Predicting Valve Train Dynamics using Simulation … American GT Conference 2017 Predicting Valve...
Transcript of Predicting Valve Train Dynamics using Simulation … American GT Conference 2017 Predicting Valve...
North American GT Conference 2017
Predicting Valve Train Dynamics using Simulation with Model
Validation
Brice Willis, EngineerKevin Ireland, Engineer
Computational Engine ResearchHonda R&D Americas, Inc.
North American GT Conference 2017
Overview• Objectives
• Validation Test Setup
• Model Build
• Model Validation
• Other Systems
• Achievements
• Q & A
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North American GT Conference 2017
Objective
Develop and validate 2D valve train modeling methodology using GT-SUITE and motoring bench testing
Develop a modeling methodology that can be used consistently for different valve train configurations and engine operating conditions
Minimize model calibration and maintain accuracy
A validated model can help; Reduce overall development cost
Lead design Reduce required testing
Predict, evaluate, and improve valve train system performance Design of experiments Evaluate cam profiles Evaluate valve spring stiffness Capture dynamic valve lift
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Testing-Simulation: One Approach
XThe test plan does not always consider what measurements are needed to validate the simulation. This leads to high levels of model calibration and non-repeatable model correlation.
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Testing-Simulation: Another Approach
Planning test measurements for model validation will reduce model calibration and increase the repeatability of model correlation.
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Crank Encoder Wheel
Painted Valves with Camera
Gap Sensor Rocker Arm Strain Gauges
Valve Spring Strain Gauges
Motoring RPM Valve Lift via calibrated voltage
Valve Lift ≤ 1mm Measured strain tappet force
Measured strain spring stress
Validation Test Setup Validation testing was completed using motoring bench testing
Constant engine temperature (25°C to maintain build condition) Speed sweeps (0-6800 RPM) High and low valve timing/lift configurations
*Exhaust rocker shown
Validation testing was intended to capture tappet force and valve lift over a range of engine speeds while maintaining the build condition.
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Test Instrumentation Layout
Due to the engine configuration, instrumentation of multiple cylinders allows six different valve train configurations to be evaluated (Front & Rear / Intake & Exhaust / High & Low).
R = Rocker Arm strain gauge
S = Spring Strain Gauge
G = Gap sensor
V = Painted Valve
Total of 40 channels
T = ThermocoupleT
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Raw Information
Intermediate Model
Direct GT Input
Optional GT Input
2D Valve Train Model
Model Build Overview
Material Properties
Valve Train
Design & Layout
Part/Assy. Geometry (3D CAD)
𝜇𝜇𝑃𝑃 = 𝜇𝜇𝑜𝑜𝑒𝑒𝛼𝛼𝑃𝑃
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Raw Information
Intermediate Model
Direct GT Input
Optional GT Input
2D Valve Train Model
Model Build Overview
Kinematic VT Layout
Material Properties
Valve Train
Design & Layout
Part/Assy. Geometry (3D CAD)
Mass Properties
𝜇𝜇𝑃𝑃 = 𝜇𝜇𝑜𝑜𝑒𝑒𝛼𝛼𝑃𝑃
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Raw Information
Intermediate Model
Direct GT Input
Optional GT Input
2D Valve Train Model
Model Build Overview
Kinematic VT Layout
Material Properties
Valve Train
Design & Layout
Part/Assy. Geometry (3D CAD)
Mass Properties
Measured
𝜇𝜇𝑃𝑃 = 𝜇𝜇𝑜𝑜𝑒𝑒𝛼𝛼𝑃𝑃
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North American GT Conference 2017
Raw Information
Intermediate Model
Direct GT Input
Optional GT Input
2D Valve Train Model
Model Build Overview
Kinematic VT Layout
Material Properties
Part Stiffness
Valve Train
Design & Layout
Part/Assy. Geometry (3D CAD)
Mass Properties
3D Finite Element Analysis
Measured
𝜇𝜇𝑃𝑃 = 𝜇𝜇𝑜𝑜𝑒𝑒𝛼𝛼𝑃𝑃
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The rocker stiffness was predicted independent from the valve train assembly and supporting structure. Using 3D finite element analysis (FEA) the rocker was defined as a flexible body while the cam and shaft were defined as rigid bodies.
FEA Rocker Stiffness Prediction
Frictionless contact between roller, cam, rocker shaft, and rocker
Rocker shaft and cam are defined as rigid bodies
Force applied to tappet through valve stem contact along valve axis
𝐹𝐹𝐹𝐹Deflection measured
from nodes at the center of the contact radius
Fixed condition applied to rigid bodies
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FEA Rocker Stiffness Prediction
𝐹𝐹
𝛿𝛿
𝜑𝜑
𝐾𝐾𝑟𝑟𝑟𝑟𝑟𝑟 =𝐹𝐹𝛿𝛿
cos𝜑𝜑
𝐾𝐾𝑟𝑟𝑟𝑟𝑟𝑟 = rocker stiffness𝐹𝐹 = force along valve axis (load axis)𝛿𝛿 = deflection along valve axis𝜑𝜑 = angle between valve axis and rocker perpendicular
roller
rocker shaft
contact center
• The red geometry annotations represent the 2D rocker element (as defined by GT)
• Actual rocker geometry is represented by the shaded green image.
• The rocker shaft is a fixed joint free to rotate and the roller is free to rotate and slide.
• The deflection values predicted by FEA are used to calculate the stiffness
The method used to predict rocker stiffness is consistent with GT’s rocker element definition.
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FEA Rocker Support Stiffness Prediction
𝐹𝐹𝐹𝐹
Rocker components are modeled as rigid bodies.
All applicable contacts are enforced
Forces are applied to rigid body reference nodes in space
All relevant boundary conditions are applied
The rocker support stiffness was predicted independent of the rocker arm and includes all relevant supporting structure and boundary conditions. Rigid body rockers were used to load the assembly.
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The boundary conditions include; bolt pretension, shaft clearances, all contact, fixed conditions at head bolts, and symmetry definitions.
FEA Rocker Support Stiffness PredictionSymmetry boundary condition to cut faces
Fixed boundary condition to faces of head bolt sleeves
Apply clearance contact to rocker shaft, cam, and journals
Apply pretension loads to all relevant bolts
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The support stiffness prediction considered the contact footprint between the rocker to the shaft and was calculated in X & Y directions consistent with GT’s coordinate system.
FEA Rocker Support Stiffness Prediction
• Loading direction must be consistent with X and Y directions in the respective GT model.
• Predict stiffness in each direction separately.
• Apply load along an axis that is coincident with the rocker shaft (pivot) center.
• Using the rocker to load the support structure captures the contact footprint
FEA Vertical
FEA Horizontal
GT X-axis
GT Y-axis
𝐹𝐹𝑥𝑥 𝐹𝐹𝑦𝑦
𝛿𝛿𝑥𝑥𝐾𝐾𝑖𝑖 =
𝐹𝐹𝑖𝑖𝛿𝛿𝑖𝑖
𝐾𝐾𝑖𝑖 = pivot stiffness𝐹𝐹𝑖𝑖 = force along local axis𝛿𝛿𝑖𝑖 = deflection along local axis𝑖𝑖 = 𝑥𝑥, 𝑦𝑦
𝛿𝛿𝑦𝑦Rigid body reference nodes
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An average stiffness for the rocker and its support was calculated by measuring respective deflections at predetermined force intervals.
Calculating Stiffness for GT
𝐹𝐹𝑖𝑖′
𝛿𝛿𝑖𝑖′
𝑦𝑦 = 𝑚𝑚𝑥𝑥 + 𝑏𝑏(linear fit)
𝑚𝑚 = 𝐾𝐾
𝑖𝑖 = 1,2,3, … ,𝑁𝑁
𝐹𝐹𝑖𝑖 = 𝑖𝑖 ∗𝐹𝐹𝑚𝑚𝑚𝑚𝑥𝑥𝑁𝑁
𝐹𝐹𝑖𝑖′ = 𝐹𝐹𝑖𝑖 − 𝐹𝐹1
𝛿𝛿𝑖𝑖′ = 𝛿𝛿𝑖𝑖 − 𝛿𝛿1
𝛿𝛿𝑖𝑖 = deflection predicted by FEA𝛿𝛿𝑖𝑖′ = shifted deflection predicted by FEA𝐹𝐹𝑖𝑖 = interval force𝐹𝐹𝑖𝑖′ = shifted interval force𝐹𝐹𝑚𝑚𝑚𝑚𝑥𝑥 = maximum force𝑖𝑖 = interval number𝐾𝐾 = calculated stiffness linear fit slope𝑁𝑁 = number of loading intervals integer
FEA Linear fit 𝐾𝐾
𝑖𝑖 = 1
𝑖𝑖 = 2
𝑖𝑖 = 𝑁𝑁
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Low Valve Timing
High Valve Timing
Basic (w/o VTEC)
Key Model Input RequirementsRequirement VT Configuration
DependenciesMust Have
Should Have
CouldHave
Rocker Stiffness Basic (w/o VTEC) ●
Rocker Stiffness High Valve Timing ●
Rocker Stiffness Low Valve Timing ●
Support Stiffness (X&Y) Base (w/o VTEC) ●
Support Stiffness (X&Y) High Valve Timing ●
Support Stiffness (X&Y) Low Valve Timing ●
Cam Journal Stiffness (X&Y) Independent ●
Valve Spring Stiffness Independent ●
Valve Stiffness Independent ●
Valve Seat Stiffness Independent ●
Spring Retainer Stiffness Independent ●
Cam Journal Clearance Independent ●
Valve Guide Clearance Independent ●
Valve Lash Independent ●
The rocker and support stiffness are dependent on operating valve train configuration and are key model inputs. Additional key model inputs include; clearances, journal stiffness, valve lash, and component mass.
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Intake High Tappet Force
Good correlation of magnitude and frequency was observed for the tappet force of the intake high rocker.
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Crank Angle (deg)
Forc
e (N
)
Intake High Tappet Force at 4000 RPM
CH27:CYL4-A
CH28:CYL4-B
CH29:CYL6-A
GT
Crank Angle (deg)
Forc
e (N
)
Intake High Tappet Force at 5000 RPM
Crank Angle (deg)
Forc
e (N
)
Intake High Tappet Force at 6000 RPM
Crank Angle (deg)
Forc
e (N
)
Intake High Tappet Force at 6800 RPM
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Intake High Valve Lift
Good correlation of magnitude and closing response was observed for the valve lift of the intake high rocker.
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Crank Angle (deg)
Lift
(mm
)
Intake High Valve Lift at 4000 RPM
CH99:CYL4-B
CH101:CYL6-A
GT
Crank Angle (deg)
Lift
(mm
)
Intake High Valve Lift at 5000 RPM
Crank Angle (deg)
Lift
(mm
)
Intake High Valve Lift at 6000 RPM
Crank Angle (deg)
Lift
(mm
)
Intake High Valve Lift at 6800 RPM
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Intake High Frequency Map
Frequency spectrum shows resonance correlation for the intake high rocker.
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Intake Low Tappet Force
Good correlation of magnitude and frequency was observed for the tappet force of the intake low rocker.
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Crank Angle (deg)
Forc
e (N
)
Intake Low Tappet Force at 4000 RPM
CH27:CYL4-A
CH28:CYL4-B
CH29:CYL6-A
GT
Crank Angle (deg)
Forc
e (N
)
Intake Low Tappet Force at 5000 RPM
Crank Angle (deg)
Forc
e (N
)
Intake Low Tappet Force at 5500 RPM
Crank Angle (deg)
Forc
e (N
)
Intake Low Tappet Force at 6000 RPM
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Intake Low Valve Lift
Good correlation of magnitude and closing response was observed for the valve lift of the intake low rocker.
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Crank Angle (deg)
Lift
(mm
)
Intake Low Valve Lift at 4000 RPM
CH99:CYL4-B
CH101:CYL6-A
GT
Crank Angle (deg)
Lift
(mm
)
Intake Low Valve Lift at 5000 RPM
Crank Angle (deg)
Lift
(mm
)
Intake Low Valve Lift at 5500 RPM
Crank Angle (deg)
Lift
(mm
)
Intake Low Valve Lift at 6000 RPM
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Intake Low Frequency Map
Frequency spectrum shows resonance correlation for the intake low rocker.
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Valve Train with Hydraulic Lash Adjuster
Fixed Rocker Pivot HLA Rocker Pivot
The methodology used for the previously explain fixed pivot system was expanded to include a system using a hydraulic lash adjuster (HLA) at the pivot.
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Engine Oil Viscosity
𝜇𝜇𝑃𝑃 = 𝜇𝜇𝑜𝑜𝑒𝑒𝛼𝛼𝑃𝑃
𝜇𝜇𝑃𝑃 = dynamic viscosity (kg/m-s) 𝜇𝜇0 = dynamic viscosity at atmospheric pressure (kg/m-s)𝛼𝛼 = viscosity-pressure coefficient (Pa-1)𝑃𝑃 = pressure (Pa)
Barus viscosity-pressure formula: • Barus formula was used to calculate dynamic viscosity of oil under high pressure
• Barus formula is valid for pressures under 0.5 GPa
• α is unknown and can be a function of pressure and temperature
Pressure effects on oil viscosity must be considered. For this study, the Barus formula, with a calibrated viscosity-pressure coefficient, was applied. Along with small calibration of oil aeration and leak down pressure.
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Key Model Inputs for HLA
Requirement Must Have
Should Have
CouldHave
Oil Temperature ●
Oil Bulk Modulus as a function of pressure and
temperature●
Oil Viscosity as a function of pressure and temperature ●
HLA Part Leak Down Time (per spec.) ●
HLA Part Leak Down Time asa function of applied
load/chamber pressure●
HLA Starting Height ●
• Oil Bulk Modulus as a function of pressure and temperature is known
• Oil Viscosity is known for temperatures between 40 and 150°C at atmospheric pressure
• Applied Barus Formula
• 𝛼𝛼 is unknown
• Calibration of 𝛼𝛼 provides HLA model accuracy for all engine speeds and operating temperatures
*All applicable inputs from a fixed pivot system must also be applied
Oil properties become a key model input for valve train systems that include a HLA. Other key inputs include; the leak down time and starting height of the HLA
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HLA Cyclic Test: LDT & Temp. at 1000 RPM (Cam)
MeasuredGT
Cyclic test results were used calibrate oil pressure-viscosity coefficient. HLA behavior correlates well for multiple leak down times (LDT) and oil temperatures (60 and 120°C). Verifying the model for LDT and temperature.
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LDT = 2.20s
LDT = 0.45s
LDT = 0.20s
HLA Hysteresis Overlay at 60C HLA Hysteresis Overlay at 120C
HLA Hysteresis Overlay at 60C HLA Hysteresis Overlay at 120C
HLA Hysteresis Overlay at 60C HLA Hysteresis Overlay at 120C
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HLA Cyclic Test: 1000-8000 RPM (Cam)
Simulation and test results diverge as engine speed increases, but correlation remains good between 1000 and 4000 RPM. This verifies the HLA model over a range of engine speeds.
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Tappet Force – Rocker Strain w/HLA Pivot
Oil Temperature = 120˚C
Using a limited data set, the frequency of the predicted tappet force was correlated to measured strain.
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Crank Angle (deg)
Forc
e (N
)
Mic
rost
rain
Tappet Force - Rocker Strain 5000 RPM
GT
Measured
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Valve Lift w/HLA Pivot
Oil Temperature = 120˚C
Good correlation was observed for valve lift magnitude and closing response.
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Crank Angle (deg)
Lift
(mm
)
Valve Lift at 5000 RPM
Measured
GT
Crank Angle (deg)
Lift
(mm
)
Valve Lift at 5500 RPM
Crank Angle (deg)
Lift
(mm
)
Valve Lift at 6000 RPM
Crank Angle (deg)
Lift
(mm
)
Valve Lift at 6500 RPM
North American GT Conference 2017
Achievement GT-SUITE accurately predicts dynamic responses for modeled valve train systems
Modeling methodology validated via correlation of predicted and measured valve train system responses Tappet force Valve lift Valve spring response
Modeling methods are valid for multiple valve train configurations and engine operating conditions High and low valve timing With and without HLA High and low temperature High and low engine speed
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Questions 33
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Appendix 34
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Calculating Tappet Force
IntakeSlope = 0.002361969
• Measured strain from rocker arms was used to calculate tappet force
• Slope was used to scale measured strain to calculate force
Component level testing of rocker arms was used to determine a calibration factor to convert measured strain to tappet force.
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ExhaustSlope = 0.001843369
North American GT Conference 2017
Raw Information
Intermediate Model
Direct GT Input
Optional GT Input
2D Valve Train Model
Model Build Overview
Kinematic VT Layout
Material Properties
Part Stiffness
Valve Train
Design & Layout
Part/Assy. Geometry (3D CAD)
Mass Properties
3D Finite Element Analysis
Measured
𝜇𝜇𝑃𝑃 = 𝜇𝜇𝑜𝑜𝑒𝑒𝛼𝛼𝑃𝑃
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Exhaust Spring Stress
The frequency of measured spring strain and predicted spring shear stress shows good correlation in the exhaust springs for multiple engine speeds.
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Intake Spring Stress
The frequency of measured spring strain and predicted spring shear stress shows good correlation in the intake springs for multiple engine speeds.
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Exhaust Tappet Force
Good correlation of magnitude and frequency was observed for the tappet force of the basic exhaust rocker.
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Crank Angle (deg)
Forc
e (N
)
Exhaust Tappet Force at 4000 RPM
CH20:CYL4-A
CH21:CYL6-A
CH22:CYL6-B
GT
Crank Angle (deg)
Forc
e (N
)
Exhaust Tappet Force at 5000 RPM
Crank Angle (deg)
Forc
e (N
)
Exhaust Tappet Force at 6000 RPM
Crank Angle (deg)
Forc
e (N
)
Exhaust Tappet Force at 6800 RPM
North American GT Conference 2017
Exhaust Valve Lift
Good correlation of magnitude and closing response was observed for the valve lift of the basic exhaust rocker.
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Crank Angle (deg)
Lift
(mm
)
Exhaust Valve Lift at 4000 RPM
CH97:CYL4-A
CH100:CYL6-B
GT
Crank Angle (deg)
Lift
(mm
)
Exhaust Valve Lift at 5000 RPM
Crank Angle (deg)
Lift
(mm
)
Exhaust Valve Lift at 6000 RPM
Crank Angle (deg)
Lift
(mm
)
Exhaust Valve Lift at 6800 RPM
North American GT Conference 2017
Exhaust Frequency Map
Frequency spectrum shows resonance correlation for the basic exhaust rocker.
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Next Steps 42
Use current models to support and drive design
Increase development support
Build confidence in model predictions
Expand modeling capabilities
Preform further validation