Bonding Theory for Metals and Alloys -  Frederick E. Wang

Bonding Theory for Metals and Alloys (eBook)

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2005 | 1. Auflage
256 Seiten
Elsevier Science (Verlag)
978-0-08-045973-8 (ISBN)
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Bonding Theory for Metals and Alloys exhorts the potential existence of covalent bonding in metals and alloys. Through the recognition of the covalent bond in coexistence with the 'free' electron band, the book describes and demonstrates how the many experimental observations on metals and alloys can all be reconciled. Subsequently, it shows how the individual view of metals and alloys by physicists, chemists and metallurgists can be unified. The physical phenomena of metals and alloys covered in this book are: Miscibility Gap between two liquid metals; Phase Equilibrium Diagrams; Phenomenon of Melting. Superconductivity; Nitinol; A Metal-Alloy with Memory; Mechanical Properties; Liquid Metal Embrittlement; Superplasticity; Corrosion; The author introduces a new theory based on 'Covalon' conduction, which forms the basis for a new approach to the theory of superconductivity. This new approach not only explains the many observations made on the phenomenon of superconductivity but also makes predictions that have been confirmed.
* Openly recognizes the electrons as the most important and the only factor in understanding metals and alloys
* Proposes 'Covalon' conduction theory, which carries current in covalent bonded pairs
* Investigates phase diagrams both from theoretical and experimental point of view
Bonding Theory for Metals and Alloys exhorts the potential existence of covalent bonding in metals and alloys. Through the recognition of the covalent bond in coexistence with the 'free' electron band, the book describes and demonstrates how the many experimental observations on metals and alloys can all be reconciled. Subsequently, it shows how the individual view of metals and alloys by physicists, chemists and metallurgists can be unified. The physical phenomena of metals and alloys covered in this book are: Miscibility Gap between two liquid metals; Phase Equilibrium Diagrams; Phenomenon of Melting. Superconductivity; Nitinol; A Metal-Alloy with Memory; Mechanical Properties; Liquid Metal Embrittlement; Superplasticity; Corrosion; The author introduces a new theory based on 'Covalon' conduction, which forms the basis for a new approach to the theory of superconductivity. This new approach not only explains the many observations made on the phenomenon of superconductivity but also makes predictions that have been confirmed.* Openly recognizes the electrons as the most important and the only factor in understanding metals and alloys* Proposes "e;Covalon"e; conduction theory, which carries current in covalent bonded pairs* Investigates phase diagrams both from theoretical and experimental point of view

Cover 1
CONTENTS 8
Preface 12
Introduction 14
Bonding Theory for Metals and Alloys 19
BASIC ASSUMPTION 19
ADDITIONAL POINTS TO CONSIDER CONCERNING THE THEORY 20
Miscibility Gap (MG) Between Two Liquid Metals 22
EXPERIMENTAL FACTS AND CONVENTIONAL THEORY 22
UNDERSTANDING OF THE MG BASED ON THE THEORY PROPOSED 23
Phase Equilibrium Diagrams 25
CORRELATION AMONG CONGRUENT-MELTING AB COMPOUNDS 27
THEORETICAL CONSIDERATION 28
Atomic Configuration in the Binary Liquid System 15 28
Effect Due to Difference in Atomic Radius 35
Fluctuation of Atomic Configurations as a Function of Time 38
Liquidus Curve in Terms of Ln( (3, T) 40
Congruent vs. Incongruent-Melting in Terms of Local Configuration 42
EXPERIMENTAL EVIDENCE IN SUPPORT OF THE THEORY 43
AB Compounds with Coordination Number of n = 4 43
AB2 Compounds 43
AB3 Compounds 50
AB4 Compounds 53
AB5 Compounds 55
AB6,AB9,AB 13 Compounds 56
A2B3 Non-Stoichiometric Compounds 56
SUMMARY AND DISCUSSION 57
REFERENCES 60
Phenomenon of Melting 62
BACKGROUND 62
MONOATOMIC MELTING IN TERMS OF MICROSCOPIC ATOMIC CONFIGURATION 63
EQUATION FOR CALCULATING MELTING TEMPERATURE 64
CALCULATED VS. OBSERVED MELTING TEMPERATURE 65
MELTING TEMPERATURE DEPENDENCE ON PRESSURE 67
MELTING TEMPERATURE DEPENDENCE ON IMPURITY 68
SUMMARY AND DISCUSSION 69
More Detailed Accounts of Nb, Ta, vs. Mo, W 70
REFERENCES 77
Superconductivity 78
BACKGROUND 78
The BCS Theory of Superconductivity 79
Experimental Facts on Superconductivity 80
COVALON CONDUCTION THEORY 81
Physical Characteristics of Covalon Conduction 91
Superconducting Mechanism 92
Prediction Based on the 'Covalon Conduction' Theory 96
Nb3Al IN TERMS OF 'COVALON CONDUCTION' 99
COVALON CONDUCTION IN [TCNQ-TTF] 105
SUMMARY AND DISCUSSION 115
REFERENCES 120
NITINOL A Metal-Alloy with Memory
BACKGROUND 122
Cooperative Atomic Shear 124
Absence of Acoustic Emission 127
Ultra Small in Size (Nitinol Crystals) 128
No Shape Change in Nitinol Transition 128
Crystallographic Distortion in Nitinol Transition 128
Second-Order Transition 128
COVALENT BOND IN NITINOL (TiNi) 129
Atomic d-Orbital Contraction for 3-d Transition Elements 131
'Covalent' vs. 'Metallic' Bond in Nitinol 132
Nitinol Transition as a Function of TiNi].x (Mx) Composition 133
Free'Electron Concentration, N(e) vs. Mechanical Property 134
Nitinol Transition in 4-d and 5-d Series of Transition Elements 134
Additional Experimental Evidence Associated with the Nitinol Transition 140
COVALENT BOND (BOSON) Left over right arrow METALLIC BOND (FERMION) 149
Qualitative Agreement 149
Quantitative Agreement 150
ADDITIONAL UNIQUE PROPERTY CHANGES OBSERVED 151
Bending a Wrought Sheet of TiNi 151
Uniaxially stretching a TiNi wire 151
An Anomalous emf Change 152
BAND STRUCTURE OF TiNi (II) and TiNi (III) 154
CONCLUSION AND DISCUSSION 159
REFERENCES 164
Mechanical Properties 166
BACKGROUND 166
GENERAL MECHANICAL PROPERTIES 168
MECHANICAL PROPERTIES IN TERMS OF COVALENT BOND AND 'FREE' ELECTRON BAND 168
Elasticity (Young's, Shear and Bulk Modulus) 171
Yield Stress 172
Plasticity (Ductility) 173
Ultimate Tensile Strength 178
Melting Temperature 179
Boiling Temperature 181
LIQUID METAL EMBRITTLEMENT (LME) 182
Principal Observations in LME 182
Theory vs. Observation 183
SUPERPLASTICITY 186
Superplasticity in Terms of the Phase Diagram 188
CORROSION RESISTANCE 195
FURTHER DISCUSSION 197
REFERENCES 199
Summary of the Bonding Theory 200
BASIC ASSUMPTION 200
CONSTANCY OF THE RATIO, R 201
THE'FREE'ELECTRON BAND 203
THE FORMATION OF Li5B4 COMPOUND ALLOY 204
CURRENT SCIENTIFIC JOURNAL REVIEW SYSTEM 210
REFERENCES 214
PARTING THOUGHT 216
SUBJECT INDEX 218

Introduction


All the things we see and feel, even the air we breathe are altogether known as ‘material.’ Through centuries of scientific investigation we have come to know and understand that all material is composed of atoms and atoms are in turn made up of nucleus and electrons. The number of electrons surrounding the nucleus defined as atomic number dictates the characteristic of that atom. There are more than 100 different types of atoms on earth and they are systematically arranged in Mendeleeve’s chart, or known as the ‘PERIODIC CHART OF THE ATOMS.’

We also know that atoms are held together through electrons in forming material. Our experience convinces us that there are two types of electron bonding: a) strong bonding and b) weak bonding. The weak bonding does not involve direct electron-electron interaction but rather utilizes Van der Waals’ forces or dipole-dipole interaction in forming bonding. The strong bonding, on the other hand, involves direct electron-electron interaction and can be differentiated into three groups: Covalent bonding, Ionic bonding and Metallic bonding.

COVALENT BONDING; involves a pair of electrons with opposite electron spin. The bond (or electron charge distribution) is essentially localized between nearest neighbor atoms that contribute electrons for the bonding. Since these electron pairs follow ‘Bose-Einstein’ statistics, therefore they are known as ‘boson.’ In this case the paired particles do not obey the Pauli Exclusion Principle and many electron pairs in the system may occupy the same energy level.

IONIC BONDING; also involves a pair of electrons with opposite electron spin. However, the bond (or electron charge distribution) is lopsided on one atom. And results in negatively charged atom on one and leaving the other atom positively charged. This creates a negative-positive charge attractive force that binds atoms together. Statistically, these particles are also ‘Boson.’

METALLIC BONDING; in this bonding, electrons are not paired and are quasi-free to roam throughout the system. Because of unpaired electron spin, they follow the ‘Fermi-Dirac’ statistics and consequently obeying the Pauli Exclusion Principle. Therefore they are known as ‘fermions’ where no two electrons can occupy the same energy level and results in an energy band. The three distinct type of bonding as described above is too abstract and difficult to follow without a Quantum-Mechanical upbringing. The understanding of these bonding may be enhanced by an illustration through an imaginary ‘dog show’ as follows.

Let us imagine that there is a dog-show to be held and people coming to the show are all exactly identical to one another in all respect. These persons are to be known as nucleus (or nuclei as you prefer). Each person is allowed to bring three dogs, which are to be called ‘electron’. Naturally, the dogs (electrons) are all identical to one another and will be on a leash. The leash will be known as ‘atomic orbital’ and be held firmly by each nucleus. As long as the nucleus holds tightly on the leash the dogs (electrons) will not run away. This unit, namely the nucleus (person) and electrons (dogs) will be known as an atom. Now, as the atoms with their nuclei and their dogs (electrons) come close to one another heading to the dog-show, the dogs (electrons) from different nuclei will be barking (interact) at one another – the closer they are, the more vigorous will be the barking (interaction). Ultimately the atoms are hurdled into the space where the dog-show is to take place and the atoms come so close to one another that the dogs (electrons) not only would bark at one another but also would actually chase one another. With this picture in mind we can now illustrate the three distinct types of bonding in the following way:

Covalent Bond: a pair of dogs (electron), each comes from two adjacent nuclei (person), chase one another in a round-and-round way so that their leashes are twisted together (Fig. 1). As long as the person (nucleus) continues to hold onto their leash the two adjacent nuclei are tied (bonded) to one another through the twisted leash and the pair of dogs (electron). This is the picture of covalent bond and otherwise known as linear-combination-of-atomic-orbital (LCAO).

Fig. 1 Conceptual illustration of ‘covalent bond’ by picturing atoms to consist of boys as nuclei and dogs as electrons. Two dogs (electrons) forming a pair-bond between two atoms (boys).

Ionic Bond: it involves also a pair of dogs (electron) from two adjacent nuclei (persons) and having their leashes twisted together in the same way. The one big difference is that there are two distinct nuclei (persons) instead of identical nuclei (people). For example, a man-nucleus and a woman-nucleus and assume the man-nucleus is stronger than the woman-nucleus. The formation of a twisted pair of electron (dog) between man-woman-pair of adjacent nuclei will take place much in the same manner as in all identical nuclei. However, in this case the weaker woman-nucleus may let go the leash and results in paired electron (dog) being pulled to the man-nucleus side (Fig. 2). This results in man-nucleus with an extra electron (dog) while woman-nucleus short of one electron (dog). Thus, there is no direct leash tie to hold man-woman-nuclei pair together. Flowever, the woman-nucleus would not leave because she sees her dog (electron) being held by the man-nucleus and cannot leave. Thus, the formation of positive-negative charged ionic bonded pair. It should be stressed therefore the ionic bond formation requires two distinct types of nuclei.

Fig. 2 Similar conceptual illustration as in Fig. 1 except this time nuclei are dissimilar (a boy and a girl) such that the weaker nucleus (in this case, a girl) cannot hold the lease and results in an ‘ionic bond’.

Metallic Bond: here we assume that each nucleus (person) is already leash-tied (covalent-bonded) to its two neighbors through leash-twisted pair of dogs (electrons) and therefore is hands-full. Under this circumstance the nucleus may not be able to hold onto the leash holding the remaining electron (dog) such that the electron (dog) may pull away from the nucleus (person) and become free to roam within the building confine. These dogs (electrons) running free are the so-called quasi-free electrons. The total number of dogs (electrons) vs. total number of people (nuclei) within the building remains the same with free-roaming dogs (electrons) providing cohesive attractive force to hold the dog-show attendants together.

Within these understanding, some specific feature of each bonding can be described. Covalent bond involves two and only two electrons. The nuclei that contribute electrons in forming the bond may or may not be the same type of atoms. Inasmuch as the bond is directly tied to the leash held by the nucleus the bond is necessarily directional and very strong and confined to the space between the two nuclei forming the bond. Since the bond requires a tight grip of the leash by the nucleus, the number of bonds can be formed by a given nucleus is therefore limited according to the strength or available atomic orbital of the nucleus.

Similarly, Ionic bond also involves electron pair but because the weaker nucleus gives up the leash entirely the bonding is not as strongly directional as well as in strength as in Covalent bond. Because the bonding is electrostatic in nature the bonding forces may involve not only the nearest neighbors but also the second, third, fourth and even higher order of neighboring attractive and repulsive forces and known as Madelung energy. Metallic bond involves all quasi-free electrons that are running free among nuclei and within the confine of the space. Therefore the bonding is totally non-directional and delocalized. They are considered as weak bonds. Due to the dynamic nature of these electrons they are treated as waves traveling in a space of periodically placed positively charged nuclei. These waves are known as Bloch-wave function. The periodic nature of nuclei distribution creates Brillouin zone boundary, which interact with the traveling Bloch waves. The bond created in this manner is found mostly in metallic elements and contributes to the conduction of electricity.

With the characteristic of each bonding type identified, we shall now show how all the material in this universe can be assigned to a particular type of bonding or a combination of bonding type as summarized in Fig. 3.

Fig. 3 Schematic representation of the relationship among the three bonding type.

In Fig. 3, a solid line ties covalent bond and ionic bond to another. This is to show that both the covalently bonded and the ionic bonded electrons are both ‘bosons.’ And quantum-mechanically they are equivalent to one another. At two extremity, i.e., 100% of covalent bond can be represented by a material known as diamond, whereas 100% of ionic bond can be represented by a material known as table-salt, Na(+)C1(-). All the organic and inorganic material in this universe can be assigned between these two extremities. The difference, from one material to another, lies only in terms of the percentage of covalency or ionicity.

It is clear that ionic bonded material is an insulator and metallic bonded...

Erscheint lt. Verlag 30.9.2005
Sprache englisch
Themenwelt Sachbuch/Ratgeber
Naturwissenschaften Chemie Analytische Chemie
Naturwissenschaften Chemie Physikalische Chemie
Naturwissenschaften Physik / Astronomie
Technik
ISBN-10 0-08-045973-0 / 0080459730
ISBN-13 978-0-08-045973-8 / 9780080459738
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