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CARBON NANOSTRUCTURES
The strain e is defined as the amount of stretch AL of the wire per unit length L
AL
L
e = -
(5.4)
where L is the length of the wire before the weight is attached. Hooke’s law says that
the increase in the length of the wire is proportional to the weight at the end of the
wire. More generally, we say stress S is proportional to strain e:
S = Ee
(5.5)
The proportionality constant E = LW/A AL is Young’s modulus, and it is a property
of a given material. It characterizes the elastic flexibility of a material. The larger the
value of Young’s modulus, the less flexible the material. Young’s modulus of steel is
about 30,000 times that of rubber. Carbon nanotubes have Young’s moduli ranging
from 1.28 to 1.8TPa. One terapascal (TPa) is a pressure very close to lo7 times
atmospheric pressure. Young’s modulus of steel is 0.21TPa, which means that
Young’s modulus of carbon nanotubes is almost 10 times that of steel. This would
imply that carbon nanotubes are very stiff and hard to bend. However, this is not
quite true because they are so thin. The deflection D of a cylindrical hollow beam of
length L with a force F on the end and the inner and outer radii of ri and r, , has been
shown to be
FL3
D=-3 EI
where I is the area. moment of inertia given by ll(r: - r:)/4, Since L
.
.
:
wall
thickness of carbon nanotubes is about 0.34nm, rz - rf is very small, somewhat
compensating for the large value of E.
When carbon nanotubes are bent, they are very resilient. They buckle like straws
but do not break, and can be straightened back without any damage. Most materials
fracture on bending because of the presence of defects such as dislocations or grain
boundaries. Because carbon nanotubes have so few defects in the structure of their
walls, this does not occur. Another reason why they do not fracture is that as they are
bent severely, the almost hexagonal carbon rings in the walls change in structure but
do not break. This is a unique result of the fact that the carbon-carbon bonds are sp2
hybrids, and these sp2 bonds can rehybridize as they are bent. The degree of change
and the amount of s-p admixture both depend on the degree of bending of the bonds.
Strength is not the same as stiffness. Young’s modulus is a measure of how stiff or
flexible a material is. Tensile strength is a measure of the amount of stress needed to
pull a material apart. The tensile strength of carbon nanotubes is about 45 billion
pascals. High-strength steel alloys break at about 2 billion pascals. Thus carbon
nanotubes are about 20 times stronger than steel. Nested nanotubes also have
improved mechanical properties, but they are not as good as their single-walled
CARBON NANOSTRUCTURES
The strain e is defined as the amount of stretch AL of the wire per unit length L
AL
L
e = -
(5.4)
where L is the length of the wire before the weight is attached. Hooke’s law says that
the increase in the length of the wire is proportional to the weight at the end of the
wire. More generally, we say stress S is proportional to strain e:
S = Ee
(5.5)
The proportionality constant E = LW/A AL is Young’s modulus, and it is a property
of a given material. It characterizes the elastic flexibility of a material. The larger the
value of Young’s modulus, the less flexible the material. Young’s modulus of steel is
about 30,000 times that of rubber. Carbon nanotubes have Young’s moduli ranging
from 1.28 to 1.8TPa. One terapascal (TPa) is a pressure very close to lo7 times
atmospheric pressure. Young’s modulus of steel is 0.21TPa, which means that
Young’s modulus of carbon nanotubes is almost 10 times that of steel. This would
imply that carbon nanotubes are very stiff and hard to bend. However, this is not
quite true because they are so thin. The deflection D of a cylindrical hollow beam of
length L with a force F on the end and the inner and outer radii of ri and r, , has been
shown to be
FL3
D=-3 EI
where I is the area. moment of inertia given by ll(r: - r:)/4, Since L
.
.
:
wall
thickness of carbon nanotubes is about 0.34nm, rz - rf is very small, somewhat
compensating for the large value of E.
When carbon nanotubes are bent, they are very resilient. They buckle like straws
but do not break, and can be straightened back without any damage. Most materials
fracture on bending because of the presence of defects such as dislocations or grain
boundaries. Because carbon nanotubes have so few defects in the structure of their
walls, this does not occur. Another reason why they do not fracture is that as they are
bent severely, the almost hexagonal carbon rings in the walls change in structure but
do not break. This is a unique result of the fact that the carbon-carbon bonds are sp2
hybrids, and these sp2 bonds can rehybridize as they are bent. The degree of change
and the amount of s-p admixture both depend on the degree of bending of the bonds.
Strength is not the same as stiffness. Young’s modulus is a measure of how stiff or
flexible a material is. Tensile strength is a measure of the amount of stress needed to
pull a material apart. The tensile strength of carbon nanotubes is about 45 billion
pascals. High-strength steel alloys break at about 2 billion pascals. Thus carbon
nanotubes are about 20 times stronger than steel. Nested nanotubes also have
improved mechanical properties, but they are not as good as their single-walled