American Helicopter Society, 65 th Annual Forum
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Transcript of American Helicopter Society, 65 th Annual Forum
American Helicopter Society, 65th Annual Forum
Measurements of Drag Torque, Lift-off Speed and Temperature in a Metal Mesh
Foil Bearing
Measurements of Drag Torque, Lift-off Speed and Temperature in a Metal Mesh
Foil Bearing
Luis San AndrésTae-Ho Kim
Thomas Abraham Chirathadam Keun Ryu
AHS Paper No. 080173
This material is based upon work funded by the TAMU Turbomachinery Research Consortium and donations from Honeywell Turbocharging Technologies
May 28, 2009
Gas foil bearings for rotorcraft applications
Elimination of complex oil lubrication system
Elimination of the requirement for sealing
Reduced system overall weight ( High power density)
Extended maintenance intervals
Enhanced reliability at high rotating speedsLarge inherent damping prevents potentially harmful rotor excursion
Low power loss
Can operate at elevated temperatures
Simple assembly procedure using cheap, commercially available materials
Metal Mesh Foil Bearing (MMFB)
MMFB COMPONENTS: Bearing Cartridge, Metal mesh ring and Top FoilHydrodynamic air film develops between rotating shaft and top foil.
Potential applications: ACMs, micro gas turbines, turbo expanders, turbo compressors, turbo blowers, automotive turbochargers, APU
Large damping (material hysteresis) offered by metal mesh
Tolerant to misalignment, and applicable to a wide temperature range
Suitable tribological coatings needed to reduce friction at start-up & shutdown
Cartridge
Metal mesh ring
TopFoil
TAMU past work (Metal Mesh Dampers)
Zarzour and Vance (2000) J. Eng. Gas Turb. & Power, Vol. 122
Advantages of Metal Mesh Dampers over SFDsCapable of operating at low and high temperaturesNo changes in performance if soaked in oil
Al-Khateeb and Vance (2001) GT-2001-0247
Test metal mesh donut and squirrel cage( in parallel)MM damping not affected by modifying squirrel cage stiffness
Choudhry and Vance (2005) Proc. GT2005
Develop design equations, empirically based, to predict structural stiffness and viscous damping coefficient
METAL MESH DAMPERS provide large amounts of damping. Inexpensive. Oil-free
MMFB ASSEMBLY
BEARING CARTRIDGE
METAL MESH RING TOP FOIL
Simple construction and assembly procedure
MMFB dimensions and specifications
Dimensions and SpecificationsBearing Cartridge outer diameter, DBo(mm) 58.15
Bearing Cartridge inner diameter, DBi(mm) 42.10
Bearing Axial length, L (mm) 28.05
Metal mesh donut outer diameter, DMMo (mm) 42.10
Metal mesh donut inner diameter, DMMi(mm) 28.30
Metal mesh density, ρMM (%) 20
Top foil thickness, Ttf (mm) 0.076
Metal wire diameter, DW (mm) 0.30
Young’s modulus of Copper, E (GPa), at 21 ºC
110
Poisson’s ratio of Copper, υ 0.34
Bearing mass (Cartridge + Mesh + Foil), M (kg)
0.316
PICTURE
Bearing cartridge
Top foil
Donut shaped metal mesh
Rotating shaft
Gas film
Ω
MMFB Rotordynamic test rig
(a) Static shaft
Max. operating speed: 75 krpmTurbocharger driven rotorRegulated air supply: 9.30bar (120 psig)
Test Journal: length 55 mm, 28 mm diameter , Weight=0.22 kg
Journal press fitted on Shaft Stub
TC cross-sectional viewRef. Honeywell drawing # 448655
Twin ball bearing turbocharger, Model T25, donated by Honeywell Turbo Technologies
Positioning (movable) table
Torque arm
Calibrated spring
MMFB
Shaft (Φ 28 mm)
String to pull bearing
Static load
Eddy current sensor
Force gauge
Top foil fixed end
Preloading using a rubber band
5 cm
Test Rig: Torque & Lift-Off measurements
Thermocouple
Test procedure
Sacrificial layer of MoS2 applied on top foil surface
Mount MMFB on shaft of TC rig. Apply static horizontal load
High Pressure cold air drives the ball bearing supported Turbo Charger. Oil cooled TC casing
Air inlet gradually opened to raise the turbine shaft speed. Valve closing to decelerate rotor to rest
Torque and shaft speed measured during the entire experiment. All experiments repeated thrice.
Journal speed and torque vs time
Rotor starts
Constant speed ~ 65 krpm
Valve open
Valve close
3 N-mm
Rotor stops
Applied Load: 17.8 N
Manual speed up to 65 krpm, steady state operation, and
deceleration to rest
Startup torque ~ 110 Nmm
Shutdown torque ~ 80 Nmm
Once airborne, drag torque is ~ 3 % of Startup ‘breakaway’
torque
Top shaft speed = 65 krpm
Iift off speed
Lift off speed at lowest torque : airborne operation
WD= 3.6 N
Varying steady state speed & torque
Rotor starts
61 krpm
Rotor stops
50 krpm
37 krpm
24 krpm
2.5 N-mm
57 N-mm 45 N-mm
2.4 N-mm 2.0 N-mm 1.7 N-mm
Manual speed up to 65 krpm, steady state operation, and
deceleration to rest
Drag torque decreases with step wise reduction in
rotating speed until the journal starts rubbing the
bearing
Shaft speed changes every 20 s : 65 – 50 – 37 - 24 krpm
Side load = 8.9 N
WD= 3.6 N
Startup torque vs applied static load
Worn MoS2 layer
Fresh coating of MoS2
Top foil with worn MoS 2
layer shows higher starup
torques
Larger difference in
startup torques at
higher static loadsStartup Torque : Peak torque measured during startup
Dry sliding operation
0
0.1
0.2
0.3
0.4
0.5
0 10 20 30 40Static load [N]
Fri
ctio
n c
oe
ffic
ien
t [-
]DRY friction coeff. vs static load
Worn MoS2 layer
Fresh MoS2 layer
With increasing operation
cycles, the MoS 2 layer
wears away, increasing the contact or dry-
friction coefficient.
Enduring coating on top foil
required for efficient MMFB
operation!
Friction coefficient f = (Torque/Radius)/(Static load)
Dry sliding operation
Bearing drag torque vs rotor speed
8.9 N (2 lb)
17.8 N (4 lb)
26.7 N (6 lb)
35.6 N (8 lb)
Rotor not lifted off
Dead weight (WD= 3.6 N)
Increasing static load (Ws) to 35.6 N
(8 lb)
0
0.5
1
1.5
2
2.5
3
3.5
4
4.5
20 30 40 50 60 70 80
Rotor speed [krpm]
Be
ari
ng
to
rqu
e [N
-mm
]
Steady state bearing drag
torque increases
with static load and rotor
speed
airborne operation
WD= 3.6 N
Side load increases
Data derived from bearing torque and rotor speed vs time data
Friction coefficient vs rotor speed
Dead weight
(WD= 3.6 N)
Increasing static load (Ws) to 35.6 N (8 lb)
f decreases with
increasing static load
Friction coefficient
f increases with rotor speed
almost linearly
airborne operation
Friction coefficient f = (Torque/Radius)/(Static load)
8.9 N (2 lb)
17.8 N (4 lb)
26.7 N (6 lb)
35.6 N (8 lb)
Bearing drag torque vs rotor speed
Lift-off speed
8.9 N (2 lb)
17.8 N (4 lb)
26.7 N (6 lb)
35.6 N (8 lb)
Max. Uncertainty ± 0.35 N-mm
Rotor accelerates
Bearing drag torque increases with increasing rotor speed and increasing applied static loads. Lift-Off speed increases almost linearly with static load
0
20
40
60
80
0 5 10 15 20 25 30Time [sec]
Sp
ee
d [
krp
m]
0
50
100
0 5 10 15 20 25 30Time [sec]B
ea
rin
g t
orq
ue
[N
-mm
]
Rotor accelerates
8.9 N (2 lb)
17.8 N (4 lb)
26.7 N (6 lb)
35.6 N (8 lb)
Friction coefficient vs rotor Speed
f ~ 0.01
Friction coefficient ( f )
decreases with increasing static
load
f rapidly decreases
initially, and then
gradually raises with increasing
rotor speed
Dry sliding Airborne (hydrodynamic)
Lift-Off speed vs applied static load
Lift-Off Speed increases ~
linearly with static load
Lift-Off Speed: Rotor speed
beyond which drag torque is
significantly small, compared
to Startup Torque
WD= 3.6 N
Side load increases
Top foil temperature (bearing outboard)
8.9 N (2 lb)
17.8 N (4 lb)
26.7 N (6 lb)
35.6 N (8 lb)
Top Foil Temperature
increases with Static Load and
Rotor Speed
Top foil temperature measured at MMFB
outboard end
Only small increase in
temperature for the range of applied
loads and rotor speeds
INCREASING STATIC LOAD
Side load increases
Room Temperature : 21°C
Conclusions Metal mesh foil bearing assembled using cheap, commercially available materials.
Bearing break away torque, during start up, increases with applied static loads. A sacrificial coating of MoS2 reduces start up torque
Bearing drag torque, while bearing is airborne, increases with static load and rotor speed
Top foil steady state temperature – increases with static load and rotor speed
Metal mesh foil bearing : Promising candidate for use in high speed oil-free rotorcraft applications