esss numerical analysis
TRANSCRIPT
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Numerical anal sis offluid flow inside airintake system
Numerical analysis of fluidflow inside air intake system
Regis AtaidesMartin Kessler Marcelo Kruger Geraldo Severi Jr.Cesareo de La Rosa Siqueira
Walter ZottinWagner Trindade
EASC 20094th European Automotive Simulation Conference
Munich, Germany6-7 July 2009
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Agenda
Introduction
Goals
Description of the numerical model
Geometry and mesh
Boundary conditions
Numerical model
Results
Comments
Introduction Air intake system is responsible for capturing and cleaning
air from vehicles surroundings, before allowing it to beinjected into the engine
In addition, information about the mass flow is extractedfrom the flow and sent to the fuel injection system, which
can calibrate the proper mixture to any specific condition. Inorder to allow for a reliable reading, the flow must be wellbehaved around the Mass Air Flow Sensor (MAFS)
EASC 20094th European Automotive Simulation Conference
Munich, Germany6-7 July 2009
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Goals Develop a computational model to study the flow inside Air
Intake Systems (AIS) Two geometries have been evaluated and the second one with two
Evaluate the pressure drop for the entire system andidentify local pressure losses. In addition, identify the flowpattern around the MAFS
Numerical model - Geometry
Model 1 Model 2
MAFS
EASC 20094th European Automotive Simulation Conference
Munich, Germany6-7 July 2009
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Numerical model Model 2 with Honeycomb
Model 2 HC1
Model 2 - HC2
The honeycomb is placedright before the MAFS toreduce the turbulence level
Boundary conditions (Same for all models)
Outlet:Pressure
Inlet: Mass flow
Filtrating element:Inertial resistanceViscous resistance
EASC 20094th European Automotive Simulation Conference
Munich, Germany6-7 July 2009
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Computational Mesh
Extension toavoid
Mesh with around2,6 million cells forboth Model 1 and 2
the outlet
Computational MeshExtension
Mesh withHoneycomb 1
with 3.1 millionsof elements Mesh with Honeycomb 2
with 4.6 millions ofelements
EASC 20094th European Automotive Simulation Conference
Munich, Germany6-7 July 2009
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Numerical model
Assumptions: Steady-state flow; Incompressible; Turbulent.
Fluid properties: Air
ens y: , g m ; Viscosity: 1,7894e-05 kg/m/s;
Results Pressure on the walls
Model 1 Model 2
Model 2 HC1 Model 2 - HC2
EASC 20094th European Automotive Simulation Conference
Munich, Germany6-7 July 2009
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Results Pressure drop along the model Average pressure taken at the following surfaces:
In
Elem-Top
DirtyAirDuct
POut
Elem-BotCleanAirDuct
Results Pressure drop
P r e s s u r e
Mod 1
Mod 2
Mod 2 HC1
Mod 2 HC2
I n
D i r t y A
i r D u c
t
E l e m_
t o p
E l e m_
b o t
C l e a n
A i r D u
c t
A f t e r
H o n e
y C o m
b P o
u t
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Results - Uniformity
In order to identify how well behaved is theflow at the outlet, the following uniformityn exes w e app e ere:
- Eccentricity;- Gamma;- Velocity ratio;
Results Uniformity Coefficients - Definitions
Eccentr ic ity ( ): Evaluate how distant from the center themaximum velocity point is:
1: In the border (worst)22
y x +=
For an ellipsis:
( )major
mid v x L
x x = max
2
( )or
mid v y L
y y
min
max2
=
EASC 20094th European Automotive Simulation Conference
Munich, Germany6-7 July 2009
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Results Uniformity Coefficients - Definitions
Gamma ( ): Evaluate how uniform is the velocity distribution ona given surface.
amma = : n orm es
Gamma = 0: Non-uniform (worst)
totalavg
iavgi
Av
Avv2
1 =
Results Uniformity Coefficients - Definitions
Velocity ratio (v ratio ): Is the ratio between the maximumand the average velocity on a surface. Around 1 is
e er.
ratio vvv max=
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Munich, Germany6-7 July 2009
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Results Uniformity CoefficientsLDV LJ1
Uniformity coefficients
LKF
Ecc Gamma Velocity ratio
Model 1 0.74 0.96 1.10
Model 2 0.75 0.97 1.13
Model 2 HC1 0.31 0.93 1.19
Model 2 HC2 0.53 0.93 1.20
Results Velocity vector at the MAFS regionModel 1 Model 2
Model 2 HC1 Model 2 HC2
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Results Turbulence intensity around the Honey Comb
Cut plane before theHoney Comb
Model 2 HC1
Model 2 HC2
Cut plane after the Honey Comb
Results Turbulence intensity around MAFS region
Model 2Model 2 HC1
Model 2 HC2
The Honey comb reducesthe turbulence intensity
around MAFS region
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Munich, Germany6-7 July 2009
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Results Pathlines
Model 1Model 2
Model 2 HC1 Model 2 HC2
Comments
Both honeycomb designs reduced the turbulence intensity at the MAFSregion when compared to the model without it;
The pressure drop, on the other hand, increased slightly with thehoneycomb;
The pressure drop curve was affected only at the honeycomb region,keeping the same behavior in the rest of the domain;
The eccentricit at a cut lane u stream the MAFS chan ed from 0.31in the first configuration with honeycomb (Model 2 HC1) to 0.53 in thesecond (Model 2 HC2).
EASC 20094th European Automotive Simulation Conference
Munich, Germany6-7 July 2009