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Modeling Molecular Structure to Tribological Performance SAE World Congress Detroit, Michigan April 2016 Chad Chichester, Aleksandra Nevskaya ,

Molecular modelling, the future of lubrication research and development

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Modeling Molecular Structure to Tribological Performance

SAE World CongressDetroit, MichiganApril 2016

Chad Chichester, Aleksandra Nevskaya,

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Outline of Presentation

• Current Siloxane Primer• Molecular Structure to Rheology to Tribology• Results, Model-Guided Design• Future technologies

2014 Dow Corning . All rights reserved

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Siloxanes: Functionalized groups in organo-silicon chemistry with Si–O–Si backbone

• Strong Bonds: Si-O (460 kJ/mol) vs. C-C (348 kJ/mol)• Long Bonds: Si-O (0.164 nm) vs. C-C (0.153 nm)• Flexible Bonds: Si-O-Si (143º) vs. C-C-C (110º) • Low Steric Hindrance: Unencumbered Oxygen• Low Glass Transition Temperature (148 K)• High Oxidative Stability PDMS (573 K) to PPMS (649 K)• Thermal-Viscous Stability: PDMS (15 kJ/mol) vs. PAO

(30 kJ/mol)• Permanent Shear Stability: Very Low Monomeric

Friction

CH3

SiH3C

CH3

OSi

OCH3

CH3

SiCH3

CH3

CH3n

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= Si = O = C = H

• Viscosity range 0.65 to 1.000.000 cSt• Very High Viscosity Indices• Excellent thermal & oxidative stability• Excellent low temperature flow ability • Low volatility (even low viscosities)• Good plastic and rubber compatibility • High chemical resistance• Insoluble in water

Three Primary Types of Silicone Polymers

• “Standard” SiliconesDimethy

l Silicone

• Additional thermal and oxidation stability

Phenyl-Methyl Silicone

• Excellent chemical resistant• Better load carrying capacity

and wear resistance

Fluoro Silicone

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H3C –Si – O – Si – O — Si – O – CH3

CH3 CH3

n

CH3

CH3CH3CH3

H3C –Si – O – Si – O — Si – O – CH3

CH3 CH3

n

CH3

CH3C6H5CH3

H3C –Si – O – Si – O — Si – O – CH3

CH3 CH3

n

CH3

CH3

CH2CH3 CH2

CF3

comparison

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SRVok load (N)

4-ball scar (mm)

400N/1hr

DSC, OOT

Visc -35°C

Visc40°C

Visc100°C VI

PAO-6 350 0.822 202 3424 26 5.6 163PDMS 300 SEVERE 286 234 35 16 466PDMS, Formulated 975 1.378 221 141 22 9.7 473Dimethyl+hexyl 2000 0.879 204 x 28 8.3 298PFPE-Y Branched 2000 0.727 500 54450 94 15.1 169Trifluoropropyl 550 1.182 246 36386 159 29.6 228PFPE-Z Linear 600 1.485 500 3591 160 46.3 332

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Film FrictionElastohydrodynamic Non-Conformal contact Hamrock-Dowson

Film thickness depends on:• Entrainment Speed• Contact Load as function of

Applied load Poison ratio of materials Young’s modulus of materials

• Geometry as function of Surface roughness of materials Diameter of moving parts

• Lubricant’s Viscosity as function of its Monomeric friction Radius of gyration Activation energy (temperature

dependence) Pressure viscosity index (pressure

dependence)

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Conventional Film Thickness Modeling Equation Example

Applying model to siloxanes assumes behavior similar to mineral oil.

Idea…Rather than repeat empirical approach…Develop molecular structure approach

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Model-Based Siloxane Structure DesignFrom Molecule to Tribology

Molecular properties

Rheological properties Tribological parameters

Tribological Properties

• Molecular structure• Molecular mass

distribution

• Volume structure andVolume Pressure Temperature• Viscosity structure andViscosity Pressure Temperature• Pressure viscosity index

• Geometry• Poisson ratio• Young Modulus• Load• Speed

• Asperity friction• Film friction

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Siloxane Structures

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Si O Si OCH3

H3CCH3

CH3

SiCH3

CH3

O Si CH3

CH3

CH3m n

DP

J

QL

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ZJLQv ,,,0 ZJLQ ,,,0

MPaPKT1.0298

MPaPKT1.0298

Molecular Structure – Specific Volume

Packing Factor

Wv

PTv ,Equation of State

Molecular Structure - Viscosity

PT ,

Viscosity (T,P)

Shear Viscosity s

00v

cXF

Viscosity Variation

Molecular to Rheological

v η

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The Stribeck Curve is divided into three primary regions Boundary Lubrication Mixed Lubrication Full Film Lubrication

22qBqA RR

h

3

10

31

0 1 3

Asperity Friction

Film Friction

Total Friction Total

FilmAsp

Friction Components

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Rheology to Tribology

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Structural OptimizationThe optimization of molecular structure can be approached as follows

Feedback to Molecular Structure DesignVariation of Input

Parameters

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Siloxane StructuresPolydimethylsiloxane: PDMS

Polycyclohexylsiloxane: PCMS

Polyphenylmethylsiloxane: PPMS

CH3

SiH3C

CH3

OSi

OCH3

CH3

SiCH3

CH3

CH3nMw

increasePDMS

PPMS

PCMS

phenyl branch

cyclohexyl branch

dimethyl branch

NEW

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Siloxane StructuresCopolymers and pendant branches

PAMS

PPAMS

Polyphenylhexylsiloxane: PPAMS

Polyalkylmethylsiloxane: PAMS

Polytrifluoropropylsiloxane: PFMS

alkyl branch

phenylalkyl branch

ALLNEW

NEW

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PA100: 100% Phenylalkyl 0% PDMSPA30: 30% Phenylalkyl 70% PDMS

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Graphic User Interface for SiloxanesSiloxane Species and

Structure

Interface Geometry and conditions

Rheological Properties

Tribological Performance

Si O Si OCH3

H3CCH3

CH3

SiCH3

CH3

O Si CH3

CH3

CH3m n

DP

J

QL

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J

L

Q DP

Film Thickness and Friction

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Newtonian and Non-Newtonian Siloxanes

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PPMS 90 (90% Phenyl) A100-12 (100% Dodecyl)

Ring branches (PPMS and PCMS) show nearly Newtonian nature High aryl and cycloalkyl content causes high pressure-viscosity PPMS 90: High monomeric friction allows a relatively low molecular mass (Mw=1990

g/mol) to build viscosity, so shear thinning is low

Linear branches may exhibit temporary shear-thinning Low to high alkyl branch length causes low pressure-viscosity coeff. A100-12: Low monomeric friction requires a relatively high molecular mass

(Mw=29900 g/mol) to build viscosity, so shear thinning is high

EHD Friction Increases With Cyclic Branch Content

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PPMS:Phenyl-methyl PCMS:Cyclohexyl-methyl

Friction at 398 K and Σ=0.5

Cyclohexyl siloxanes have greater thermal stability of performanceFriction at 303 K and Σ=0.5

Siloxane Is Adaptable To Diverse Applications

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CH3

SiH3C

CH3

OSi

OCH3

CH3

SiCH3

CH3

CH3n

PCMS:Cyclohexyl-methyl

PDMS:Dimethyl

PAMS:Alkyl-methyl

Traction Fluids Energy-Efficient Lubricants

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Boundary Friction and WearLubricants were tested using a ball-on-disk machine to determine the effects of molecular structure on boundary friction and wear

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Comparison with Existing Technologies

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Future Research Opportunities

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Si O Si OCH3

H3CCH3

CH3

SiCH3

CH3

O Si CH3

CH3

CH3m n

DP

J

QL

Other types of chemical structures

Mixtures Functional groups Additives

Selected fluids from this work exhibit the following properties: Additive compatibility Miscibility with Hydrocarbons Special High Temperature

Summary

• Silicones stand out synthetic fluids for their exceptional thermal stability and temperature-viscosity indices

• Newly synthesized siloxanes are examples of the tribological potential beyond currently use of silicones– Temporary shear thinning Polyalkylmethyl siloxanes– High traction Polycyclohexylmethylsiloxanes– High temperature Ph/F co-polymers

• Flexible structure of new Ph/F copolymers allows design of fluids with high termal stability and improved wear resistance

• Their additive acceptance offers additional possibilities for lubricant formulation

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Summary

• Silicones stand out synthetic fluids for their exceptional thermal stability and temperature-viscosity indices

• Newly developed silicone fluids offers enhanced lubricity in combination with high temperature resistance

• Additionally additive acceptance offers new possibilities for lubricant formulation

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