A dream? Dr. Jürgen Bredenbeck Tire Technology Expo, February 2012 Cologne

Similar documents
Cornering & Traction Test Rig MTS Flat-Trac IV CT plus

Modeling tire vibrations in ABS-braking

JRS Dynamic Rollover Test Scion xb

Tech Tip: Trackside Tire Data

Analysis and control of vehicle steering wheel angular vibrations

TSFS02 Vehicle Dynamics and Control. Computer Exercise 2: Lateral Dynamics

ALWAYS ON THE SAFE SIDE

Identification of tyre lateral force characteristic from handling data and functional suspension model

Cars, The high measuring accuracy of the precision load cells is retained during transmission, since digitization takes place on the wheel to

Wind Turbine Emulation Experiment

SPMM OUTLINE SPECIFICATION - SP20016 issue 2 WHAT IS THE SPMM 5000?

Fully Active vs. Reactive AWD coupling systems. How much performance is really needed? Thomas Linortner Manager, Systems Architecture

Actuator Units NEW All-in-one-solution

Analysis. Techniques for. Racecar Data. Acquisition, Second Edition. By Jorge Segers INTERNATIONAL, Warrendale, Pennsylvania, USA

WFT-C x. precise robust quick setup. Flexible 6-component wheel force transducer for road testing and test stands. productive testing

JRS Dynamic Rollover Test Toyota Prius

Extracting Tire Model Parameters From Test Data

Simulation of Collective Load Data for Integrated Design and Testing of Vehicle Transmissions. Andreas Schmidt, Audi AG, May 22, 2014

JRS Dynamic Rollover Test Chevrolet Malibu

How and why does slip angle accuracy change with speed? Date: 1st August 2012 Version:

JRS Dynamic Rollover Test Toyota Camry

Bus Handling Validation and Analysis Using ADAMS/Car

ROLLOVER CRASHWORTHINESS OF A RURAL TRANSPORT VEHICLE USING MADYMO

Model 6A Series 6-Axis Load Cells (Fx Fy Fz Mx My Mz)

RoaDyn S: Multi-Component Test Stand Hubs

METHOD FOR TESTING STEERABILITY AND STABILITY OF MILITARY VEHICLES MOTION USING SR60E STEERING ROBOT

The Multibody Systems Approach to Vehicle Dynamics

Active Suspensions For Tracked Vehicles

Ultra Series: Crossed Roller Ultra Precision Stages

FEASIBILITY STYDY OF CHAIN DRIVE IN WATER HYDRAULIC ROTARY JOINT

OPTIMIZATION STUDIES OF ENGINE FRICTION EUROPEAN GT CONFERENCE FRANKFURT/MAIN, OCTOBER 8TH, 2018

Multi-Body Simulation of Powertrain Acoustics in the Full Vehicle Development

SWIFT Evo SPINNING WHEEL INTEGRATED FORCE TRANSDUCER

Use of Simpack at the DaimlerChrysler Commercial Vehicles Division

Modification of IPG Driver for Road Robustness Applications

Tire Testing Why? Performance and Durability

Dynamical Simulation of Gear Shift Processes in BMW Motorcycle Gear Boxes.

Active Driver Assistance for Vehicle Lanekeeping

Study of the Performance of a Driver-vehicle System for Changing the Steering Characteristics of a Vehicle

FRONTAL OFF SET COLLISION

SPMM OUTLINE SPECIFICATION - SP20016 issue 2 WHAT IS THE SPMM 5000?

Lap Time Simulation Crucial for Racecar Concept Evaluation Fabrice Oehler AMZ Racing, Christoph Hahn MathWorks

96

TECHNICAL NOTE. NADS Vehicle Dynamics Typical Modeling Data. Document ID: N Author(s): Chris Schwarz Date: August 2006

MCRT 27000T Non-Contact WHEEL TORQUEMETERS (TORQUE WHEELS) Designing and Making the World s Best Torque Instruments Since 1960

WFT-Cx. precise robust quick setup. Flexible 6-component wheel force transducer for road testing and test stands. productive testing

Linear Units with Belt Drive and Slide Guide

Efficient use of professional sensors in car and tire performance measurement and comparison

124

A5 BELT-DRIVEN RODLESS ELECTRIC AXIS, SERIES ELEKTRO BK

Screw Driven automation tables

Technical Report Lotus Elan Rear Suspension The Effect of Halfshaft Rubber Couplings. T. L. Duell. Prepared for The Elan Factory.

Modelling of electronic throttle body for position control system development

Testing of Emissions- Relevant Driving Cycles on an Engine Testbed

Booming Noise Optimization on an All Wheel Drive Vehicle

Parameter Design and Tuning Tool for Electric Power Steering System

Co-Simulation of GT-Suite and CarMaker for Real Traffic and Race Track Simulations

Designing Drive Systems for Low Web Speeds

Multi-body Dynamical Modeling and Co-simulation of Active front Steering Vehicle

Cars, Light Trucks Application The RoaDyn P650 is suited for measurements of wheel forces and -moments during all kinds of driving manoeuvres

Vehicle functional design from PSA in-house software to AMESim standard library with increased modularity

Planetary Roller Type Traction Drive Unit for Printing Machine

SUMMARY OF STANDARD K&C TESTS AND REPORTED RESULTS

Robustness Analysis in Vehicle Ride Comfort

A new approach to steady state state and quasi steady steady state vehicle handling analysis

MODELING SUSPENSION DAMPER MODULES USING LS-DYNA

Design and Validation of Hydraulic brake system for Utility Vehicle

a) Calculate the overall aerodynamic coefficient for the same temperature at altitude of 1000 m.

Preliminary Study on Quantitative Analysis of Steering System Using Hardware-in-the-Loop (HIL) Simulator

Vehicle Simulation for Engine Calibration to Enhance RDE Performance

Theory of Machines II EngM323 Laboratory User's manual Version I

Research on Skid Control of Small Electric Vehicle (Effect of Velocity Prediction by Observer System)

1-3 RAMP AND TORQUE BOOST EXERCISE OBJECTIVE

Driving dynamics and hybrid combined in the torque vectoring

Vibration Analysis of an All-Terrain Vehicle

Rotational Kinematics and Dynamics Review

Application of Steering Robot in the Test of Vehicle Dynamic Characteristics

PNEUMATIC HIGH SPEED SPINDLE WITH AIR BEARINGS

Jaroslav Maly & team CAE departament. AV ENGINEERING, a.s.

Reduction of Self Induced Vibration in Rotary Stirling Cycle Coolers

Development and validation of a vibration model for a complete vehicle

ELECTRIC ACTUATOR - RODLESS ELEKTRO SK SERIES ACTUATORS

Non-Contact Sensor Performance Report

Submitted by: Sr. Engineer. Sr. Product Engineer. Product Engineer. Director Power Market Sales. Approved by: Director of Engineering

Estimation of Friction Force Characteristics between Tire and Road Using Wheel Velocity and Application to Braking Control

Weatherproof Tubular Slip Ring Assembly

itpms-in-the-loop Solution for Comprehensive Validation Tasks for indirect Tire Pressure Monitoring Systems According to the New ECE-R 64 Regulation

APPLICATION OF A NEW TYPE OF AERODYNAMIC TILTING PAD JOURNAL BEARING IN POWER GYROSCOPE

Sizing of Ultracapacitors and Batteries for a High Performance Electric Vehicle

Integrating piezo. components in. system solutions. The number and variety of piezo applications is growing in all industries, such as semicon,

CHAPTER 4 : RESISTANCE TO PROGRESS OF A VEHICLE - MEASUREMENT METHOD ON THE ROAD - SIMULATION ON A CHASSIS DYNAMOMETER

Goals. Software. Benefits. We can create and evaluate multiple vehicle setups for a track. OptimumDynamics - Case Study Track Study

Predictive Control Strategies using Simulink

Preliminary Study of the Response of Forward Collision Warning Systems to Motorcycles

CALIBRATION DATA-SET OF A SIX COMPONENT INTERNAL STRAIN- GAUGE BALANCE, B667

MAGTROL. TF Series Torque Flange Sensor. TF data sheet FEATURES. DESCRIpTION. AppLICATIONS

Dynamic Behavior Analysis of Hydraulic Power Steering Systems

VALIDATION OF A HUMAN-AND-HARDWARE-IN-THE- LOOP CONTROL ALGORITHM

GLOBAL ORGANIZATION - LOCAL SUPPORT TESTING EQUIPMENT

ME 466 PERFORMANCE OF ROAD VEHICLES 2016 Spring Homework 3 Assigned on Due date:

Transcription:

Rolling resistance measurement on the road: A dream? Dr. Jürgen Bredenbeck Tire Technology Expo, 14.-16. February 2012 Cologne

Content Motivation Introduction of the used Measurement Equipment Introduction of the theoretical approach Description of the Test procedure Results Summary / Conclusions

Motivation The demand to higher efficiency concerns each component of future vehicles Tire resistance is identified as one of the areas for efficiency improvements independent of vehicle drive concepts Understanding the behavior in real road conditions will become more important Standard testing methods (drum based) do not deliver road condition related information Real road conditions measurement was suffering from: Accurate measurement equipment for the forces as Tire resistance value is relative low Low repeatability Ability to separate different influence sources

Motivation Introduction of the used Measurement Equipment Introduction of the theoretical approach Description of the Test procedure Results Summary / Conclusions

Measurement Equipment on Road Vehicle measurement System (VMS) Wheel Force Sensor(WFS) Wheel Position Sensor (WPS) Other sensors such as GPS Vehicle ECU Information

Rig Measurement Equipment Flat belt tire testing rig (steel belt) Best simulation of the road Test is performed with the same sensor used for the vehicle testing Rig Specification Velocity Slip Angle Camber Angle Up & Down Load Flatness of the steel belt (under load condition) Bearing under the belt 0~200km/h ±20deg(0~3Hz) ±15deg(0~1Hz) g 0~50mm(0~25Hz) Fx: ±10 kn Fy: ± 10 kn Fz: 12 kn Less than 10 μm Air bearing

Wheel Force Sensor (WFS) 6 component in wheel force sensor main properties 3 axis of force and 3 axis of moment Total error 0.1% Capacity: Fx = 24KN, Fy = 15KN, Fz = 24KN Mx= 4.5 KNm, My =4 KNm, Mz = 4.5KNm Resolution 1/4000 6N or 1.8Nm Data acquisition up to 1kHz Lightweight 3.2 Kg

Unique Force Detection Method Model Based Sensor concept Shared force detection method Eight bridges are applied to the spring element No direct detection ti of each component Components are re-composed by model based calculation using real time calculation DSP platform Digital conversion of all signals and electronically re-composing overcomes disadvantages of analogue approach Cross talk error can be canceled out Distributed force bridge High speed A/D High speed DSP

Minimized Temperature effects Vehicle measurement is a challenge for the temperature influence Temperature gradient e.g. break side outside Quick change of temperature depending on driving maneuver Need for robust design against Temperature effects Share Force method allows to place the strain gauges very close to each other T: High Total gradient on each gauge is very small Small temperature effect on the measurement At the same time robustness against dynamic temperature changes 4 elements gauge T: Low

Mechanical and Electrical sensitivity Application needs stiff sensor and high accuracy Sensor sensitivity: Mechanical sensitivity x electrical sensitivity Stiff Spring element design results in: Increase of robustness Increase of eigenfrequency Reduction of mechanical sensitivity Increase electrical sensitivity by utilizing: High precision A/D converting of nv order Low noise design from less analog circuit Optimized temperature compensation from gauge layout The combination of all technology results in a high accurate sensor with 1/4000 resolution

Wheel Force Sensor Configuration

Motivation Introduction of the used Measurement Equipment Introduction of the theoretical approach Description of the Test procedure Results Summary / Conclusions

Tire Loss Theory Tire loss can be calculated from measured parameters on the wheel Measurement parameters Tire rolling inertia J 2 t in kg m Driven Wheel Tire effective radius r t in m Wheel torque My in Nm Tire Tire longitudinal force Fx in N Tire Angular speed ω in rad/s Tire Angular acceleration ώ rad/s 2 Calculated parameter Tire loss (rolling resistance) Rx in N My J R x Fx r t t My Fx Rx

Motivation Introduction of the used Measurement Equipment Introduction of the theoretical approach Description of the Test procedure Results Summary / Conclusions

Testing procedure on the test track Target: Determine Tire Loss from real driving condition Test car: BMW Mini Cooper S Test Track: - Total length: 1,792m - East straight line: 550m - West straight line: 554m Driving Maneuver: Acceleration at west straight line Cost down at East straight line Test laps: 10 laps 100Hz data acquisition Stop Startt Accele eration Coast do own

Motivation Introduction of the used Measurement Equipment Introduction of the theoretical approach Description of the Test procedure Results Summary / Conclusions

Test Track Measurement Results Example plot of one round Fx shows mainly difference between front and rear wheel Fz shows change between left and right Acceleration Stop Coast Down 70s 0s 60s Start 10s 50s 20s 30s 40s Bank Bump

Parameter Determination Direct Measures from the sensor: Wheel torque My in Nm Tire longitudinal force Fx in N Indirect Measures: Tire rolling inertia J t in kg m 2 R My J t x rt Fx Tire effective radius r t in m Tire Angular acceleration ώ rad/s 2

Wheel inertia Tire rolling inertia is premeasured using free load rotating wheel in acceleration and deceleration condition Measurement items Tire angular speed ω [rad/s] Angular acceleration ώ [rad/s 2 ] Wheel torque My free [Nm] Rolling inertia formula: T V A l l ti My free Jt Torque Vs. Angular acceleration

Angular acceleration determination Tire angular speed is measured from sensor angle encoder. Tire angular acceleration is calculated from angular speed signal by time derivative Measurement item: Tire angular speed ω [rad/s] Tire angular acceleration dω dt 70s 0s 10s 20s 30s 60s 50s 40s

Tire radius determination Tire mean radius is calculated from vehicle velocity and tire angular speed. Vehicle velocity is measured from optical Doppler sensor Instant tire mean radius is measured. Measurement items Vehicle velocity against road Vph [m/s] Tire angular speed ω [rad/s] Tire radius formula (Not considering tire slip) Vph rt [m]

Measurement parameter: Wheel torque and longitudinal force Wheel torque My and longitudinal force Fx are measured from 6 components of the Wheel Force Sensor (WFS) 70s 60s 0s 10s 50s 20s 30s 40s

Rolling Resistance Results To avoid tire slip error, driven wheel data is evaluated 10 laps of data To avoid some high frequency noise a low pass filter (4 Hz) is applied to the measurement data Very good repeatability for 10 laps 70s 60s 0s 10s 50s 20s 30s 40s

Rear Left Wheel results Average Rx: Rx = -76.1N (Acceleration), Rx = -72.8N (Cost down) 10 laps data variation 3σ : 2.8N (Acceleration), 3.6N (Cost down) Rx for Acceleration and Rx for Cost down data are very close to each other: 3.3N Acceleration Coast Down Bump Acceleration Coast Down

Rear Right Wheel results Average Rx: Rx = -87.6N (Acceleration). Rx = -82.6N (Cost down) 10 laps data variation 3σ: 2.5N (Acceleration)., 6.6N (Cost down) Rx for Acceleration and Rx for Cost down data are very close to each other: 5.0N Acceleration Bump Coast Down Acceleration Coast Down

Measurement result :Test rig Test condition: Slip angle :0 [deg] Camber angle: 0 [deg] Wheel driven by steel belt Vertical load Fz: 1kN, 2kN, 5kN Static velocity: 5km/h, 10km/h, 20km/h, 60km/h, 80km/h, 120km/h Rolling resistance is directly measured from Fx using same sensor as on the road Results: Rolling resistance is proportional to the vertical load and is not a function of velocity Rolling resistance at 2.7kN is 42N

Comparison: Real road vs Test rig Real road rolling resistance : Rx(Left) = 74 N Rx(Right) = 82 N Test rig: Rx = 42 N Reasons for the difference: Tire alignment on Road and rig is different Road surface condition Environment conditions Windforcetotire tire Temperature Measurement errors Tire effective radius measurement

Motivation Introduction of the used Measurement Equipment Introduction of the theoretical approach Description of the Test procedure Results Summary / Conclusions

Summary and Conclusion Summary: A&D Sensor delivers high h quality data Repeatability of 10 lab data did show good match It was possible to measure the tire loss (rolling resistance) during real driving condition Great match on the results though 10 laps of data Rolling resistance measurement result is depending on driving conditions We did observer difference between acceleration and coast down conditions There are differences between road and test rig results Conclusion: WFS is a useful tool for analyzing energy loss at real driving condition We are very close to the dream and will continue this investigation

Thank you for your attention! You can find us on booth no. 8387 of the Expo