1.3.2 Documents of Research Methodology Courses imparting ...
Introduction to Turbomachinery · Centrifugal Pump • rotor, stator – accelerate flow by...
Transcript of Introduction to Turbomachinery · Centrifugal Pump • rotor, stator – accelerate flow by...
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Pumping Machinery
2001 ASME Fluids Engineering Division Summer Meeting
Dr. Adiel Guinzburg
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What is Turbomachinery?
Using working fluids to Boostoutput,
either increase or decrease pressureby using Machinery
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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High Pressure Fuel Turbopump
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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High Pressure Oxygen Turbopump
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Turbomachine Classification
• Turbines. Pumps and Compressors• Incompressible. Compressible• Axial-flow, Mixed-flow, Radial-flow geometry• Single stage. Multi-stage• Turbo-pump. Turbo-compressor. Torque-converter• Impulse. Reaction
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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From Customer Requirements to Final Product
• Specification• Preliminary Design, Conceptual design, ...• Component Design• Component Test, Analysis• Acceptance Test• .....
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Design Trade-offs• Performance• Weight• Cost• Life• Reliability• Structural Strength• Maintainability• Envelope
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Design Process
• In-house design database - scale• Detail design
– (2D, Quasi 3D, CFD <=> stress analysis• Test Data Evaluation
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Turbomachine
]gz)2v(hgz)
2v[(hmPs in
2
out
2
++−++= &
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Turbines
• Impart Kinetic Energy to rotor as Mechanical Energy of rotation
• Impulse – high Pressure, low Flow
• Reaction– low Pressure, high Flow
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Pump Classification
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Centrifugal Pump
• rotor, stator– accelerate flow by imparting kinetic energy– decelerate (diffuse) in stator– results in increase in fluid pressure
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Elements of a Centrifugal Flow Pump
• From Huzel, D. K. and Huang, D. H.
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Rotor
• Inducer• Impeller• Bearings• Shaft
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Inducer
• Axial flow• Increase total pressure• permits non cavitating operation in impeller• used as boost pump, permits main pump to
operate at higher speeds• e.g. LPOTP is only inducer
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Inducer
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Stator
• Casing• Diffuser vanes• Volute• Seals
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Vane Island Diffuser(shown without shroud)
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Impeller Profiles
•
Axial FlowMixed FlowRadial Flow
From BWIP pump pocket book
Ns
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Pump Configurations• From Huzel, D. K. and Huang, D. H.
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Velocity Triangle• From Huzel, D. K. and Huang, D. H.
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Velocity Triangle• From Huzel, D. K. and Huang, D. H.
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Impeller Loss Components
• Skin Friction• Blade Loading • Incidence• Wake Mixing• Impeller-shroud Clearance Leakage• Disk Friction• Recirculation
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Flow Variables
PT = P + ρv2
PT = P + ρ (vθ2 + vm
2)
hT = h + ρv2 + gz
2
21
21
1
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Dimensionless Quantities
• Head coefficient
• Flow Coefficient
22RgH
Ω=Ψ
RAQΩ
=Φ
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Head rise
)v(vguH 12 θθ −=
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Isentropic Enthalpy Rise
∆H=144.∆p/ρ∆P (psi)∆H (ft)ρ(lb/ft3)
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Affinity Laws
• Q ~ ΩD3
• H ~ Ω2D2
• T ~ ρΩ2D5
• P ~ ρΩ3D5
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Engine System Resistance and Pump Characteristics
• From Huzel, D. K. and Huang, D. H.
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Specific speed
43
21
(gH)Qs Ω
=Ω• Consistent units– Ω (rad/s)– Q (m3/s)– H (m)
• US 2734.6Nss =Ω
43
21
(ft.)RPM.(GPM)Ns =
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Impeller Profiles
•
Axial FlowMixed FlowRadial Flow
From BWIP pump pocket book
Ns
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Effect of Ns on H-Q curve
• From Cameron Hydraulic Data
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Profiles and Efficiencies Based on Specific Speed
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Issues
• H-Q instability• Stall• Cavitation induced dynamic pressure• Radial loads• Discharge and suction recirculation
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Separation and Stall
Jet and wake observed in each impeller passage. The eddying wake is seen on the suction side of the channel from Fischer and Thoma, 1932
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Recirculation
Secondary flows in a centrifugal pump from Brennen (1994)
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Recirculation
Sudden increase in pressure pulsation from Fraser (1981)
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Stator Effect on Head Characteristics
(steepens H-Q curve)• reduce impeller inlet Cu at low flow• increase impeller inlet Cu at high flow• provide stability over wide operating range• increase stator and impeller incidence angle
at off design• reduces inception of stall with negative
incidence
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Vaned Diffuser Effect on Head Characteristics
(flattens H-Q curve)• convert kinetic energy of fluid leaving the
impeller into static pressure rise• flow incidence sensitive• leading edge stall phenomenon believed to
be cause of loss of diffuser performance• rapid head falloff at low flow
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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0
0.2
0.4
0.6
0.8
1
1.2
1.4
0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 1.1 1.2 1.3Flow/Flow des
Pum
p H
ead/
Pum
p H
ead
des
WFR
no stall
no diffuser stall
no stator stall
Stator stallDiffuser stall
Impeller stall
Stall Characteristics
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Two-Dimensional Diffuser Map
Flow Regimes in Straight Wall, Two-Dimensional Diffusers from Moore and Kline, 1955.
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Slot Optimization
Slot geometry configuration optimization from Gostelow and Watson, 1972.
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Blade Loading
From Guinzburg et al. (1997)
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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CFD as a Tool
• Before using a particular CFD code in a rotating machinery component design process, it is important to bracket the accuracy of the code results for that particular type of component.
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Interpretation of CFD
• Another important issue is how accurately the component inlet flow boundary conditions have to be known (pre-computation) to get results that are consistent with test data.
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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CFD Process
• Validate a computational fluid dynamic code for integration into the impeller design process.
• The validation process consists of computing the impeller flow for a range of inlet conditions.
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Accuracy of the CFD Results
• number of nodes used to discretize the flow domain
• accuracy of the numerical discretization scheme
• type of turbulence model used.
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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CFD Capabilities
• Transient Analysis• Two Phase Flow• Heat Transfer• Temperature Dependent Properties• Moving Mesh• Non-inertial Reference Frames• Selection of Turbulence Models• Wall Function Models
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Diffusion
The diffusion factor D, can be adapted for pumps from Lieblein (1965) as follows:
1
12
12
1
2
W2
VrrV
+ WW-1 = D
σ
θθ
−
Duncombe (1964) explicitly examined the diffusion on both the suction (s) and pressure (p) sides of the blade and expressed the result as follows:
W
W-1 +
WW-1 = D
1
minp,
maxs,
2
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Cavitation
Typical cavity configuration within an impeller. Flowrate is half that of BEP; so, the cavity is broken up by recirculating flow. From Sloteman et al (1995).
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Cavitation
• Thoma number, cavitation number
221
v
vp-p
ρσ =
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Suction Specific speed
43
21
(gNPSH)Qss Ω
=Ω• Consistent units– Ω (rad/s)– Q (m3/s)– NPSH (m)
• US 2734.6Nssss =Ω
43
21
(ft.)RPM.(GPM)Nss =
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Pump Suction Performance• From Huzel, D. K. and Huang, D. H.
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Bucket Curve
0
1
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9
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0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6
φ/φd
NPS
H/N
PSH
d
design point
Predicted
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Experimental Inducer Cavitation
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Leading Edge Cavitation Damage
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Typical Pump performance curve, showing NPSH required a) to maintain hydraulic performance or pump head (NPSHR), b) to limit cavitation damage and therefore maintain pump life (NPSHd), c) to prevent bubble formation entirely (NPSHi)
from Cooper and Antunes(1983)
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Pump Losses
• mechanical• hydraulic• disk friction• leakage
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Radial Load
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Radial Load Profiles for Volutes of Different Specific Speed
Pumps
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Axial Calculation
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Axial Load Balancing Schemes
• Seal Leakage Return Path• Pump out ribs or vanes• Balance Drum• Balance Disk
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Pump Balance Piston
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Rotordynamics
Relationship between the forces in the pump frame and the rotordynamic forces from Brennen (1994)
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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Impact Testing
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001
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References• Anderson, H. H. Centrifugal pumps. The Trade and Technical Press Ltd., England• Balje, O. E. (1981). Turbomachines. A guide to selection and theory. John Wiley and Sons, New York.• BWIP Pump Pocket Book. • Brennen, C. E. 1994. Hydrodynamics of Pumps. Concepts ETI, Inc. and Oxford University Press. New York.• Brennen, C. E. 1995. Cavitation and Bubble Dynamics. Oxford University Press. New York.• Cameron Hydraulic Data. (1988) Ingersoll-Rand Company. • Cooper, P. and Antunes, F. F. 1983. “Cavitation damage in boiler feed pumps.” Symposium Proceedings on: Power Plant Feed Pumps - The
State of the Art, EPRI CS-3158, Cherry Hill, New Jersey, pp. 2.24-2.29.• Csanady, G. T. (1964) Theory of turbomachines. McGraw-Hill, New York.• Duncombe, E., 1964, “Aerodynamic Design of Axial Flow Turbines,” in Aerodynamics of Turbines and Compressors, W. R. Hawthorne, Ed.,
Princeton University Press, p. 512.• Fraser, W. H. 1981. “Recirculation in Centrifugal Pumps,” Materials of Construction of Fluid Machinery and Their Relationship to Design
and Performance, ASME Nov. 15-20. Pp. 65-86.• Fischer, K. and Thoma, D. 1932. “Investigation of flow conditions in a centrifugal pump,” Transactions of the ASME, Vol. 54, pp. 141-155.• Furst, R B. (1973) Liquid Rocket Engine Centrifugal Flow Turbopumps. NASA SP-8109.• Karassik, I. J. And Carter, R. (1960) Centrifugal pumps. F. W. Dodge Corporation, New York• Huzel, D. K. and Huang, D. H. Modern Engineering for Design of Liquid-Propellant Rocket Engines. AIAA, Washington D. C. • Katsanis, T., and McNally, W. D., 1969, “Revised Fortran Program for Calculating Velocities and Streamlines on a Blade-to-Blade Stream
Surface of a Turbomachine,” NASA TM X-1764.• Katsanis, T., and McNally, W. D., 1977, “Revised Fortran Program for Calculating Velocities and Streamlines on the Hub-Shroud Stream
Surface of an Axial-, Radial-, or Mixed-Flow Turbomachine or Annular Duct,” NASA TN D-8430.• Lazarkiewicz, S. And Troskolanski, A. T. (1965) Impeller pumps. Pergamon Press, New York• Leiblein, S., “Experimental Flow in Two-Dimensional Cascades,” in Aerodynamic Design of Axial-Flow Compressors, NASA SP-36, p. 203.• Macaluso, S B. (1974) Liquid Rocket Engine Centrifugal Flow Turbopumps. NASA SP-8110.• Sloteman, D. P., Wotring, T. L., March, P., McBee, D, and Moody, L. 1995. “Experimental evaluation of high energy pump improvements
including effects of upstream piping,” Proceedings of the 12th International Pump Users Symposium, Houston, Texas.• Stepanoff, A. J. (1973) Centrifugal and axial flow pumps. John Wiley and Sons, New York.
Fluids Engineering Division Annual Summer Meeting, New Orleans, LA, 29 May 2001