 1.27 mmPanel thickness: 1.27 mm
14/31 15 May 2012
CAV Effects of Ribs on Noise
Flow speed: 210 m/s (Uc=147 m/s)
TBL model: Modified Chase-Howe
Corcos
Flow characteristics*: 32,000 ft
Decay constants: α1=0.07, α3=0.70
Assumed damping: 0.01
*Flight data provided by D. Palumbo, NASA Langley
( kx / kc = 50 – 1.3 )
f
15/31 15 May 2012
CAV Effects of Pressurization on Noise
• Cabin pressurization has little effect on isotropic
panels but large effect on ribbed panels
• Pressure loading of 34474 N (5 psi, 25,000ft) applied
to panel
• Modes, wavenumbers and radiated sound power
recalculated
• Temperature effects not included
16/31 15 May 2012
CAV Effects of Pressurization on Noise
Flow speed: 210 m/s (Uc=147 m/s)
TBL model: Modified Chase-Howe
Corcos
Flow characteristics*: 32,000 ft
Decay constants: α1=0.07, α3=0.70
Assumed damping: 0.01
( kx / kc = 50 – 1.3 )
f
17/31 15 May 2012
CAV Next Steps
• Develop procedure to find optimal rib locations for
minimizing key radiating modes
– Attempt to use global optimization routines
– Need fast concept analyses
– Modal approach with component mode synthesis
• Constraints on static response and stress
18/31 15 May 2012
CAV
Parallel Solutions for Rotationally
Symmetric Acoustic Boundary Element
Computations
Advisors: J.B. Fahnline, S.M. Shontz
Student: Ken Czuprynski (M.S. Computer Engineering)
Sponsor:
19/31 15 May 2012
CAV Block Circulant BE Acoustic
Matrices
Ax b
1 2 3 4A A A A A
1 2 3 4
4 1 2 3
3 4 1 2
2 3 4 1
A A A A
A A A AA
A A A A
A A A A
Throw away
X Y
Z
V 2
Rotational symmetries
provide block circulant
structure
Store only the
unique blocks.
Solve and reassemble full solution using parallel processing
20/31 15 May 2012
CAV Block Circulant BE Acoustic
Matrices
Number of processors
Speedup improves with problem size
21/31 15 May 2012
CAV
Behavior of Marine Propellers in
Crashback Conditions
Advisors: S.A. Hambric and R.L. Campbell
[email protected], [email protected]
Student: Abe Lee (PhD, Acoustics)
Sponsor:
22/31 15 May 2012
CAV Initial Study – cylinder in cross
flow
23/31 15 May 2012
CAV
Re-characterization of the
CAV Anechoic Room and Transmission
Loss Suite
Advisor: A.R. Barnard
Student: Paul Bauch (M.S. Acoustics)
Sponsor:
24/31 15 May 2012
CAV Instrumentation and Data
Acquisition
Traverse Method ISO 3745 (2003)
• 70 points in space
• 12 traverse paths
• 50 to 10k Hz range
CAV TL Suite – Anechoic Chamber (V=93.24m3)
Rev
erb
Room
(V
=132.4
0 m
3)
TL Window (0.9 m X 0.9 m) Traverse Paths
25/31 15 May 2012
CAV Results so far…
• Hemi-anechoic at low frequencies.
• Transitions towards fully anechoic at
frequencies above 5 kHz due to carpeting.
• Deviation from free field is within allowable
tolerance described in ISO 3745 for f < 10kHz.
• Further study at frequencies 10kHz< f < 20kHz
is in progress.
0 0.5 1 1.5 2 2.5 3-4-3-2-101234
Deviation from free field propagation f < 630 Hz
Distance from Physical Source Center (m)
Devia
tion (
dB
)
Measured Dev. 95% confidence
Acceptable Dev.
0 0.5 1 1.5 2 2.5 3-4-3-2-101234
800 < f < 5000 Hz
Distance from Physical Source Center (m)
Devia
tion (
dB
)
0 0.5 1 1.5 2 2.5 3-4-3-2-101234
6300 < f < 10,000 Hz
Distance from Physical Source Center (m)
Devia
tion (
dB
)
500 1k 1.5k 2k 2.5k 3k 3.5k 4k 4.5k 5k100
120
140
160
180
Frequency (Hz)
Norm
aliz
ed S
PL r
ef.
20
Pa/(
m3/s
)
CAV Anechoic Chamber Experimental vs. Theory (Traverse #4 pos. 5)
Experimental (FRF)
Hemi-Anechoic
Full-Anechoic
26/31 15 May 2012
CAV
Investigation of Static Load Effects on
Vibration Based Structural Health
Monitoring
Advisor: S.C. Conlon
Student: Justin Long (B.S. Aerospace Engineering)
Sponsor:
27/31 15 May 2012
CAV Research Focus
Justin was awarded the Anthony E. Wolk Senior Thesis Award
Quantify static loading effects for active vibration based damage detection
Develop procedures to enhance / optimized damage detection
• Varying tensile and compressive load conditions
can effect the vibrational characteristics of
damage
Beam-skin Joint
Lap Joint
UH-60A Black Hawk:
Transmission Frame
28/31 15 May 2012
CAV Key Outcomes
• Increased static loading results in decreased detection sensitivity
• Challenge for newly emerging nonlinear vibration based NDE techniques
• Significant sensitivity regained by re-optimizing (active) drive frequency & amplitudes
• Sensitivity can even be enhanced in the case of compressive loads
• Study also showed nonlinear vibration based detection features outperformed linear counterparts
• Important results for future development of embedded SHM systems
Critical fatigue damage zones –
significant static / quasi-static
loading
29/31 15 May 2012
CAV Future Projects
• Modeling of sonic fatigue
in jet engine discharge
regions
– CFD simulations of nozzle
and discharge flow (led by
Dr. Phil Morris, Aerospace)
– Finite element and/or
Statistical Energy Analysis
simulations of nozzle and
discharge panel response
(led by Drs. Hambric and
Campbell)
• Students: Matt Shaw
(PhD, Acoustics), Unmanned Air Vehicle(UAV)
30/31 15 May 2012
CAV Future Projects – DoE Cyber
Wind Facility
WAKE-
TURBINE
INTERACTIONS
(wind plant)
*BLADE AND *TOWER
ELASTIC DEFORMATION
(FEM + Modal model)
*BLADE AERODYNAMICS,
SPACE-TIME LOADINGS
(Hybrid URANS/LES + Overset)
WAKE TURBULENCE
BLADE-WAKE-ATMOSPHERE
(Actuator Vortex Body
Embedding within LES)
MESO-SCALE, WEATHER
(URANS)
*MARINE ATMOSPHERIC
BOUNDARY LAYER
TURBULENT WINDS
(4-D LES + Overset)
*sensors,
controllers,
diagnostics
*PLATFORM-WAVE
HYDRODYNAMICS
6-DOF MOTIONS
(Hybrid URANS/LES
+VOF+ Overset)
*Shaft Torque, *Gearbox Loadings
• Objective: Develop a “Cyber Wind Facility” to generate the
highest fidelity, most well-resolved 4-D data possible
simultaneously over an entire off-shore wind turbine
• Involves high-performance computing of fully-coupled
CFD/CSD for turbine-platform-wake interactions with the
atmosphere and ocean
• James Brasseur (ME, PI)
• Eric Paterson (ARL/ME, Co-PI)
• Sven Schmitz (AERSP, Co-PI)
• Robert Campbell (ARL, Co-PI)
31/31 15 May 2012
CAV Welcome to the Big Apple
Inter-Noise 2012
Quieting the World’s Cities
New York City , USA
19-22 August 2012
Stephen Hambric, General Chair
Stephen Conlon, Technical Chair
www.internoise2012.com
NCAD
Strong Participation Over 1000 papers expected (1430 abstracts)
1200-1500 attendees
70 exhibitors