
Heat Transfer 1
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to its involvement in the field of practice. Being linked to the
management, transport and exchange of energy in thermal form, it
impacts all aspects of human life and activity.
Heat transfers are, by nature, classified as conduction, convection (which
inserts conduction into fluid mechanics) and radiation. The importance
of these three transfer methods has resulted justifiably in a separate
volume being afforded to each of them. This first volume is dedicated to
thermal conduction, and, importantly, assumes an analytical approach to
the problems presented, and recalls the fundamentals.
Heat Transfer 1 combines a basic approach with a deeper understanding
of the discipline and will therefore appeal to a wide audience, from
technician to engineer, from doctoral student to teacher-researcher.
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Rouen, France. He was also Director of the UMR CNRS CORIA, then
Regional Delegate for Research and Technology in Upper Normandy,
France. Specializing in fluid mechanics and transfers, he has worked in
the fields of reactive boundary layers and spraying. Currently retired, he
is an adviser to the Conservatoire National des Arts et Metiers in
Normandy, collaborating with the Institute of Industrial Engineering
Techniques (ITII) in Vernon, France.
Abdelkhalak El Hami is Full Professor of Universities at INSA-RouenNormandie, France. He is the author/co-author of several books and is
responsible for the Chair of mechanics at the Conservatoire National des
Arts et Metiers in Normandy, as well as for several European pedagogical
projects. He is a specialist in problems of optimization and reliability in
multi-physical systems.
Content
Introduction xiii
Chapter 1. The Problem of Thermal Conduction: General Comments 1
1.1. The fundamental problem of thermal conduction 1
1.2. Definitions 2
1.2.1. Temperature, isothermal surface and gradient 2
1.2.2. Flow and density of flow 4
1.3. Relation to thermodynamics 5
1.3.1. Calorimetry 5
1.3.2. The first principle 6
1.3.3. The second principle 6
Chapter 2. The Physics of Conduction 9
2.1. Introduction 9
2.2. Fourier's law 9
2.2.1. Experiment 9
2.2.2. Temperature profile 12
2.2.3. General expression of the Fourier law 14
2.3. Heat equation 16
2.3.1. General problem 16
2.3.2. Mono-dimensional plane problem 18
2.3.3. Case of the axisymmetric system 24
2.3.4. Case of the spherical system 25
2.4. Resolution of a problem 26
2.5. Examples of application 29
2.5.1. Problems involving spherical symmetry 40
Chapter 3. Conduction in a Stationary Regime 53
3.1. Thermal resistance 53
3.1.1. Thermal resistance: plane geometry 53
3.1.2. Thermal resistance: axisymmetric geometry. The case of a cylindrical wall 62
3.1.3. Thermal resistance to convection 65
3.1.4. Critical radius 67
3.2. Examples of the application of thermal resistance in plane geometry 69
3.3. Examples of the application of the thermal resistance in cylindrical geometry 85
3.4. Problem of the critical diameter 92
3.5. Problem with the heat balance 99
Chapter 4. Quasi-stationary Model 103
4.1. We can perform a simplified calculation, adopting the following hypotheses 103
4.2. Method: instantaneous thermal balance 104
4.3. Resolution 106
4.4. Applications for plane systems 107
4.5. Applications for axisymmetric systems 152
Chapter 5. Non-stationary Conduction 183
5.1. Single-dimensional problem 183
5.1.1. Temperature imposed at the interface at instant t = 0 184
5.2. Non-stationary conduction with constant flow density 190
5.3. Temperature imposed on the wall: sinusoidal variation 193
5.4. Problem with two walls stuck together 200
5.5. Application examples 204
5.5.1. Simple applications 204
5.5.2. Some scenes from daily life 213
Chapter 6. Fin Theory: Notions and Examples 237
6.1. Notions regarding the theory of fins 237
6.1.1. Principle of fins 237
6.1.2. Elementary fin theory 238
6.1.3. Parallelepiped fin 242
6.2. Examples of application 249
Appendices 263
Appendix 1. Heat Equation of a Three-dimensional System 265
Appendix 2. Heat Equation: Writing in the Main Coordinate Systems 273
Appendix 3. One-dimensional Heat Equation 283
Appendix 4. Conduction of the Heat in a Non-stationary Regime: Solutions to Classic Problems 291
Appendix 5. Table of erf (x), erfc (x) and ierfc (x) Functions 295
Appendix 6. Complementary Information Regarding Fins 297
Appendix 7. The Laplace Transform 301
Appendix 8. Reminders Regarding Hyperbolic Functions 309
References 313
Index 315
Introduction
I.1. Preamble
Thermal energy was probably first perceived (if not identified) by humanity, through the Sun. The themes of night and day are found at the center of most ancient myths. Humanity's greatest fear was probably that the Sun would not return again in the morning. Fire became controlled in approximately 400,000 BP. Thermal transfer was therefore a companion of Homo ergaster, long before Homo sapiens sapiens.
However, it took a few hundred thousand years before so-called "modern" science was born. Newtonian mechanics dates from three centuries ago. Paradoxically, another century and a half passed by before energy was correctly perceived by scientists, in terms of the new field of thermodynamics. Furthermore, a systematic study of heat transfer mechanisms was carried out at the end of the 19th century, and even later for the study of limit layers, the basis of convection.
Heating, lighting and operating the steam engines of the 19th century were all very prosaic concerns. Yet this is where revolutions in the history of physics began: the explosion of statistical thermodynamics driven by Boltzmann's genius, and quantum mechanics erupted with Planck, again with Boltzmann's invovlement.
Advances in radiation science, particularly in sensor technology, have enabled us to push back our "vision" of the universe by a considerable number of light years. To these advances we owe, in particular, the renewed interest in general relativity that quantum mechanics had slightly eclipsed, through demonstration of black holes, the physics of which may still hold further surprises for us.
Closer to home, fundamental thermal science, whether it is conduction, convection or radiation, contributes to the improvement of our daily lives. This is particularly true in the field of housing where it contributes, under pressure from environmental questions, to the evolution of new concepts such as the active house.
The physics that we describe in this way, and to which we will perhaps introduce some readers, is therefore related both to the pinnacles of knowledge and the banality of our daily lives. Modestly, we will place our ambition in this latter area.
There are numerous heat transfer textbooks in different formats: "handbooks" attempting to be exhaustive are an irreplaceable collection of correlations. High-level courses, at universities or engineering schools, are also quite exhaustive, but they remain demanding for the listener or the reader. Specialist, more empirical thematic manuals are still focused on specialists in spite of all this.
So why do we need another book?
The authors have taught at university level and in prestigious French engineering schools, and have been involved in the training of engineers on block-release courses. This last method of teaching, which has been gaining popularity in recent years, particularly in Europe, incorporates a distinctive feature from an educational point of view. Its practice has, in part, inspired this book.
The aim is to help learners who have not had high-level mathematical training in their first years following the French Baccalaureate (therefore accessible to apprentices), and pupils with more traditional profiles. At the same time, we would like to show this broad audience the very new possibilities in the field of digital processing of complex problems.
When a miner wants to detach a block of coal or precious mineral from a wall, they pick up a pneumatic drill. If we want to construct a tunnel, we must use dynamite. The same is true for physicists.
Whether they are researchers, engineers or simply teachers, scientists have two tools in their hands: a calculator and a computer (with very variable power). Since both authors are teacher researchers, they know they owe everything to the invention of the computer. From the point of view of teaching, however, each one of the two authors has remained specialist, one holding out for the calculator and "back-of-the-napkin" calculations, and the other one using digital calculations.
The revolution that digital tools has generated in the world of "science" and "technical" fields, aside from the context of our daily lives, no longer needs to be proved. We are a "has been" nowadays if we do not talk about Industry 4.0. The "digital divide" is bigger than the social divide, unless it is part of it..
Indeed, the memory of this revolution is now fading. Have students today ever had a "slide rule" in their hands? Do they even know what it is? Yet, all the physicists behind the laws of thermal science had only this tool in hand, giving three significant figures (four with good visibility and tenacity), leaving the user to find the power of ten of the result. It goes without saying that a simple calculation of a reversible adiabatic expansion became an ordeal, which played a part in degrading the already negative image of thermodynamics held by the average student.
This reminder will seem useless to some; slide rules are at best sleeping in drawers. But there is a moral to this story: no matter what type of keyboard we type on, a calculator or a computer, our head must have control over our fingers. This book has been written on the basis of this moral.
A good physicist must have a perfect understanding of the idea of an "order of magnitude". For this, the tool is a calculator. We always do a rough sizing of a project before moving on to detailed modeling and numerical calculations.
The two authors belong to the world of engineering sciences, meaning most of their PhD students have entered the private sector. One of them, having moved into the aerospace sector, came back to see us very surprised by the recurrence of "back-of-the-napkin" calculations in his day-to-day work.
Fundamental or "basic physics" concepts are taken from a type of manual that is resolutely different from those dedicated to the numerical approach. In this case, the authors allow themselves to believe that it is no bad thing to collect them all together in a single book, for once. This is a significant difference that will surprise some and, without doubt, be criticized by others. Nevertheless, when reading this book, an "average" student will be initiated to a field that teaching models generally promised "for later on" (or never if he/she never goes beyond a certain level of education). It is also true that fully immersed in equations and complex calculations, specialist readers will be able to "be refreshed" when faced with the short exercises, which can sometimes surprise and encourage them - why not - to go back to their roots (assuming they had indeed been there).
Another significant difference is that this book is directed at a large scientific audience, which covers possibly the entire field: researchers, PhD students or those who have obtained Confirmation and are just starting out in the field, technicians, students or professionals, engineers. This last type of scientist is perhaps the main target of this book.
So, what is this book for?
Above all, it contains problems to be worked on, of which most are accessible to all, from the level of an apprentice technician upwards, either one or two years after the Baccalaureate. This book was written in France, where scientific teaching is structured around universities, engineering Grandes Écoles, engineering training through apprenticeships and two types of technician training sections at high schools or universities. In countries with simpler models, readers should also find it useful.
It seems necessary to surround these problems with strong reminders of past learning, so that the reader does not need to permanently refer back to their manuals. We see two advantages in this: a presentation of the scientific material focusing on the problems, and a second chance for readers to integrate notions that perhaps had not been well understood in the initial teaching.
Lastly, upon rereading, the authors also recommend this book as an introduction to the taught disciplines.
I.2. Introduction
Thermal science is to thermodynamics as decree means is to law. It answers the following question - which all good leaders must (or should) ask themselves whenever they have an "idea": "How would this work in practice?".
In a way, thermal science "implements" thermodynamics, of which it is a branch.
A thermodynamics specialist is a kind of energy economist. Applying the first principle, they create a "grocery store". With the second principle, they talk about the quality of their products. I add or remove heat from a source or work from a system. And the temperature, among other things, defines the quality of the energy for me.
But by what means do I take or do I give? Even calculations of elementary reversible transformations do not tell us by what process heat passes from a source to a system.
Thermal science specifies how, but "evacuates" the work. If in a given problem related to, for example, a convector where electrical energy (therefore in the "work" category) appears, it is immediately dissipated into heat by the Joule effect.
Three heat transfer modes can be identified: conduction and radiation - which can be seen separately, although they are often paired up - and convection, which is by nature an interaction...
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