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Turbomachinery Class 8a

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Presentation on theme: "Turbomachinery Class 8a"— Presentation transcript:

1 Turbomachinery Class 8a

2 Axial Flow Turbomachine Design
Three-dimensional flow through machine very complex Decompose problem into series of two-dimensional problems Blade-to-blade [Cascade] – (x, y=) Plane cascade (no spanwise effect) Stream surface (span effect modeled within 2D construct Through flow [Meanline] – (r, x) Blades modeled as thin or actuator discs Secondary flow [normal to mainstream] – (r, ) Design problem largely treated as inviscid analysis with viscous effects accounted for through empirical and semi-empirical methods

3 Airfoil/Cascade Design
Cascade - array of airfoils providing forces that change flow vectors. Requirements: Produce required forces Low total pressure loss Wide range of low loss incidence: operate at off-design points Stable exit angles Turning should be produced so that losses are minimum Airfoils [compressors] typically selected from family or “series” of airfoils

4 Geometry of a Rectilinear Cascade
Geometry Parameters Solidity Stagger angle: angle between chord line and leading edge front of cascade Camber / Turning Maximum thickness Leading edge / trailing edge thickness / radius Uncovered turning

5 Airfoil Nomenclature Chord: c or b = xTE-xLE; straight line connecting leading edge and trailing edge Camber line: locus of points halfway between upper and lower surface, as measured perpendicular to mean camber line itself Camber: maximum distance between mean camber lineand chord line Thickness t(x), tmax Angle of attack: , angle between freestream velocity and chord line

6 Geometry of a Rectilinear Cascade

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8 Geometry of a Rectilinear Cascade

9 Compressor Airfoil Design
Compressor Airfoil Series - geometric families Circular arc (CA): for high Mach number flows mean camber line is circular arc with max camber and max thickness at 50%c 65-series for moderate subsonic Mach numbers mean camber line is a parabola with max camber at 50%c and max thickness at 40%c 400-series for low Mach numbers max camber at 40%c and max thickness at 30%c thickness distribution NACA SP-36 p.198 or Abbot and Von Doenhoff

10 Compressor Airfoil Design

11 Compressor Airfoil Design
Compressor Airfoil Series - geometric families Initially developed from wing data Used through 1970's Large bodies of cascade data NASA, P&W, UTRC, DFVLR, NGTE, ONERA Loss & flow turning = f (incidence, Mach no., area ratio & geometry) Experimental Data Verifies Design Codes

12 Airfoil/Cascade Performance
Shear layer development over solid surface

13 Airfoil/Cascade Performance
Friction effects can adversely affect cascade performance

14 Airfoil/Cascade Performance
Boundary layer thickness assessment parameters: * = displacement thickness  = momentum thickness H = shape factor = * /  (1< H < 2.2) Equal mass =

15 Airfoil/Cascade Performance
Boundary layer thickness assessment parameters: * = displacement thickness Howell correlation

16 Airfoil - Cascade Comparisons
Isolated Wing Lift-Drag Curve Observations Cd dependence on Mach is small until critical Mcr Cl dependence on Mach is strong Shocks & shock boundary layer interaction lead to flow separation, lift loss, drag rise

17 Airfoil - Cascade Comparisons
Transonic flow shocks M<1 M>1

18 Airfoil - Cascade Comparisons
Plane Cascade Lift-Drag Curve Lift  Circulation ( )  turning  deflection Drag  total pressure change  loss Dixon – Howell [1942] What observations can you make about these curves?

19 Loss “Bucket”

20 Minimum loss incidence range
Choke Stall

21 Limits of Compressor Cascade Operation
Stall Analogous to wing stall High positive incidence, separation from suction side Loss & Deviation (difference between flow and exit camber angles) rising rapidly, work & efficiency fall Choke Pressure surface separation due to negative incidence Actual choke: not enough area at throat to pass mass flow Choke margin decreases as flow becomes more axial (M=const)

22

23 Airfoil/Cascade Design
Airfoil shapes constructed to have desirable surface pressure distributions and boundary layer characteristics Airfoil shapes must also meet structural criteria Low pressure, high Mach number [suction side] Adverse gradient T.E. Kutta condition High pressure, low Mach number [pressure side] % chord

24 Design for Lift, Min Loss, Max Range & Choke Margin
Avoid leading edge sep. bubble Ideal Avoid separation Avoid flow reversal Can also view this in terms of ps/p0

25 Airfoil/Cascade Design
Cascade Testing: Vital Requirements Periodicity Endwall boundary layer control Uniform flow Accurate pitch-wise Traverse data

26 Compressor Airfoil/Cascade Design
Additional Factors: AVDR - Axial Velocity - Density Ratio - area ratio due to end wall boundary layer growth [Geometry 2D but flow 3D]– Effects deviation [ ] Contraction of streamlines due to boundary layer thickening

27 Compressor Airfoil/Cascade Performance
Background: Boundary layer thickness parameters:  = momentum thickness * = displacement thickness H = shape factor = * /  (1< H < 2.2)

28 Compressor Airfoil/Cascade Performance
Loss Analysis - Lieblein's Dfactor [Diffusion Factor] Momentum Integral Equation describes the growth of boundary layer thickness along the suction surface: where: V = relative velocity at edge of boundary layer x = distance along airfoil surface - Boundary layer eqns. - Integrate y: 0 to  Boundary layer PDE integrated over y from 0 to 

29 Compressor Airfoil/Cascade Performance
Vmaximum Lieblien's insight: Correlation of cascade pressure distribution data for constant radius: Velocities are in Relative Frame [V=W]. Solidity =b/s. The 2 is empirical [from cascade data]. Now to connect Df to loss……... V(x) Vsurf V2

30 Wake Momentum Thickness vs. Calculated Diffusion
Empirical relation [Leiblien] connecting /c (or loss) to Df

31 Compressor Airfoil/Cascade Performance
Uses of Dfactor Today - Preliminary design surge margin limit for known clearance & aspect ratio - Low speed loss prediction in mean line systems 0 < Dfactor < 0.7 - Given loss [ /c ], now find loss coefficient [  ]

32 Example A compressor rotor with the following conditions:
U=200 mps Cx1=Cx2=150 mps 2=35 degs. Calculate W1, W2, Df

33 Loss Coefficient Directly Related to Wake Momentum
Thickness Ratio, /c

34 Relation Between /c and  [Extra]
Empirical expression

35 What is the Impact of D-factor on Airfoil Shape
Carter’s Rule for compressor cascades For HWK 6.3, since  =1 Metal angle decreases to achieve design exit angle goals

36

37 Compressor Airfoil/Cascade Performance
Compressor Airfoil Performance Dfactor sets Wake Thickness Wake Thickness and # Wakes sets Loss Coefficient Loss Coefficient and Work Coefficient sets Efficiency

38 Turbomachinery Class 8b

39 Overview of Loss Analysis - Lieblein's Dfactor
Correlation of cascade data [Velocities in Relative Frame] or de Haller [ 0.72<W2/W1<1] Momentum thickness [ ] correlated to Dfactor [0 < Dfactor < .7] Loss coefficient related to cascade wake momentum thickness Efficiency related to loss coefficient

40 Compressor Airfoil/Cascade Performance
High deflection compressor airfoil [reducing 2 with fixed 1] means reducing V2. Early diffusion based design method by de Haller called for 0.72<V2/V1<1 to avoid high losses. Lieblien [NACA] related diffusion to velocity gradient and solidity Vmaximum V(x) Vsurf V2

41 Compressor Airfoil/Cascade Performance
Repeating stage, repeating row [mirror image airfoil]

42 Compressor Airfoil/Cascade Performance
Dfactor analysis for repeating row stage

43 Airfoil/Cascade Performance
Airfoil Sections Now Designed to Pressure Distributions Compressible Potential flow code for local M<1.1 (no shocks) Integral Boundary Layer codes for performance prediction (viscous effects) Wake Mixing (Stewart’s Control Volume) Analysis to Obtain Relative P0 Loss Navier-Stokes codes for studies near separation (viscous & inviscid flow solved at once)

44 Compressor Airfoil/Cascade Design
Controlled Diffusion Airfoils GE) Higher peak Mach no., tapered dV/dx More camber in front half of chord Elliptical Leading edges Stall range assured by gradual initial acceleration Not optimum at end walls

45 Turbine Airfoil/Cascade Design
Turbine Airfoil Design Historically more Analytical than Compressors Accelerating Flow...Probably the Reason Boundary layer separation easier to avoid Design to Pressure Distributions Correct for deviation effects Zweifel Load Coefficient & Convergence Desirable Pressure Distributions

46 Turbine Rotor 2  3 Constant Cx, no exit swirl [3=0]
High loading stage [E<<0, turbine] Lower weight, lower stage efficiency  lower R

47 Turbine Rotor 2  3 For repeating row design and no exit swirl E=2[R-1]

48 Cascade Design Problem
Desirable pressure distributions Pressure side Exit Pressure Suction side Good Poor- too much diffusion

49 What is the Impact of Deviation on Airfoil Shape
Carter’s Rule for turbine cascades Metal angle decreased to achieve design exit angle goals Effect for turbine is much smaller for turbines due to thinner boundary layers

50 Zweifel Coefficient Derivation
Solidity play important role in turbine efficiency: (1) spacing small, fluid gets maximum turning force with large wall friction forces; (2) spacing large, fluid gets small turning force with small wall friction losses. Area Fideal Area F Solidity issue: Enough airfoils must be used so that F = change in tangential momentum of the fluid.

51 Zweifel Coefficient Derivation

52 Turbine Airfoil/Cascade Design
Zweifel Load Coefficient: where bx is the axial chord and h is the streamtube spanwise width and x = bx / s Treating the pressure difference incompressibly:

53 Turbine Airfoil/Cascade Design
Simplifying: Zweifel Coefficient: 1st estimate of solidity.

54 Turbine Airfoil/Cascade Design
Zweifel Coefficient: 1st estimate of solidity. Zweifel noted that turbine min. loss for z 0.8. Optimum spacing estimated from given inlet and outlet angles.

55 Turbine Airfoil/Cascade Design
Zweifel Coefficient: 1st estimate of solidity. Other Factors: Pressure Distributions Cooling Resonances Disk Stress Weight Cost Some of this covered after meanline analysis

56 Turbine Airfoil/Cascade Design
Turbine Airfoil Design Approach [covered in following charts] Balance Acceleration & Diffusion Use Laminar Boundary layer where possible Diffuse with Turbulent Boundary layer Control Maximum Mach No. & Shocks Control Leading Edge Overspeed Manage Uncovered Turning

57 Turbine Airfoil/Cascade Design
Balance Front End Acceleration With Rear Diffusion Laminar boundary layers on suction surface reduces losses on front, turbulent boundary layers on rear more tolerant to flow separation.

58 More Blades Increases Solidity [ = b/s] Reduces Force per Blade

59 Aft Curvature Moves Loading Aft

60 Turbine Airfoil/Cascade Design
High Convergence Eases Cascade Design Like an area ratio: Aan is an annulus area Convergence is Function of Velocity Diagrams, not airfoil shape High Reaction = higher blade convergence

61 Turbine Airfoil/Cascade Design

62 Turbine Airfoil/Cascade Design
Thin Edges are best for Aerodynamic Performance Trailing Edge Blockage Drives Base Drag TET = Trailing Edge Thickness Stewart’s mixing loss correlation is function of TET and *s.s. , *p.s. Casting capability, stress & cooling set minimum edge thickness High wedge angle eases effect at leading edge Elliptical LE is better Pressure Distribution Improved; Overspeed reduced in both surfaces

63 Turbine Airfoil/Cascade Design
Manage Uncovered Turning Transonic Flow: More uncovered turning lowers base pressure loss (<pex) but higher boundary layer loss. Subsonic Flow: Base pressure  pex Uncovered turning Throat

64 Consequences of Stagnation Point Location

65 Turbine Airfoil/Cascade Design
Manage Uncovered Turning Uncovered turning is less of an issue for subsonic turbine airfoils

66 Thermo & Kinematic View of Compressor Stage
Note: U>C

67 Thermo & Kinematic View of Turbine Stage
Note: U<C Cu3 Cu2

68 Thermo & Kinematic View of Turbine Stage


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