Title: TEXAS A
1 -
- TEXAS AM CENTER FOR SPACE POWER
- AT NORTHRUP GRUMMAN
- 01 AUGUST 2006
- PRESENTATION II - RELATED CAPABILITIES
- Dr. Alan Palazzolo, Clinton Johnson
- Erwin Thomas
2- Background
- The Vibration Control and Electromechanics Lab
VCEL at TAMU was Founded by Dr. Palazzolo in
1986. - Specialty Areas Magnetic Bearings for Flywheels
and Turbomachinery, High Temperature (1,000F
Magnetic Bearings and Motors), Rotordynamics,
Machinery and Structural Vibration Control,
Active Vibration Control, Bearing and Seal
Analysis - Sponsors Include TAMU Center for Space Power,
NASA Glenn, NASA Marshall, Office of Naval
Research, TAMU Turbomachinery Research
Consortium, US Flywheels, Optimal Energy
(Flywheels), Rockwell Scientific,Korean Institute
of Metals and Materials
3- Achievements (General)
- 50 Archival Journal Publications
- 6M Funded Research
- 1 US Patent Magnetic Bearing Controller for High
Power Density Flywheels - 1 US Patent Pending Redundant / Fault Tolerant
Magnetic, Homopolar Magnetic Bearings - 1 RD 100 Award High Temperature Magnetic
Bearing (1,000 F)
4- Achievements (Flywheel Magnetic Bearing Related)
- Supplied Magnetic Bearing Digital Controller and
Commissioning Services for Initial Startup of 40
krpm and 60 krpm (DEV-1) Flywheels at US
Flywheels Inc. - Designed and Built Magnetic Bearings for NASA
Glenn G2 Flywheels - Designed Magnetic Bearings for NASA Glenn G3
Flywheel - Supplied Magnetic Bearing Design, Digital
Controller, Commissioning Services and Power
Electronics for Optimal Energy Magnetic Bearing
Flywheel - Supplied a Digital Controller, Commissioning
Services and Power Electronics for Univ. of
Texas Train Flywheel - Designed and Built PLM (Preload Loss Monitor)
Flywheel Module Including the Magnetic Bearings
and Controller / Power Electronics / Sensor
System. Successfully Spun at 42,000 rpm on the
ground and at 0, 1 and 2 gs in the NASA Zero
Gravity Plane.
5Left DEV-1 , Top Right G2 (581 Watt-Hours),
Bottom Right G3 (2136 Watt- Hours)
6- Recent Publications
- Kenny, A. and Palazzolo, A., Single
Plane Radial, Magnetic Bearings Biased with Poles
Containing Permanent Magnets, ASME J. of
Mechanical Design, March 2003, Vol. 125, pp.
178-185. - Minihan, T., Lei, S., Sun, G. and
Palazzolo, A., Large Motion Tracking Control for
Thrust Magnetic Bearings With Fuzzy Logic,
Sliding Mode, and Direct Linearization, Journal
of Sound and Vibration, 263 (2003), 549-567. - Sun, G., Palazzolo, A., Provenza, A. and
Montague, G., Detailed Ball Bearing Model for
Magnetic Suspension Auxiliary Service, J. of
Sound and Vibration, Vol. 269, Issues 3-5, 22
January 2004, pp. 933-963. - Kenny, A., Palazzolo, A., Montague, G.
and Kascak, A., Theory and Test Correlation for
Laminate Stacking Factor Effect on Homopolar
Magnetic Bearing Stiffness, ASME J. of
Engineering for Gas Turbines and Power, Vol. 126,
January 2004, pp. 142-146. - Li, Ming Hsiu, Palazzolo,A., Kenny, A.,
Provenza, A., Beach,R., Kascak,A., Fault
Tolerant Homopolar Magnetic Bearings,
IEEE Trans. On Magnetics, Vol. 40, No. 5, Sept.
2004, pp. 3308 3318. - Provenza, A., Montague, G., Jansen,
M., Palazzolo, A., and Jansen, R., High
Temperature Characterization of a Radial Magnetic
Bearing for Turbomachinery, J. of Engineering
for Gas Turbines and Power. , v 127, n 2, April,
2005, p 437-444
7SOLID MODEL of PLM FLYWHEEL MODULE
8Flywheel Radial Magnetic Bearing
93D Electromagnetic Finite Element Model of G2
Bearing
10G2 Magnetic Bearing Design Correlation
Contour Plot of Gap Flux Density When Rotor
Offset .004 in from center Air Gap .016 to
.024 inch.
11Magnetic Bearing Control Diagram Showing CDMs
for Fault Tolerant Control (FTC)
12 Rotor Displacements in the Radial and
Axial Directions This example illustrates the FTC
operation. Both bearings have the same failure
combination, pole 1-2-3-4 failure. The power
amplifier (PA) failures initiate at 0.1 (s), and
the time delay for swapping CDMs is 20 (ms).
13 Currents in Combo Bearing
During Pole 1-2-3-4- Failure
14Sensor Development Test Rig in Vacuum Vessel
(55,000 rpm)
15- G2 Magnetic Bearing Stiffness Measurements
- Using a linear force model the bearing forces can
be modeled as where j signifies the corresponding
bearing (i.e. j CB, RB), And i signifies the
ith coordinate direction. Where
Magnetic bearing levitation force diagram
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17- G2 Magnetic Bearing Design Correlation
18G2 Magnetic Bearing Correlation Summary
G2 Radial Bearing Parameters G2 Radial Bearing Parameters G2 Radial Bearing Parameters G2 Radial Bearing Parameters G2 Radial Bearing Parameters
Predicted Value Predicted Value Measured Value Measured Value
Position Stiffness -6.16 lbs/mil -6.8 lbs/mil
Current Stiffness 8.8 lbs/Amp 10.4 lbs/Amp
Load Capacity 70 lbs 85 lbs
Bias Flux Density --- Tesla 0.82 Tesla
Pole Inductance 1.35 mH 1.2 mH
19G2 Combo Bearing Parameters G2 Combo Bearing Parameters G2 Combo Bearing Parameters G2 Combo Bearing Parameters G2 Combo Bearing Parameters
Predicted Value Predicted Value Measured Value Measured Value
Position Stiffness -6.9 lbs/mil -8.3 lbs/mil
Current Stiffness 9.3 lbs/Amp 8.5 lbs/Amp
Load Capacity 74 lbs 90 lbs
Bias Flux Density 0.82 Tesla --- Tesla
Pole Inductance 1.35 mH --- mH
20PLM Flywheel Mounted on Bottom of Spin Pit
Lid
21Empty Spin Pit and Pit With PLM Flywheel
Enclosed