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Molecular Dynamics
Simulation On The Tribology
Properties Of Two Hard
Nanoparticles Confined By
Two Iron Blocks
By: Brij Nandan Tripathi
MET (Mechanical Engineering)
17MT001599
Chengzhi Hua, Minli Bai, Jizu Lv, Zhihai Kou, Xiaojie Li
Introduction
 Tribology behaviour of Diamond and
Silicon Dioxide nanoparticles
examination via Molecular Dynamics
(MD) Simulation
Why Nanoparticles
 Over past two decades
nanomaterials have attracted
great interest for their confirmed
:
 Friction performances
 Wear performances
 Important tribological
applications
Statistical data by ISI ( Institute for Scientific
Information ) database on 22 Feb 2017
 Studying tribological properties of all
nanoparticles is impractical and a
classification into soft and hard
particles represents more efficient
manner of performing investigation for
simulation
 Hard particles: diamond and silicond
dioxide
Why diamond and SiO2
 Many experiments have reported
improvement in friction properties,
due to their addition
 Lubrication mechanism of these
two additives exhibits similar
characteristics
a) They act as billions of rolling
particles between the rubbing
surfaces
b) They separate the rubbing
surfaces and prevent direct
contact
Model Setup
 Two similar iron blocks are used as
friction pair
15Å
300K
Molecular Dynamics
Simulation
 It is a computer simulation method for
studying the physical movements of
atoms and molecules.
 The atoms and molecules are allowed
to interact for a fixed period of time,
giving a view of dynamic evolution of
the system.
 Trajectories are determined using
Newton’s equation of motion
 Forces are determined by EAM
 LAMMPS MD is used
EAM (Embedded Atomic
Method)
 It is an approximation describing the
energy between atoms, an interatomic
potential
 C-C interaction: Tersoff potential
method
 SiO2 : BKS potential model
 Fe-C, Fe-Si, Fe-O : Lennard Jones
model
Simulation Procedure
 The simulation were performed using
the classical open source MD
LAMMPS code.
Results and Discussion
• Under low load (500 Mpa)
• Under High load (1000 MPa)
Friction
state with
low velocity
(10 m/s)
• Under low load (500 Mpa)
• Under High load (1000 MPa)
Friction
state with
high velocity
(500 m/s)
1.1 Low Velocity + Low Load
Inference
1. Both nanoparticles separate the rubbing faces
and hence prevent direct contact by acting as ball
bearings.
2. Hard nanoparticles reduce both the wear and
smooth the worn surfaces more than pure base
oil when used as additives.
3. Direct contact between the friction surfaces and
plastic deformation results into adhesive and
contact fatigue.
4) Figure shows that nanoparticles (np) rotated
clockwise for most of the sliding process.
This is an evidence of mechanism of anti-wear and
friction reduction by np which converted sliding
friction to rolling plus sliding.
A positive
value
suggests the
CW rotation
V=10 m/s
P= 500 MPa
5) Under boundary lubricating conditions the two hard
nanoparticles have a polishing effect on the friction surfaces.
Morphology
changes of friction
surface of lower
block
Surface roughness
asperities are polished
by np.
Diamond is harder
than SiO2
6) Hard np added lubricants were
effective in reducing the temperature of
friction pair due to less shear than that
in direct contact
Temp profile along
Y dimension at a
sliding time of
400ps ,
V=10 m/s
P= 500 MPa
1.2 Low Velocity + High Load
Under high load of 1000 MPa , owing to hardness of diamond its
shape didn’t change and rolling occurred where as in SiO2 it distorted
Even the digging was less in later case
Most of the SiO2 points are negative.
Diamond particles constitute rolling + Sliding
SiO2 only sliding
V = 10m/s
P= 1000
MPa
Friction Force
Friction force
without np= 5GPa
V=10 m/s
Friction force for
diamond is lower
in both case due
to smaller
interaction
strength Fe-C as
shown earlier in
slide
2.1 High velocity + Low Load
SiO2
V=500 m/s
P=500 MPa
 SiO2 prevented direct contact initially
but later it developed transfer layer
 Diamond remains unaffected and is
more effective than SiO2 in improving
the high velocity low load tribological
properties.
Temp distribution at 800 ps
Middle region
(transfer layer)
2.2 High velocity + High load
 Both of the np were trapped into
transfer layer only after a short sliding
time.
V= 500 m/s
P= 1000 MPa
 Formation of early transfer layer
results into high plastic deformation,
frictional heating, amorphization, non-
equilibrium material flow
Conclusion
 Tribological behaviour of two np was
quite similar under low load and low
sliding velocity
: Improved temp distribution and friction forces
: np acted as ball bearing
: hard np had polishing effect
 At high load diamond properties were
least affected
 At high velocity low load only diamond
prevented direct contact
 At high velocity and load both failed
and formed transfer layer.
REFRENCE
 [1] TangZ,LiS.Areviewofrecentdevelopmentsoffrictionmodifiers forliquid lubricants
(2007–present). CurrOpinSolidStateMater2014;18:119–39.
 [2] Choi Y,LeeC,HwangY,ParkM,LeeJ,ChoiC,etal.Tribologicalbehaviorof copper
nanoparticlesasadditivesinoil.CurrApplPhys2009;9:124–7.
 [3] Guo D,XieG,LuoJ.Mechanicalpropertiesofnanoparticles:basicsand applications.
JPhysD:ApplPhys2014;47:013001–25.
 [4] Qiu S,ZhouZ,DongJ,ChenG.PreparationofNinanoparticlesandevaluation of
theirtribologicalperformanceaspotentialadditivesinoils.ASMEJTribol
2001;123:441–3.
 [5] KolodziejczykL,Martínez-MartínezD,RojasTC,FernándezA,Sánchez-López JC.
Surface-modified Pdnanoparticlesasasuperioradditiveforlubrication. J
NanopartRes2006;9:639–45.
 [6] Chou R,BattezAH,CabelloJJ,ViescaJL,OsorioA,SagastumeA.Tribological
behaviorofpolyalphaolefin withtheadditionofnickelnanoparticles.Tribol Int
2010;43:2327–32.
 [7] Pan Q,ZhangX.Synthesisandtribologicalbehaviorofoil-solubleCu nanoparticles
asadditiveinSF15W/40lubricatingoil.RareMetMaterEng 2010;39:1711–4.
 [8] Sánchez LópezJC,AbadMD,KolodziejczykL,GuerreroE,FernándezA. Surface-
modified PdandAunanoparticlesforanti-wearapplications.Tribol Int 2011;44:720–6.
Molecular dynamics simulation on the tribology properties of two hard nanoparticles confined by two iron blocks

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Molecular dynamics simulation on the tribology properties of two hard nanoparticles confined by two iron blocks

  • 1. Molecular Dynamics Simulation On The Tribology Properties Of Two Hard Nanoparticles Confined By Two Iron Blocks By: Brij Nandan Tripathi MET (Mechanical Engineering) 17MT001599 Chengzhi Hua, Minli Bai, Jizu Lv, Zhihai Kou, Xiaojie Li
  • 2. Introduction  Tribology behaviour of Diamond and Silicon Dioxide nanoparticles examination via Molecular Dynamics (MD) Simulation
  • 3. Why Nanoparticles  Over past two decades nanomaterials have attracted great interest for their confirmed :  Friction performances  Wear performances  Important tribological applications
  • 4. Statistical data by ISI ( Institute for Scientific Information ) database on 22 Feb 2017
  • 5.  Studying tribological properties of all nanoparticles is impractical and a classification into soft and hard particles represents more efficient manner of performing investigation for simulation  Hard particles: diamond and silicond dioxide
  • 6. Why diamond and SiO2  Many experiments have reported improvement in friction properties, due to their addition  Lubrication mechanism of these two additives exhibits similar characteristics a) They act as billions of rolling particles between the rubbing surfaces b) They separate the rubbing surfaces and prevent direct contact
  • 7. Model Setup  Two similar iron blocks are used as friction pair 15Å 300K
  • 8. Molecular Dynamics Simulation  It is a computer simulation method for studying the physical movements of atoms and molecules.  The atoms and molecules are allowed to interact for a fixed period of time, giving a view of dynamic evolution of the system.  Trajectories are determined using Newton’s equation of motion  Forces are determined by EAM  LAMMPS MD is used
  • 9.
  • 10. EAM (Embedded Atomic Method)  It is an approximation describing the energy between atoms, an interatomic potential  C-C interaction: Tersoff potential method  SiO2 : BKS potential model  Fe-C, Fe-Si, Fe-O : Lennard Jones model
  • 11. Simulation Procedure  The simulation were performed using the classical open source MD LAMMPS code.
  • 12. Results and Discussion • Under low load (500 Mpa) • Under High load (1000 MPa) Friction state with low velocity (10 m/s) • Under low load (500 Mpa) • Under High load (1000 MPa) Friction state with high velocity (500 m/s)
  • 13. 1.1 Low Velocity + Low Load
  • 14. Inference 1. Both nanoparticles separate the rubbing faces and hence prevent direct contact by acting as ball bearings. 2. Hard nanoparticles reduce both the wear and smooth the worn surfaces more than pure base oil when used as additives. 3. Direct contact between the friction surfaces and plastic deformation results into adhesive and contact fatigue.
  • 15. 4) Figure shows that nanoparticles (np) rotated clockwise for most of the sliding process. This is an evidence of mechanism of anti-wear and friction reduction by np which converted sliding friction to rolling plus sliding. A positive value suggests the CW rotation V=10 m/s P= 500 MPa
  • 16. 5) Under boundary lubricating conditions the two hard nanoparticles have a polishing effect on the friction surfaces. Morphology changes of friction surface of lower block Surface roughness asperities are polished by np. Diamond is harder than SiO2
  • 17. 6) Hard np added lubricants were effective in reducing the temperature of friction pair due to less shear than that in direct contact Temp profile along Y dimension at a sliding time of 400ps , V=10 m/s P= 500 MPa
  • 18. 1.2 Low Velocity + High Load Under high load of 1000 MPa , owing to hardness of diamond its shape didn’t change and rolling occurred where as in SiO2 it distorted Even the digging was less in later case
  • 19. Most of the SiO2 points are negative. Diamond particles constitute rolling + Sliding SiO2 only sliding V = 10m/s P= 1000 MPa
  • 20. Friction Force Friction force without np= 5GPa V=10 m/s Friction force for diamond is lower in both case due to smaller interaction strength Fe-C as shown earlier in slide
  • 21. 2.1 High velocity + Low Load SiO2 V=500 m/s P=500 MPa
  • 22.  SiO2 prevented direct contact initially but later it developed transfer layer  Diamond remains unaffected and is more effective than SiO2 in improving the high velocity low load tribological properties.
  • 23. Temp distribution at 800 ps Middle region (transfer layer)
  • 24. 2.2 High velocity + High load  Both of the np were trapped into transfer layer only after a short sliding time. V= 500 m/s P= 1000 MPa
  • 25.  Formation of early transfer layer results into high plastic deformation, frictional heating, amorphization, non- equilibrium material flow
  • 26. Conclusion  Tribological behaviour of two np was quite similar under low load and low sliding velocity : Improved temp distribution and friction forces : np acted as ball bearing : hard np had polishing effect  At high load diamond properties were least affected
  • 27.  At high velocity low load only diamond prevented direct contact  At high velocity and load both failed and formed transfer layer.
  • 28. REFRENCE  [1] TangZ,LiS.Areviewofrecentdevelopmentsoffrictionmodifiers forliquid lubricants (2007–present). CurrOpinSolidStateMater2014;18:119–39.  [2] Choi Y,LeeC,HwangY,ParkM,LeeJ,ChoiC,etal.Tribologicalbehaviorof copper nanoparticlesasadditivesinoil.CurrApplPhys2009;9:124–7.  [3] Guo D,XieG,LuoJ.Mechanicalpropertiesofnanoparticles:basicsand applications. JPhysD:ApplPhys2014;47:013001–25.  [4] Qiu S,ZhouZ,DongJ,ChenG.PreparationofNinanoparticlesandevaluation of theirtribologicalperformanceaspotentialadditivesinoils.ASMEJTribol 2001;123:441–3.  [5] KolodziejczykL,Martínez-MartínezD,RojasTC,FernándezA,Sánchez-López JC. Surface-modified Pdnanoparticlesasasuperioradditiveforlubrication. J NanopartRes2006;9:639–45.  [6] Chou R,BattezAH,CabelloJJ,ViescaJL,OsorioA,SagastumeA.Tribological behaviorofpolyalphaolefin withtheadditionofnickelnanoparticles.Tribol Int 2010;43:2327–32.  [7] Pan Q,ZhangX.Synthesisandtribologicalbehaviorofoil-solubleCu nanoparticles asadditiveinSF15W/40lubricatingoil.RareMetMaterEng 2010;39:1711–4.  [8] Sánchez LópezJC,AbadMD,KolodziejczykL,GuerreroE,FernándezA. Surface- modified PdandAunanoparticlesforanti-wearapplications.Tribol Int 2011;44:720–6.