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AERODYNAMICS OF RACING YACHT: APPLICATIONS. A Sail Boat is a complex aerodynamic system immersed in two fluid in relative motion . The interaction between the ‘air part’ and the ‘water part’ of the system determines the overall boat performance. DESIGN TOOLS. - PowerPoint PPT Presentation
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AERODYNAMICS OF RACING YACHT:APPLICATIONS
A Sail Boat is a complex aerodynamic system immersed in two fluid in relative motion
The interaction between the ‘air part’ and the ‘water part’of the system determines the overall boat performance
DESIGN TOOLS
AERODYNAMIC TOOLS
HULL AND APPENDAGES------------------
Tank TestCFD
SAIL PLAN--------------
Wind TunnelFull scale test
CFD
OVERALL PERFORMANCE
PREDICTION
VELOCITY PREDICTION PROGRAM
VELOCITY PREDICTION PROGRAM
The VPP provides a steady state speed of the Yacht given the wind direction and
magnitude
VPP has a two part structure comprised of the HYDRODYNAMIC FORCE MODELS and AERODYNAMIC FORCE MODELS
The JOB of the Solution Algorithm is to find that combination of Boat Speed and
Heel angle so that aero and hydrodynamic forces are in equilibrium
This is a typical polar plot which shows the boat speed for a specific true wind and heading
VELOCITY PREDICTION PROGRAM
The “cores” of a VPP are the HYDRODYNAMIC and AERODYNAMIC FORCE MODELS
The quality of the solution is dependent on the accuracy of the data of the force models.
The models are usually based on both theory and empiricism
HYDRODYNAMIC MODEL
1. Theoretical relationships2. Systematic Tank Test (e.g. Delft series)3. Computational Fluid Dynamics
AERODYNAMIC MODEL
1. Full scale Test2. Wind Tunnel3. Computational Fluid Dynamics
Usually the total hydrodynamic drag of the yacht is assumed to be the sum of the following components:
HYDRODYNAMIC FORCE MODEL
1. Wave resistance of the canoe body (systematic Tank tests)2. Appendage and canoe body friction and form drag (theoretical
relationships, empiric coefficients)3. Induced drag. Drag associated to the generation of lift (theoretical
relationships)4. Added resistance in waves. Unsteady motion due to the sea waves
(empirical correlations, tank tests)
The model has to provide the total drag as a function of boat speed and leeway (angle of attack)
AERODYNAMIC FORCE MODEL
The model has to provide the DRIVING FORCE and the HEELING FORCE as a function of Apparent Wind Speed (AWS) and Apparent Wind Angle (AWA).
The polar plot of the sail plan is determined making use of Tunnel Wind Test or CFD analysis
VPP
The final results of the VPP analyses are estimates of yacht speeds and sailing times during a regatta, the best true indicator of performance.
This tool is widely used by the naval architects in the early stages of the design process to compare a large number of configurations with different overall parameters (such as displacement, length, sail area, ….)
COMPUTATIONAL FLUID DYNAMICS (CFD)
IMPROVEMENTS IN COMPUTER PERFORMANCE
HAVE MADE THE USE OF Reynolds Averaged Navier-Stokes
(RANS) equations FEASIBLE FOR PRACTICAL DESIGN
APPLICATIONS
LATEST GENERATION OF RACING YACHT HAS
GREATLY BENEFITED OF THESE TOOLS, ORIGINALLY
DEVELOPED FOR AEROSPACE APPLICATIONS
COMPUTAIONAL FLUID DYNAMICS (CFD)
While VPP provides an overall performance prediction, CFD methods allows to reach a refined
aerodynamic optimization
CFD methods allows one to investigate in details the flow fields and to reach a better understanding
of the flow phenomena
1. Panel method, inviscid potential flow equations.2. RANS, Reynolds Averaged Navier-Stokes equations.
Capable of solve viscous effects
PANEL METHODSBased on the inviscid potential flow equation.
Panels are distributed over the model surfaces.Over each panel is distributed a constant sourceand/or doublet singularity, which satisfiesthe governing equations
Low computaional cost
COMPUTAIONAL FLUID DYNAMICS (CFD)
Principal CFD methods:
VISCOUS METHODSRANS equations spatially discretized on a computational grid.
Grid points clustered in regions where viscous effects are important.
Spatial Discretization:• Finite element • Finite volume
Steady state solutionUnsteady solution: periodic fluctuations of the main fluidynamic quantities
Unstructured computational grid Structured computational grid
CFD APPLIED TO HULL AND APPENDAGES
HULL
Wave Resistance Prediction
KEEL AND RUDDER
2D Analysis:Laminar foil for low
Reynolds number, capable to shift downstream the
location of transition onset
3D Analysis:--Plan form--Bulb, winglet--Interaction between keel and wave system
CFD APPLIED TO SAILS
UPWIND CONDITIONS
MAINSAIL GENOA AND
MAST CONFIGURATION
DOWNWIND CONDITIONS
MAINSAIL WITH GENNAKER OR
SPINNAKER---------------
Large separationsand unsteadyness
CFD APPLIED TO RACING YACHTS
THE AERODYNAMIC OPTIMIZATION IS A COMPLEX TASK REQUIRING KNOWLEDGE OF AERODYNAMICS AND HOW TO ACT ON THE GEOMETRY IN ORDER TO
IMPROVE THE PERFORMANCE.OPTIMIZATION TECHNIQUES CAN BE USEFUL IN THIS
KIND OF DESIGN PROCESS
Optimization techniques:
• Gradient Based Methods
• Design of Experiments
• Evolutionary algorithms
OPTIMIZATION METHODOLOGIES
Design process as optimization of transfer function:
Pj=Pj(Xi) Pj Performance parameters j=1,M
Xi Geometrical parameters i=1,N
Geometrical parameterization:
• Bezier Curves
• NURBS
Gradient Based Methods
• Exploration of original configuration neibourhood
• Evaluation of the gradient of TF
• Solution moved toward maximum gradient direction
• Time cost depending on initial configuration choice
• Few iterations required
• Widely used for local optimum searching
OPTIMIZATION METHODOLOGIES
Design of Experiments (DOE)• Transfer function approximated with a polynomius:
P= β0+ β1X1+… β11X12+ …β12X1X2 +…β123X1X2X3…
• Evaluation of transfer functions on a set of configurations
• DOE Theory Determination of ß coefficients through least squares
regression
3 Levels - Full Resolution
456153
N. Of runsN. of input parameters
OPTIMIZATION METHODOLOGIES
Genetic Algorithms• Based on Darwin’s evolutionary theory
• Initial set of design configurations (population) randomly selected
• Direct evaluation of TF for each configuration
• Three genetic operators: selection, recombination and mutation
• Sequential generation of improved populations
Time Cost
1506N. Of runsN. of input parameters
OPTIMIZATION METHODOLOGIES
Comparison between different strategies
TF approximationSuitable for simple multipeak TF
Design of Experiments
Suitable for complex multipeak TF
Low computational cost
Advantages
Genetic Algorithms
Gradient Based Methods
High computational cost
Only local optimum
Drawbacks
OPTIMIZATION METHODOLOGIES
ON THE USE OF CFD TO ASSIST WITH SAIL DESIGN INTRODUCTION
TRADITIONALLY THE SAIL DEVELOPMENT IS DELEGATED TO THE SAILMAKERS EXPERIENCE
COMPUTATIONAL FLUID DYNAMICS CAN BE AN
INNOVATIVE TOOL THAT ALLOWS TO TEST AND
COMPARE A LARGE NUMBER OF
CONFIGURATIONS IN A RELATIVELY SHORT
AMOUNT OF TIME
ON THE USE OF CFD TO ASSIST WITH SAIL DESIGN
Aerodynamic design of an IACC sail plan in upwind condition.
Optimal Sails profiles depending on:
•Hull and appendages features
•Wind speed and angle
•Sailing style and trim
Critical for:
•Manufacturing problems
•Sail shapes not fixed, varying with wind pressure
and sail trim
Sails are often compared to aircraft wings.
Unfortunately classic aeronautical design criteria are only
partially useful:
• Contrary to wings, sails must work in a wide operative range
(i.e. angle of attack)
• The goal in the aeronautical design is to minimize the losses
(drag). In sail design the goal is to maximize the driving force,
without taking into account losses.
• The classic Lift-Force projection must replaced with the sailing
aerodynamics terms “Driving-force Heeling-Force”
• The flow is often separated (depending on the angle of attack)
DESIGN CRITERIA
Design Operating Conditions:
•True Wind Speed
•Apparent Wind Angle
DESIGN CRITERIA
Under fundamental hypothesis of a constrained Heeling Moment,
the GOAL is to find a maximum driving force configuration.
Input data:
•Initial configuration recovered
from pictures (deformed shape)
•Righting Moment available
GEOMETRY DATA ACQUISITION
Superimposition of Bezier curves.
Principal parameters used to describe the profile:
• CAMBER
• DRAFT
• Entry Angle
• Exit Angle
• Twist Angle
NAVIER-STOKES Solver “Hydro”
• 3D, fully viscous, multi-grid, multi-block code developed by the
University of Florence
• Acceleration techniques employed:
1. Local time-stepping
2. Residual smoothing
3. Multi-grid Full Approximation Storage (FAS)
• Boundary Conditions:
1. Solid walls: no-slip condition
2. Inlet: total pressure and flow angles
3. Outlet: static pressure
The Earth’s boundary layer can be taken into account imposing
spanwise variable inlet conditions.
GRID GENERATION
The size (number of points) of the computational grid has to fulfill three main requirements:
1. To solve the flow phenomena of interest (e.g. boundary layer)
2. To compute solutions sufficiently grid-independent
3. To match computational times to design needs
Mainsail
Genoa
The first step is to generate a computational grid around the sail plan.
The computational grid represents the domain where the solver computes the solution.
GRID GENERATION
The boundaries have
to be defined far
enough from the
sails, where the
flow is
indisturbed.
GRID GENERATION
Mainsail
Genoa
HORIZONTAL SECTION OF THE GRIDThe Grid consists of three
block.
Structured H-type grids
were employed in
computations.
The grid generation is based
on an elliptic procedure
on 2D grids which are
subsequently stacked in
the vertical direction.
GRID GENERATION
Details of the viscous grid around the mast
2 200 000 grid point was judged to
be a good compromise (memory
requirements of about 650MB) for
mainsail-genoa configuration
For a complete mast model, a viscous
grid with 285 x 129 x 93 grid points in
the chordwise, chordwise-orthogonal,
and spanwise directions, was used
(3 400 000 grid point,
1000 MB memory requirements)
Grid points clustered near the solid walls in
order to solve the boundary layer
VISCOUS SOLUTION
The RANS codes allow to take into
account the viscous effect such as
boundary layer, separation bubble.
Compared to other design tools, the
RANS solution allows to investigate in
detail the flow structures
PARAMETRIC ANALYSIS
The first analysis presented is
obtained through a parametric
variation of the Genoa Camber on the
whole span from the initial value 11%
up to 21%. The design Apparent Wind
Angle (AWA) is 16 deg.
PARAMETRIC ANALYSIS
The results of the
computations, for
incompressible flow,
are the velocity vectors
and the static pressure
field (one value for
each grid point)
Static pressure distribution on the genoa profile
LEA
DIN
G E
DG
E
TRA
ILIN
G E
DG
E
PARAMETRIC ANALYSIS
Obviously the Camber variations from its initial value involve both driving force
and heeling moment changes.
PARAMETRIC ANALYSIS
Which is the Optimal Genoa Camber value?
-- The optimal Camber is a comprime solution between heeling-moment and driving
force.
-- It is necessary to evaluate the trade-off between heeling moment and driving force.-- To this aim the initial Heeling Moment (constrained) has to be re-
established through the Mainsail Twist Distribution
-- This is a well-known practice for reducing the heeling moment used by
every yachtsmenHeeling force
PARAMETRIC ANALYSIS
--Three parametric curve for three
separate mainsail twist
--To re-establish the initial Heeling
Moment (which is the
optimization process constraint)
the mainsail twist is varied
Heeling Moment Coefficient definition:
dmSAAWSChmHm 2
21
Where:Hm: Heeling MomentChm: Heeling Moment CoefficientSA: Sail Areadm: Distance between CLR and mast-head
Chm TWS
PARAMETRIC ANALYSIS
IT SHOULD BE NOTED THAT THE HEELING MOMENT COEFFICIENT IS
CORRELATED TO THE WIND SPEED
SINCE Hm IS UPPER BOUNDED BY THE BOAT STABILITY, THE GREATER
THE WIND SPEED (AWS), THE LOWER THE HEELING MOMENT
COEFFICIENT (Chm) MUST BE
PARAMETRIC ANALYSIS
Which is the Optimal Genoa Camber value?
-- Points A,B and C represent the optimal camber values for three
separate wind magnitude
Light Wind
Moderate Wind
Heavy Wind
GENOA CAMBER PARAMETRIC ANALYSIS
PLOTTING THE DRIVING FORCE
IN A THIRD DIMENSION WITH THE
AID OF THE CONTOUR LINES
(lines at constant driving force)
GIVEN THE RESULT OF THE
ANALYSIS,
THE ESSENTIAL FEATURES OF
SAILS IS ITS ABILITY TO BE
ADJUSTED TO MATCH THE
WIND SPEED CHANGES
GENOA CAMBER PARAMETRIC ANALYSIS
NEED FOR MANY SAILS FOR EACH WIND SPEED
SAIL REQUIREMENTS:
ABILITY TO BE ADJUSTED TO MATCH
THE WIND SPEED CHANGES
In upwind conditions, an America’s Cup Class has 2/3
different mainsail and 5/6 different genoa:
• Genoa code 1: <6 kn TWS
• Genoa code 2: 8 kn TWS
• Genoa code 3: 12 kn TWS
• Genoa code 4: 16 kn TWS
• Genoa code 5: 20 kn TWS
MAINSAIL CAMBER PARAMETRIC ANALYSIS
THE ANALYSIS HAS BEEN
REPEATED FOR THE
MAINSAIL CAMBER
(AWA 16 deg)
True Wind Speed Optimal camber
8 kn 9.8%
13 kn 6%
MAINSAIL CAMBER PARAMETRIC ANALYSIS
GIVEN THE RESULT OF THE
ANALYSIS, MAINSAIL SHOULD BE
FLATTER THAN GENOA.
TWS 8 kn Optimal camber
Mainsail 9.8%Genoa 16%
Genoa Base
Genoa Head
Main Head
Main Base
Mainsail Genoa
This fact can be explained by taking into
account the load distribution:
The aerodynamic load on the Genoa is
greater than the load on the mainsail
OPTIMUM SPANWISE CAMBER DISTRIBUTION
To go further in the analysis is it possible to consider the optimum spanwise
distribution of the Genoa camber
LIGHT WIND CONDITION
CAMBER
should
increase
with
increasing
height
OPTIMUM SPANWISE CAMBER DISTRIBUTION
To go further in the analysis is it possible to consider the optimum spanwise
distribution of the Genoa camber
MODERATE WIND CONDITION
CAMBER
should
decrease
with
increasing
height
OPTIMUM SPANWISE CAMBER DISTRIBUTION
SPANWISE LOAD
DISTRIBUTION
--Light Wind: increasing load with
increasing height
--Moderate Wind: decreasing load with
increasing height
Genoa Twist distribution fixed
Load on the Genoa is induced by
the Mainsail twist distribution
CONCLUSION
From the 1983 turning point in the America’s Cup hystory to
today, the use of CFD in the yacht design process has quickly
increased
While no CFD methos should claim to replace other design tools
(wind tunnel, tank test…), CFD play an important role in a
modern design process
Improvements in computer performance have made the use of
RANS the main CFD tool for practical design applications,
opening new frontiers in racing yacht design