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Parametric 3D Blade Geometry Modeling Tool for
Turbomachinery Systems
A thesis submitted to the
Graduate School
of the University of Cincinnati
in partial fulfillment of the
requirements for the degree of
Master of Science
in the School of Aerospace Systems
of the College of Engineering and Applied Science
by
Kiran Siddappaji
B.Tech, Maulana Azad National Institute of Technology, India, 2008
Committee Chair: Dr. Mark G. Turner
Abstract
Turbomachinery blades are an integral part of air breathing propulsion systems, gas and steam
turbines and other energy conversion devices. The blade design is a very important process
since it defines component performance. A parametric approach for the blade geometry design
has been implemented. A variety of three dimensional blade shapes can be created using only a
few basic parameters and limited interaction with a CAD system. Using a general approach for
creating the blade geometries makes the process easy and robust for creating 3D blade shapes
for various turbomachinery components. The geometry of the blade is defined by a very basic
set of geometric and aerodynamic parameters. Parameters such as flow angles, axial chord,
thickness to chord ratio and streamline meridional coordinates are defined. The leading edge
and trailing edge are defined by curves as part of the input. Using these parameters, a specified
number of 2D airfoils are created and are radially stacked on the desired stacking axis. The
sweep and lean perturbations of the blade are defined by splines as a function of a few control
points. The design tool generates a specified number of 3D blade sections and each section
consists of a defined number of coordinates in the cartesian coordinate system. These sections
can be lofted in a CAD package to obtain a solid 3D blade model, which has been demonstrated
using Unigraphics-NX. Parametric update of the spline points defining the 3D blade sections
creates new blade shapes without going back into the CAD interface. This approach for the
design is very beneficial as the geometry can be modified quickly and easily as per the needs
of the designer at any point of time. Using this tool, blade shapes of a 10 stage compressor
similar to the GE/NASA EEE HPC, a 3 stage booster, a reverse engineered GE 1.5 MW wind
turbine and a centrifugal compressor based on a NASA design are constructed as examples. The
general capabilty of the design tool is demonstrated through these examples.
i
Acknowledgments
The author is grateful to NASA for funding and support through NRA project- "Advanced
Design Techniques for MDAO of Turbomachinery with Emphasis for the Engine System". The
MDAO project meetings with the rest of the members proved to be very helpful in terms of their
feedback.
Rob Ogden deserves a special thanks for his system related support and the members of
the UC Gas Turbine Simulation Laboratory for their assistance and clearing out certain mis-
concepts. Thanks to David Gutzwiller and Kevin Park for taking time out of their schedule to
provide necessary input and helping in debugging the code several times.
Sincere thanks to Dr. Ali Merchant for providing assistance and guidance at odd hours
inspite of his hectic schedule. The preliminary version of the blade geometry generator was
part of T-Axi that Dr. Merchant wrote. For that also, the author is grateful. Author is grateful
to Dr. Dario Bruna for providing clear suggestions in the initial phase. Thanks are due to Istvan
Iszabo and Soumitr Dey for giving very valuable lessons and tips in UG/NX which saved a lot
of modeling time.
The author would like to thank his thesis advisor, Dr. Mark G. Turner, for his insight,
guidance and feedback. His methods of tackling an issue and solving it in a simple way is
worth the mention.
Lastly, a special thanks to my parents and friends for providing me the constant support and
encouragement.
iii
Contents
Abstract i
Acknowledgments iii
Contents vi
List of Figures ix
Nomenclature x
1 Introduction 1
1.1 Motivation . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 1
1.2 Literature Review and Previous Work . . . . . . . . . . . . . . . . . . . . . . 2
1.3 Goals and Thesis Layout . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 4
2 3D Blade Generator 6
2.1 Input File . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 6
2.2 Governing Equations . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 8
2.3 Blade section construction . . . . . . . . . . . . . . . . . . . . . . . . . . . . 10
2.3.1 Variety of Airfoil shapes . . . . . . . . . . . . . . . . . . . . . . . . . 19
2.4 Leading Edge and Trailing Edge Curves . . . . . . . . . . . . . . . . . . . . . 19
2.5 Streamwise Mapping of the Blade Sections . . . . . . . . . . . . . . . . . . . 20
2.6 Sweep and Lean to the Blade . . . . . . . . . . . . . . . . . . . . . . . . . . . 22
2.6.1 Construction of Uniform B-Splines . . . . . . . . . . . . . . . . . . . 24
2.7 Radial Stacking of 3D Blade Sections . . . . . . . . . . . . . . . . . . . . . . 26
iv
2.8 Coordinate Transformation . . . . . . . . . . . . . . . . . . . . . . . . . . . . 26
2.9 Output files . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 27
2.10 3D Blade CAD Model . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 28
2.11 Connecting with CAPRI . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 28
2.12 Extruded Blade . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 29
3 CFD Analysis of the 3D blade 31
3.1 Gridding . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 31
3.2 CFD solver: Euranus . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 31
4 Structural Analysis of the 3D Blade 36
5 Example Design Problems 39
5.1 10 Stage EEE High Pressure Compressor Design . . . . . . . . . . . . . . . . 39
5.1.1 Free vortex Design . . . . . . . . . . . . . . . . . . . . . . . . . . . . 39
5.1.2 Full Definition 10 stage Design . . . . . . . . . . . . . . . . . . . . . 43
5.2 3 Stage Booster Design for Turbofan Engine . . . . . . . . . . . . . . . . . . . 46
5.3 Reverse-Engineered Wind Turbine Design . . . . . . . . . . . . . . . . . . . . 50
5.4 Low-Speed Centrifugal Compressor design . . . . . . . . . . . . . . . . . . . 55
6 Conclusion and Future Work 58
6.1 Conclusion . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 58
6.2 Future Work . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 59
References 60
Appendix 62
A Input Files for Example Cases 63
A.1 Rotor 3 of 10 Stage EEE HPC Free Vortex Design . . . . . . . . . . . . . . . . 63
A.2 Rotor 3 of 10 Stage EEE HPC Full Definition Design . . . . . . . . . . . . . . 78
A.2.1 Blade Metal Angles from the NASA Report [1] . . . . . . . . . . . . . 94
A.3 Rotor 3 of 3 Stage Booster Design . . . . . . . . . . . . . . . . . . . . . . . . 95
v
A.4 Reverse Engineered Wind Turbine Design . . . . . . . . . . . . . . . . . . . . 111
A.5 Low Speed Centrifugal Compressor Design . . . . . . . . . . . . . . . . . . . 128
vi
List of Figures
2.1 3D Blade Design Process Flowchart. . . . . . . . . . . . . . . . . . . . . . . . 7
2.2 r − x− θ space for the 3D blade. . . . . . . . . . . . . . . . . . . . . . . . . . 8
2.3 Meridional view of the blade showing axisymmetric streamlines as construction
curves. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 9
2.4 A blade showing the blade sections. . . . . . . . . . . . . . . . . . . . . . . . 10
2.5 Blade section on the mean camber curve. . . . . . . . . . . . . . . . . . . . . 11
2.6 Relationship between (m′b, θb) system and (u, v) system. . . . . . . . . . . . . . 12
2.7 Plot of the camber line of blade sections 10 and 11 of the rotor 1 blade from the
10 stage HPC design. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 14
2.8 Camber angle plot of blade sections 10 and 11 of the rotor 1 blade from the 10
stage HPC design. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 15
2.9 Plot showing the curvature of the camber line of blade sections 10 and 11 of the
rotor 1 blade from the 10 stage HPC design. . . . . . . . . . . . . . . . . . . . 16
2.10 Thickness distribution over a non-dimensional unit camber length [2]. . . . . . 16
2.11 Blade section on the normalized unit chord. . . . . . . . . . . . . . . . . . . . 18
2.12 Variety of airfoils generated by 3DBGB in addition to circular and 4 digit
NACA airfoils. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 19
2.13 Stream surface for an axial machine and a radial machine respectively. . . . . . 20
2.14 m′sLE obtained using inverse spline on m′s. . . . . . . . . . . . . . . . . . . . . 20
2.15 x3D obtained by spline evaluation at each m′3D of each blade section. . . . . . . 21
2.16 r3D obtained by spline evaluation at each m′3D of each blade section. . . . . . . 22
2.17 Mapping of the blade section to the corresponding stream surface. . . . . . . . 22
vii
2.18 δm′ evaluated at each span. . . . . . . . . . . . . . . . . . . . . . . . . . . . . 23
2.19 Forward and backward swept blades respectively. . . . . . . . . . . . . . . . . 24
2.20 Spanwise lean modification on rotor 3 of a booster optimum resulting in lean
near the hub. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 24
2.21 Construction of a uniform non-rational B-spline curve. [3] . . . . . . . . . . . 25
2.22 θ offset defined for various stacking option. . . . . . . . . . . . . . . . . . . . 27
2.23 3D Blade lofted in UG. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 28
2.24 Offset at the hub streamline. . . . . . . . . . . . . . . . . . . . . . . . . . . . 29
2.25 Extruded blade at the tip with hub and casing. . . . . . . . . . . . . . . . . . . 30
3.1 Creating the meridional and blade to blade mesh. . . . . . . . . . . . . . . . . 32
3.2 Characteristic curve showing Total PR vs mass flow rate. . . . . . . . . . . . . 33
3.3 Characterisitic curve showing Isentropic efficiency vs mass flow rate. . . . . . . 34
3.4 Relative Mach contours of rotor 3 of the optimized booster with stream ribbons
at over the tip clearance. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 34
3.5 Spanwise lean modification on rotor 3. . . . . . . . . . . . . . . . . . . . . . . 35
3.6 Iso surface comparison of axial velocity for original and modified rotor 3 of the
booster optimum point 2 [4]. . . . . . . . . . . . . . . . . . . . . . . . . . . . 35
4.1 Blade meshed in ANSYS V12.0. . . . . . . . . . . . . . . . . . . . . . . . . . 37
4.2 Contour plots of Displacement vector sum for first 7 modes of a blade under
Nodal solution. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 37
4.3 Contour plots of Displacement vector sum for last 7 modes of a blade under
Nodal solution. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 38
4.4 Displaced blade. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 38
5.1 E3 10 Stage Compressor Cross Section. [1] . . . . . . . . . . . . . . . . . . . 40
5.2 Axisymmetric grid showing the streamlines of 10 Stage HPC free vortex design
and the straight leading and trailing edge locations of the blade rows in green. . 40
5.3 Rotor 1 and rotor 3 of EEE HPC free vortex design created using 3DBGB. . . . 41
5.4 Rotor 1 and Rotor 3 blisk assembly for EEE HPC free vortex design. . . . . . . 42
viii
5.5 Axisymmetric grid showing the streamlines of E3 10 Stage HPC full definition
design and the leading and trailing edge locations of the blade rows in green. . . 43
5.6 Comparison of blade metal angles of EEE-HPC rotor 3 given in the report [1]
and generated by 3DBGB. . . . . . . . . . . . . . . . . . . . . . . . . . . . . 44
5.7 Rotor 3 of GE EEE HPC full definition design with non-straight leading and
trailing edges. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 44
5.8 Rotor and stator assembly for 10 stage HPC full definition design from the
GE/E3 parameters. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 45
5.9 3 stage booster of a GE90 turbofan engine.[5] . . . . . . . . . . . . . . . . . . 46
5.10 Axisymmetric grid of the 3-stage optimized booster showing the streamlines
and the leading and trailing edge locations of the blade rows in green. . . . . . 47
5.11 3 stage booster rotor assembly with the fan blades. . . . . . . . . . . . . . . . 47
5.12 3 stage booster assembly with split casing. . . . . . . . . . . . . . . . . . . . . 48
5.13 Tetrahedral mesh of rotor 3 of a 3 stage booster in ANSYS. . . . . . . . . . . . 49
5.14 Contour plots of displacement vector sum of all 14 modes of rotor 3 under
Modal solution. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 49
5.15 GE 1.5 MW wind turbine blade. [6] . . . . . . . . . . . . . . . . . . . . . . . 50
5.16 Axisymmetric grid of the reverse engineered GE 1.5 MW wind turbine blade. . 51
5.17 Reverse engineered GE 1.5 MW wind turbine blade geometry created using
3DBGB. . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . . 51
5.18 Reverse Engineered GE 1.5 MW wind turbine assembly. . . . . . . . . . . . . 52
5.19 Meshed wind-turbine blade with 8 node Hexahedron Brick 185 element. . . . . 53
5.20 Von-Mises Stress plot on GE reverse engineered blade. . . . . . . . . . . . . . 53
5.21 First 5 Modal solution of GE reverse engineered blade. . . . . . . . . . . . . . 54
5.22 LSCC flowpath with actual measurements. [7] . . . . . . . . . . . . . . . . . . 55
5.23 A radial compressor flowpath showing the hub and casing with streamlines and
the leading and trailing edge locations. . . . . . . . . . . . . . . . . . . . . . . 56
5.24 Velocity triangle at the leading edge for the radial compressor. . . . . . . . . . 57
5.25 Radial compressor model compared with NASA LSCC [7]. . . . . . . . . . . . 57
ix
Nomenclature
a Offset value
b Intermediate extruded blade scale factor
i Incidence angle
L Reference length
m Meridional coordinate
mm Millimeters
m′ Normalized Meridional coordinate
np Number of points
nspn Number of blade sections
r Radial coordinate
u Non-dimensional chordwise coordinate
v Non-dimensional coordinate perpendicular to u
N Rotational Speed
U Wheel Speed
V Absolute flow velocity
x Axial coordinate
Greek
α Absolute flow angle
β Relative flow angle
β∗ Blade metal angle
δ Deviation angle
x
ζ Stagger angle
θ Tangential direction
π 3.14149
φ Meridional plane flow angle = tan−1(Vr/Vx)
ω Loss coefficient
Subscripts
b Blade
bbot Blade bottom
bstgr Blade stagger
btop Blade top
r Radial
ref Reference
x Axial
s Streamline
t Tip
z Axial
LE Leading Edge
ND Non Dimensional
Norm Normal
TE Trailing Edge
3D Three dimensional
Units
Hz Hertz
m/s meters per second
MPa Mega Pascals
MW Mega Watts
xi
Abbreviations
2D Two Dimensional
3D Three Dimensional
3DBGB Three Dimensional Blade Geometry Builder
CAD Computer Aided Design
CAPRI Computational Analysis PRogramming Interface
CFD Computational Fluid Dynamics
EEE Energy Efficient Engine
FEA Finite Element Analysis
GUI Graphic User Interface
IGES Initial Graphics Exchange Specification
IGV Inlet Guide Vane
NACA National Advisory Committee for Aeronautics
NURBS Non Uniform Rational B-Spline
RE Reverse Engineered
RPM Rotations Per Minute
UG UniGraphics-NX
xii
Chapter 1
Introduction
1.1 Motivation
The gas turbine blade design process has become more challenging recently as the approach has
become more parametric and innovative. However, the basic philosophy of any blade design
still remains the same in terms of building the 2D sections utilizing all the necessary geometric
parameters and then constructing the 3D model. There are many software tools available which
are built based on the user needs. The attempt here is to build a blade design tool based on very
few but essential parameters both geometric and aerodynamic, which can be automated and be
a part of any optimization chain and above all be flexible to create a wide range of geometries
with minimal parametric modifications. The 3D model is created using the 3D blade sections
output from the design tool and the final blade model is obtained by the limited interaction with
a CAD package. Subsequent blade models can be generated by parametric spline updates on
the base model created using the CAD package. The 3D blade shape is ready for validation
through 3D CFD analysis and FEA analysis. The geometry can be quickly modified by just
changing the parameters and the process is continued without losing time in remodeling.
There are many 3D blade design packages which are either completely proprietary or com-
mercial implementations of CAD based models. The tool presented here has general capability
of designing various turbomachinery blade shapes and the parametric approach is beneficial in
linking the whole tool to an optimizer to obtain optimized blade shapes with single or multi-
objective functions or even an automated process cycle. Design of Experiments approaches can
1
also be automated which are often used to create meta models which can be optimized. Also,
this design tool provides a bridge between the low fidelity and the high fidelity analysis/design
process. Certain CAD features like union of solids and fillets can be achieved by integrating the
tool with CAD.
1.2 Literature Review and Previous Work
There have been many blade design models developed, which have various approaches for
building the blade model. There are several papers on a parametric approach to the blade ge-
ometry. One paper by Grasel et al. [8] describes a complete parametric model for the blade
design where the blades are free form shapes defined by Spline-functions. It also describes
modification of aerofoils with the help of the curvature distribution defined by control points.
Interaction with a CAD interface and how the parameters are optimized is also discussed.
Dutta et al. [9] describes an automated process of a non-dimensional quasi-3D blade design
with parameterization of the camber-line angle and thickness distributions and blade inlet and
outlet angles. It discusses an optimization loop including geometry generation, certain blade-
to-blade computations and post-processing, and how each parametric variable has an impact on
the optimizer.
Kioni et al. [10] describes a tool for parametric design of the turbomachinery blades. Using
the design parameters, 2D blade sections are created and using NURBS surfaces, 3D bladings
are obtained. These geometries can be exported to any CAD or mesh generation and analysis
software. The tool can also be used for design optimization purposes. Various geometries can be
handled smoothly due to the object oriented structure of the code. The blade sections are formed
by a mean camber line curve and a distribution of control points or interpolation points of a
NURBS curve defines the thickness distribution around the mean curve. The desired number
of blade sections are constructed and intially, all their leading edges are made to coincide with
the origin of the 2D reference system used for the construction. The stacking of the sections is
controlled either by a guide line which is a straight line (common radius) or a 3D NURBS curve
that passes through the leading edges or through the centres of gravity of the blade sections
as explained in the paper [10]. The meridional profiles are generated with the help of the
2
control points. Conformal mapping of the 2D blade sections to the cylindrical surfaces using
the corresponding meridional curves with respect to a stacking line results in the 3D blade
shape. Coordinate transformation from the cylindrical system to the 3D Cartesian system is
helpful in constructing the 3D blade surface as a single NURBS surface, where all the sections
have the same number of points. The tool also has the capability of creating the hub and the
shroud surfaces as a single NURBS surface with the help of the control points. The single curve
construction approach minimizes the curvature discontinuity errors and the 3D blade generation
is simplified as explained in the paper.
Korakianitis [11] describes a method for generating 2D blade shapes. A mixture of analytic
polynomials and a desired curvature distribution on a 2D plane is mapped with the blade ge-
ometry such that the blade surfaces have continuous slope of curvature throughout their length.
The leading edge is defined by 2 thickness distributions around 2 independent construction lines
which avoids the overspeed regions near the leading edge. The design method presented in this
paper ensures that the boundary layer is not perturbed unintentionally. Effects of stagger angle
on blade loading and wake thickness has also been explored.
Anders et al. [12] described the blade profile using two Bezier curves of order five. The lead-
ing and trailing edges were defined using circles or ellipses. Slope continuity was maintained,
except for some curvature discontinuities at certain junctions. The design system consisted of
automatic blading, which utilized the parametric approach to create blades for existing and new
compressors such as the BR715 Booster, HP9 research compressor, Trent500 and Trent800 HP
compressor. The next step was optimizing the 2D blade profiles based on the desired aerody-
namic properties. A parametric 3D blade manipulation was carried out by 3D blade stacking
followed by radial blade smoothing and interpolation, which created a smooth 3D blade. This
whole process was automated and optimized to generate blade shapes satisfying the required
objectives.
Bezier or B-spline curves are used for airfoil design either as a single closed (or open) curve
or as separate curves and introducing circles (or ellipses) at the leading and trailing edge have
become popular. Usually, Bezier curves of order 3 or higher are used for the mean camber
definition to avoid curvature discontinuites and NURBS are used for joining curves since it
3
is the most widely used set of spline curves in many CAD systems. Using control points as
parameters proves to be more useful in obtaining desired airfoil shapes. This system is helpful
for airfoil design optimization purposes.
Several academic or commercial software packages are present for blade design and opti-
mization purposes. BladeCAD, an interactive geometric design tool was developed by Oliver et
al. [13] in 1996 under NASA supervision. Using this interface, blade sections were created with
respect to general surfaces of revolution and the entire design was defined using a non-uniform
rational B-spline (NURBS) surface. The IGES file format was used as the output file which is
portable to most analysis and design applications. The blade design was defined by construct-
ing the mean camber line, which is a bezier curve of third degree defined by blade angles and
the stagger angle. The shape of the mean camber was specified in the angle preserving space
m′ − θ. The blade section was constructed by defining the suction side and the pressure side
curves along with the thickness definition normalized by the chord. Using an inverse mapping
procedure as explained in the paper, the blade section constructed in m− rθ space is converted
to its respective stream surface in r− z − θ space. A stacking axis was defined to loft the blade
sections in 3D space. The software has an input panel which contains a thickness function edi-
tor, section editor, which uses NURBS curve to define the mean camber geometry, and a blade
metal angle editor. It also has the capability of creating general stream surfaces which improves
the exisiting blade design methodology.
1.3 Goals and Thesis Layout
The work presented in this thesis has been mostly funded by a NASA NRA grant [14], and
hence will attempt to meet the goals set forth in that proposal. The unique aspects of this work
are:
1. An adherence to consistency.
2. Simplicity of the input while allowing the largest design space.
3. General capability and flexibility of the design tool.
4
4. Availability of the code in executable form.
Additional goals of this research and the layout of the thesis are:
1. Parameterization of blade geometry inputs which is a very key aspect as it can be modified
very easily and can be incorporated in automation and optimization chains. This goal is
achieved and is documented in Chapter 2.
2. The development of a stand-alone 3D blade geometry builder called 3DBGB (3 Dimen-
sional Blade Geometry Builder) which produces blade shapes that can be modified to get
newer blade shapes by simply updating the spline data with limited interaction with CAD
systems. This goal is achieved and is documented in Chapter 2.
3. The integration of 3DBGB into a large, system wide multi-disciplinary analysis and opti-
mization (MDAO) project. Chapters 3 and 4 document progress related to this project.
4. The application of 3DBGB in creating bladeshapes of the 10 stage High Pressure Com-
pressor developed from the GE/NASA program [1], both free vortex and full definition
design. This is documented in Chapter 5.
5. The application of 3DBGB in creating bladeshapes of a 3-stage booster for a turbofan
engine and performing a CFD and FEA analysis on rotor 3. This is documented in Chapter
5.
6. A reverse engineered wind turbine design was also created using this tool to demonstrate
the generality of the design tool and is documented in Chapter 5.
7. The development of a general blade geometry builder which creates both axial and ra-
dial turbomachinery blades. This is demonstrated by designing a radial compressor as
explained in Chapter 5.
5
Chapter 2
3D Blade Generator
This chapter deals with the development of the blade generator explaining how the input param-
eters are utilized in creating blade sections and performing mathematical operations to finally
obtain a 3D blade model. The 3DBGB [15] code creates the 3D blade shapes presented as exam-
ples. The executable with several cases is available at http://gtsl.ase.uc.edu/3DBGB/. Figure 2.1
explains the process flow involved.
2.1 Input File
The input file for the 3DBGB (3 Dimensional Blade Geometry Builder) code [15] contains
aerodynamic and geometric parameters defining the blade geometry required to build a 3D
blade shape. The parameters are defined at each streamline passing through the blade as below:
1. flow angles at leading edge and trailing edge of the blade.
2. relative inlet mach number.
3. thickness to chord ratio.
4. axial chord values.
5. incidence and deviation angles (if these are zero, then the flow angles represent the blade
metal angle).
6
The input also has 2D curves representing the leading and trailing edges, airfoil stacking
information and a control table which defines the sweep and lean perturbation and any required
quantity with a few control points for adding more definition to the blade geometry. The input
file also contains the xs and rs coordinates for all the nspn streamlines defined from an axisym-
metric run like T-Axi [16, 17, 18, 19], or by smooth construction curves between the hub and
the casing.
2.2 Governing Equations
Figure 2.2: r − x− θ space for the 3D blade.
The coordinate system used is shown in Figure 2.2. The meridional view of the streamlines
with the leading edge and the trailing edge is shown in Figure 2.3. The curve in Figure 2.3 is
referred to as a streamline since an axisymmetric streamline has traditionally been used as a
construction line or curve. A smooth construction curve can be used in place of an axisymmet-
ric streamline to define the blade geometry. The 3D blade is constructed using the following
mathematical approach:
1. streamline coordinates: m′s, xs, rs.
2. airfoil coordinates: m′b, θb.
The projection of the streamline or smooth construction curve onto the meridional plane
8
Figure 2.3: Meridional view of the blade showing axisymmetric streamlines as constructioncurves.
x− r is given by:
dms =√
(drs)2 + (dxs)2 (2.1)
The normalized differential arc length is defined by:
dm′s =dms
rs(2.2)
The m′s coordinate of the streamline is obtained by integrating:
m′s =
∫dms
rs=
∫ √(drs)2 + (dxs)2
rs(2.3)
If the airfoil is designed on constant radius sections, then
m′s =
∫dxsrs
=xsrs
(2.4)
which represents a normalized axial coordinate.
9
2.3 Blade section construction
Figure 2.4: A blade showing the blade sections.
The blade section construction procedure documented in this section is adopted from the
procedure used in T-Axi [16, 17, 18, 19] co-authored by Dr. Ali Merchant. The same procedure
is also used in T-Axi Blade [20] which is a GUI based, free-vortex blade row design and visual-
ization program. It’s main emphasis is on the relationship between velocity triangles and blade
shapes, cascade views for hub, pitch and tip, Smith charts and Loading vs Aspect Ratio charts.
A 3D blade contains a specified number of blade sections stacked radially as shown in Fig-
ure 2.4. A blade section contains a mean camber curve passing through the leading edge and
trailing edge of the blade section and has a suction side curve and a pressure side curve built
around it as shown in Figure 2.5. Also in Figure 2.5, the blade metal angle at inlet (leading
edge) is defined by β∗in and at the exit (trailing edge) is defined by β∗out. The flow angles at inlet
and exit are βin and βout respectively. In this figure, β∗in, β∗out and ζ are all negative based on the
10
sign convention used. The incidence angle i and the deviation angle δ are given as below:
1. Incidence Angle, i: If β∗in greater than zero then i = βin− β∗in and if β∗in is less than zero
then i = β∗in − βin.
2. Deviation Angle, δ: If camber is negative then δ = βout − β∗out and if camber is positive
then δ = β∗out − βout.
Figure 2.5: Blade section on the mean camber curve.
An elliptical leading edge and circular trailing edge are used for connecting the pressure
side and suction side curves. The elliptical leading edge helps in reducing overspeeds and for
certain Reynolds numbers, helps to keep the flow attached and laminar [21]. Also, the user has
an option of choosing the shape of the leading and trailing edges. The mean camber line is
built using the blade metal angles (β∗in, β∗out), thickness to chord ratio and the meridional chord
value. A mixed camber line is defined which is partly cubic in nature. The analytical form of the
camber line cam is a cubic polynomial which is a function of a non-dimensional coordinate u. v
is the corresponding non-dimensional coordinate perpendicular to u. The relationship between
(m′b, θb) system and (u, v) system is shown in the Figure 2.6.
11
Figure 2.6: Relationship between (m′b, θb) system and (u, v) system.
The analytical form of the camber line cam is:
cam = aa(ub)3 + bb(ub)2 + cc(ub) + dd (2.5)
camu = 3aa(ub)2 + 2bb(ub) + cc (2.6)
ub = u− u1 (2.7)
xb = u2 − u1 (2.8)
aa =s1 + s2 − 2( c2−dd
xb)
(xb)2(2.9)
bb =−s1(xb)− aa(xb)3 + c2 − dd
(xb)2(2.10)
cc = s1 (2.11)
dd = c1 (2.12)
In Eq.(2.5), aa, bb, cc and dd are the coefficients of the cubic equation representing the
12
camber line and ub is the varying parameter. Also,
s1 = tan β∗in (2.13)
s2 = tan β∗out (2.14)
u1 = fl1 cos β∗in (2.15)
c1 = fl1 sin β∗in (2.16)
u2 = 1− fl2 cos β∗out (2.17)
c2 = −fl2 sin β∗out (2.18)
where,
1. s1, s2 are the slopes at inlet and exit of the blade section.
2. fl1 = constant slope at inlet as seen in Figure 2.8.
3. fl2 = constant slope at exit as seen in Figure 2.8.
4. c1, c2 are the derivatives of u1, u2 with respect to the blade metal angle.
The camber line plot of the 10th and 11th blade sections for rotor 1 blade of the 10 stage high
pressure compressor developed from GE/NASA program [1] is shown in Figure 2.7. Figure 2.8
shows the plot of camber angle for the same rotor blade sections. Also, the curvature of the
camber line for the 10th and 11th blade sections are plotted in Figure 2.9. All these plots are
with respect to u, the non-dimensional coordinate spanning the interval [0,1]. An equally spaced
grid of 100 points (can be varied) in this interval was used for the plot.
The camber angle, ang is given by differentiating Eq. (2.5) with respect to ub and taking the
arctangent of the value obtained.
ang = tan−1(camu) (2.19)
The non dimensional coordinates for suction side (ubtop, vbtop) and pressure side (ubbot, vbbot) are
13
Figure 2.7: Plot of the camber line of blade sections 10 and 11 of the rotor 1 blade from the 10stage HPC design.
calculated as below:
ubbot = u+ thk sin (ang) (2.20)
vbbot = cam− thk cos (ang) (2.21)
ubtop = u− thk sin (ang) (2.22)
vbtop = cam+ thk cos (ang) (2.23)
where thk is the thickness distribution defined over a non-dimensional unit camber length
(0.0 to 1.0) as given by Wennerstrom [2]. The thickness distribution is described in Figure 2.10
and the nomenclature is as below:
1. x = non-dimensional camber-line length.
2. xT = location of maximum airfoil thickness.
3. t1 = leading edge thickness.
4. T = maximum airfoil thickness.
5. t2 = trailing edge thickness.
6. y1 = airfoil half-thickness upstream of xT .
14
Figure 2.8: Camber angle plot of blade sections 10 and 11 of the rotor 1 blade from the 10 stageHPC design.
7. y2 = airfoil half-thickness downstream of xT .
The thickness equation for x < xT :
y1 = ax3 + bx2 + cx+ d (2.24)
y1′= 3ax2 + 2bx+ c (2.25)
y1′′
= 6ax+ 2b (2.26)
15
Figure 2.9: Plot showing the curvature of the camber line of blade sections 10 and 11 of therotor 1 blade from the 10 stage HPC design.
Figure 2.10: Thickness distribution over a non-dimensional unit camber length [2].
and the thickness equation for x > xT :
y2 = e(x− xT )3 + f(x− xT )2 + g(x− xT ) + h (2.27)
y2′= 3e(x− xT )2 + 2f(x− xT ) + g (2.28)
y2′′
= 6e(x− xT ) + 2f (2.29)
When xT ≥ 0.5, the boundary conditions are:
16
At x = 0
y1 =t12
(2.30)
y1′′
= 0 (2.31)
At x = xT
y1 = y2 =T
2(2.32)
y1′= y2
′= 0 (2.33)
y1′′
= y2′′
(2.34)
At x = 1.0
y2 =t22
(2.35)
(2.36)
From these, the coefficients a through h are derived as explained by the author, Wennerstrom in
his book [2]. When xT < 0.5, the leading and trailing edge boundary conditions are reversed to
obtain the coefficients.
The suction side and pressure side coordinates are merged into a single array of specified
number (199 in this case) of non-dimensional coordinates (ub, vb) respectively, such that the
array starts from the trailing edge and goes counter-clockwise through the leading edge and
comes back to the trailing edge. Since the leading edge and trailing edge coordinates of the
pressure side and suction side are the same, only a single value of the leading edge coordinate
is used in the array and the first and last point in the array is the same trailing edge coordinate.
The non dimensional leading edge is chosen as (0,0) and trailing edge as (1,0) for convenience.
The stagger angle, ζ is calculated by taking the average of the blade metal angles at inlet and
17
exit. The normalized staggered airfoil coordinates (m′bstgr, θbstgr) are as given below:
ζ = (β∗in + β∗out)/2 (2.37)
m′bstgr = ub cos (−ζ) + vb sin (−ζ) (2.38)
θbstgr = −ub sin (−ζ) + vb cos (−ζ) (2.39)
Figure 2.11 shows the airfoil rotated by the stagger angle and is placed on the unit chord on
the non-dimensioanl spacing array system (u, v). chrdx is the non dimensional meridional
chord which is the difference between m′TE and m′LE . The actual chord is calculated and the
airfoil coordinates are scaled by multiplying the staggered coordinates (m′bstgr, θbstgr) with the
non-dimensional actual chord as below:
chrdx = |m′TE −m′LE| (2.40)
chrd = chrdx/ |cos ζ| (2.41)
m′b = m′bstgr(chrd) (2.42)
θb = θbstgr(chrd) (2.43)
Figure 2.11: Blade section on the normalized unit chord.
The resultant 2D blade section contains np values of m′b, θb coordinates in the meridional
coordinate system.
18
2.3.1 Variety of Airfoil shapes
3DBGB is flexibile in its capability of generating different airfoil shapes to cope with a variety
of blade designs. Since each blade section is constructed independently through parameters,
it is possible to have different blade sections at different spanwise locations. For example, a
wind turbine blade has a circular hub and progresses towards an S809 airfoil shape radially.
The general capability of the blade section construction makes it easy to deal with such shapes.
Currently, 3DBGB is capable of generating the S809 airfoil, NACA 4-digit airfoils, a circular
section, and the default airfoil which is a mixed camber airfoil as shown in Figure 2.12. In addi-
tion to these, the tool is flexible in adding various airfoil shapes parametrically. It is recognized
that the default blade section is inadequate for a transonic fan, but those sections can be added
in a parametric fashion. This is also true for many other blade types. The integrated ability for a
general blade section and consistent 3D stacking in a rigorous manner sets this blade generator
apart.
Figure 2.12: Variety of airfoils generated by 3DBGB in addition to circular and 4 digit NACAairfoils.
2.4 Leading Edge and Trailing Edge Curves
The leading and trailing edge are defined by 2D cubic spline curves in x, r. A cubic spline is
used to fit the streamline coordinates xs, rs with m′s as the spline parameter. The intersection of
these curves and the 2D streamline curves produces the leading and trailing edge coordinates
19
(xLE, rLE, xTE, rTE) on the corresponding streamlines. This information is used to obtain the
m′sLE , the leading edge m′s value, which is crucial in streamwise mapping of the blade sections.
2.5 Streamwise Mapping of the Blade Sections
The 2D blade sections created are mapped with their corresponding streamlines. The stream-
lines are defined both upstream and the downstream of the blade for robust mapping. Typical
streamsurfaces are defined by revolving the streamlines about the x-axis. For an axial and radial
machine this is shown in Figure 2.13. m′sLE , the leading edge m′s value is calculated by taking
the inverse spline of x(m′s) evaluated at xLE on each of the streamline as shown in Figure 2.14.
The meridional offset between the blade leading edge m′bLE and the streamline leading edge
Figure 2.13: Stream surface for an axial machine and a radial machine respectively.
Figure 2.14: m′sLE obtained using inverse spline on m′s.
20
m′sLE is calculated and is necessary for precise conformation of the blade section on the corre-
sponding streamline. This is because the zero m′s on each streamline is different from the m′bLE
on each corresponding blade section and this offset is expressed as:
δm′ = m′sLE −m′bLE (2.44)
Similarly, there exists a tangential offset which is added to the θb coordinates to obtain stream-
wise θ3D coordinates for the blade:
θ3D = θb + δθ (2.45)
Once all the offsets are calculated, the streamwise meridional coordinates m′3D for each blade
section is obtained using:
m′3D = m′b + δm′ (2.46)
The m′3D coordinates are used to calculate the streamwise x3D and r3D coordinates by evaluat-
ing the spline at every streamwise meridional coordinate as below:
1. x3D = spline evaluated at each m′3D for all the np points of each blade section.
2. r3D = spline evaluated at each m′3D for all the np points of each blade section.
The spline evaluation process is depicted in Figure 2.15 and Figure 2.16.
Figure 2.15: x3D obtained by spline evaluation at each m′3D of each blade section.
Figure 2.17 shows the mapping of the blade section on the corresponding stream surface.
In this manner, all the blade sections are mapped consistently. x3D, r3D and θ3D coordinates for
21
Figure 2.16: r3D obtained by spline evaluation at each m′3D of each blade section.
Figure 2.17: Mapping of the blade section to the corresponding stream surface.
all the nspn 3D blade sections are thus calculated in the cylindrical coordinate system as shown
in section 2.8.
2.6 Sweep and Lean to the Blade
Spanwise Sweep and Lean are applied as perturbations using a specific number of control points
(span, δm′) and (span, δθ). The control points are used to construct a smooth sweep and lean
definition spanwise using uniform B-splines as explained later in this section. The normalized
22
span of the nth streamline for an axial machine is given by :
Lref = rLETIP − rLEHUB (2.47)
span(n) = r(n)− rHUB (2.48)
˜span(n) = span(n)/(Lref ) (2.49)
where Lref is the blade height.
The sweep perturbation, δm′ values at each streamline are evaluated by interpolating the
δm′ curve at each spanwise location on each streamline as depicted in Figure 2.18. In this
manner, the sweep is added to the blade whenever required. Figure 2.19 shows blades with
forward and backward sweep respectively.
Figure 2.18: δm′ evaluated at each span.
Similarly, the lean is added to the blade as required by defining the lean perturbation with
few control points and obtaining the δθ values at each streamline as explained above. This
method as shown in Figure 2.20 was used to modify the lean near the hub of rotor 3 of the
booster optimum shown as point 2 in the paper by Park et al. [4] to eliminate the corner sep-
aration at the exit which increased the adiabatic efficiency for the isolated blade row 3D CFD
analysis of rotor 3 as explained by Siddappaji et al. [15].
23
Figure 2.19: Forward and backward swept blades respectively.
Figure 2.20: Spanwise lean modification on rotor 3 of a booster optimum resulting in lean nearthe hub.
2.6.1 Construction of Uniform B-Splines
A group of local control points are used to determine the geometry of curve segments which
form a B-spline. A curve segment does not necessarily have to pass through a control point but
its desired at the two end points of the B-spline. Cubic B-splines are popular because of their
continuity characteristics which make the segment joints smooth [3]. Figure 2.21 shows a cubic
curve constructed from a series of curve segments S0, S1, S2, ..., Sm−3,... using m + 1 control
points P0, P1, P2, ..., Pm.
Any single segment Si(t) of a B-spline curve is defined by
Si(t) =3∑r=0
Pi+rBr(t) (2.50)
24
Figure 2.21: Construction of a uniform non-rational B-spline curve. [3]
where t (0 ≤ t ≤ 1) is a parameter and the B-spline basis functions are as below [3]
B0(t) =−t3 + 3t2 − 3t+ 1
6=
(1− t)3
6(2.51)
B1(t) =3t3 − 6t2 + 4
6(2.52)
B2(t) =−3t3 + 3t2 + 3t+ 1
6(2.53)
B3(t) =t3
6(2.54)
The B-spline curve, Q1(t) is represented in matrix form [3] by
Q1(t) =
[t3 t2 t 1
]1
6
−1 3 −3 1
3 −6 3 0
−3 0 3 0
1 4 1 0
Pi
Pi+1
Pi+2
Pi+3
(2.55)
where Pi, Pi+1, Pi+2 and Pi+3 are the 4 consecutive control points of the total number of
control points. So, if there are 5 control points then the first curve segment is made up of the
first 4 control points (1, 2, 3, 4) and the second curve segment is made up of the second 4
consecutive control points (2, 3, 4, 5).
This method of construction is used in adding the lean and sweep to the blade. Once the B-
25
spline is constructed, a simple 2D-curve and a line intersection procedure will give the desired
point on the spline curve. For example, spanwise sweep is defined by the control points (span,
δm′). A B-spline curve of δm′ is constructed as explained above. The δm′ value at a particular
spanwise location is obtained by intersecting the 2D δm′ curve with the line (parallel to X-axis)
passing through that location as shown in Figure 2.18.
2.7 Radial Stacking of 3D Blade Sections
The 3D blade sections are stacked radially by including a θ offset, θstack for each individual
blade section. Stacking is defined as a fraction of the non-dimensional actual chord. This
value is transformed into the average θ3D coordinate, which is subtracted from the array of θ3D
coordinates to obtain the stacking. The stacking can be done at the leading edge, trailing edge,
at any percentage of the chord and at the area centroid of a blade section.
θ3D = θb + δθ + θstack (2.56)
Figure 2.22 explains the theta offset defined for stacking the blade at the leading edge, percent-
age chord and the trailing edge correspondingly. Finally, using the coordinate transformation
the 3D blade coordinates in the cartesian system is obtained for this case.
2.8 Coordinate Transformation
The normal practice is to obtain a 3D blade in the cartesian coordinate system as most of the
CAD packages exist in this system. Therefore a coordinate transformation from the cylindrical
system to the cartesian system is necessary. The engine axis is assumed to be along the X-axis
which makes the x-values remain the same in both coordinate systems.
The transformation is as follows:
26
Figure 2.22: θ offset defined for various stacking option.
x3D = x3D (2.57)
y3D = r3D × sin θ3D (2.58)
z3D = r3D × cos θ3D (2.59)
2.9 Output files
The blade generator code outputs nspn data files, which contain np values of 3D coordinates
for all the nspn blade sections. The number of coordinates in the 3D blade sections are kept the
same as the number of coordinates in the 2D airfoil sections. The 3D blade section files can act
as input files for any CAD package to obtain a 3D Blade CAD model.
27
2.10 3D Blade CAD Model
All the data files are imported in Unigraphics (CAD package) and a lofting procedure is per-
formed to create 3D blade surfaces passing through the blade sections to obtain a smooth 3D
blade as shown in the Figure 2.23. The parameters used in lofting are the 3D spline data ob-
tained as the 3D blade section data from 3DBGB for each blade section .
Figure 2.23: 3D Blade lofted in UG.
2.11 Connecting with CAPRI
CAPRI stands for Computational Analysis PRogramming Interface. The 3D Blade constructed
in UG is a base model and using CAPRI [22, 23], newer blade shapes are obtained by simply
updating the spline information of each 3D blade section on the base model. A simple program
written in C integrates the 3D blade part file and the CAPRI interface through which the spline
update is done and hence the blade geometry is morphed parametrically. The advantage of
using CAPRI is that the geometry data remains in the CAD system and avoids the geometry
translation errors during morphing of the blade geometry.
CAPRI saves significant time and effort in development, deployment, and maintenance of
multi-disciplinary design suites that need to interface with CAD. It does not require low-level
expertise in CAD or CAD programming to use, and provides an intuitive engineering interface
to CAD for MDAO applications.
28
2.12 Extruded Blade
In some cases, grid generators require an extruded blade due to tolerance issues and extrusion
is a property which is useful for other purposes as well. It is achieved through a simple offset
of the hub and the tip streamline coordinates in the normal direction to the streamline. At any
point m′s, the normal in the x-direction, xNORM and the normal in the r-direction, rNORM are
calculated by using the orthogonal property between the normal and the slope at that point.
xNORM =drsdm′s
(2.60)
rNORM = − dxsdm′s
(2.61)
So, the offset in the normal direction as shown in Figure 2.24 is given by
∆n = aLref , (2.62)
where a is the percent offset desired and Lref is the reference length.
Figure 2.24: Offset at the hub streamline.
Also,
∆n = b√xNORM 2 + rNORM 2 (2.63)
where b is an intermediate extruded blade scale factor. b is solved using the 4 equations above,
and the offset at the hub and the tip is obtained as below:
1. streamline coordinates at the hub : xsHUB, rsHUB
29
2. streamline coordinates at the tip : xsTIP , rsTIP
xsExtruded = xsHUB + (b× xNORM) (2.64)
rsExtruded = rsHUB + (b× rNORM) (2.65)
and the offset at the tip as
xsExtruded = xsTIP − (b× xNORM) (2.66)
rsExtruded = rsTIP − (b× rNORM) (2.67)
The new extruded hub and tip streamline coordinates are used instead of the original coordinates
and the blade parameters corresponding to the original hub and tip streamlines are used as the
input to obtain an extruded 3D blade as shown in Figure 2.25 using the procedure as explained
before.
Figure 2.25: Extruded blade at the tip with hub and casing.
30
Chapter 3
CFD Analysis of the 3D blade
A CFD simulation is used to analyze the resulting 3D blade geometry. FINETM/Turbo v8 by
Numeca [24] was used for the 3D CFD analysis on the blade model obtained. FINETM/Turbo
is a high fidelity package which has its own gridding tool, solver and a post processor.
3.1 Gridding
The 3D blade section geometry created along with the hub and the shroud definition was im-
ported into a gridding tool called AutoGrid5 [25]. The blade geometry is the rotor 3 blade of
the 3 stage booster from a paper by Park et. al [4]. The blade model thus imported is given
a tip clearance and other necessary input details such as the rotational speed and type of tur-
bomachinery system. The tip clearance is 0.15% of rotor tip radius which is representative of
a compressor with tight but realistic tip clearance. The grid generated is medium type with
858149 grid points. The flow path is generated and blade to blade mesh is created as shown in
Figure 3.1.
3.2 CFD solver: Euranus
Euranus, the FINETM/Turbo solver is run with inlet boundary conditions of absolute total
pressure, absolute total temperature, spanwise distribution of αx at inlet and φ coming from the
previous blade row and static pressure as the exit boundary condition. An isolated blade row
31
3D CFD analysis of rotor 3 of the booster optimum shown as point 1 in paper by Park et. al
[4] has been performed. Because of the thick boundary layer of the axisymmetric analysis, the
first displaced streamline was used to define the hub and the last displaced streamline was used
to define the casing. The simulation resulted in an adiabatic efficiency of 91.25% at the design
flow rate. This compares 93.47% from the T-Axi axisymmetric code loss model [17]. Several
runs were made on this case by varying the back pressure to create a speed line (the design mass
flow rate is 92.229 kg/s). Figure 3.2 shows the mass flow rate variation with the total pressure
ratio and Figure 3.3 shows the variation of mass flow rate with the isentropic efficiency and the
wide range of the mass flow rate for the booster can be noticed. Figure 3.4 shows the contour
plot of relative mach numbers from 0.2 to 0.8 on three constant radius cut-planes across rotor
3 of the booster. It also shows stream ribbons across the tip clearance showing the tip vortex.
Reasonable agreement between the axisymmetric and 3D demonstrates how the coupled system
can be used for optimizing a design.
Figure 3.2: Characteristic curve showing Total PR vs mass flow rate.
The isolated blade row 3D CFD analysis of rotor 3 of the booster optimum shown as point
2 in the paper by Park et. al [4] was also performed which resulted in corner separation at the
33
Figure 3.3: Characterisitic curve showing Isentropic efficiency vs mass flow rate.
Figure 3.4: Relative Mach contours of rotor 3 of the optimized booster with stream ribbons atover the tip clearance.
34
exit with an adiabatic efficiency of 93.17%. The lean of the 3D blade geometry was modified as
shown in Figure 3.5 which eliminated the separation near the exit as shown in Figure 3.6 which
is the comparison of the iso surface of axial velocity for the original and modified rotor 3 for
this case. The adiabatic efficiency increased to 93.93%. This compares to the T-Axi efficiency
of 95.27% for this rotor. It should be noted that this is still not an optimum. The shape shows
that there might be stress issues except that the wheel speed is so low which is why the coupling
with a finite element structural solver is so important.
Figure 3.5: Spanwise lean modification on rotor 3.
Figure 3.6: Iso surface comparison of axial velocity for original and modified rotor 3 of thebooster optimum point 2 [4].
35
Chapter 4
Structural Analysis of the 3D Blade
Structural Analysis is a critical design simulation capability and its use is demonstrated on the
blade geometry. ANSYS V12.0 [26] is used. A CAD part file of the 3D blade model is imported
and a script file called ’Blade.ain’ is used which contains the material properties of the blade
and also the instructions for meshing the blade. This creates a meshed blade with hexagonal
mesh as shown in Figure 4.1 and is ready for structural analysis. The blade model used is the
rotor 1 blade of the 10 stage High Pressure Compressor. A modal analysis is performed with 14
modes and the procedure is as follows:
• Analysis type is defined.
Solution→ Analysis Type→ New Analysis→Modal.
• Analysis option is set.
Solution→Analysis Type→Analysis Options→ Preconditioned Conjugate Gradient (PCG)
Lanczos.
• Number of modes to extract is 14 and it extracts modes for all Degrees Of Freedoms
(DOF’s).
• Constraints are applied.
Solution→ Define Loads→ Apply→ Structural→ Displacement→ On Areas.
• The hub area of the blade is selected.
36
Figure 4.1: Blade meshed in ANSYS V12.0.
• The system is solved.
Solution→ Solve→ Current Load Step (LS).
After the solution is complete post processing is performed. Figures 4.2 and 4.3 shows
the contour plots of the Displacement vector sum of Degrees Of Freedom (DOF) solution under
Nodal solution for all the 14 modes of the blade. The plots are of a deformed shape of the blade.
Figure 4.2: Contour plots of Displacement vector sum for first 7 modes of a blade under Nodalsolution.
37
Figure 4.3: Contour plots of Displacement vector sum for last 7 modes of a blade under Nodalsolution.
Also, Figure 4.4 shows the displaced blade with the undisplaced blade shape keeping the
hub of the blade fixed. This completes the structural analysis of the blade.
Figure 4.4: Displaced blade.
38
Chapter 5
Example Design Problems
The capability of the 3DBGB is demonstrated through the following examples. The examples
include a 10 stage EEE high pressure compressor design, a 3 stage booster, a low speed centrifu-
gal compressor, all of which are generated using the design data from reports. A wind turbine
design is also demonstrated, and has been reverse engineered from pictures, marketing literature
[6] and a report [27]. All these example cases are available at http://gtsl.ase.uc.edu/3DBGB/.
5.1 10 Stage EEE High Pressure Compressor Design
The GE Energy Efficient Engine (E3) high pressure compressor (HPC) as shown in Figure 5.1
was used as an example, which has 21 blade rows with 10 stages and an IGV. Two cases were
generated, one with free vortex having straight leading and trailing edges and the other with full
definition of spanwise angular momentum having non-straight leading and trailing edges.
5.1.1 Free vortex Design
|
The angular momentum is kept constant along the blade span for all the blade rows for
this case and it has straight leading and trailing edges. The input files for running T-Axi (ax-
isymmetric solver) [16, 17, 18, 19] for this case are available on the T-Axi website[16] under
input.zip/T-AXI Input Files/EEE-HPC-des. The axisymmetric grid of this 10 stage HPC (free
vortex) is shown in Figure 5.2. The grid is created by the hub and casing definitions used in
39
Figure 5.1: E3 10 Stage Compressor Cross Section. [1]
the solver and the green lines represent the leading and trailing edges of the blade rows coming
from the T-Axi input file.
The T-Axi solution provides information about flow angles, relative mach number and other
Figure 5.2: Axisymmetric grid showing the streamlines of 10 Stage HPC free vortex design andthe straight leading and trailing edge locations of the blade rows in green.
aerodynamic data at each streamline along with providing the location of the leading and trail-
ing edges on each streamline. It also outputs the input file for 3DBGB, containing the required
aerodynamic and geometric parameters to generate the 3D blade shape. For this case, the flow
angles are used as the blade metal angles to generate the airfoil sections. All the values of co-
ordinates were normalized using the leading edge tip radius of rotor 1. The chord is internally
calculated. The maximum thickness to chord ratio for rotors is defined linearly from 0.1 at the
hub to 0.025 at the tip, for stators from 0.05 at the hub to 0.1 at the tip and for IGV a constant
value of 0.085. These numbers are based on the GE EEE report [1]. The 3D blade shape has 10
blade sections. One of the 3D blade is built using 3DBGB and lofted using UG-NX. The rest of
40
the blades are obtained by updating the spline data on the initial blade using CAPRI [22, 23].
The spline data is produced as 3D blade section data for the respective blades by 3DBGB. The
blades are stacked at their leading edge for this case. The rotor 1 and rotor 3 blade shapes for
the free vortex design are shown in Figure 5.3.
Figure 5.3: Rotor 1 and rotor 3 of EEE HPC free vortex design created using 3DBGB.
In this manner, all the 21 blade rows are constructed and are assembled with their corre-
sponding disks optimized with T-Axi Disk [5, 20] to obtain blisks. Rotor 1 and rotor 3 blisks
are shown in Figure 5.4.
41
5.1.2 Full Definition 10 stage Design
The angular momentum along the blade span is not constant for the E3 case and it has non-
straight leading and trailing edges. The input files for running T-Axi for this case are available
on the T-Axi website [16] under input.zip/T-AXI Input Files/EEE-HPC-analyse. The axisym-
metric grid of the GE EEE HPC (full definition) is shown in Figure 5.5. The grid is created by
the hub and casing definitions used in the solver and the green lines represent the leading and
trailing edges of the blade rows coming from the T-Axi input file.
Figure 5.5: Axisymmetric grid showing the streamlines of E3 10 Stage HPC full definitiondesign and the leading and trailing edge locations of the blade rows in green.
The T-Axi solution gives flow angles and other aerodynamic data for all the specified 21
streamlines and also outputs 3DBGB input containing required information for 21 streamlines.
For this case, the blade metal angles from the NASA report[1] were used to construct the airfoil
sections. The NASA report contains data tables of blade metal angles, maximum thickness
to chord ratio and other parameters tabulated spanwise for all 21 bladerows of the GE EEE
High Pressure Compressor. The report has data tabulated at 12 spanwise locations for each
blade. These 12 values of the blade metal angles and the maximum thickness to chord ratio
were interpolated to 21 values since this 3DBGB input has 21 spanwise locations. All the
values of coordinates were normalized using the leading edge tip radius of rotor 1. A spanwise
comparison of the 12 values of blade metal angles (β∗1 , β∗2) at inlet and exit of rotor 3 as given
in the NASA report [1] with 21 interpolated values obtained by 3DBGB is shown in Figure 5.6.
Using these interpolated values and the internally calculated leading and trailing edge locations,
a 3D blade shape with non-straight leading and trailing edge is constructed for rotor 3 in this
case and is shown in Figure 5.7. The first 5 rotors were stacked at the center of the 2D airfoil
43
Figure 5.6: Comparison of blade metal angles of EEE-HPC rotor 3 given in the report [1] andgenerated by 3DBGB.
area and the rest were stacked at quarter chord radially. All the other 20 blades are constructed
using CAPRI and respective spline data as explained before. A complete assembly with all the
10 rotors, 10 stators and the IGV is created in UG without the hub and the casing definition and
is shown in Figure 5.8.
Figure 5.7: Rotor 3 of GE EEE HPC full definition design with non-straight leading and trailingedges.
44
Figure 5.8: Rotor and stator assembly for 10 stage HPC full definition design from the GE/E3
parameters.
45
5.2 3 Stage Booster Design for Turbofan Engine
A 3 stage booster for a turbofan engine (CFM56 class machine) was designed. Boosters are
used in turbofan engines before the high pressure compressor. The 3 stage booster of the GE90
turbofan engine shown in Figure 5.9 depicts where the boosters are used.
Figure 5.9: 3 stage booster of a GE90 turbofan engine.[5]
A 3 stage booster flow path geometry along with the blades was optimized as explained in
the paper by Park et. al [4] and the best result was used for generating 3D blades. The ax-
isymmetric grid of the optimized booster is shown in Figure 5.10 which shows the streamlines
calculated by T-Axi and the leading and trailing edges of blade rows in green lines. The axisym-
metric solver (T-Axi) is run and the input for 3DBGB was obtained. The flow angles are used as
the blade metal angles for the 2D airfoils construction. The maximum thickness to chord ratio
for rotors is defined linearly from 0.1 at the hub to 0.025 at the tip and for stators from 0.05 at
the hub to 0.1 at the tip. All the blade rows are created as explained in the previous example
and the rotors and stators are assembled as shown in Figures 5.11 and 5.12.
The validation of rotor 3 was done by performing a 3D-CFD analysis which is explained in
Chapter 3. The FEA structural analysis was also performed on rotor 3 with a tetrahedral mesh
as shown in Figure 5.13. A modal analysis on the blade resulted in 14 modal shapes and the
46
Figure 5.10: Axisymmetric grid of the 3-stage optimized booster showing the streamlines andthe leading and trailing edge locations of the blade rows in green.
Figure 5.11: 3 stage booster rotor assembly with the fan blades.
47
contour plots of the displacement vector sum is shown in Figure 5.14.
Figure 5.13: Tetrahedral mesh of rotor 3 of a 3 stage booster in ANSYS.
Figure 5.14: Contour plots of displacement vector sum of all 14 modes of rotor 3 under Modalsolution.
49
5.3 Reverse-Engineered Wind Turbine Design
Wind turbines can be treated as turbines without the nozzle. All the turbomachinery principles
apply to them. 3DBGB is capable of creating wind turbine blades due to its generality. This
capability is demonstrated by building the reverse engineered GE 1.5 MW wind turbine blade as
shown in Figure 5.15. Pictures, marketing literature [6] and a report [27] were used for reverse
engineering.
Figure 5.15: GE 1.5 MW wind turbine blade. [6]
The case for T-Axi was set up as explained in the Masters thesis by Dey [28]. The axisym-
metric grid of the reverse engineered GE wind turbine blade is shown in Figure 5.16. The wind
turbine was treated as a half stage turbine with extended tip in T-Axi solver. T-Axi generates the
input for 3DBGB and the wind turbine 3D blade geometry is created as shown in Figure 5.17. It
is then assembled with the bullet nose and a wind turbine model with 3 blades is created using
UniGraphics as shown in Figure 5.18. While generating a similar wind turbine blade shape,
one of the issues encountered was going beyond axial (ζ equal to 92 degrees), where the blade
shapes failed to be generated since the chrd value calculated according to the Eq.(2.41) became
a non-defined value as cosine of the stagger angle reaches zero. To overcome this issue, a switch
was added in the input file which would read the actual non-dimensional chord values chrd for
such high staggered cases instead of using Eq.(2.41). The addition of this option expands the
capability of the tool to include blades with very high stagger.
The utility of the blade generation is demonstrated by performing CFD analysis as explained
in the Masters thesis by Dey [28]. FEA structural analysis was also performed by treating the
blade as a rotating cantilever beam. The meshed blade has 8 node hexahedron brick 185 element
50
Figure 5.16: Axisymmetric grid of the reverse engineered GE 1.5 MW wind turbine blade.
Figure 5.17: Reverse engineered GE 1.5 MW wind turbine blade geometry created using3DBGB.
51
as shown in Figure 5.19. Structural analysis was executed and the Von-Mises plot is shown in
Figure 5.20. Aluminium material was used for the blade which has the yield strength of 414
MPa. The maximum value of the von-mises stress obtained was 47.417 MPa, which is less than
one third times the yield strength.
Figure 5.19: Meshed wind-turbine blade with 8 node Hexahedron Brick 185 element.
Figure 5.20: Von-Mises Stress plot on GE reverse engineered blade.
The first 5 mode shapes for the reverse engineered GE wind turbine blade is shown in
Figure 5.21.
53
(a) Mode-1 04.131 Hz (flapwise). (b) Mode-2 05.576 Hz (edgewise).
(c) Mode-3 18.318 Hz (flapwise). (d) Mode-4 20.778 Hz (mixed).
(e) Mode-5 26.648 Hz (mixed).
Figure 5.21: First 5 Modal solution of GE reverse engineered blade.
54
5.4 Low-Speed Centrifugal Compressor design
3DBGB is also capable of designing 3D blades for radial machines. The low-speed centrifugal
compressor (LSCC) blade model is generated as an example case. The compressor is based on a
NASA design [7] and has 20 blades with the speed of 1862 rpm. The flowpath of the compressor
with the actual experimental setup measurements is shown in Figure 5.22. Figure 5.23 shows
the radial grid of the compressor with hub and casing definition and the streamlines along with
leading edge and trailing edge locations denoted by green lines.
Figure 5.22: LSCC flowpath with actual measurements. [7]
The NASA report [7] contains hub and tip streamline coordinates and other airfoil geometry
data. The hub and tip flowpath were linearly interpolated in the radial direction to generate more
construction lines. A total number of 5 construction lines including the hub and tip streamlines
were generated. All the coordinates were normalized with the leading edge tip radius value.
The inlet was treated to be purely axial with constant axial velocity, Vz. The wheel speed at the
tip, Ut is given to be 153 m/s. The report had spanwise plots of VzUt
ratios and an average value
of 0.4 at 50% pitch was used to calculate the constant axial velocity as 61.2 m/s. Figure 5.24
shows the velocity triangle for the purely axial flow at the leading edge, where the relative flow
angles at the leading edge for different spans are calculated as below:
55
Figure 5.23: A radial compressor flowpath showing the hub and casing with streamlines andthe leading and trailing edge locations.
1. Vz = Axial flow velocity.
2. U = Wheel speed.
3. N = Wheel rotational speed in RPM.
4. W = Relative flow velocity = U = ωr.
5. r = radius in meters.
6. ω = 2πN60
7. Wθ = Tangential relative flow velocity.
8. βz = Relative flow angle = tan−1 Wθ
Vz.
The outlet was treated to be purely radial with constant relative flow angle of 55o spanwise.
The design methodology used to create axial blades was applied except, the blade was stacked at
the trailing edge. Also, a condition was added to check the slope of the streamline to distinguish
between radial and axial machines. When,
∣∣∣∣ drsdm′s
∣∣∣∣ > ∣∣∣∣ dxsdm′s
∣∣∣∣ (5.1)
56
Figure 5.24: Velocity triangle at the leading edge for the radial compressor.
normalized rs values (in radial cases) are used to obtain m′TE (or m′LE when the flowpath starts
as radial) through inverse spline, instead of the usual method of using normalized xs values (in
axial cases) while calculating the non-dimensional meridional chord. The 3D blade sections
are created and stacked with the trailing edge as the stacking axis. Once the blade sections are
obtained, they are lofted using Unigraphics-NX to obtain a solid blade model. The assembled
compressor with 20 blades and its comparison to the model from the NASA report [7] is shown
in figure 5.25.
Figure 5.25: Radial compressor model compared with NASA LSCC [7].
57
Chapter 6
Conclusion and Future Work
6.1 Conclusion
The development of a parametric 3D blade geometry modeling tool for turbomachinery has been
presented. The tool is capable of generating a specified number of data files containing np coor-
dinates of 3D blade sections based on very few geometric and aerodynamic parameters. The 3D
blade sections can be imported into a CAD package to obtain a smooth lofted blade. The geom-
etry modification process is made quicker and easier by the parametric definition of the splines.
The benefits of this new method are a large design space including many stacking options with a
small number of parameters. The flexibility of the tool has been demonstrated by locally modi-
fying the lean in the hub of rotor 3 of a 3-stage booster for turbofan engine to eliminate a corner
separation. The geometry tool and the demonstrated connection of this tool to a CFD code and
FEA code is part of a complete high fidelity design system. The capability to create 3D blades
for various types of turbomachinery has demonstrated the generality of the approach through
various example cases. The utility of the 3D blade geometry generation is demonstrated by per-
forming a 3D-CFD analysis and an FEA structural analysis on the obtained blade shape. The
flexibility and generality of the tool is also demonstrated through the examples. The executable
that creates the 3D blades is freely available at http://gtsl.ase.uc.edu/3DBGB/ along with the
example cases.
58
6.2 Future Work
The tool is ready for adding many other capabilities which will make it more general and robust.
The parametrization of the camber and thickness distribution will make designing of transonic
airfoils possible. Future work also includes more options for blade sections and defining the 2D
blade sections parametrically as a combination of many different sections. Also, this tool can
be tied to an optimizer to obtain optimized 3D blade geometries. 3DBGB can really grow into
a powerful and an extremely flexible geometry generator.
59
References
[1] Holloway, P., Knight, G., Koch, C., and Shaffer, S., 1982. Energy efficient engine high
pressure compressor detail design report. Tech. rep., General Electric Company, NASA-
CR-165558.
[2] Wennerstrom, A. J., 2000. Design of Highly Loaded Axial-flow Fans and Compressors.
Concepts ETI, Inc., Vermont.
[3] Vince, J., 2006. Mathematics for Computer Graphics 2nd Edition. Springer, New Jersey.
[4] Park, K., Turner, M. G., Siddappaji, K., Dey, S., and Merchant, A., 2011. “Optimization
of a 3-stage booster part 1: The axisymmetric multi-disciplinary optimization approach to
compressor design”. ASME Paper Number GT2011-46569.
[5] Gutzwiller, D. P., 2009. “Automated design, analysis, and optimization of turbomachinery
disks”. Master’s thesis, University of Cincinnati, Cincinnati, OH, September.
[6] GE-Power. http://www.gepower.com/prod\_serv/products/wind\
_turbines/en/15mw/index.htm.
[7] Hathaway, M. D., Chriss, R. M., Strazisar, A. J., and Wood, J. R., 1995. Laser anemometer
measurements of the three-dimensional rotor flow field in the nasa low-speed centrifugal
compressor. Tech. rep., NASA ARL-TR-333.
[8] Grasel, J., Keskin, A., Swoboda, M., Przewozny, H., and Saxer, A., 2004. “A full para-
metric model for turbomachinery blade design and optimisation”. DETC Paper Number
DETC2004-57467.
60
[9] Dutta, A. K., Flassig, P. M., and bestle, D., 2008. “A non-dimensional quasi-3d blade
design approach with respect to aerodynamic criteria”. ASME Paper Number GT2008-
50687.
[10] Koini, G. N., Sarakinos, S. S., and Nikolos, I. K., 2009. “A software tool for paramet-
ric design of turbomachinery blades”. Advances in Engineering Software, 40, January,
pp. 41–51.
[11] Korakianitis, T., 1993. “Prescribed-curvature-distribution airfoils for the preliminary geo-
metric design of axial turbomachinery cascades”. ASME Journal of Turbomachinery, 115,
April, pp. 325–333.
[12] Anders, J. M., Haarmeyer, J., and Heukenkamp, H., 1999. “A parametric blade design
system (part 1 + 2)”. In Von Karman Institute for fluid dynamics: lecture series 1999-
2002 turbomachinery blade design systems.
[13] IV, P. L. M., Oliver, J. H., Miller, D. P., and Tweet, D. L., 1996. “Bladecad: An interactive
geometric design tool for turbomachinery blades”. 41st Gas Turbine and Aeroengine
Congress sponsored by ASME, NASA Technical Memorandum 107262.
[14] NASA Research Announcement NNNC07CB61C-06-SSFW2-06-0071, Advanced De-
sign Techniques for MDAO of Turbomachinery with Emphasis for the Engine System.
[15] Siddappaji, K., Turner, M. G., Dey, S., Park, K., and Merchant, A., 2011. “Optimization
of a 3-stage booster- part 2: The parametric 3d blade geometry modeling tool”. ASME
Paper Number GT2011-46664.
[16] University of Cincinnati T-Axi Website http://gtsl.ase.uc.edu/T-AXI/.
[17] Turner, M. G., Merchant, A., and Bruna, D., 2006. “A turbomachinery design tool for
teaching design concepts for axial-flow fans, compressors, and turbines”. ASME Paper
Number GT2006-90105.
[18] Turner, M. G., Bruna, D., and Merchant, A., 2007. “Applications of a turbomachinery
design tool for compressors and turbines”. AIAA Paper Number 2007-5152.
61
[19] Bruna, D., Cravero, C., Turner, M. G., and Merchant, A., 2007. “An educational software
suite for teaching design strategies for multistage axial flow compressors”. ASME Paper
Number GT2007-27160.
[20] Gutzwiller, D. P., Turner, M. G., and Downing, M. J., 2009. “Educational software for
blade and disk design”. ASME Paper Number GT2009-59692.
[21] Goodhand, M. N., and Miller, R. J., 2010. “The impact of real geometries on three-
dimensional separations in compressors”. ASME Paper Number GT2010-22246.
[22] Haimes, R., and Follen, G. J., 1998. “Computational analysis programming interface”. 6th
International Conference on Numerical grid generation in computational field simulations.
[23] Merchant, A., and Haimes, R., 2003. “A cad-based blade geometry model for turboma-
chinery aero design systems”. In GT-2003-38305.
[24] NUMECA International. FINE/Turbo http://numeca.be/index.php?id=16.
[25] NUMECA International. Autogrid http://numeca.be/index.php?id=25.
[26] ANSYS Inc. www.ansys.com/products/Workflow+Technology.
[27] A.Griffin, D. Tech. rep., Global Energy Concepts,LLC, Washington,USA. SAND2002-
1879.
[28] Dey, S., 2011. “Wind turbine blade design system - aerodynamic and structural analysis”.
Master’s thesis, University of Cincinnati, Cincinnati, OH, May.
62
Input parameters (version 1 . 0 )
e3c−des
Blade row # :
6
Number of blades in this row :
50
Blade Scaling factor (mm ) :
350.700000000000
Number of streamlines :
21
Non−dimensional Actual chord (0=no , 1=yes ) :
0
J in_Beta out_Beta mrel_in chord t /c_max Incidence Deviation Sec . Flow Angle
1 −54.45378568 −34.39556205 0 .83674931 0 .14516934 0 .10000000 0 .00000000 0 .00000000 0 .00000000
2 −55.14168979 −35.61221762 0 .84411465 0 .14191943 0 .09625000 0 .00000000 0 .00000000 0 .00000000
3 −55.82137412 −36.65746602 0 .85230672 0 .13871866 0 .09250000 0 .00000000 0 .00000000 0 .00000000
4 −56.45007999 −38.03929806 0 .86180055 0 .13540971 0 .08875000 0 .00000000 0 .00000000 0 .00000000
5 −57.10874871 −39.44286108 0 .87366224 0 .13191032 0 .08500000 0 .00000000 0 .00000000 0 .00000000
6 −57.64493298 −40.71282164 0 .88426519 0 .12861769 0 .08125000 0 .00000000 0 .00000000 0 .00000000
7 −58.11412665 −41.99550525 0 .89502469 0 .12533620 0 .07750000 0 .00000000 0 .00000000 0 .00000000
8 −58.61624717 −43.28572053 0 .90780043 0 .12207390 0 .07375000 0 .00000000 0 .00000000 0 .00000000
9 −59.07111963 −44.53789880 0 .92071561 0 .11883727 0 .07000000 0 .00000000 0 .00000000 0 .00000000
10 −59.48807345 −45.71110426 0 .93380343 0 .11563147 0 .06625000 0 .00000000 0 .00000000 0 .00000000
11 −59.90159667 −46.94121033 0 .94713464 0 .11246059 0 .06250000 0 .00000000 0 .00000000 0 .00000000
12 −60.31118168 −48.05673163 0 .96134154 0 .10932787 0 .05875000 0 .00000000 0 .00000000 0 .00000000
13 −60.69878423 −49.16722571 0 .97579120 0 .10623587 0 .05500000 0 .00000000 0 .00000000 0 .00000000
14 −61.06564215 −50.19665595 0 .98960204 0 .10319161 0 .05125000 0 .00000000 0 .00000000 0 .00000000
15 −61.45947417 −51.22287760 1 .00527050 0 .10017988 0 .04750000 0 .00000000 0 .00000000 0 .00000000
16 −61.83652305 −52.21555570 1 .02005852 0 .09721474 0 .04375000 0 .00000000 0 .00000000 0 .00000000
17 −62.21836349 −53.11690457 1 .03477831 0 .09429861 0 .04000000 0 .00000000 0 .00000000 0 .00000000
18 −62.62239995 −53.91798953 1 .05017808 0 .09143510 0 .03625000 0 .00000000 0 .00000000 0 .00000000
19 −63.08901141 −54.67551014 1 .06535098 0 .08863005 0 .03250000 0 .00000000 0 .00000000 0 .00000000
20 −63.60623898 −55.35913372 1 .07943082 0 .08589361 0 .02875000 0 .00000000 0 .00000000 0 .00000000
21 −64.13495390 −55.94734533 1 .09180298 0 .08324520 0 .02500000 0 .00000000 0 .00000000 0 .00000000
LE / TE curve (x ,r ) definition :
Number of Curve points :
2
64
xLE rLE xTE rTE
0 .91899200 0 .70675600 1 .02250000 0 .72333900
0 .93725400 0 .94021300 1 .01388300 0 .93371600
Airfoil type{bf1 (sect1 ) + bf2 (sect2 ) + . . . } :
J type
1 sect1
2 sect1
3 sect1
4 sect1
5 sect1
6 sect1
7 sect1
8 sect1
9 sect1
10 sect1
11 sect1
12 sect1
13 sect1
14 sect1
15 sect1
16 sect1
17 sect1
18 sect1
19 sect1
20 sect1
21 sect1
Control table for blending section variable :
5 0 0
span bf1 bf2
0.000000000000000E+000 1 0
0.250000000000000 1 0
0.500000000000000 1 0
0.750000000000000 1 0
1.00000000000000 1 0
Stacking axis as a fraction of chord ( 2 . =centroid ) :
0 . 2 5
65
Control points for delta_m :
5
span delta_m
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for delta_theta :
5
span delta_theta
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for in_beta* :
5
span in_beta*
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for out_beta* :
5
span out_beta*
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for chord :
5
66
span chord
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for tm /c :
5
span tm /c
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Hub offset
0.000000000000000E+000
Tip offset
0.000000000000000E+000
Streamline Data
x_s r_s
−0.300000000000000 0.492475000000000
−0.200000000000000 0.492475000000000
−0.100000000000000 0.492475000000000
−5.000000000000000E−002 0.492475000000000
0.000000000000000E+000 0.492475000000000
6.640000000000000E−004 0.492545000000000
0.100306000000000 0.503049000000000
0.140864000000000 0.507324000000000
0.422865000000000 0.583169000000000
0.456012000000000 0.592084000000000
0.570901000000000 0.622984000000000
0.608699000000000 0.633150000000000
0.760491000000000 0.671114000000000
0.806337000000000 0.682580000000000
0.889386000000000 0.703351000000000
0.918992000000000 0.710756000000000
67
1.02250000000000 0.727339000000000
1.06183400000000 0.733641000000000
1.13265500000000 0.744987000000000
1.16505200000000 0.750178000000000
1.24483500000000 0.757601000000000
1.28248100000000 0.761104000000000
1.34497700000000 0.766919000000000
1.37353300000000 0.769577000000000
1.43689600000000 0.770937000000000
1.46249900000000 0.771486000000000
1.51795200000000 0.772677000000000
1.56858900000000 0.773763000000000
1.62055600000000 0.775954000000000
1.64641300000000 0.777043000000000
1.70237400000000 0.779402000000000
1.72838100000000 0.780498000000000
1.78114700000000 0.780206000000000
1.80915200000000 0.780050000000000
1.86586300000000 0.779736000000000
1.91677400000000 0.779454000000000
1.96782300000000 0.780179000000000
1.99820500000000 0.780610000000000
2.05502500000000 0.781416000000000
2.08450500000000 0.781834000000000
2.13184700000000 0.781235000000000
2.16284600000000 0.780843000000000
2.21513700000000 0.780180000000000
2.24599000000000 0.779790000000000
2.28900500000000 0.780295000000000
2.32042700000000 0.780664000000000
2.37099600000000 0.781258000000000
2.39886900000000 0.781586000000000
2.44886900000000 0.781586000000000
2.49886900000000 0.781586000000000
2.59886900000000 0.781586000000000
2.69886900000000 0.781586000000000
0 0
0.887027885345457 0.714158560015747
0.898121204156214 0.716613437507956
68
0.909227551237750 0.718994592353480
0.920358329740695 0.721263142568342
0.931524449485138 0.723394872581633
0.942729760476537 0.725416162343746
0.953972302161670 0.727372105706888
0.965246876184555 0.729280883009763
0.976546163726705 0.731138126989663
0.987861464567192 0.732927628357163
0.999183338646702 0.734637422762338
1.01050230179137 0.736272391963223
1.02180987190148 0.737857199609050
1.03310127869830 0.739430202208498
1.04438004942671 0.741019033039606
1.05565265737710 0.742630404827388
1.06692520102676 0.744277707429729
0 0
0.887530786012880 0.723953914765393
0.898647988484292 0.726174002744471
0.909779116071509 0.728324640841682
0.920929453701887 0.730383117696121
0.932105692995070 0.732334715314499
0.943312714056185 0.734206259638705
0.954550606189579 0.736039687746519
0.965815984561839 0.737847451966079
0.977103121336275 0.739616776559897
0.988404790604791 0.741323920642173
0.999713032885463 0.742951917695323
1.01101999550058 0.744502589924324
1.02231906498525 0.745998056966711
1.03360687736118 0.747475567279002
1.04488576751362 0.748962621778329
1.05616009805065 0.750470664572624
0 0
0.888055772231440 0.733993008879992
0.899192691495258 0.735990273604496
0.910342738872589 0.737928399820692
0.921507732919570 0.739792242755987
0.932692179518577 0.741572454114179
0.943901175520140 0.743296545682390
69
0.955135928640186 0.745004850928974
0.966394343109894 0.746704978017070
0.977671985414048 0.748377188091378
0.988962914613382 0.749991216865181
1.00026047745635 0.751525401643972
1.01155816560762 0.752978904593823
1.02285062568079 0.754373291572454
1.03413513729183 0.755746045241440
1.04541332464835 0.757125659842511
1.05668821762825 0.758523590971057
0 0
0.899752041834668 0.746048568086788
0.910917028672683 0.747787442762525
0.922093533498067 0.749468192216781
0.933284831390208 0.751082918741596
0.944495988693739 0.752659827980109
0.955728848696631 0.754239909319875
0.966982227765011 0.755825988646962
0.978252714968684 0.757392611758612
0.989535438058985 0.758903792182033
1.00082482757861 0.760333722017034
1.01211541858327 0.761679712589621
1.02340270310220 0.762963970320697
1.03468429287106 0.764224576092222
1.04596138792137 0.765490252869619
1.05723619903728 0.766771195086638
0 0
0.900323941984663 0.756335304437585
0.911501153377962 0.757885462244486
0.922687113542332 0.759391266393577
0.933884362389418 0.760848912091724
0.945097885780166 0.762285139093301
0.956329911501288 0.763736536092733
0.967579906441835 0.765202582791977
0.978845250737930 0.766653463100314
0.990121928096028 0.768049472096731
1.00140523037463 0.769362595293850
1.01269047998140 0.770589844142177
1.02397375089723 0.771755060716253
70
1.03525286087564 0.772896645800766
1.04652876966312 0.774042297242936
1.05780319915467 0.775200452466180
0 0
0.900907021728567 0.766839591902578
0.912094604408319 0.768209242897784
0.923288677867156 0.769547000468173
0.934491326614849 0.770850414348401
0.945707466821370 0.772144767409042
0.956939576266779 0.773464308896631
0.968187591255606 0.774805135235913
0.979449494472620 0.776133681565170
0.990721936105404 0.777406966233100
1.00200087371866 0.778595262497818
1.01328221837250 0.779695923336508
1.02456246053798 0.780735099164639
1.03583957262450 0.781751690486626
1.04711439410175 0.782772005322957
1.05838836665390 0.783802824332952
0 0
0.901500369203350 0.777553487471240
0.912697067129929 0.778749247866209
0.923898394929159 0.779923551381090
0.935106149019358 0.781074675019252
0.946325199211879 0.782226518075019
0.957558196813384 0.783411359460293
0.968805420564116 0.784622381307286
0.980065307073955 0.785822599227095
0.991335015496409 0.786966204549945
1.00261100975076 0.788022307014097
1.01388964175513 0.788989257779112
1.02516771223241 0.789896214110991
1.03644332536149 0.790782722643516
1.04771727705927 0.791673313269174
1.05899085865673 0.792573313557684
0 0
0.902103365881728 0.788471903425610
0.913308343679915 0.789498795531759
0.924516400250428 0.790512981711744
71
0.935729147390743 0.791513135449572
0.946951429106921 0.792521788053461
0.958186023088509 0.793569360126700
0.969433460021625 0.794646372690337
0.980692516132532 0.795712731022275
0.991960734766012 0.796720215050946
1.00323496230057 0.797637339240838
1.01451188339638 0.798464133135123
1.02578853787510 0.799233483161924
1.03706314837199 0.799985685419341
1.04833651411984 0.800743043980159
1.05960985535918 0.801509603622146
0 0
0.902715583206547 0.799592066081638
0.913928305413466 0.800454024842128
0.925142797319818 0.801310513695796
0.936360551092840 0.802160480165959
0.947586399278979 0.803025094725509
0.958823214370522 0.803932908488709
0.970071713667244 0.804871932591696
0.981330926797153 0.805799218142918
0.992598685737675 0.806664542713125
1.00387212570827 0.807436405089324
1.01514818524224 0.808117213339141
1.02642409318921 0.808744324930305
1.03769817975379 0.809358820044197
1.04897127408572 0.809980232442250
1.06024457237346 0.810611426366149
0 0
0.903336717161928 0.810913477780812
0.914556864119898 0.811613540073086
0.925777660188231 0.812314030935366
0.937000518817288 0.813014096771694
0.948230269731188 0.813733571810794
0.959469857652436 0.814499068218262
0.970720138998049 0.815296184798246
0.981980332818685 0.816079352031997
0.993248488285121 0.816796761196121
1.00452195996424 0.817417494478790
72
1.01579788253727 0.817947052099538
1.02707363703416 0.818428007924729
1.03834765056915 0.818902154962124
1.04962079547461 0.819385634404940
1.06089427059547 0.819880145534638
0 0
0.903966547173881 0.822437653094714
0.915193955956300 0.822978139151305
0.926421038823453 0.823523716316983
0.937649155987980 0.824073681548963
0.948883138737229 0.824646572780972
0.960125987264887 0.825266968555919
0.971378662601882 0.825918137405696
0.982640526490889 0.826552136888573
0.993909792929694 0.827116027057174
1.00518398492932 0.827580107105969
1.01646039092824 0.827953679993572
1.02773651613819 0.828285249071254
1.03901087387450 0.828617092143559
1.05028438447795 0.828961285036653
1.06155826348107 0.829318552744538
0 0
0.904604911154151 0.834167880231908
0.915839534263819 0.834550544354666
0.927072967069164 0.834941753500734
0.938306531891713 0.835340909832461
0.949545063092743 0.835765313952511
0.960791603755349 0.836237411932548
0.972047194770506 0.836738246559163
0.983311307179812 0.837217810056962
0.994582282291567 0.837622586146667
1.00585777488035 0.837924797894863
1.01713519609470 0.838138218586063
1.02841215370115 0.838317855481079
1.03968723676179 0.838506041175081
1.05096141331381 0.838710023660603
1.06223592176893 0.838930236112229
0 0
0.905251691527969 0.846108908766509
73
0.916493568738052 0.846335098955359
0.927733472836532 0.846572015152037
0.938972696651792 0.846819100641764
0.950216077259958 0.847092489085165
0.961466691365623 0.847412413604490
0.972725642617581 0.847757869530260
0.983992488511134 0.848077221896812
0.995265671874397 0.848317083659195
1.00654295365020 0.848452565126849
1.01782184533243 0.848502508707963
1.02910004049970 0.848528425392865
1.04037619405225 0.848571928595403
1.05165131831907 0.848635144385274
0 0
0.905906808916157 0.858266477947560
0.917156049419444 0.858337352107426
0.928402590472200 0.858419667717368
0.939647698547450 0.858512798313014
0.950896211819070 0.858631860675138
0.962151234294651 0.858794848838255
0.973413921802891 0.858978944988328
0.984683904333577 0.859131473075119
0.995959710203946 0.859200124042293
1.00723919001134 0.859163961036637
1.01851994020657 0.859048724780500
1.02979972730427 0.858919870991752
1.04107726267546 0.858817304962510
1.05235359745306 0.858739757504847
0 0
0.906570221341917 0.870646562862791
0.917826994887500 0.870563436000443
0.929080375918667 0.870490646294923
0.940331602838107 0.870427195543400
0.951585512326383 0.870387197022144
0.962845232502749 0.870386444433114
0.974111967228014 0.870400946538176
0.985385413445111 0.870378193259957
0.996664177906466 0.870268466632541
1.00794619248056 0.870056232004482
74
1.01922912917570 0.869774859490136
1.03051081754112 0.869491872204514
1.04179001606482 0.869243787520855
1.05306780715541 0.869026290168814
0 0
0.907241927632080 0.883254179155750
0.918506465049052 0.883019137627707
0.929766926395893 0.882790947068424
0.941024514316088 0.882567591524498
0.952284060510284 0.882362047578040
0.963548718297108 0.882188054656365
0.974819743165881 0.882021588922630
0.986096902802730 0.881812380329651
0.997378884794687 0.881515681940872
1.00866370217747 0.881123029755610
1.01994909878133 0.880675663063816
1.03123295916003 0.880241413488208
1.04251407814410 0.879850862198738
1.05379355877366 0.879495665413159
0 0
0.907921974569812 0.896091591795506
0.919194580785756 0.895708562923615
0.930462408910169 0.895325839284198
0.941726608342382 0.894938928809615
0.952992001626087 0.894558965268747
0.964261776148055 0.894197774642250
0.975537253988177 0.893833438050219
0.986818289240090 0.893421865621828
0.998103663991481 0.892927361232265
1.00939148219743 0.892350716376996
1.02067956214483 0.891740529993681
1.03196583534069 0.891161654508859
1.04324911754084 0.890634893044761
1.05453051597440 0.890146204513232
0 0
0.908610465447499 0.909155788083838
0.919891553146234 0.908632380667655
0.931167104226081 0.908099193305308
0.942438177058634 0.907546281306159
75
0.953709581737463 0.906980111418532
0.964984566638962 0.906410182697114
0.976264554389459 0.905820906294897
0.987549516939898 0.905182379685425
0.998838358573587 0.904475894734507
1.01012929771193 0.903714264099007
1.02142023982167 0.902950639801949
1.03270915102720 0.902240153888482
1.04399484073403 0.901588153985542
1.05527839293730 0.900972676854946
0 0
0.909307566725715 0.922435724625846
0.920597729574518 0.921784769901979
0.931881484290918 0.921113485163341
0.943159707660954 0.920398212210849
0.954437202903721 0.919632174075317
0.965717357071043 0.918818845591264
0.977001759561247 0.917957028808097
0.988290549582591 0.917050232979390
0.999582796384239 0.916112415290881
1.01087687849150 0.915172100050783
1.02217082724370 0.914277086145626
1.03346261412076 0.913458882063822
1.04475098598653 0.912698526190771
1.05603695710761 0.911966102416431
0 0
−0.300000000000000 1.03253500000000
−0.200000000000000 1.03253500000000
−0.100000000000000 1.03253500000000
−5.000000000000000E−002 1.03253500000000
0.000000000000000E+000 1.03253500000000
1.000000000000000E−006 1.03253500000000
0.100939000000000 1.01763900000000
0.220473000000000 1.00000000000000
0.357722000000000 0.986321000000000
0.451479000000000 0.976977000000000
0.574907000000000 0.964675000000000
0.644189000000000 0.957770000000000
0.738452000000000 0.950836000000000
76
0.803980000000000 0.946016000000000
0.891492000000000 0.939579000000000
0.937254000000000 0.936213000000000
1.01388300000000 0.929716000000000
1.06023300000000 0.925785000000000
1.13410700000000 0.919521000000000
1.17601000000000 0.915968000000000
1.24073600000000 0.910472000000000
1.28135100000000 0.907022000000000
1.34601700000000 0.901531000000000
1.38049900000000 0.898603000000000
1.43471800000000 0.893267000000000
1.46166300000000 0.890615000000000
1.51875000000000 0.884997000000000
1.57317100000000 0.879641000000000
1.61932300000000 0.876129000000000
1.64582600000000 0.874113000000000
1.70292300000000 0.869769000000000
1.73207700000000 0.867551000000000
1.78028700000000 0.864124000000000
1.80869300000000 0.862105000000000
1.86630800000000 0.858010000000000
1.91983500000000 0.854206000000000
1.96718800000000 0.852155000000000
1.99783500000000 0.850828000000000
2.05537900000000 0.848336000000000
2.08707100000000 0.846963000000000
2.13136400000000 0.845082000000000
2.16253200000000 0.843759000000000
2.21544400000000 0.841512000000000
2.24823100000000 0.840120000000000
2.28860600000000 0.839638000000000
2.32032400000000 0.839260000000000
2.37110000000000 0.838655000000000
2.39886900000000 0.838324000000000
2.44886900000000 0.838324000000000
2.49886900000000 0.838324000000000
2.59886900000000 0.838324000000000
0 0
77
Input parameters (version 1 . 0 )
e3c
Blade row # :
6
Number of blades in this row :
50
Blade Scaling factor (mm ) :
350.700000000000
Number of streamlines :
21
Non−dimensional Actual chord (0=no , 1=yes ) :
0
J in_Beta out_Beta mrel_in chord t /c_max Incidence Deviation Sec . Flow Angle
1 −47.74103879 −21.07916156 0 .81598141 0 .16079164 0 .05000000 0 .00000000 0 .00000000 0 .00000000
2 −50.36799862 −24.17675644 0 .82451632 0 .15784957 0 .05250000 0 .00000000 0 .00000000 0 .00000000
3 −52.60298736 −28.19977065 0 .83428679 0 .15403994 0 .05500000 0 .00000000 0 .00000000 0 .00000000
4 −54.64961849 −32.22052200 0 .84516206 0 .14962863 0 .05750000 0 .00000000 0 .00000000 0 .00000000
5 −56.58294072 −36.36828929 0 .85493487 0 .14490221 0 .06000000 0 .00000000 0 .00000000 0 .00000000
6 −58.08132184 −40.03255742 0 .86469469 0 .14020504 0 .06250000 0 .00000000 0 .00000000 0 .00000000
7 −59.29166496 −43.01361345 0 .87465797 0 .13564417 0 .06500000 0 .00000000 0 .00000000 0 .00000000
8 −60.24801914 −45.21021304 0 .88531781 0 .13131148 0 .06750000 0 .00000000 0 .00000000 0 .00000000
9 −60.90668031 −47.01809843 0 .89742328 0 .12693227 0 .07000000 0 .00000000 0 .00000000 0 .00000000
10 −61.41044604 −48.51784126 0 .90958083 0 .12278554 0 .07250000 0 .00000000 0 .00000000 0 .00000000
11 −61.86128706 −49.79323314 0 .92232325 0 .11886825 0 .07500000 0 .00000000 0 .00000000 0 .00000000
12 −62.21755867 −50.93682041 0 .93634488 0 .11503666 0 .07750000 0 .00000000 0 .00000000 0 .00000000
13 −62.46532790 −51.90329734 0 .95147763 0 .11124481 0 .08000000 0 .00000000 0 .00000000 0 .00000000
14 −62.59772126 −52.62402340 0 .96776919 0 .10756342 0 .08250000 0 .00000000 0 .00000000 0 .00000000
15 −62.66246973 −53.17527385 0 .98517247 0 .10392348 0 .08500000 0 .00000000 0 .00000000 0 .00000000
16 −62.59914159 −53.51076661 1 .00297384 0 .10027077 0 .08750000 0 .00000000 0 .00000000 0 .00000000
17 −62.31728495 −53.59651506 1 .02277631 0 .09655697 0 .09000000 0 .00000000 0 .00000000 0 .00000000
18 −61.64037772 −52.81336513 1 .04436091 0 .09285570 0 .09250000 0 .00000000 0 .00000000 0 .00000000
19 −60.13935299 −50.40917816 1 .07055385 0 .08940998 0 .09500000 0 .00000000 0 .00000000 0 .00000000
20 −57.10407385 −45.36021419 1 .10328804 0 .08646850 0 .09750000 0 .00000000 0 .00000000 0 .00000000
21 −52.33335984 −38.94930521 1 .14431262 0 .08430268 0 .10000000 0 .00000000 0 .00000000 0 .00000000
LE / TE curve (x ,r ) definition :
Number of Curve points :
12
79
xLE rLE xTE rTE
0 .75222700 0 .70732200 0 .86601000 0 .72724000
0 .75273400 0 .72086600 0 .86485100 0 .73933500
0 .75447200 0 .74636100 0 .86180900 0 .76099100
0 .75628300 0 .77018900 0 .85927400 0 .78112600
0 .75773200 0 .79314800 0 .85688400 0 .80060800
0 .75881800 0 .81545600 0 .85471100 0 .81994600
0 .75997700 0 .83747400 0 .85268300 0 .83914000
0 .76113600 0 .85912900 0 .85072800 0 .85811500
0 .76258400 0 .88064000 0 .84884500 0 .87709100
0 .76425000 0 .90229600 0 .84688900 0 .89642900
0 .76548100 0 .91888200 0 .84558600 0 .91192900
0 .76664000 0 .93619200 0 .84486100 0 .92960100
Airfoil type{bf1 (sect1 ) + bf2 (sect2 ) + . . . } :
J type
1 sect1
2 sect1
3 sect1
4 sect1
5 sect1
6 sect1
7 sect1
8 sect1
9 sect1
10 sect1
11 sect1
12 sect1
13 sect1
14 sect1
15 sect1
16 sect1
17 sect1
18 sect1
19 sect1
20 sect1
21 sect1
Control table for blending section variable :
80
5 0 0
span bf1 bf2
0.000000000000000E+000 1 0
0.250000000000000 1 0
0.500000000000000 1 0
0.750000000000000 1 0
1.00000000000000 1 0
Stacking axis as a fraction of chord ( 2 . =centroid ) :
2 . 0 0
Control points for delta_m :
5
span delta_m
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for delta_theta :
5
span delta_theta
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for in_beta* :
5
span in_beta*
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for out_beta* :
81
5
span out_beta*
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for chord :
5
span chord
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for tm /c :
5
span tm /c
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Hub offset
0.000000000000000E+000
Tip offset
0.000000000000000E+000
Streamline Data
x_s r_s
−0.300000000000000 0.494387000000000
−0.200000000000000 0.494387000000000
−0.186572000000000 0.494387000000000
−7.025421900000001E−002 0.492938365000000
0.000000000000000E+000 0.507423771000000
0.263851669000000 0.580068081000000
82
0.293891489000000 0.588552850000000
0.398736643000000 0.618549342000000
0.440935757000000 0.630187586000000
0.603606866000000 0.673643804000000
0.636633592000000 0.681538350000000
0.714130514000000 0.699645108000000
0.752227131000000 0.707322373000000
0.866009995000000 0.727239806000000
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92
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0 0
93
A.2.1 Blade Metal Angles from the NASA Report [1]
e3c
6
radius (n .d . ) beta1* beta2* tm /c
0.717279726 50 .30 9 . 6 3 0 .0875
0 .730111206 51 .01 16 .77 0 .0749
0 .753692615 52 .14 2 7 . 7 0 .0634
0 .775648703 53 .28 34 .19 0 .0592
0 .796863416 54 .53 38 .43 0 .0579
0 .817707442 55 .83 41 .72 0 .0579
0 .838266324 57 .14 44 .49 0 .0581
0 .858625606 58 .41 45 .68 0 .057
0 .87887083 59 .67 48 .65 0 .0497
0 .899344169 61 .00 50 .08 0 .0358
0 .915397776 62 .11 48 .24 0 .0299
0 .932905617 63 .46 43 .28 0 .0265
94
Input parameters (version 1 . 0 )
booster
Blade row # :
7
Number of blades in this row :
64
Blade Scaling factor (mm ) :
533.400000000000
Number of streamlines :
21
Non−dimensional Actual chord (0=no , 1=yes ) :
0
J in_Beta out_Beta mrel_in chord t /c_max Incidence Deviation Sec . Flow Angle
1 −32.34786863 16.39081413 0 .51524073 0 .26636075 0 .10000000 0 .00000000 0 .00000000 0 .00000000
2 −32.77970985 14.24191701 0 .51812678 0 .25662973 0 .09625000 0 .00000000 0 .00000000 0 .00000000
3 −33.45701135 12.11597110 0 .52263750 0 .24812215 0 .09250000 0 .00000000 0 .00000000 0 .00000000
4 −34.15031139 10.73976182 0 .52718591 0 .23956306 0 .08875000 0 .00000000 0 .00000000 0 .00000000
5 −34.85698076 8 .72249523 0 .53162874 0 .23289792 0 .08500000 0 .00000000 0 .00000000 0 .00000000
6 −35.54846714 6 .56302383 0 .53547396 0 .22676233 0 .08125000 0 .00000000 0 .00000000 0 .00000000
7 −36.20280194 4 .52250474 0 .53955428 0 .22104709 0 .07750000 0 .00000000 0 .00000000 0 .00000000
8 −36.85780764 2 .40568978 0 .54466434 0 .21567989 0 .07375000 0 .00000000 0 .00000000 0 .00000000
9 −37.28699911 0 .32857136 0 .54760009 0 .21160019 0 .07000000 0 .00000000 0 .00000000 0 .00000000
10 −37.90693856 −1.74132991 0 .55319080 0 .20675521 0 .06625000 0 .00000000 0 .00000000 0 .00000000
11 −38.46660404 −3.94436818 0 .55851225 0 .20214631 0 .06250000 0 .00000000 0 .00000000 0 .00000000
12 −38.99837218 −6.14471075 0 .56421530 0 .19775495 0 .05875000 0 .00000000 0 .00000000 0 .00000000
13 −39.48980958 −7.73945002 0 .57003914 0 .19273529 0 .05500000 0 .00000000 0 .00000000 0 .00000000
14 −39.92005537 −10.00784480 0 .57650539 0 .18879360 0 .05125000 0 .00000000 0 .00000000 0 .00000000
15 −40.27548783 −12.35816131 0 .58361143 0 .18505240 0 .04750000 0 .00000000 0 .00000000 0 .00000000
16 −40.55354397 −14.70287413 0 .59188417 0 .18151538 0 .04375000 0 .00000000 0 .00000000 0 .00000000
17 −40.79161600 −17.22652548 0 .59773419 0 .17887199 0 .04000000 0 .00000000 0 .00000000 0 .00000000
18 −40.91318605 −19.72421987 0 .60712127 0 .17575068 0 .03625000 0 .00000000 0 .00000000 0 .00000000
19 −40.93737425 −22.37832111 0 .61793616 0 .17289346 0 .03250000 0 .00000000 0 .00000000 0 .00000000
20 −40.76878420 −25.15490030 0 .63130205 0 .17034785 0 .02875000 0 .00000000 0 .00000000 0 .00000000
21 −40.46635987 −28.02965509 0 .64536295 0 .16834439 0 .02500000 0 .00000000 0 .00000000 0 .00000000
LE / TE curve (x ,r ) definition :
Number of Curve points :
2
96
xLE rLE xTE rTE
1 .42662000 0 .56594500 1 .56106600 0 .50955900
1 .46635100 0 .82344600 1 .59968100 0 .81176900
Airfoil type{bf1 (sect1 ) + bf2 (sect2 ) + . . . } :
J type
1 sect1
2 sect1
3 sect1
4 sect1
5 sect1
6 sect1
7 sect1
8 sect1
9 sect1
10 sect1
11 sect1
12 sect1
13 sect1
14 sect1
15 sect1
16 sect1
17 sect1
18 sect1
19 sect1
20 sect1
21 sect1
Control table for blending section variable :
5 0 0
span bf1 bf2
0.000000000000000E+000 1 0
0.250000000000000 1 0
0.500000000000000 1 0
0.750000000000000 1 0
1.00000000000000 1 0
Stacking axis as a fraction of chord ( 2 . =centroid ) :
0 . 2 5
97
Control points for delta_m :
5
span delta_m
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for delta_theta :
5
span delta_theta
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for in_beta* :
5
span in_beta*
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for out_beta* :
5
span out_beta*
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for chord :
5
98
span chord
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for tm /c :
5
span tm /c
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Hub offset
0.000000000000000E+000
Tip offset
0.000000000000000E+000
Streamline Data
x_s r_s
−0.400000000000000 0.582708000000000
−0.300000000000000 0.609519000000000
−0.200000000000000 0.636331000000000
−0.100000000000000 0.663142000000000
−5.000000000000000E−002 0.676548000000000
0.000000000000000E+000 0.689954000000000
0.386494000000000 0.793579000000000
0.444881000000000 0.810558000000000
0.537136000000000 0.825487000000000
0.641532000000000 0.823872000000000
0.746643000000000 0.807657000000000
0.808771000000000 0.793543000000000
0.933377000000000 0.758004000000000
1.01451600000000 0.730822000000000
1.11849400000000 0.692351000000000
1.21366900000000 0.654524000000000
99
1.34714900000000 0.599318000000000
1.42662000000000 0.565945000000000
1.56106600000000 0.509559000000000
1.66619400000000 0.466152000000000
1.79245900000000 0.415597000000000
1.92196900000000 0.366510000000000
2.05147900000000 0.321558000000000
2.18098800000000 0.282710000000000
2.31049800000000 0.253316000000000
2.44000700000000 0.240429000000000
0 0
1.40429383424248 0.604251328970274
1.41575717794288 0.599595865620261
1.42721958827711 0.594948768189965
1.43868096869341 0.590315950073252
1.45014119704695 0.585700882655653
1.46160014129899 0.581100309657059
1.47305767500809 0.576509547545632
1.48451369022275 0.571917316222892
1.49596810958367 0.567309394640229
1.50742089804785 0.562671423491721
1.51887207409883 0.557991707166250
1.53032172007597 0.553263265251998
1.54176999113854 0.548484615491701
1.55321712231006 0.543659094147465
1.56466343294773 0.538793491475356
1.57610932559549 0.533894917342525
1.58755528215448 0.528971655489270
1.59900186426533 0.524027636631809
0 0
1.40478731218145 0.620633812798105
1.41625523590073 0.616075325488751
1.42772199501149 0.611523575500410
1.43918712348326 0.606978653145053
1.45065011722496 0.602444726248986
1.46211045549471 0.597924415695068
1.47356762338859 0.593416127532266
1.48502113457988 0.588913388844212
1.49647055449575 0.584404945493248
100
1.50791552357048 0.579876923230391
1.51935578004801 0.575315359386821
1.53079118157625 0.570708706144827
1.54222172465390 0.566049576274957
1.55364756087825 0.561335316180665
1.56506900888726 0.556567397502921
1.57648655961271 0.551750682330780
1.58790087593662 0.546891586251169
1.59931279014053 0.541996767989308
1.61072329376885 0.537072414336507
0 0
1.40528249310667 0.635743511797357
1.41675531965570 0.631268236194671
1.42822707789882 0.626799873544677
1.43969693668334 0.622336964503857
1.45116400366803 0.617883024107245
1.46262735431201 0.613441477730134
1.47408606209735 0.609014064440637
1.48553923031154 0.604596168881665
1.49698602558641 0.600177885961784
1.50842571251827 0.595745434375703
1.51985768851665 0.591283602840780
1.53128151775641 0.586778418176270
1.54269696284121 0.582219282570086
1.55410401258814 0.577600004086418
1.56550290424442 0.572918715762778
1.57689413734082 0.568176652799479
1.58827847932652 0.563377875086679
1.59965696496429 0.558528735648061
1.61103088439469 0.553635876050593
0 0
1.40577849009791 0.650085189690984
1.41725669943902 0.645684172551928
1.42873430446592 0.641292395266556
1.44021010952030 0.636906879842102
1.45168282561083 0.632529496819934
1.46315110657821 0.628163483060634
1.47461358690052 0.623812776170882
1.48606892200841 0.619475158731312
101
1.49751583163438 0.615142229461209
1.50895314559428 0.610800501450514
1.52037985105606 0.606433478436619
1.53179513993281 0.602024467898956
1.54319845460878 0.597559290688663
1.55458952984356 0.593028116052572
1.56596842845864 0.588426071060257
1.57733556723357 0.583753060735158
1.58869173221115 0.579011608439900
1.60003808433093 0.574206449577547
1.61137614970915 0.569343473931321
0 0
1.40627390927987 0.663891192787225
1.41775810357631 0.659557410270264
1.42924257707044 0.655237117111200
1.44072576796510 0.650926097052566
1.45220598025424 0.646624161951155
1.46368142624830 0.642333893779914
1.47515027119432 0.638060325869908
1.48661068127294 0.633802498872584
1.49806087594762 0.629553002277611
1.50949918440997 0.625298550566632
1.52092410535802 0.621021821228843
1.53233436872347 0.616704230093940
1.54372899729271 0.612328910078292
1.55510736553716 0.607883013158745
1.56646925246637 0.603358844408006
1.57781488392923 0.598753866166086
1.58914496239169 0.594068888811951
1.60046068386909 0.589307461100073
1.61176373527973 0.584474326684383
0 0
1.40676680660267 0.677289329990262
1.41825766878806 0.673016542447843
1.42975017688178 0.668763417601065
1.44124240003308 0.664524735020007
1.45273222367520 0.660297694072591
1.46421739759623 0.656083837564523
1.47569558624280 0.651888550967875
102
1.48716442304424 0.647711447697694
1.49862157037519 0.643545633580891
1.51006478553987 0.639377939363020
1.52149199253391 0.635190423678530
1.53290135849728 0.630963033128996
1.54429137278948 0.626676685822995
1.55566092560822 0.622315870551352
1.56700938216219 0.617870130328228
1.57833664663860 0.613334355357208
1.58964321250796 0.608707365786686
1.60093019719525 0.603991187415634
1.61219935280523 0.599189375643913
0 0
1.40725463921439 0.690356634576662
1.41875288365683 0.686138964624070
1.43025470006251 0.681948721749260
1.44175778466924 0.677780400162661
1.45325959225173 0.673628362114297
1.46475738912640 0.669492502003710
1.47624830778216 0.665377782645609
1.48772940560341 0.661283635828420
1.49919773022676 0.657203365422295
1.51065039293561 0.653123838956812
1.52208465081729 0.649026656023023
1.53349799735928 0.644890586866505
1.54488825982018 0.640694642818971
1.55625370020464 0.636420857010180
1.56759311516738 0.632056063049938
1.57890592778748 0.627592467615682
1.59019226591378 0.623026734969912
1.60145302289795 0.618359084824871
1.61268989010581 0.613591686162987
0 0
1.41924052661763 0.698973208840186
1.43075298802556 0.694841737796040
1.44226891439413 0.690740585625959
1.45378531713743 0.686663760701412
1.46529895903444 0.682609483532223
1.47680641175805 0.678579093038388
103
1.48830411645790 0.674571573410376
1.49978845121847 0.670580119491789
1.51125580830815 0.666591609463722
1.52270268350958 0.662587382900948
1.53412577863310 0.658545360255675
1.54552211661400 0.654442949694474
1.55688916649561 0.650259894753959
1.56822497329409 0.645980306696261
1.57952828442920 0.641593557814039
1.59079866525078 0.637093941210966
1.60203659656921 0.632479675597353
1.61324354030096 0.627751374181588
0 0
1.41971659956500 0.711549688296913
1.43124105386583 0.707472960538196
1.44277191484448 0.703436553637079
1.45430573585641 0.699430485987488
1.46583875696915 0.695452331264731
1.47736696416264 0.691504687543186
1.48888614865264 0.687586346720781
1.50039197186606 0.683689877327921
1.51188004109660 0.679800928787183
1.52334600045155 0.675899108982745
1.53478564050856 0.671960235249463
1.54619502812913 0.667959427475349
1.55757065516142 0.663874108233370
1.56890960146562 0.659686088013406
1.58020970306745 0.655382419642956
1.59146971563144 0.650955214458974
1.60268946248027 0.646400639795844
1.61386994868547 0.641717622892821
0 0
1.42017625757280 0.723886244160158
1.43171400708736 0.719860328236869
1.44326196521330 0.715886804646330
1.45481620683272 0.711953778792355
1.46637242935349 0.708056592544896
1.47792601304452 0.704195893656479
1.48947207554998 0.700370993102273
104
1.50100552834645 0.696573913873054
1.51252114299906 0.692789270818792
1.52401363503443 0.688995123027455
1.53547777227282 0.685165296763471
1.54690851245714 0.681272606272838
1.55830117184189 0.677292015015774
1.56965162204232 0.673202862366472
1.58095650609551 0.668989754911547
1.59221346186391 0.664642498634054
1.60342133763511 0.660155196349436
1.61458037520503 0.655525015042364
0 0
1.42061373392719 0.735991290518487
1.43216597826904 0.732011964514941
1.44373322425370 0.728100027385233
1.45531103456962 0.724241652295075
1.46689453860074 0.720429304069410
1.47847849484906 0.716660927380246
1.49005733695709 0.712935371327875
1.50162521408603 0.709244017491899
1.51317603721167 0.705570343204702
1.52470354330774 0.701890833983031
1.53620138887765 0.698177323119819
1.54766328270725 0.694400316329967
1.55908316457597 0.690532299699771
1.57045543151670 0.686550093243416
1.58177520490978 0.682435881831125
1.59303862575553 0.678177070859224
1.60424315839634 0.673765654314864
1.61538786984215 0.669197002595792
0 0
1.42102225715565 0.747865576872744
1.43259004387505 0.743927955605198
1.44417876665230 0.740076054894993
1.45578341508513 0.736293903281074
1.46739851013682 0.732570354529509
1.47901817231609 0.728900327133155
1.49063615577995 0.725281507761512
1.50224586349172 0.721704023492583
105
1.51384035998360 0.718149866326389
1.52541239873712 0.714593690618296
1.53695448121181 0.711005189464651
1.54845896403190 0.707352520415479
1.55991822882126 0.703605738815781
1.57132492430858 0.699739235704036
1.58267228047067 0.695732748078612
1.59395448459941 0.691571489061903
1.60516709614585 0.687245379420761
1.61630745762628 0.682747756110792
1.62737505786326 0.678074566039811
0 0
1.42139395221108 0.759503158456305
1.43297814830539 0.755601179869874
1.44459053370245 0.751807214224983
1.45622541280568 0.748102993637343
1.46787662503788 0.744472195565302
1.47953762707441 0.740905496564400
1.49120151205754 0.737399011195633
1.50286098838624 0.733941742495241
1.51450834218413 0.730514658754341
1.52613540625943 0.727091030428627
1.53773355818430 0.723638471639828
1.54929377129217 0.720122339488187
1.56080674334556 0.716509457060440
1.57226312559515 0.712770997534134
1.58365386567163 0.708883887525926
1.59497066407898 0.704830720761037
1.60620652223888 0.700599704154162
1.61735632896218 0.696182941434304
1.62841742129005 0.691574779245572
0 0
1.42171971023044 0.770891730538989
1.43332101434147 0.767017567332264
1.44495929952683 0.763278378860992
1.45662798103111 0.759653739438772
1.46832008008015 0.756121434707103
1.48002833648607 0.752667040481990
1.49174520978687 0.749283698731202
106
1.50346280638903 0.745958169370859
1.51517277117086 0.742669666524246
1.52686617288338 0.739389732429963
1.53853340945446 0.736083842725827
1.55016416207819 0.732714653212069
1.56174743340112 0.729245876376197
1.57327171080885 0.725645515958972
1.58472529306705 0.721887588091698
1.59609680486873 0.717952267556638
1.60737589072891 0.713826005538250
1.61855402783837 0.709499565343694
1.62962536670110 0.704966151445647
0 0
1.43360802240241 0.778155714129873
1.44527464828153 0.774466310450335
1.45698103788794 0.770922137661456
1.46871914100890 0.767494726309647
1.48048087071515 0.764163195336041
1.49225808024722 0.760915846062501
1.50404241122768 0.757735641156720
1.51582508716139 0.754599185744753
1.52759668888366 0.751475845807087
1.53934693507842 0.748328857988054
1.55106449346292 0.745118232465482
1.56273686215051 0.741804623594184
1.57435038120813 0.738352834282991
1.58589045106293 0.734733912742169
1.59734203504856 0.730925578264247
1.60869048269351 0.726912617417550
1.61992262012478 0.722684708067824
1.63102797799549 0.718234315577530
0 0
1.43382701994430 0.788985275012891
1.44552494616166 0.785338451400185
1.45727360792136 0.781873235111867
1.46906341957587 0.778557144334041
1.48088525209742 0.775361786369379
1.49273037150944 0.772265796728290
1.50459014251206 0.769247088331995
107
1.51645568027086 0.766278350556404
1.52831749170661 0.763326189224396
1.54016511069433 0.760351521243174
1.55198673050973 0.757311876226856
1.56376885712549 0.754164981103505
1.57549604705505 0.750872388184703
1.58715084907900 0.747401976505350
1.59871412357555 0.743728838130788
1.61016590181990 0.739836033949736
1.62148679323613 0.735712440824963
1.63265973858311 0.731350409424274
0 0
1.43396398699122 0.799463782895956
1.44569726671288 0.795848626854229
1.45749403346118 0.792459812949538
1.46934231177807 0.789258342935531
1.48123152360643 0.786206797635494
1.49315237240601 0.783275200993810
1.50509620892337 0.780434363751918
1.51705445565173 0.777651488159851
1.52901809716075 0.774889065502845
1.54097718158931 0.772104674477543
1.55292028173347 0.769252600374201
1.56483388488694 0.766287109102680
1.57670172799992 0.763166125562983
1.58850419362898 0.759854050202730
1.60021806057152 0.756323110434043
1.61181708782555 0.752554718561318
1.62327375402014 0.748537372380572
1.63456175240321 0.744264007665423
0 0
1.43400243075609 0.809529338624064
1.44577718120522 0.805929823107049
1.45763025353135 0.802610817443484
1.46954566226726 0.799529906756078
1.48151058848778 0.796638215590704
1.49351531388416 0.793891321969487
1.50555160252208 0.791249532197064
1.51761172139718 0.788671985349592
108
1.52968778809492 0.786116058608570
1.54177121308955 0.783536082843759
1.55385209076530 0.780883723361353
1.56591841496742 0.778110340102829
1.57795500080651 0.775170333941280
1.58994204324406 0.772024036125373
1.60185350410783 0.768639741331186
1.61365635056563 0.764996136384857
1.62531260702046 0.761081054199220
1.63678325241507 0.756888527108160
0 0
1.43392228891871 0.819084215054128
1.44574820044809 0.815477362879331
1.45767010269498 0.812214757602292
1.46966478074233 0.809255858334677
1.48171539834932 0.806539739254790
1.49381255244515 0.804000449958712
1.50594927857542 0.801581496113626
1.51811939073514 0.799230282142100
1.53031681380820 0.796897569740365
1.54253514427275 0.794534591246011
1.55476720316355 0.792091516702614
1.56700440293825 0.789517999955149
1.57923567195557 0.786765400538302
1.59144543818110 0.783789546893407
1.60360965566679 0.780552586641544
1.61568934187191 0.777028295696999
1.62763255996686 0.773202328503811
1.63938318540552 0.769069703700946
0 0
−0.400000000000000 0.929259000000000
−0.300000000000000 0.946302000000000
−0.200000000000000 0.963790000000000
−0.100000000000000 0.981698000000000
−5.000000000000000E−002 0.990803000000000
1.874800000000000E−002 1.00000500000000
0.369839000000000 1.04072000000000
0.557157000000000 1.06244200000000
0.647496000000000 1.05731700000000
109
0.709779000000000 1.05605700000000
0.835462000000000 1.05218500000000
0.872151000000000 1.04139000000000
0.997813000000000 1.03343000000000
1.08448700000000 1.01366200000000
1.18101000000000 0.950623000000000
1.26509400000000 0.923437000000000
1.39716200000000 0.846730000000000
1.46635100000000 0.823446000000000
1.59968100000000 0.811769000000000
1.68599600000000 0.785249000000000
1.81141600000000 0.670782000000000
1.93713400000000 0.638396000000000
2.06285300000000 0.615033000000000
2.18857100000000 0.596667000000000
2.31428900000000 0.584004000000000
0 0
110
Input parameters (version 1 . 0 )
wt
Blade row # :
1
Number of blades in this row :
3
Blade Scaling factor (mm ) :
5000.00000000000
Number of streamlines :
21
Non−dimensional Actual chord (0=no , 1=yes ) :
0
J in_Beta out_Beta mrel_in chord t /c_max Incidence Deviation Sec . Flow Angle
1 12 .45562628 11 .58919273 0 .02278984 1 .12075435 0 .10000000 7 .00000000 2 .00000000 0 .00000000
2 27 .32203810 27 .42127957 0 .02561209 0 .47431997 0 .10000000 7 .00000000 2 .00000000 0 .00000000
3 39 .65366474 38 .43167319 0 .02948784 0 .36541958 0 .10000000 7 .00000000 2 .00000000 0 .00000000
4 49 .58412618 50 .07936717 0 .03366132 0 .29513555 0 .46704871 7 .00000000 2 .00000000 0 .00000000
5 57 .28440557 59 .50479019 0 .03830699 0 .18939585 0 .28308823 7 .00000000 2 .00000000 0 .00000000
6 62 .77312369 64 .42634779 0 .04383765 0 .12221097 0 .20950000 7 .00000000 2 .00000000 0 .00000000
7 66 .59463828 67 .47286642 0 .05035082 0 .08894665 0 .20950000 7 .00000000 2 .00000000 0 .00000000
8 69 .41506660 70 .03835878 0 .05717569 0 .06501837 0 .20950000 7 .00000000 2 .00000000 0 .00000000
9 71 .64639494 72 .09481928 0 .06329578 0 .04918450 0 .20950000 7 .00000000 2 .00000000 0 .00000000
10 73 .45621122 73 .76165186 0 .06957453 0 .03782664 0 .20950000 7 .00000000 2 .00000000 0 .00000000
11 74 .95040439 75 .18552386 0 .07651366 0 .02952151 0 .20950000 7 .00000000 2 .00000000 0 .00000000
12 76 .19534329 76 .37648945 0 .08338789 0 .02328140 0 .20950000 7 .00000000 2 .00000000 0 .00000000
13 77 .22936113 77 .37255156 0 .09016621 0 .01853625 0 .20950000 7 .00000000 2 .00000000 0 .00000000
14 78 .12434366 78 .24124915 0 .09709075 0 .01468774 0 .20950000 7 .00000000 2 .00000000 0 .00000000
15 78 .89184827 78 .98771989 0 .10349107 0 .01182742 0 .20950000 7 .00000000 2 .00000000 0 .00000000
16 79 .55980654 79 .64352064 0 .10968886 0 .00955871 0 .20950000 7 .00000000 2 .00000000 0 .00000000
17 80 .11912811 80 .20679375 0 .11668292 0 .00764802 0 .20950000 7 .00000000 2 .00000000 0 .00000000
18 80 .49150500 80 .54722155 0 .12366317 0 .00610067 0 .20950000 7 .00000000 2 .00000000 0 .00000000
19 80 .78905133 80 .81674351 0 .13085810 0 .00481404 0 .20950000 7 .00000000 2 .00000000 0 .00000000
20 81 .09844253 81 .12168384 0 .13777265 0 .00376634 0 .20950000 7 .00000000 2 .00000000 0 .00000000
21 81 .36601270 81 .34613040 0 .14378952 0 .00287562 0 .20950000 7 .00000000 2 .00000000 0 .00000000
LE / TE curve (x ,r ) definition :
Number of Curve points :
19
112
xLE rLE xTE rTE
9 .65819000 0 .02800000 9 .69679000 0 .02800000
9 .65885000 0 .08227000 9 .69613000 0 .08227000
9 .65951000 0 .13656000 9 .70590000 0 .13656000
9 .66018000 0 .19083000 9 .70950000 0 .19083000
9 .66084000 0 .24511000 9 .69820000 0 .24511000
9 .66150000 0 .29939000 9 .69234000 0 .29939000
9 .66216000 0 .35367000 9 .68787000 0 .35367000
9 .66282000 0 .40794000 9 .68441000 0 .40794000
9 .66348000 0 .46222000 9 .68173000 0 .46222000
9 .66414000 0 .51650000 9 .67962000 0 .51650000
9 .66481000 0 .57078000 9 .67796000 0 .57078000
9 .66547000 0 .62506000 9 .67665000 0 .62506000
9 .66613000 0 .67933000 9 .67552000 0 .67933000
9 .66679000 0 .73361000 9 .67481000 0 .73361000
9 .66745000 0 .78789000 9 .67419000 0 .78789000
9 .66811000 0 .84217000 9 .67372000 0 .84217000
9 .66878000 0 .89644000 9 .67337000 0 .89644000
9 .66944000 0 .95072000 9 .67314000 0 .95072000
9 .67010000 1 .00500000 9 .67299000 1 .00500000
Airfoil type{bf1 (sect1 ) + bf2 (sect2 ) + . . . } :
J type
1 sect1
2 sect1
3 sect1
4 sect1
5 sect1
6 sect1
7 sect1
8 sect1
9 sect1
10 sect1
11 sect1
12 sect1
13 sect1
14 sect1
15 sect1
16 sect1
113
17 sect1
18 sect1
19 sect1
20 sect1
21 sect1
Control table for blending section variable :
5 0 0
span bf1 bf2
0.000000000000000E+000 1 0
0.250000000000000 1 0
0.500000000000000 1 0
0.750000000000000 1 0
1.00000000000000 1 0
Stacking axis as a fraction of chord ( 2 . =centroid ) :
0 . 2 5
Control points for delta_m :
5
span delta_m
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for delta_theta :
5
span delta_theta
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for in_beta* :
5
span in_beta*
114
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for out_beta* :
5
span out_beta*
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for chord :
5
span chord
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for tm /c :
5
span tm /c
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Hub offset
0.000000000000000E+000
Tip offset
0.000000000000000E+000
Streamline Data
115
x_s r_s
9.60786600000000 3.421300000000000E−002
9.65786600000000 3.373300000000000E−002
9.65835000000000 3.373300000000000E−002
9.78083300000000 3.373300000000000E−002
9.83083300000000 3.373300000000000E−002
9.88083400000000 3.373300000000000E−002
9.98083300000000 3.373300000000000E−002
10.0808330000000 3.373300000000000E−002
0 0
9.65516215977055 7.888355685631525E−002
9.65651346758753 7.887271365531129E−002
9.65786477832673 7.886136518178523E−002
9.65921609132450 7.884964676025143E−002
9.66056740490809 7.883784665393663E−002
9.66191871900116 7.882590906161524E−002
9.66327003358673 7.881377643949738E−002
9.66462134864843 7.880140607155896E−002
9.66597266417049 7.878876880174804E−002
9.66732398013775 7.877584650959731E−002
9.66867529653559 7.876263165201416E−002
9.67002661334994 7.874913087718784E−002
9.67137793056724 7.873536188104782E−002
9.67272924817444 7.872134472908271E−002
9.67408056615894 7.870710341868967E−002
9.67543188450863 7.869267114895202E−002
9.67678320321183 7.867808405981165E−002
9.67813452225728 7.866337372717980E−002
9.67948584163412 7.864857128518354E−002
9.68083716133190 7.863371684802355E−002
9.68218848134054 7.861886056171385E−002
9.68353980165031 7.860401990717066E−002
9.68489112225185 7.858921729669484E−002
9.68624244313611 7.857452188683195E−002
9.68759376429437 7.855995849845217E−002
9.68894508571824 7.854548294586533E−002
9.69029640739959 7.853106673888934E−002
9.69164772933061 7.851675032959246E−002
9.69299905150375 7.850259820536078E−002
116
9.69435037391172 7.848861863766605E−002
9.69570169654749 7.847472757863709E−002
9.69705301940430 7.846079659285876E−002
9.69840434247557 7.844672206046627E−002
9.69975566575500 7.843244907489649E−002
9.70110698923648 7.841797472431963E−002
0 0
9.65651388181472 0.124824579052054
9.65786519614864 0.124803042643318
9.65921651237178 0.124781395420360
9.66056782882989 0.124759489775856
9.66191914546438 0.124737452023520
9.66327046227512 0.124715396459335
9.66462177926186 0.124693408524054
9.66597309642416 0.124671546753128
9.66732441376146 0.124649847465668
9.66867573127309 0.124628325358761
9.67002704895824 0.124606965909810
9.67137836681600 0.124585731790859
9.67272968484535 0.124564580726803
9.67408100304518 0.124543462404887
9.67543232141433 0.124522307845679
9.67678363995151 0.124501042478970
9.67813495865540 0.124479601769492
9.67948627752459 0.124457922960936
9.68083759655764 0.124435925976582
9.68218891575303 0.124413511595922
9.68354023510920 0.124390649221019
9.68489155462456 0.124367299832160
9.68624287429748 0.124343330529027
9.68759419412629 0.124318701653938
9.68894551410930 0.124293517114401
9.69029683424477 0.124267849895785
9.69164815453098 0.124241632473847
9.69299947496615 0.124214749249173
9.69435079554852 0.124187201476536
9.69570211627629 0.124159180706043
9.69705343714768 0.124130968808925
9.69840475816087 0.124102793808975
117
9.69975607931406 0.124074780435904
9.70110740060544 0.124046944346143
9.70245872203320 0.124019188418082
9.70381004359553 0.123991299065369
9.70516136529062 0.123963030488247
9.70651268711669 0.123934202976211
9.70786400907193 0.123904716308721
9.70921533115455 0.123874548079693
0 0
9.65651406015439 0.171501454801391
9.65786537763608 0.171452046546516
9.65921669689509 0.171400805770319
9.66056801627792 0.171347832769801
9.66191933572687 0.171293007599282
9.66327065524283 0.171236227923563
9.66462197482665 0.171177428117315
9.66597329447911 0.171116578170578
9.66732461420096 0.171053678005487
9.66867593399287 0.170988758087381
9.67002725385549 0.170921892712840
9.67137857378941 0.170853190892093
9.67272989379517 0.170782769080872
9.67408121387327 0.170710756968534
9.67543253402414 0.170637315013484
9.67678385424821 0.170562614475525
9.67813517454584 0.170486813526387
9.67948649491735 0.170410071092120
9.68083781536302 0.170332577580589
9.68218913588311 0.170254558008828
9.68354045647781 0.170176134658409
9.68489177714730 0.170097449248628
9.68624309789172 0.170018797106573
9.68759441871117 0.169940333077871
9.68894573960573 0.169861994366497
9.69029706057542 0.169783776916633
9.69164838162026 0.169705907923775
9.69299970274023 0.169628699466521
9.69435102393528 0.169552288990748
9.69570234520533 0.169476525850248
118
9.69705366655029 0.169401131764598
9.69840498797003 0.169325927837139
9.69975630946440 0.169250901924448
9.70110763103323 0.169176207347485
9.70245895267632 0.169102165998390
9.70381027439346 0.169029270259789
9.70516159618441 0.168958046259298
9.70651291804892 0.168888895799013
9.70786423998672 0.168822075115342
9.70921556199752 0.168757699944980
9.71056688408103 0.168695749127859
9.71191820623690 0.168636068091836
9.71326952846481 0.168578437340961
9.71462085076441 0.168522658298744
0 0
9.65786546777081 0.219551801004688
9.65921678889306 0.219498574182061
9.66056811010007 0.219443476432644
9.66191943133383 0.219386542777970
9.66327075259500 0.219327803825289
9.66462207388422 0.219267291126898
9.66597339520211 0.219205042262400
9.66732471654926 0.219141106107819
9.66867603792625 0.219075538995498
9.67002735933366 0.219008382693436
9.67137868077202 0.218939674937230
9.67273000224186 0.218869486074309
9.67408132374370 0.218797907657594
9.67543264527803 0.218725023977833
9.67678396684532 0.218650937721221
9.67813528844603 0.218575800881782
9.67948661008060 0.218499790651191
9.68083793174946 0.218423060883204
9.68218925345302 0.218345733870317
9.68354057519167 0.218268094313759
9.68489189696577 0.218190407181793
9.68624321877570 0.218112719786577
9.68759454062180 0.218035283319666
9.68894586250439 0.217958657265062
119
9.69029718442378 0.217883300703586
9.69164850638027 0.217809316738418
9.69299982837414 0.217736661916729
9.69435115040567 0.217665519204020
9.69570247247509 0.217596455401427
9.69705379458266 0.217530177938027
9.69840511672859 0.217467196651816
9.69975643891309 0.217407726179568
9.70110776113636 0.217351690475923
9.70245908339859 0.217298718343127
9.70381040569995 0.217248144199945
9.70516172804058 0.217199212892368
9.70651305042065 0.217151315690830
0 0
9.65786551666958 0.269155372044769
9.65921683889378 0.269126840316003
9.66056816118672 0.269097626264975
9.66191948349018 0.269067673163402
9.66327080580460 0.269036919072249
9.66462212813040 0.269005322699891
9.66597345046799 0.268972896390872
9.66732477281778 0.268939699203412
9.66867609518017 0.268905841088570
9.67002741755557 0.268871510680327
9.67137873994436 0.268836956426943
9.67273006234692 0.268802430363150
9.67408138476362 0.268768197584308
9.67543270719484 0.268734568441404
9.67678402964092 0.268701854851494
9.67813535210223 0.268670318915013
9.67948667457911 0.268640197730117
9.68083799707190 0.268611761629792
9.68218931958093 0.268585315533980
9.68354064210652 0.268560920299671
9.68489196464899 0.268538637121106
9.68624328720865 0.268518792611282
9.68759460978580 0.268501382905166
9.68894593238073 0.268485922096996
9.69029725499374 0.268472008035750
120
9.69164857762511 0.268459673893309
9.69299990027510 0.268449088326344
9.69435122294399 0.268440027276251
9.69570254563203 0.268431651786568
9.69705386833949 0.268422852204063
9.69840519106659 0.268412727934398
0 0
9.65786554468832 0.319356017992612
9.65921686757057 0.319346416323929
9.66056819051411 0.319336746512238
9.66191951346056 0.319327089046330
9.66327083641022 0.319317518114587
9.66462215936338 0.319308083251179
9.66597348232034 0.319298815675623
9.66732480528137 0.319289751867519
9.66867612824676 0.319280922723597
9.67002745121679 0.319272309822369
9.67137877419174 0.319263863450919
9.67273009717188 0.319255569655704
9.67408142015747 0.319247427525892
9.67543274314880 0.319239394731136
9.67678406614611 0.319231434220508
9.67813538914968 0.319223570251935
9.67948671215975 0.319215840854787
9.68083803517658 0.319208205097504
9.68218935820043 0.319200527891974
9.68354068123153 0.319192941127240
9.68489200427014 0.319185500910671
9.68624332731649 0.319177819732675
9.68759465037081 0.319169859723115
9.68894597343336 0.319162126229637
9.69029729650434 0.319154893553885
9.69164861958399 0.319147723927875
9.69299994267253 0.319139873357194
9.69435126577019 0.319131010654992
0 0
9.65921688457051 0.369518404334914
9.66056820790875 0.369511810353981
9.66191953124597 0.369504893643117
121
9.66327085458240 0.369497588235652
9.66462217791826 0.369489823641915
9.66597350125375 0.369481550264004
9.66732482458909 0.369472766013582
9.66867614792450 0.369463528952945
9.67002747126017 0.369454009983622
9.67137879459632 0.369444461031257
9.67273011793315 0.369435116224714
9.67408144127086 0.369426209527590
9.67543276460967 0.369418032809829
9.67678408794976 0.369410859839051
9.67813541129135 0.369404857989354
9.67948673463462 0.369400137163934
9.68083805797977 0.369396858989274
9.68218938132700 0.369395244166409
9.68354070467650 0.369395087908207
9.68489202802846 0.369396204619697
9.68624335138308 0.369398906470136
9.68759467474052 0.369402956966394
9.68894599810099 0.369407320966664
9.69029732146467 0.369411197572298
9.69164864483173 0.369414668593060
0 0
9.65921689485626 0.419607645712716
9.66056821843644 0.419604333052278
9.66191954201345 0.419601034765514
9.66327086558746 0.419597807091026
9.66462218915864 0.419594677245410
9.66597351272716 0.419591649716528
9.66732483629319 0.419588768361756
9.66867615985689 0.419586110148782
9.67002748341843 0.419583702732628
9.67137880697798 0.419581547543100
9.67273013053570 0.419579725815550
9.67408145409175 0.419578349511431
9.67543277764630 0.419577457033610
9.67678410119951 0.419577081895603
9.67813542475154 0.419577336926534
9.67948674830255 0.419578320653064
122
9.68083807185270 0.419579948191424
9.68218939540215 0.419581920337041
9.68354071895106 0.419584335597642
9.68489204249958 0.419587100688652
9.68624336604787 0.419589307045148
9.68759468959608 0.419590597340581
9.68894601314437 0.419591612821979
0 0
9.66056822488891 0.469604568373001
9.66191954861408 0.469602941264430
9.66327087233499 0.469601181020884
9.66462219605176 0.469599256927153
9.66597351976454 0.469597111963240
9.66732484347348 0.469594664663033
9.66867616717871 0.469591907616122
9.67002749088037 0.469589000484290
9.67137881457861 0.469586217019633
9.67273013827356 0.469583777328590
9.67408146196536 0.469581874787511
9.67543278565416 0.469580771134443
9.67678410934009 0.469580668170876
9.67813543302328 0.469581562261177
9.67948675670388 0.469583334126844
9.68083808038201 0.469585943409903
9.68218940405783 0.469589452685680
9.68354072773145 0.469593236928942
9.68489205140303 0.469596753773064
9.68624337507268 0.469600542988857
0 0
9.66056822887515 0.519490352461817
9.66191955269232 0.519489614110068
9.66327087650445 0.519488925897413
9.66462220031168 0.519488316137641
9.66597352411413 0.519487766568868
9.66732484791193 0.519487281694042
9.66867617170520 0.519486938256226
9.67002749549406 0.519486758740056
9.67137881927865 0.519486742164185
9.67273014305909 0.519487029207157
123
9.67408146683549 0.519487808375847
9.67543279060799 0.519489130407280
9.67678411437670 0.519491010406829
9.67813543814176 0.519493558413568
9.67948676190327 0.519496819361649
9.68083808566137 0.519500495983183
9.68218940941617 0.519503913882747
9.68354073316781 0.519507156151984
9.68489205691639 0.519510616814410
0 0
9.66191955522472 0.569278157620496
9.66327087909369 0.569278560491194
9.66462220295728 0.569278882096327
9.66597352681562 0.569279098250732
9.66732485066881 0.569279084661822
9.66867617451698 0.569278719502899
9.67002749836024 0.569278163238219
9.67137882219870 0.569277768095869
9.67273014603249 0.569277791176085
9.67408146986170 0.569278423418743
9.67543279368647 0.569279931442174
9.67678411750689 0.569282438784315
9.67813544132310 0.569285689974368
9.67948676513519 0.569289215744740
9.68083808894328 0.569292682767409
9.68218941274749 0.569296321758111
0 0
9.66191955680239 0.618953296217077
9.66327088070683 0.618954614098718
9.66462220460562 0.618956072137790
9.66597352849885 0.618957697999355
9.66732485238664 0.618959483075405
9.66867617626911 0.618961408216128
9.67002750014635 0.618963391822756
9.67137882401847 0.618965345564578
9.67273014788560 0.618967430337208
9.67408147174783 0.618969882229723
9.67543279560527 0.618972689082234
9.67678411945803 0.618975744831132
124
9.67813544330622 0.618979064607288
9.67948676714995 0.618982546020951
9.68083809098933 0.618986121740904
9.68218941482446 0.618989610589910
0 0
9.66191955778756 0.668521116139369
9.66327088171419 0.668523028678877
9.66462220563498 0.668524839606476
9.66597352955003 0.668526518518404
9.66732485345946 0.668527961135835
9.66867617736338 0.668528983833123
9.67002750126187 0.668529712812790
9.67137882515506 0.668530622809705
9.67273014904305 0.668532050181473
9.67408147292593 0.668534205515822
9.67543279680382 0.668537372967971
9.67678412067683 0.668541544411470
9.67813544454504 0.668546060825539
9.67948676840858 0.668550536351449
9.68083809226754 0.668555022864891
0 0
9.66327088234457 0.717965447544422
9.66462220627914 0.717970508488622
9.66597353020787 0.717975881813359
9.66732485413085 0.717981648316461
9.66867617804820 0.717987751525747
9.67002750196002 0.717993862692469
9.67137882586640 0.717999763436832
9.67273014976745 0.718005704508968
9.67408147366328 0.718012027410793
9.67543279755399 0.718018551073737
9.67678412143968 0.718024787788266
9.67813544532045 0.718030838243904
9.67948676919640 0.718036947005048
0 0
9.66327088274022 0.767247266428986
9.66462220668344 0.767252717106766
9.66597353062075 0.767258043272034
9.66732485455225 0.767263194243319
125
9.66867617847804 0.767267974977934
9.67002750239821 0.767272357218988
9.67137882631289 0.767276669891222
9.67273015022215 0.767281109704908
9.67408147412611 0.767285785666038
9.67543279802487 0.767291050977554
9.67678412191852 0.767297054790168
9.67813544580718 0.767303470948269
9.67948676969093 0.767310128245189
0 0
9.66462220693870 0.816378242775614
9.66597353088143 0.816399228571721
9.66732485481830 0.816420556363189
9.66867617874942 0.816442272864818
9.67002750267488 0.816463939300565
9.67137882659479 0.816485070498962
9.67273015050924 0.816506223101386
9.67408147441834 0.816528163540004
9.67543279832218 0.816550619808308
9.67678412222087 0.816573027689895
9.67813544611451 0.816595446484451
0 0
9.66462220710210 0.864839459077206
9.66597353104830 0.864875150224544
9.66732485498862 0.864912437914752
9.66867617892315 0.864951390951180
9.67002750285199 0.864991924453093
9.67137882677525 0.865033590786879
9.67273015069302 0.865075351721989
9.67408147460540 0.865116110755639
9.67543279851251 0.865155479397900
9.67678412241442 0.865193578606233
9.67813544631124 0.865230467531955
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9.66597353115867 0.912292185792756
9.66732485510126 0.912317587522265
9.66867617903805 0.912342860281730
9.67002750296913 0.912367896008824
9.67137882689461 0.912392343762583
126
9.67273015081458 0.912416538964366
9.67408147472914 0.912441399628051
9.67543279863839 0.912467005607508
9.67678412254244 0.912493041602616
9.67813544644137 0.912519418059807
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9.66597353123719 0.958961932571384
9.66732485518141 0.958987398696239
9.66867617911980 0.959014201960980
9.67002750305248 0.959042443619122
9.67137882697953 0.959071721900208
9.67273015090106 0.959100885167314
9.67408147481717 0.959129012153517
9.67543279872796 0.959155887892263
9.67678412263352 0.959181597028489
9.67813544653396 0.959206227943230
0 0
9.60786600000000 1.00500000000000
9.65786600000000 1.00500000000000
9.70936800000000 1.00500000000000
9.72981500000000 1.00500000000000
9.77981600000000 1.00500000000000
9.82981600000000 1.00500000000000
9.92981500000000 1.00500000000000
0 0
127
A.5 Low Speed Centrifugal Compressor Design
Input parameters (version 1 . 0 )
radial
Blade row # :
1
Number of blades in this row :
20
Blade Scaling factor (mm ) :
435 .12
Number of streamlines :
5
Non−dimensional Actual chord (0=no , 1=yes ) :
0
J in_Beta out_Beta mrel_in chord t /c_max Incidence Deviation Sec . Flow Angle
1 34 .374 55 .000 0 .26668693 2 .054652 0 . 0 2 0 . 0 0 . 0 0 . 0
2 40 .684 55 .000 0 .29430884 2 .054652 0 . 0 2 0 . 0 0 . 0 0 . 0
3 45 .991 55 .000 0 .32115916 2 .054652 0 . 0 2 0 . 0 0 . 0 0 . 0
4 50 .446 55 .000 0 .34589247 2 .054652 0 . 0 2 0 . 0 0 . 0 0 . 0
5 54 .196 55 .000 0 .44589247 2 .054652 0 . 0 2 0 . 0 0 . 0 0 . 0
LE / TE curve (x ,r ) definition :
Number of Curve points :
2
xLE rLE xTE rTE
0 .00000 0 .493430 1 .069073 1 .75124
0 .00000 1 .000000 0 .740135 1 .75124
Airfoil type{bf1 (sect1 ) + bf2 (sect2 ) + . . . } :
J type
1 sect1
2 sect1
3 sect1
4 sect1
5 sect1
Control table for blending section variable :
5 0 0
span bf1 bf2
0.000000000000000E+000 1 0
0.250000000000000 1 0
0.500000000000000 1 0
0.750000000000000 1 0
1.00000000000000 1 0
Stacking axis as a fraction of chord ( 2 . =centroid ) :
1 . 0 0
Control points for delta_m :
5
span delta_m
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
128
1.00000000000000 0.000000000000000E+000
Control points for delta_theta :
5
span delta_theta
0.000000000000000E+000 0.0000000000000E+000
0.350000000000000 0.0000000000000E+000
0.500000000000000 0.0000000000000E+000
0.800000000000000 0.0000000000000E+000
1.00000000000000 0.0000000000000E+000
Control points for in_beta* :
5
span in_beta*
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for out_beta* :
5
span out_beta*
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for chord :
5
span chord
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Control points for tm /c :
5
span tm /c
0.000000000000000E+000 0.000000000000000E+000
0.250000000000000 0.000000000000000E+000
0.500000000000000 0.000000000000000E+000
0.750000000000000 0.000000000000000E+000
1.00000000000000 0.000000000000000E+000
Hub offset
0.000000000000000E+000
Tip offset
0.000000000000000E+000
Streamline Data
x_s r_s
−0.384306398 0 .351355028
−0.116751701 0 .451820188
−0.029189649 0 .483692774
−0.01684271 0.487299596
0 .00000 0.493429629
0.042094824 0 .508785852
129
0.084125529 0 .52431743
0 .12603121 0 .540182938
0.167753493 0 .556524177
0.209238371 0 .573458586
0.250433673 0 .591087976
0.291289529 0 .609489336
0.331756527 0 .628728397
0.371790541 0 .648850892
0.411350432 0 .669895891
0.450392535 0 .691887295
0.488874334 0 .714840504
0.526755148 0 .738774361
0.563992002 0 .76369806
0.600538472 0 .789624701
0 .63634078 0 .816567154
0.671343078 0 .844543574
0 .70547688 0 .87357005
0.738667264 0 .903675308
0 .77082414 0 .934881182
0.801845698 0 .967213872
0.831618174 1 .000698428
0.860019765 1 .035355304
0.886916713 1 .071196222
0.912169516 1 .10820854
0.935655222 1 .146370886
0.957251563 1 .18563155
0.976862475 1 .225919057
0.994426825 1 .267145385
1.009916805 1 .309191258
1.023349651 1 .351939925
1.034776154 1 .395267053
1.044285255 1 .439055663
1.051993703 1 .483188316
1 .058041 1.527586413
1 .06257745 1 .572159174
1.065766685 1 .616857189
1.067781991 1 .661583701
1.068807685 1 .706330897
1.069073129 1 .747738555
1.069073129 1 .751241037
1.069073129 1 .766420757
1 .06524499 1 .780430686
1.061462125 1 .794440614
1.057749586 1 .808450542
1.049903935 1 .838803089
1.042618818 1 .867992738
1.028678985 1 .926365141
1.003180962 2 .043116841
0 0
−0.34076703 0.513516271
−0.122588596 0 .588865141
−0.039404647 0 .612769581
−0.02576634 0.615474697
−0.008756205 0 .620072221
0.027193016 0 .631589389
0.063094491 0 .643238072
0.102119588 0 .655188684
0.140979442 0 .667648292
0.179641995 0 .680742784
0.218062891 0 .694572819
130
0 .25619783 0 .70921671
0.294001712 0 .724739842
0 .33143041 0 .741190131
0.368441177 0 .758609234
0.404988107 0 .777024729
0.441024487 0 .796456897
0 .4765047 0.816926825
0.511379677 0 .838446291
0.545598341 0 .861027705
0.579102489 0 .884682386
0.611833115 0 .90942378
0.643720583 0 .935259986
0.674691752 0 .962207035
0.704662622 0 .990274694
0.733541322 1 .019473364
0.761228282 1 .049811087
0.787619277 1 .081289874
0.812602788 1 .113903923
0.836065166 1 .147628585
0.857906555 1 .182431168
0.878030141 1 .218256286
0.896360946 1 .255032577
0 .91285157 1 .292675699
0.927481729 1 .331080219
0.940267283 1 .370141053
0.951250862 1 .40974892
0.960504344 1 .449799538
0.968122874 1 .490191901
0.974220273 1 .530853385
0.978919608 1 .571702461
0 .98235527 1 .612690809
0.984670895 1 .653738337
0.986020351 1 .69482976
0.986594388 1 .733433018
0.986788932 1 .74363032
0.986838688 1 .762624448
0.983967584 1 .77761244
0.981130435 1 .792600777
0.978346031 1 .811660576
0.972461792 1 .843181191
0.966997955 1 .873829633
0 .95654308 1 .935121346
0.937419562 2 .057709942
0 0
−0.297227661 0 .675677514
−0.128425492 0 .725910094
−0.049619645 0 .741846387
−0.034689971 0 .743649798
−0.01751241 0.746714814
0.012291207 0 .754392926
0.042063454 0 .762158715
0.078207966 0 .770194429
0.114205392 0 .778772408
0 .15004562 0 .788026981
0.185692108 0 .798057662
0.221106132 0 .808944084
0.256246897 0 .820751287
0.291070279 0 .833529371
0.325531922 0 .847322578
0.359583678 0 .862162162
131
0.393174641 0 .87807329
0.426254252 0 .895079288
0.458767352 0 .913194521
0.490658209 0 .932430709
0.521864198 0 .952797619
0.552323152 0 .974303985
0.581964286 0 .996949922
0.610716239 1 .020738762
0.638501103 1 .045668206
0.665236946 1 .071732855
0.690838389 1 .098923745
0 .71521879 1 .127224444
0.738288863 1 .156611624
0.759960815 1 .18704863
0.780157887 1 .218491451
0.798808719 1 .250881021
0.815859418 1 .284146098
0.831276315 1 .318206012
0.845046654 1 .352969181
0.857184915 1 .388342181
0 .86772557 1 .424230787
0.876723433 1 .460543413
0.884252045 1 .497195486
0.890399545 1 .534120358
0.895261767 1 .571245748
0.898943855 1 .60852443
0 .9015598 1.645892972
0.903233016 1 .683328622
0.904115646 1 .719127482
0.904504734 1 .736019604
0.904604247 1 .758828139
0.902690177 1 .774794195
0.900798745 1 .79076094
0.898942476 1 .81487061
0 .89501965 1 .847559294
0.891377091 1 .879666529
0.884407175 1 .943877551
0.871658163 2 .072303043
0 0
−0.253688293 0 .837838757
−0.134262387 0 .862955047
−0.059834643 0 .870923194
−0.043613601 0 .871824899
−0.026268616 0 .873357407
−0.002610602 0 .877196463
0.021032416 0 .881079357
0.054296344 0 .885200175
0.087431341 0 .889896523
0.120449244 0 .895311179
0.153321325 0 .901542506
0.186014433 0 .908671458
0.218492083 0 .916762732
0.250710149 0 .925868611
0.282622667 0 .936035921
0.314179249 0 .947299596
0.345324795 0 .959689683
0.376003804 0 .973231752
0.406155026 0 .987942751
0.435718078 1 .003833713
0.464625908 1 .020912852
132
0.492813189 1 .039184191
0.520207989 1 .058639858
0.546740727 1 .079270489
0.572339584 1 .101061719
0 .59693257 1 .123992347
0.620448497 1 .148036404
0.642818303 1 .173159014
0.663974938 1 .199319326
0.683856465 1 .226468675
0 .70240922 1 .254551733
0.719587298 1 .283505757
0 .73535789 1 .313259618
0.749701059 1 .343736326
0.762611578 1 .374858143
0.774102546 1 .40654331
0.784200278 1 .438712654
0.792942522 1 .471287289
0.800381217 1 .504199072
0.806578817 1 .53738733
0.811603925 1 .570789035
0.815532439 1 .604358051
0.818448704 1 .638047608
0.820445682 1 .671827484
0.821636905 1 .704821946
0.822220537 1 .728408887
0.822369806 1 .75503183
0.821412771 1 .771975949
0.820467055 1 .788921102
0 .81953892 1 .818080644
0.817577507 1 .851937397
0.815756228 1 .885503424
0 .81227127 1 .952633756
0.805896764 2 .086896144
0 0
−0.210148924 1 .00000
−0.140099283 1 .00000
−0.070049641 1 .00000
−0.052537231 1 .00000
−0.035024821 1 .00000
−0.01751241 1 .00000
1 .37893E−06 1 .00000
0.030384721 1 .00020592
0 .06065729 1 .001020638
0.090852868 1 .002595376
0.120950542 1 .005027349
0.150922734 1 .008398833
0.180737268 1 .012774177
0.210350018 1 .018207851
0.239713412 1 .024749265
0.268774821 1 .032437029
0.297474949 1 .041306076
0.325753355 1 .051384216
0.353542701 1 .062690982
0.380777946 1 .075236716
0.407387617 1 .089028084
0.433303227 1 .104064396
0.458451691 1 .120329794
0.482765214 1 .137802215
0.506178066 1 .156455231
0.528628195 1 .176251839
133
0.550058605 1 .197149062
0.570417816 1 .219093583
0.589661013 1 .242027027
0.607752114 1 .26588872
0.624660553 1 .290612015
0.640365876 1 .316130493
0.654856361 1 .342373138
0.668125804 1 .369266639
0.680176503 1 .396747104
0.691020178 1 .424744438
0.700674986 1 .453194521
0.709161611 1 .482031164
0.716510388 1 .511202657
0 .72275809 1 .540654302
0.727946084 1 .570332322
0.732121024 1 .600191671
0.735337608 1 .630202243
0.737658347 1 .660326347
0.739158163 1 .690516409
0.739936339 1 .720798171
0.740135365 1 .751235521
0.740135365 1 .769157704
0.740135365 1 .787081265
0.740135365 1 .821290678
0.740135365 1 .856315499
0.740135365 1 .89134032
0.740135365 1 .961389961
0.740135365 2 .101489244
0 0
134