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6 • Chapter 1 / Introduction
Density (g/cm
3 ) (logarithmic scale)
40
20
10
8
6
4
2
1.0
0.8
0.6
0.2
0.4
0.1
Metals
Platinum
Silver
Copper
Iron/Steel
Titanium
Aluminum
Magnesium
Composites
GFRC
CFRC
Woods
Polymers
PTFE
PVC
PS
PE
Rubber
ZrO 2
Al 2 O 3
SiC, Si 3 N 4
Glass
Concrete
Ceramics
Figure 1.3
Bar-chart of
room-temperature
density values for
various metals,
ceramics, polymers,
and composite
materials.
Chapter 3), and in comparison to the ceramics and polymers, are relatively dense
(Figure 1.3). With regard to mechanical characteristics, these materials are relatively
stiff (Figure 1.4) and strong (Figure 1.5), yet are ductile (i.e., capable of large amounts
of deformation without fracture), and are resistant to fracture (Figure 1.6), which ac-
counts for their widespread use in structural applications. Metallic materials have
large numbers of nonlocalized electrons; that is, these electrons are not bound to
particular atoms. Many properties of metals are directly attributable to these elec-
trons. For example, metals are extremely good conductors of electricity (Figure 1.7)
and heat, and are not transparent to visible light; a polished metal surface has a lus-
trous appearance. In addition, some of the metals (viz., Fe, Co, and Ni) have desirable
magnetic properties.
Figure 1.8 is a photograph that shows several common and familiar objects that
are made of metallic materials. Furthermore, the types and applications of metals
and their alloys are discussed in Chapter 13.
10
1.0
0.1
100
1000
0.01
0.001
Stiffness [Elastic (or Young’s) Modulus (in units of
gigapascals)] (logarithmic scale)
Composites
GFRC
CFRC
Polymers Woods
PVC
PTFE
PE
Rubbers
PS, Nylon
Metals
Tungsten
Iron/Steel
Aluminum
Magnesium
Titanium
Ceramics
SiC
AI 2 O 3
Si 3 N 4
ZrO 2
Glass
Concrete
Figure 1.4
Bar-chart of
room-temperature
stiffness (i.e., elastic
modulus) values for
various metals,
ceramics, polymers,
and composite
materials.