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 Project Number Introduction Test rig and measurement system Mathematical model Measured results Analysis results Comparison between measured and calculated data Conclusions 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 architecture, engine speed and lubricant temperature etc. Crankshaft group 2 Valvetrain group Valvetrain group contributing – ~35% of total friction @ 1000 rpm – Reduces with engine speed – ~10% of total friction @ >6000 rpm Valvetrain friction of high performance engine is relatively high, reasons being: 1.2 1 0.8 0.4 0.2 ## Month 2010 8000 7500 7000 6500 6000 5500 5000 4500 4000 3500 0 3000 – Large valve diameter for high performance which leads to high valve mass. Combined with high speed and large valve lift, leads to requirement of high spring force Client Confidential – Client Name 1.4 0.6 – Use direct acting valvetrain – sliding contact between cam and tappet Project Number 1.6 2500 Reciprocating group 1500 Test data in general based on motored strip measurements 1000 Whole engine - no load (bar) 1.8 2000 2.2 Engine speed (rpm) RD.10/######.# © Ricardo plc 2010 3 Contents Project Number Introduction Test rig and measurement system Mathematical model Measured results Analysis results Comparison between measured and calculated data Conclusions Client Confidential – Client Name ## Month 2010 RD.10/######.# © Ricardo plc 2010 4 Test rig and measurement system Cylinder head from a V12 engine was used Intake camshaft was driven by an electric motor connected to the end of the camshaft Camshaft operated 12 intake valves via hydraulic tappets 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 Project Number Introduction Test rig and measurement system Mathematical model Measured results Analysis results Comparison between measured and calculated data Conclusions 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 Hydraulic tappet 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 Project Number Introduction Test rig and measurement system Mathematical model Measured results Analysis results Comparison between measured and calculated data Conclusions 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 Project Number Introduction Test rig and measurement system Mathematical model Measured results Analysis results Comparison between measured and calculated data Conclusions 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 Project Number Introduction Test rig and measurement system Mathematical model Measured results Analysis results Comparison between measured and calculated data Conclusions 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 friction with standard steel tappets and friction coefficient of 0.045 Project Number Client Confidential – Client Name Comparison of measured and calculated friction with standard steel tappets and variable friction coefficient ## 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 Project Number Introduction Test rig and measurement system Mathematical model Measured results Analysis results Comparison between measured and calculated data Conclusions 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/bore 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
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