Introduction to Convective Heat Transfer A Software-Based Approach Using Maple and MATLAB
, by Onur, Nevzat- ISBN: 9781119766766 | 1119766761
- Cover: Hardcover
- Copyright: 4/18/2023
A highly practical intro to solving real-world convective heat transfer problems with MATLAB® and MAPLE
In Introduction to Convective Heat Transfer, accomplished professor and mechanical engineer Nevzat Onur delivers an insightful exploration of the physical mechanisms of convective heat transfer and an accessible treatment of how to build mathematical models of these physical processes.
Providing a new perspective on convective heat transfer, the book is comprised of twelve chapters, all of which contain numerous practical examples. The book emphasizes foundational concepts and is integrated with explanations of computational programs like MATLAB® and MAPLE to offer students a practical outlet for the concepts discussed within. The focus throughout is on practical, physical analysis rather than mathematical detail, which helps students learn to use the provided computational tools quickly and accurately.
In addition to a solutions manual for instructors and the aforementioned MAPLE and MATLAB® files, Introduction to Convective Heat Transfer includes:
- A thorough introduction to the foundations of convective heat transfer, including coordinate systems, and continuum and thermodynamic equilibrium concepts
- Practical explorations of the fundamental equations of laminar convective heat transfer, including integral formulation and differential formulation
- Comprehensive discussions of the equations of incompressible external laminar boundary layers, including laminar flow forced convection and the thermal boundary layer concept
- In-depth examinations of dimensional analysis, including the dimensions of physical quantities, dimensional homogeneity, and dimensionless numbers
Ideal for first-year graduates in mechanical, aerospace, and chemical engineering, Introduction to Convective Heat Transfer is also an indispensable resource for practicing engineers in academia and industry in the mechanical, aerospace, and chemical engineering fields.
Nevzat Onur is Emeritus Professor of Mechanical Engineering at Gazi University. He pursued his undergraduate studies in mechanical engineering at the University of California, Davis, U.S.A, where he received B.S. degree in 1974. He then attended the Tennessee Technological University, Cookeville, U.S.A, completing M.S. and Ph.D. degree in 1976 and 1980. He taught at different universities in Turkey and he retired from Gazi University in 2011. He has over thirty years’ experience in heat transfer research and development. His research interests have mainly been in viscous flow and convection heat transfer. He lives in Ankara, Turkey.
PREFACE
1 FOUNDATIONS OF CONVECTIVE HEAT TRANSFER
1.1. Fundamental concepts
1.2 Coordinate systems
1.3 The continuum and thermodynamic equilibrium concepts
1.4 Velocity and acceleration
1.5 Description of a fluid motion: Eulerian and Lagrangian coordinates and
substantial derivative
1.5.1 Lagrangian approach
1.5.2 Eulerian approach
1.6 Substantial derivative
1.7 Conduction heat transfer
1.8 Fluid flow and heat transfer
1.9 External flow
1.9.1 Velocity boundary layer and Newton’s viscosity relation
1.9.2 Thermal boundary layer
1.10 Internal Flow
1.10.1 Mean velocity
1.10.2 Mean temperature
1.11 Thermal radiation heat transfer
1.12 The Reynolds transport theorem: Time rate of change of an extensive property
of a system expressed in terms of a fixed finite control volume
REFERENCES
PROBLEMS
2 FUNDAMENTAL EQUATIONS OF LAMINAR CONVECTIVE HEAT
TRANSFER
2.1 Introduction
2.2 Integral Formulation
2.2.1 Conservation of mass in integral form
2.2.2 Conservation of linear momentum in integral form
2.2.3 Conservation of energy in integral form
2.3 Differential formulation of conservation equations
2.3.1. Conservation of mass in differential form
2.3.2 Conservation of linear momentum in differential form
2.3.3. Conservation of energy in differential form
REFERENCES
PROBLEMS
3 EQUATIONS OF INCOMPRESSIBLE EXTERNAL LAMINAR BOUNDARY LAYERS
3.1 Introduction
3.2 Laminar momentum transfer
3.3 The momentum boundary layer concept
3.4 The Thermal boundary layer concept
3.5 Summary of Boundary Layer Equations of Steady Laminar Flow
REFERENCES
PROBLEMS
4 INTEGRAL METHODS IN CONVECTIVE HEAT TRANSFER
4.1 Introduction
4.2 Conservation of Mass
4.3 The momentum integral equation
4.4 Alternative form of momentum integral equation
4.5 Momentum integral equation for two-dimensional flow
4.6 Energy integral equation
4.7 Alternative form of energy integral equation
4.8 Energy integral equation for two-dimensional flow
REFERENCES
PROBLEMS
5 DIMENSIONAL ANALYSIS
5.1 Introduction
5.2-Dimensional Analysis
5.2.1-Dimensional homogeneity
5.2.2 Buckingham theorem
5.2.3 Determination of Terms
5.3 Nondimensionalization of basic differential equations
5.4 Dimensionless Numbers
5.5 Correlations of experimental data
REFERENCES
PROBLEMS
6 ONE-DIMENSIONAL SOLUTIONS IN COVECTIVE HEAT TRANSFER
6.1 Introduction
6.2 Couette Flow
6.3 Poiseuille Flow
6.4 Rotating Flows
REFERENCES
PROBLEMS
7 LAMINAR EXTERNAL BOUNDARY LAYERS: MOMENTUM AND HEAT TRANSFER
7.1 Introduction
7.2 Velocity boundary layer over a semi-infinite flat plate: Similarity Solution.
7.3 Momentum transfer over a wedge (Falkner- Skan Wedge Flow): Similarity
solution
7.4 Application of integral methods to momentum transfer problems
7.4.1 Laminar forced flow over a flat plate with uniform velocity
7.4.2 Two-dimensional laminar flow over a surface with pressure gradient
(Variable free stream)
7.5 Viscous incompressible constant property parallel flow over a semi-infinite
flat plate: Similarity solution for uniform wall temperature boundary
condition
7.6 Low Prandtl number viscous incompressible constant property parallel flow
over a semi-infinite flat plate: Similarity solutions for uniform wall temperature
boundary condition
7.7 High Prandtl number viscous incompressible constant property parallel flow
over a semi-infinite flat plate: Similarity solutions for uniform wall temperature
boundary condition
7.8 Viscous incompressible constant property parallel flow over a semi-infinite
flat plate: Similarity solution for uniform heat flux boundary condition
7.9 Viscous incompressible constant property parallel flow over a semi-infinite
flat plate: Similarity solutions for variable wall temperature boundary condition
7.9.1 Superposition principle
7.10 Viscous incompressible constant property flow over a wedge (Falkner-Skan
Wedge Flow): Similarity solution for uniform wall temperature boundary
condition
7.11 Effect of property variation
7.12 Application of integral methods to heat transfer problems
7.12.1 Viscous flow with constant free stream velocity along a semi-infinite
plate under uniform wall temperature: With unheated length or
adiabatic segment
7.12.2 Viscous flow with constant free stream velocity along a semi-infinite
plate with uniform wall heat flux: With unheated starting length
(Adiabatic segment)
7.13 Superposition principle
7.13.1 Superposition principle applied to slug flow over a flat plate: Arbitrary
variation in wall temperature
7.13.2 Superposition principle applied to slug flow over a flat plate: Arbitrary
variation in wall heat flux
7.13.3 Superposition principle applied to viscous flow over a flat plate: Stepwise
variation in wall temperature
7.13.4 Superposition principle applied to viscus flow over a flat plate: Stepwise
variation in surface heat flux
7.14 Viscous flow over a flat plate with arbitrary surface temperature
7.15 Viscous flow over a flat plate with arbitrarily specified heat flux
7.16 One Parameter Integral Method for incompressible two-dimensional laminar
flow heat transfer: Variable and constant
7.17 One Parameter Integral Method for incompressible laminar flow heat
transfer over a constant temperature a body of revolution
REFERENCES
PROBLEMS.
8 LAMINAR INTERNAL FLOW: MOMENTUM AND HEAT TRANSFER
8.1 Introduction
8.2 Momentum transfer
8.2.1 Hydrodynamic considerations in ducts
8.2.2 Fully developed laminar flow in circular tube
8.2.3 Fully developed flow between two infinite parallel plates
8.3 Thermal considerations in ducts
8.4 Heat transfer in entrance region of ducts
8.4.1 Circular pipe: Slug flow heat transfer in entrance region
8.4.1.1 Heat transfer for low Prandtl number fluid flow (slug flow) in the
entrance region of circular tube subjected to constant wall
temperature
8.4.1.2 Heat transfer to low Prandtl number fluid flow (slug flow) in the
entrance region of circular tube subjected to constant heat flux
8.4.1.3 Empirical and theoretical correlations for viscous flow heat transfer in the
entrance region of circular tube.
8.4.2 Parallel plates: Slug flow heat transfer in entrance region
8.4.2.1 Heat transfer to a low Prandtl number fluid (slug flow) in the
entrance region of parallel plates: Both plates are subjected to
constant wall temperatures
8.4.2.2 Heat transfer for low Prandtl number fluid flow (slug flow) in the
entrance region of parallel plates: both plates are subjected to
uniform heat flux.
8.4.2.3 Heat transfer for low Prandtl number fluid flow (slug flow) in the
entrance region of parallel plates: upper plate is insulated while the
lower plate is subjected to constant wall temperature.
8.4.2.4 Heat transfer for low Prandtl number fluid flow (slug flow) in the
entrance region of parallel plates: Upper plate is insulated while the
lower plate is subjected to constant heat flux.
8.4.2.5 Empirical and theoretical correlations for viscous flow heat transfer in the
entrance region of parallel plates.
8.5 Fully developed heat transfer
8.5.1 Circular tube
8.5.1.1 Hydrodynamically fully developed (HFD) and thermally fully
developed (TFD) laminar forced convection heat transfer for slug
flow in a circular pipe subjected to constant wall heat flux
8.5.1.2 Hydrodynamically fully developed (HFD) and thermally fully
developed (TFD) laminar forced convection heat transfer for viscous
flow in a circular tube subjected to constant wall heat flux
8.5.1.3 Hydrodynamically fully developed (HFD) and thermally fully
developed (TFD) laminar forced convection heat transfer for viscous
flow in a circular tube subjected to constant wall temperature
8.5.2 Infinite parallel plates
8.5.2.1 Hydrodynamically fully developed (HFD) and thermally fully
developed (TFD) laminar forced convection heat transfer for viscous
flow between a parallel plate channel. Both plates are subjected to
constant wall heat flux boundary condition
8.6 Heat transfer in thermal entrance region
8.6.1 Circular tube
8.6.1.1 Graetz Problem: Hydrodynamically fully developed (HFD) and
thermally developing flow in circular tube under constant wall
temperature boundary condition
8.6.1.2 The Leveque solution: Uniform wall temperature boundary
condition
8.6.1.3 Graetz Problem: Hydrodynamically fully developed (HFD) and
thermally developing flow in circular tube under uniform wall heat
flux boundary condition
8.6.1.4 Empirical and theoretical correlations for viscous flow in thermal entrance
region of pipe
8.6.2 Two infinite parallel plates
8.6.2.1 Graetz problem: Hydrodynamically fully developed (HFD) and
thermally developing flow between parallel plates subjected to
constant wall temperature
8.6.2.2 Graetz Problem: Hydrodynamically fully developed (HFD) and
thermally developing flow between parallel plates subjected to
constant wall heat flux
8.6.2.3 Empirical and theoretical correlations for viscous flow in thermal entrance
region of parallel plates
8.7 Circular pipe with variable surface temperature distribution in the axial direction
8.8 Circular pipe with variable surface heat flux distribution in the axial direction
8.9 Short tubes
REFERENCES
PROBLEMS
9 TURBULENT FLOWS
9.1 Introduction
9.2 The Reynolds experiment
9.3 Nature of turbulence
9.4 Time averaging and fluctuations
9.5 Isotropic homogeneous turbulence
9.6 Reynolds averaging
9.7 Governing equations of incompressible steady mean turbulent flow
9.8 Turbulent momentum boundary layer equation
9.9 Turbulent energy equation
9.10 Turbulent boundary layer energy equation
9.11 Closure problem of turbulence
9.12 Eddy diffusivity of momentum
9.13 Eddy diffusivity of heat
9.14 Transport equations in cylindrical coordinate system
9.15 Experimental work on the turbulent mean flow
9.15.1 Turbulent flow in pipe: Velocity profiles
9.15.2 Turbulent flow over a flat plate: Velocity profiles
9.16 Transition to turbulent flow
REFERENCES
PROBLEMS
10 TURBULENT EXTERNAL BOUNDARY LAYERS: MOMENTUM AND HEAT TANSFER
10.1 Introduction
10.2 Turbulent momentum boundary layer
10.3 Turbulence models
10.3.1 Zero-equation models
10.4 Turbulent Flow over a flat plate with constant free stream velocity: Couette flow
approximation
10.5 The Universal velocity profile
10.5.1 Three layer ( von Karman ) model for velocity profile
10.5.2 Other velocity models
10.6 Approximate solution by integral method for the turbulent momentum
boundary layer over a flat plate
10.7 Laminar and turbulent boundary layer
10.8 Other eddy diffusivity momentum models
10.9 Turbulent heat transfer
10.10 Analogy between momentum and heat transfer
10.10.1 Reynold’s analogy
10.10.2 Chilton-Colburn analogy
10.10.3 Prandtl-Taylor analogy
10.10.4 Von Karman analogy
10.11 Some other correlations for turbulent flow over a flat plate
10.12 Turbulent Flow along a semi-infinite plate with unheated starting length:
Constant temperature solution
10.13 Flat plate with arbitrarily specified surface temperature
10.14 Constant free stream velocity flow along a flat plate with uniform heat
flux
10.15 Turbulent flow along a semi-infinite plate with arbitrary heat flux
distribution
10.16 Turbulent transition and overall heat transfer
REFERENCES
PROBLEMS
11. TURBULENT INTERNAL FLOW: MOMENTUM AND HEAT TANSFER
11.1 Introduction
11.2 Momentum transfer
11.2.1 Momentum transfer in infinite two parallel plates
11.2.2 Momentum transfer in circular pipe flow
11.3 Fully developed turbulent heat transfer
11.3.1 Thermally and hydrodynamically fully developed turbulent flow between
parallel plates subjected to uniform heat flux
11.3.2 Thermally and hydrodynamically fully developed turbulent flow in a pipe
subjected to uniform heat flux
11.4 Hydrodynamically fully developed thermally developing turbulent heat transfer
11.4.1 Circular duct with uniform wall temperature
11.4.2 Circular duct with uniform wall heat flux
11.5 Analogies for internal flow
11.5.1 Reynold’s analogy
11.5.2 Colburn analogy
11.5.3 Prandtl-Taylor analogy
11.5.4 Von Karman analogy
11.5.5 The analogy of Kadar and Yaglom
11.5.6 The analogy of Yu et al.
11.5.7 Martinelli analogy
11.6 Combined entrance region
11.7 Empirical and theoretical correlations for turbulent flow in channels
11.8 Heat transfer in transitional flow
REFERENCES
PROBLEMS
12 FREE CONVECTION HEAT TRANSFER
12.1 Introduction
12.2 Fundamental equations and dimensionless parameters of free convection
12.3 Scaling in natural convection
12.4 Similarity solution for laminar boundary layer over a for semi-infinite vertical
flat plate
12.4.1 Constant wall temperature
12.4.2 Uniform Heat Flux
12.5 Integral Method (von Karman-Pohlhausen Method): An approximate analysis of
laminar free convection on a vertical plate
12.5.1 Constant wall temperature
12.5.2 Uniform Heat Flux
12.6 Turbulent free convection heat transfer on a vertical plate
12.7 Empirical Correlations for Free Convection
12.7.1 Vertical Plate
12.7.2 Horizontal plate
12.7.3 Inclined plates
12.7.4 Vertical cylinders
12.7.5 Horizontal cylinder
12.7.6 Inclined cylinder
12.7.7 Free convection from vertical cylinders of small diameter
12.8 Free convection within parallel plate channels
12.8.1 Vertical parallel plate channel
12.8.2 Horizontal parallel plate channel
12.8.3 Inclined parallel plate channel
12.9 Rectangular enclosures
12.9.1 Horizontal rectangular enclosure ( )
12.9.2 Vertical rectangular enclosure
12.9.3 Inclined rectangular enclosure
12.10 Horizontal concentric cylinders
12.11 Concentric spheres
12.12 Spheres
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