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Transcript of 1 Luis San Andrés Mast-Childs Professor Identification of SFD force coefficients Large Clearance...
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Luis San Andrés Mast-Childs Professor
Identification of SFD force coefficients
Large Clearance Open Ends SFDTRC-SFD-01-2012
Linear Nonlinear Force Coefficients for SFDs
32nd Turbomachinery Research Consortium Meeting
TRC Project 32513/1519FB
May 2012
2
Typical squeeze film damper (SFD) with a central groove
SFD with a central groove
Conventional knowledge regards a groove is indifferent to the kinematics of journal motion, thus effectively isolating the adjacent film lands.
housing
journal
lubricant film
shaft
anti-rotation pin
ball bearing
Feed
groove
oil inlet Pressurized lubricant flows
through a central groove to fill the
squeeze film lands.
Dynamic pressures in the film lands
generate reaction forces aiding to damp
excessive amplitudes of
rotor whirl motion.
3
P&W SFD test rig
Static loader
Shaker assembly (Y direction)
Shaker assembly (X direction)
Static loader
Shaker in X direction
Shaker in Y direction
Top view
Isometric view
SFD test bearing
4
Test rig description
shaker Xshaker Y
Static loader
SFD
base
support rods
X
Y
Shaker X Shaker Y
Static loader
SFD
Base
Static loader
X
Y
Support rods
X Y
5
SFD Test Rig – cut section
in
Test rig main features
Journal diameter: 5.0 inch
Film clearance: 9.9 mil
Film length: 2 x 1 inch
Support stiffness: 100 klbf/inBearing Cartridge
Test Journal
Main support rod (4)
Journal BasePedestal
Piston ring seal (location)
Flexural Rod (4, 8, 12)
Circumferential groove
Supply orifices (3)
6
Lubricant flow path
Oil inlet
in
ISO VG 2 oil
7
Objective & tasks
Evaluate dynamic load performance of SFD with a central groove.
Dynamic load measurements: circular orbits (centered and off centered) and identification of test system and SFD force coefficients
X
Y static load
e
c
45o
X
Y
r
eS
centered and off-centered circular orbits
8
Structure static stiffness
0
100
200
300
400
0 0.5 1 1.5 2 2.5 3 3.5 4
static radial eccentricity, (mil)
stat
ic r
adia
l lo
ad (
lbf)
e S
K S ~ 100 klbf/in
X
Y F
•Pull test using static loader to determine static structure stiffness
1780
1335
890
445
stat
ic r
adia
l lo
ad (
N)
(101.6 μm)
9
Structural parameters • Dry test system• Circular Centered Orbits • Frequency 50-210 Hz
DirectXX YY
US SI US SI
Stiffness Ks 107 klbf/in 19 MN/m 120 klbf/in 21 MN/m
Damping Cs 8 lbf-s/in 1.4 kN-s/m 9 lbf-s/in 1.6kN-s/m
Mass M -4 lb -2 kg -3 lb -1 kg
System Mass MBC 48 lb 22 kg 48 lb 22 kg
Natural frequency fns 148Hz 156Hz
Damping ratio ξs 4% 4%
10
SFD dimensions & operating conds. • Maximum static load 324 lbf
• Centered and off-centered, eS= 1, 2, and 3 mil• Frequency range: 50-210 Hz, Orbit amplitude r = 0.5 mil
ISO VG 2 OilViscosity at 73 oF [cPoise] 3.10
Density [kg/m3] 785
Inlet pressure [psig] 1.6
Outlet pressure [psig] 0
Radial Clearance [mil] 9.9
Journal Diameter [inch] 5.0
Central groove length [inch]& depth
0.5000.375
Land length, L [inch] 1.0 x 2
Total Length [inch] 2.5
Oil out, Qb
BaseSupportrod
Bearing Cartridge
Journal (D) Oil out, Qt
Oil in, Qin
Central groove
L
½ L
L
End groove
End groove
Oil outOil collector
c
11
SFD
Ks = 100 klbf/inMBC = 48 lb
Cs= 8-9 lbf-s/inNat freq = 148-156 HzDamping ratio = 4%
DRY system parameters
CSFD=Clubricated - Cs
MSFD=Mlubricated - MBC
KSFD=Klubricated - Ks
Difference between lubricated system and dry system (baseline) coefficients
SFD force coefficients
IVFM parameter identification method
X
Y
esc
45o
12
SFD force coefficients - theory
3* * *
tanh2 12 π 1XX YY
LR DC C C L
LcD
3* * *
tanhπ2 1XX YY
LLR DM M M
LcD
Centered journal (es=0), no lubricant cavitationTwo film lands separated by a plenum: central groove has no effect on squeeze film forces.
Damping
Inertia
Stiffness KXX = KYY = KXY=KYX=0 X
Y
13
SFD force coefficients - theory
3* * *
tanh2 12 π 1XX YY
LR DC C C L
LcD
3* * *
tanhπ2 1XX YY
LLR DM M M
LcD
Damping
Inertia
c=5.5 mil
C* = 7,121 N.s/m (40.7 lbf.s/in)
c=9.9 mil
C* = 1,255 N.s/m (7.16 lbf.s/in)
c=5.5 mil
M* = 2.98 kg (6.58 lbm)
c=9.9 mil
M* = 1.67 kg (3.69 lbm)X
Y
14
Experimental SFD damping coeffs.
• Open ends SFD• Circular orbits (r = 0.5 mil)
SFD (1 inch land lengths)
0
20
40
60
80
100
120
140
160
180
0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5
static eccentricity, e S (mil)
Dam
pin
g c
oef
fici
ents
(lb
f -s/in
)
C SFD
CXX c=9.9 mil
CYY c=9.9 mil
CYY c=5.5 mil
CXX c=5.5 mil
classical theory (7.1 lbf.s/in)
classical theory (40.6 lbf.s/in)
31.5 kNs/m
(89 μm)
X
Y
esc
45o
15
Experimental SFD inertia coeffis.
• Open ends SFDs• Circular orbits (r = 0.5 mil)
SFD (1 inch land lengths)
0
10
20
30
40
50
60
70
80
0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5
static eccentricity, e S (mil)
Ad
ded
mas
s co
effi
cien
ts (
lb)
M SFD
M XX c= 9.9 mil
M YY c= 9.9 mil
M YY c= 5.5mil
M XX c= 5.5 mil
classical theory (3.7 - 6.6 lb)
89 μm
36 kg
X
Y
esc
45o
16
Pressure sensors in bearing
Pressure sensor
Bottom Land
Pressure sensor locations
and
Central groove
and,
Central groove
Top Land
BC
25.4 mm
25.4 mm
Side view: Sensors located at middle plane of film lands
Top view: Sensors around bearing circumference
63.5 mm
12.7 mm
Pressure sensor
Pressure sensor
Pressure sensor
Bottom Land
Pressure sensor locations
and
Central groove
and,
Central groove
Top Land
BC
25.4 mm
25.4 mm
Side view: Sensors located at middle plane of film lands
Top view: Sensors around bearing circumference
63.5 mm
12.7 mm
Pressure sensor
Pressure sensor
17
Dynamic pressures: films & groove
0 1 2 3 410
5
0
5
10
top land (120 deg)bottom land (120 deg)
Pressures at film lands
time (-)
pres
sure
(psi
)
Whirl frequency 130 Hz
Number of periods
psi 0.69 barfilm lands
es=0, circular orbit r=0.5 mil. Groove pressure PG = 0.72 bar
0
-0.69 bar
Top and bottom film lands show
similar pressures.
Dynamic pressure in the groove is
not zero!0
0 1 2 3 44
2
0
2
4
groove (165 deg)groove (285 deg)
Pressures at central groove
time (-)
pres
sure
(psi
)
psigroove
0.28 bar
-0.28 bar
Number of periods
ASME GT2012-68212
18
Peak-peak lubricant pressures
0 100 2000
10
20
30Top land (120)Top land (240)Bottom land (120)Bottom land (240)Groove (165)Groove (285)
peak-peak pressures
frequency (Hz)
P-P
pre
ssur
e (p
si)
Frequency (Hz)
P-P
dyn
amic
pre
ssu
re (
psi
)
100 200
30
20
10
0
c=5.5 mil
groove
Lands(top & bottom)
207 (kPa)
Piezoelectric pressure sensors (PCB) location
Bearing Cartridge
bottom land
top land
groove
Mid-plane
19
0 100 2000
5
10
15Top land (120)Top land (240)Bottom land (120)Bottom land (240)Groove (165)Groove (285)
peak-peak pressures
frequency (Hz)
P-P
pre
ssur
e (p
si)
Peak-peak lubricant pressures
Frequency (Hz)
100 200
15
10
5
0
c=9.9 mil
groove
lands (top & bottom)
Piezoelectric pressure sensors (PCB) location
Bearing Cartridge
bottom land
top land
groove
Mid-plane
P-P
dyn
amic
pre
ssu
re (
psi
)
20
0 100 2000
1
2
3
4Top land (120)Top land (240)
peak-peak pressures
frequency (Hz)
P-P
pre
ssur
e (p
si)
Ratio of groove/film land pressures
Frequency (Hz)
P-P
pre
ssu
re r
atio
s
100 2000
c=5.5 mil
groovelands (top)
1.0
Groove generates
large hydrodyna
mic pressures!
3/8”~70 c
1 “ 0.5” 1”
21
0 100 2000
1
2
3
4Top land (120)Top land (240)
peak-peak pressures
frequency (Hz)
P-P
pre
ssur
e (p
si)
Ratio of groove/film land pressures
Frequency (Hz)
P-P
pre
ssu
re r
atio
s
100 200
1.0
c=9.9 mil
groovelands (top)
Groove generates
larger hydrodyna
mic pressures!!Larger than in the film!
1 “ 0.5” 1”
3/8”~35 c
22
z
LLG
do
Bearing
Journal
End seal
c : clearance
Lubricant in
Lubricant out
orifice
groove
film land
dG
D, diameter
Lubricant in
recirculationzone
Effective groove depth
streamline
Lubricant out
separation line
d
Lubricant in
recirculationzone
Effective groove depth
streamline
Lubricant out
separation line
d
Model SFD with a central groove
2
3 3 2
212
P P h hh h h
R R z z t t
SFD geometry and nomenclature
Solve modified Reynolds equation (with fluid inertia)
Use effective depth d=1.6c
23
19
1725
3341
49
57
65
73
81
89
S1
S8
0.00
0.10
0.20
0.30
0.40
0.50
0.60
circ coordinate (node #)
axial coordinate
0.5-0.6
0.4-0.5
0.3-0.4
0.2-0.3
0.1-0.2
0.0-0.1
Inner Film
Pressure
Feed hole (3 x 120 deg)
groove
land
z
Pressure (bar)
19
1725
3341
49
57
65
73
81
89
S1
S8
0.00
0.10
0.20
0.30
0.40
0.50
0.60
circ coordinate (node #)
axial coordinate
0.5-0.6
0.4-0.5
0.3-0.4
0.2-0.3
0.1-0.2
0.0-0.1
Inner Film
Pressure
Feed hole (3 x 120 deg)
groove
land
z
Pressure (bar)
Example predicted pressure field
Static pressure at
groove shows circumferenti
al variation due to feed
holes spacing
groove
3/8”~35 c
1 “ 0.5” 1”
24
0
20
40
60
80
100
120
140
160
180
200
0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0
static eccentricity, eS (mil)
Da
mp
ing
co
eff
icie
nts
(lb
f -s/in
)
CSFD
CXX c=9.9 mil
CYY c=9.9 mil
CYY c=5.5 mil
CXX c=5.5 mil
lines : predictions
symbols:test data
classical theory (7.1 lbf.s/in)
classical theory (40.6 lbf.s/in)
Damping coefficients: test & predictions
Model predicts
small c SFD: larger damping coefficient than
test values
large c SFD: less damping
than test values
25
Inertia coefficients: test & predictions
0
10
20
30
40
50
60
70
80
0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5 4.0
Ad
de
d m
ass
co
eff
icie
nts
(lb
)
MSFD
MXX c=9.9 mil
MYY c=9.9 mil
MYY c=5.5mil
MXX c=5.5 mil
classical theory (3.7 - 6.6 lb)
static eccentricity, eS (mil)
lines : predictions
symbols:test data
Classical theory
predicts ~ 1/7 of test values
Model predicts
small c SFD: less inertia than
test values
Large c SFD: larger inertia than
test values
26
Conclusions
• Central grove is NOT a zone of constant pressure: dynamic pressures as large as in film lands.
• Classical theory predicts too low SFD added masses: 1/7 of test values
•Using an effective shallow groove depth, new model predictions agree well with test results.
Conducted measurements of dynamic load response in large clearance (c=9.9 mil) open ends SFD with circular orbits, centered and off-centered.
27
P&W funded project (2012)
Modify test rig and construct SFD w/o a central groove, conduct measurements of film pressures and identify force coefficients.
28
Proposed tasks TRC (2012-13)
X
Y
X
Y
X
Y
elliptical orbitscircular orbits
centered journal off-centered journal
1. Test damper w/o groove with dynamic loads (20-300 Hz) inducing off-centered elliptical orbital motions to reach 0.8c.
2. Identify SFD force coefficients from test impedances, and correlate coefficients with linear force coefficients and experimental coefficients for smallest whirl amplitude (0.05c).
3. Perform numerical experiments, similar to the physical tests, to extract linearized SFD force coefficients from the nonlinear forces. Quantify goodness of linear-nonlinear representation from an equivalence in mechanical energy dissipation.
29
TRC Budget (2012-13)
X
Y
X
Y
X
Y
elliptical orbitscircular orbits
centered journal off-centered journal
eight months Year II
Support for graduate student (20 h/week) x $ 2,200 x 8 months $ 17,600
Fringe benefits (0.6%) and medical insurance ($197/month) $ 1,682
Travel to (US) technical conference $ 1,200
Tuition three semesters ($227 credit hour x 15 ch x 1.7 fees multiplicative factor)
$ 5,789
Supplies for test rig $ 2,200
Total Cost: $ 28,470
Year I started on Jan 2012
30
Acknowledgments
Thanks to • Pratt & Whitney Engines• Turbomachinery Research Consortium• Sung-Hwa Jeng, RA for making the presentation
Learn more
http:/rotorlab.tamu.edu
Questions (?)