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8/2/2019 Fakhar Title Defence_Final
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Thesis SupervisorDr. M. Afzaal Malik
Guidance & Evaluation CommitteeCol Dr. Syed Waheed-ul-Haq
Lt Col Dr. Aamer Ahmed Baqai
Mr. Raja Aamir Azim
MS Student
Fakhar-e-Alam Khan
2009-NUST-MSPhD-MECH-12
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Sequence Motivation
Introduction
Research Plan Knowledge Base
Literature Survey
Development of Model/Sub-Models (Mathematical Equations)
Numerical Scheme
MATLAB Code Integration of all Sub-Models
Simulation of Results
Conclusions
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Motivation Interest in Thermal Sciences/Internal Combustion
Engines.
I am working at a testing lab in a private sector commercial
organization. To look after Short Circuit Generator especially its
lubricating oil unit.
Lubricants make fluid film bearings reduce friction & wear,
and Provide load capacity.
That why I was keen to understand the Lubrication theoryof bearings and how heat affects its load carrying capacity.
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Introduction The piston and top compression ring come into direct
contact with hot combustion gases.
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Introduction (Contd) The heat energy in the piston is absorbed by the rings.
The rings then transfer this heat into the cylinderwalls.
Approx. 70% of the piston's heat is carried away by thepiston rings, under both unloaded and loaded engine
operation conditions, at 1,500 and 3,000 rpm.
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Research Plan
Knowledge Base
Literature Survey
Development of Model/Sub-Models (MathematicalEquations)
Numerical Scheme
MATLAB Code
Integration of all Sub-Models
Simulation of Results Conclusions
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Knowledge BaseWhole or part of the following books were studied:
Fundamentals of Fluid Film Lubricationby Bernard J.Hamrock & Steven R. Schmid
EngineeringTribologyby Gwidon W. Stachowiak & AndrewW. Batchelor
Elasto-HydrodynamicLubrication by D.Dowson &
G.R.Higginson AppliedTribologyby Michael M. Khonsari & E. Richard
Booser
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Knowledge Base (Contd) ComputationalFluidDynamics by John D. Anderson, Jr.
ComputationalHeatTransfer by Yogesh Jaluria & Kenneth E.
Torrance HeatTransferCalculationsusingFiniteDifferenceEquations
by David R. Croft & David G. Lilley
InternalCombustionEngineFundamentals by John B.Heywood
ComputationalFluidDynamics(Volume)by Klaus A.Hoffmann & Steve T. Chiang
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Knowledge Base (Contd) Mathematical Statements of Physical processes
(Differential Forms in Cartesian Coordinates):
Continuity Equation (Mass is conserved):
Conservation of Momentum (Momentum isconserved):
x-Momentum:
0)()()(
z
w
y
v
x
u
t
BxzxyxxxF
x
p
zyxz
uw
y
uv
x
uu
t
u
)()(
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Knowledge Base (Contd) y-Momentum:
z-Momentum:
ByzyyyxyF
y
p
zyxz
vw
y
vv
x
vu
t
v
)()(
BzzzyzxzF
zp
zyxzww
ywv
xwu
tw
)()(
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Knowledge Base(Contd) Energy Equation (Energy is conserved):
Reynolds's Equation:
The differential equation governing the pressure distribution in
fluid film lubrication is known as the Reynolds equation.
)()()()(
z
Tk
zy
Tk
yx
Tk
xz
Tw
y
Tv
x
Tu
t
TCp
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Knowledge Base (Contd)
Couette term can further be expanded to:
expansionlocalsqueezenormal
squeezegeometric
sheartoduerateflownetterm:Couette
gradientspresuretoduerateflownet:termsPoiseuille
3
)(])([2
1
12 thww
x
hUhUU
x)
x
P
h(
xabbba
wedgedensity
wedgephysicalstretchphysical
sheartoduerateflownetterm:Couette
)(2
1)(2
1)(2
1])([2
1
xhUU
x
hUUUUx
hhUUx
babababa
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Literature Survey Following journals were explored.
ASME Journal of Engineering for Gas Turbines and Power
ASME Journal of Heat Transfer
ASME Journal of Thermal Science and EngineeringApplications
ASME Journal of Tribology
SAE Technical Paper Series
SAGE Journal of Automobile Engineering Proceedings of IMechE
Elsevier Journal of Applied Thermal Engineering
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Literature Survey (Contd) Journal of Tribology International
MIT MS/PhD thesis from dspace.mit.edu/
Bulletin of The Japan Society of Mechanical Engineers (JSME)
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Literature Survey (Contd) Yasuo Harigaya, Michiyoshi Suzuki, Fujio Toda, Masaaki Takiguchi,
Analysis of Oil Film Thickness and Heat Transfer on a Piston Ring of aDiesel Engine: Effect of Lubricant Viscosity, ASME Journal of Engineeringfor Gas Turbines and Power, July 2006, Vol. 128/685.
Jordan A. Kaplan, Modeling The Spark Ignition Engine Warm-Up ProcessTo Predict Component Temperatures, MS Thesis, MIT, 1990.
Jordan A. Kaplan and John B. Heywood , Modeling the Spark IgnitionEngine Warm-Up Process to Predict Component Temperatures and
Hydrocarbon Emissions, SAE paper 910302, 1991.
V. Esfahanian, A. Javaheri, M. Ghaffarpour, Thermal analysis of an SIengine piston using different combustion boundary condition treatments,Applied Thermal Engineering 26 (2006) 277-287.
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Literature Survey (Contd) Yong Liu and R. D. Reitz, Modeling of heat conduction within chamber
walls for multidimensional internal combustion engine simulations, Int. J.Heat & Mass Transfer, Vol. 41, Nos 6-7, pp. 859-869, 1998.
Ravindra Prasad and N. K. Samria, Transient heat transfer analysis in aninternal combustion engine piston, Computers & Structures Vol. 34, No.5,pp.787-793,1990.
Toshio TADA, Shoichi Furuhama, On the Heat Flow from the Pistons in a
Farm Type Gasoline Engine, Bulletin of JSME, 621.434-242:621.434.016.4.
Toshio TADA, Yoshitane OYA, Piston Temperatures of an AutomobileEngine, Bulletin of JSME, 621.434-242:621.434.016.4.
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Mathematical Modeling
Energy Equation in Cylindrical Coordinates:
Energy Equation in Cylindrical Coordinates is:
In absence of motion and neglecting the source term , the
energy equation reduces to the governing equation for heatconduction in Piston Crown and Top Ring.
)()(
1)(
1)(
2 z
Tk
z
Tk
rr
Tkr
rrz
Tu
T
r
w
r
Tv
t
TCp
)()(1
)(1
2z
Tk
z
Tk
rr
Tkr
rrt
TCp
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Energy Equation in Cylindrical
Coordinates (Contd)
Assuming constant thermal conductivity and
axisymmetry, the conduction heat equation is:
)()(
1
z
T
kzr
T
krrrt
T
Cp
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Numerical Scheme Normally Closed form/exact solutions for real world
engineering problems do not exist.
Numerical Scheme is used.
Real world Engineering problems are mostly solved byusing any one of the following numerical schemes:
Finite Difference Scheme Finite Volume Scheme
Finite Element Scheme
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Numerical Scheme (Contd) Finite Difference Scheme will be used.
Finite Difference Schemes are further classified asExplicit or Implicit Schemes.
Explicit schemes are easier to implement but these areconditionally stable schemes.
Implicit schemes are unconditionally stable schemes.
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Numerical Scheme (Contd) 2-D Parabolic Partial Differential Equations are
normally solved by Alternating Direction Implicit(ADI) scheme.
Split the time step into half.
For the first half, treat one term implicitly while theother explicitly to get the solution by tridiagonal
algorithm. For the next half, reverse the implicit-explicit
formulation to again get the solution by tridiagonalalgorithm.
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Numerical Scheme (Contd) Finite Differencing of 2-D Heat Equation using ADI
Scheme:
Let = Thermal Diffusivity
&
First Half:
pC
k
2)(
)(
r
trr
2)(
)(
z
trz
n
ji
n
ji
n
ji
n
ji
n
ji
n
ji Tr
rrrTrT
r
rrrTrTrTr
rrrrzzz ,1,,1
1
1,
1
,
1
1, )2
()21()2
()21(
Implicitz(j)Explicit,)( ir
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Numerical Scheme (Contd) Second Half: Explicitz(j)Implicit,)( ir
1
1,
1
,
1
1,
2
,1
2
,
2
,1 )21()2
()21()2
(
n
ji
n
ji
n
ji
n
ji
n
ji
n
ji TrTrTrTr
rrrTrT
r
rrr
zzzrrrrr
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Code Development Normally, simulation of results are obtained by using
Either Commercial Software
Writing Own Code in any Programming Language like C,FORTRAN, MATLAB etc
Due to strong graphics capabilities, the numerical
programming code is being written in MATLAB.
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Integration of all sub-models The following equations will be coupled to get the
overall simulation results:
2-D Heat Equation in Piston Crown
1-D Heat Equation in Top Compression Ring
Convective Heat Transfer in lubricant film
Reynolds's Equation
Piston Dynamics Equation
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Simulation of Results/Conclusions
Simulation of results will show the effect ofCombustion Heat over the load carrying capacity ofthe top compression ring.
Conclusions will be drawn from the above simulation
results.
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Thank You