Fullerenes and related nanostructures
10.5.3 Fullerenes and related nanostructures
In the mid-1980s, research on vaporized carbon led to the discovery of the C 60 molecule, the third and
a novel form of pure carbon. The C 60 molecule has 60 carbon atoms forming a truncated icosahedron shell structure known as buckminsterfullerene (Figure 10.18). Fullerenes larger than C 60 , such as C 70 and molecules containing more than 200 C atoms, have also been found to exist. A related class of
538 Physical Metallurgy and Advanced Materials
Figure 10.18 Various fullerene-based structures ( from Inagaki, 2000).
important nanomaterials, known as carbon nanotubes (CNTs), is illustrated in Figure 10.19. CNTs can be imagined to be formed by rolling up a graphene sheet of carbon atoms arranged in a 2-D hexagonal honeycomb lattice. To form a CNT, a hoop vector, called the chiral vector, is first chosen to connect (0,0) and (m,n) in Figure 10.19d, and the tube is formed by rolling up the graphene sheet with this chiral vector forming a closed circle on the circumference of the tube. The chiral vector (m,n) thus defines the diameter as well as the structure of the tube; for example, an armchair configuration (Figure 10.19a) has a chiral vector (m,m) and a zigzag configuration (Figure 10.19b) (m,0) or (0,n).
Another commonly used measure for the chirality is the chiral angle θ, which is the angle the chiral vector makes with the zigzag orientation on the graphene sheet. Thus, a zigzag tube has θ =0 ◦ and an armchair tube has θ = 30 ◦ , and a general chiral structure (Figure 10.19c) has a θ between 0 ◦ and
30 ◦ . Apart from the single-wall architecture in Figure 10.19, multi-walled CNTs also exist in which multiple graphene layers are rolled up to form an assembly of concentric tubes. CNTs can be fabricated using a range of methods. In laser ablation, an intense pulsed laser beam is incident on a target of graphite doped with cobalt or nickel, which act as a catalyst. The target is heated to ∼1200 ◦
C and the laser evaporates carbon from the target to form CNTs, which are carried away by a stream of argon gas and collected by a cooled substrate outside the furnace. In the electric-arc method, a voltage is applied between two graphite electrodes situated in a helium atmosphere. An electric arc forms and carbon atoms are ejected from the anode to the cathode, forming CNTs on the latter. If pure graphite electrodes are used, multi-walled CNTs will be formed, and to produce single- walled CNT, a metallic catalyst needs to be introduced onto the anode. Finally, in the chemical vapor deposition method, a hydrocarbon gas such as methane is decomposed at an elevated temperature. The resultant carbon atoms then form CNTs on a cooled surface containing a metallic catalyst. In all the processes mentioned above, a metallic catalyst in the form of nanopowder is involved. Figure 10.20 shows an in situ experiment in which a CNT was observed to grow by the catalytic action of a trapped
Non-metallics I – Ceramics, glass, glass-ceramics 539
(1,1) (2,1) (3,1) (4,1) (5,1) (6,1) (7,1) (8,1) (9,1) (10,1) (2,2) (3,2) (4,2) (5,2) (6,2) (7,2) (8,2) (9,2) (10,2) a – 1 (3,3) (4,3) (5,3) (6,3) (7,3) (8,3) (9,3) (4,4) (5,4) (6,4) (7,4) (8,4) (9,4) a – 2 (5,5) (6,5) (7,5) (8,5) (5,6) (7,6) (8,6) Armchair
(d)
Figure 10.19 Different forms of single-walled carbon nanotubes: (a) armchair structure, (b) zigzag structure, (c) chiral structure. (d) graphene sheet of carbons.
Ni nanoparticle at its head, during decomposition of methane inside the TEM. The propulsion of the Ni nanoparticle drew out the CNT, as shown in Figure 10.20h. Fullerene-based structures and in particular CNTs are an important class of building block materials for nanotechnology, and more details are given in Chapter 12.
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(h) Figure 10.20 In situ growth of CNT in a TEM. Methane gas is decomposed inside the TEM over a
catalyst consisting of Ni nanoclusters supported on MgAl 2 O 4 . (Helveg and co-workers, 2004).
Parts
» Physical Metallurgy and Advanced Materials
» Interatomic bonding in materials
» Crystal directions and planes
» Crystallization from the melt
» Principles and applications of phase diagrams
» The mechanism of phase changes
» Defect behavior in common crystal structures
» Analytical electron microscopy
» Specialized bombardment techniques
» Differential scanning calorimetry
» Free energy of transformation
» Anelasticity and internal friction
» Influence of ordering on properties
» Anti-ferromagnetism and ferrimagnetism
» Reflection, absorption and transmission effects
» Variation of yield stress with temperature and strain rate
» Dislocation source operation
» Yield points and crystal structure
» Solute–dislocation interaction
» Dislocation locking and temperature
» Influence of grain boundaries on plasticity
» Nucleation and growth of twins
» Development of preferred orientation
» Tresca and von Mises criteria
» General effects of annealing
» Transient and steady-state creep
» Grain boundary contribution to creep
» Creep-resistant alloy design
» Engineering aspects of fatigue
» Structural changes accompanying fatigue
» Crack formation and fatigue failure
» Fatigue at elevated temperatures
» Precipitation hardening of Al–Cu alloys
» Precipitation hardening of Al–Ag alloys
» Mechanisms of precipitation hardening
» Time–temperature–transformation diagrams
» Austenite–pearlite transformation
» Austenite–martensite transformation
» Griffith microcrack criterion
» Cleavage and the ductile–brittle transition
» Factors affecting brittleness of steels
» Hydrogen embrittlement of steels
» Voiding and fracture at elevated temperatures
» Atomistic simulations of defects
» Nickel-based superalloy development
» Basic alloying and heat-treatment features
» Applications of aluminum alloys
» Oxidation at high temperatures
» The coating and modification of surfaces
» Surface coating by vapor deposition
» Surface coating by particle bombardment
» Surface modification with high-energy beams
» Some engineering and commercial ceramics
» Structure and characteristics
» Fullerenes and related nanostructures
» Strength measurement for brittle materials
» Statistical nature and size dependence of strength
» A case study: thermal protection system in space shuttle orbiter
» Introduction and bio-requirements
» Introduction to bone and tissue
» Case consideration of replacement joints
» Biomaterials for heart repair
» Materials for nanotechnology
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