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Valvetrain Friction - Modeling, Analysis and Measurement of a High Performance Engine Valvetrain System Michele Calabretta and Diego Cacciatore, Automobili Lamborghini Phil Carden, Ricardo UK

www.ricardo.com RD.10/######.# © Ricardo plc 2010 Contents

 Introduction

 Test rig and measurement system

 Mathematical model

 Measured results

 Analysis results

 Comparison between measured and calculated data

 Conclusions

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 2 Introduction

 Valvetrain friction makes a significant contribution to the whole engine friction loss, esp. at low engine speed 2.4 Auxiliaries group  The total amount depends on the valvetrain type, engine 2.2 group architecture, engine speed and lubricant temperature 2 etc. Valvetrain group 1.8 Reciprocating group  Test data in general based on motored strip measurements 1.6

 Valvetrain group contributing 1.4 – ~35% of total friction @ 1000 rpm 1.2

– Reduces with engine speed 1 – ~10% of total friction @ >6000 rpm 0.8

 Valvetrain friction of high performance engine is WholeWholeengineengine nono loadload- - (bar) (bar) 0.6 relatively high, reasons being: – Use direct acting valvetrain – sliding contact between 0.4

and 0.2 – Large valve diameter for high performance which 0 leads to high valve mass. Combined with high speed and large valve lift, leads to requirement of high 1000 1500 2000 2500 3000 3500 4000 4500 5000 5500 6000 6500 7000 7500 8000 spring force Engine speed (rpm) Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 3 Contents

 Introduction

 Test rig and measurement system

 Mathematical model

 Measured results

 Analysis results

 Comparison between measured and calculated data

 Conclusions

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 4 Test rig and measurement system

 head from a V12 engine was used

 was driven by an electric motor connected to the end of the camshaft

 Camshaft operated 12 intake valves via hydraulic

 Drive torque was measured by electric motor

 Valve motion was also measured using a laser system to verify the physical dynamic behaviour

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 5 Contents

 Introduction

 Test rig and measurement system

 Mathematical model

 Measured results

 Analysis results

 Comparison between measured and calculated data

 Conclusions

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 6 Mathematical model

 Dynamic model of a single valvetrain modelled using VALDYN

 Valvetrain represented as a series of lumped mass/inertia nodes connected by stiffness and damping

 Cam node connected to a stiffness element representing camshaft bending and support stiffness

 Tappet top stiffness modelled as a function of eccentricity of cam-tappet contact

 modelled as two mass nodes connected by a HLA element to account for the action of – High pressure chamber – Expansion spring – Check valve

 Tappet connected to the valve using lash stiffness element representing the stiffness of the valve stem between the tip and the centre of mass

 Valve and spring retainer modelled as a single mass node

 Valve node connected to ground by another lash stiffness representing valve head and seat stiffness

 Valvetrain have double spring pack

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 7 Mathematical model ( cont. )

 The cam profile designed to meet the many conflicting requirements for – Engine breathing – Acceptable durability – High speed dynamics etc.

 The spring pack designed to maintain contact between cam and follower at high engine speed

 VALDYN calculated dimensions of cam tappet contact ellipse based on Hertzian theory

 MOFT at cam-tappet contact calculated using isothermal EHL theory

 Greenwood & Tripp model utilized for asperity contact friction force prediction

 Lubricant Non-Newtonian behaviour taken into account

 Total friction torque calculated due to oil shear and asperity contact effects

 Camshaft bearing friction calculated using ENGDYN

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 8 Contents

 Introduction

 Test rig and measurement system

 Mathematical model

 Measured results

 Analysis results

 Comparison between measured and calculated data

 Conclusions

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 9 Measured results – camshaft drive torque

 Camshaft drive torque measured with standard steel tappets

 Friction torque reduced with increasing camshaft speed

 Increasing the oil supply temperature gave increased friction at low speed and reduced friction at high speed but the effect was quite small

 No significant change in behavior at very high engine speed was observed - friction torque continued to decrease

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 10 Measured results – friction comparison

 Steel tappets replaced with DLC coated ones

 Comparison between whole valvetrain measurements at 90°C – Use of DLC gave a strong reduction in valvetrain friction • 24% at 350 rpm • 33% at 1000 rpm • 24% at 4000 rpm camshaft speed

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 11 Measured results – camshaft bearing torque

 The final build involved removal of the valves, springs and tappets and operation with only the camshaft present

 This build measured to quantify the losses at the camshaft bearings with low load to assist with the understanding of the relative contributions to the total system friction

 Drive torque increased with camshaft speed

 The highest loss occured at lowest oil supply temperature

 Bearings are operating mainly in hydrodynamic lubrication regime – Losses are due to oil shear effect

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 12 Contents

 Introduction

 Test rig and measurement system

 Mathematical model

 Measured results

 Analysis results

 Comparison between measured and calculated data

 Conclusions

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 13 Analysis results - 1

 Calculated camshaft bearing friction torque with and without valvetrain loads

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 14 Analysis results - 2

 The cam/tappet friction power loss is a function of – Cam-tappet sliding velocity – Cam-tappet contact force – MOFT between cam and tappet

 At low speed – Sliding velocity low – Cam-tappet contact force high on the nose low on the flanks – MOFT low

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 15 Analysis results - 3

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 16 Analysis results - 4

 Total power loss increased roughly linearly with speed and the largest loss occurred at the cam/tappet contact

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 17 Contents

 Introduction

 Test rig and measurement system

 Mathematical model

 Measured results

 Analysis results

 Comparison between measured and calculated data

 Conclusions

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 18 Comparison between measured and calculated data - 1

 First predicted camshaft bearing friction compared with the measured data

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 19 Comparison between measured and calculated data - 2

Comparison of measured and calculated Comparison of measured and friction with standard steel tappets and calculated friction with standard friction coefficient of 0.045 steel tappets and variable friction coefficient

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 20 Comparison between measured and calculated data - 3

 Coefficient of friction required for good correlation at low engine speed

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 21 Comparison between measured and calculated data - 4

 Comparison between predicted and measured data for whole valvetrain friction as a function of oil supply temperature – standard steel tappets (on the left) and – DLC tappets (on the right)

 Model shows the same trends as the measured data; friction increased with oil temperature at low speed and friction decreased with temperature at high speed

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 22 Contents

 Introduction

 Test rig and measurement system

 Mathematical model

 Measured results

 Analysis results

 Comparison between measured and calculated data

 Conclusions

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 23 Conclusion

 The model indicated that friction losses are dominated by losses at the cam/tappet contact particularly at low engine speed

 Tappet/ interactions were less important but still worth considering

 Camshaft bearing losses were shown to make a very small contribution to total losses even at high engine speed

 Model shown in this paper can be used to evaluate the effect on valvetrain friction of many variations in valvetrain design

Project Number Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 24