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"Shape-Memory Polymers". In: Encyclopedia of Polymer Science and Technology
SHAPE-MEMORY POLYMERS
Introduction
Besides finding high performance materials, material scientists concentrate on
designing “intelligent” and “self-repairing materials.” In this context, materials
showing a thermally induced shape-memory effect, such as metallic alloys or gels,
have been studied intensively, and a class of polymers showing shape-memory
behavior has found growing interest (1–5). The relatively easy manufacturing
and programming of shape-memory polymers makes these materials a cheap and
efficient alternative to well-established metallic alloys. These polymers usually
surpass by far the recovery properties of shape-memory alloys, which can recover
deformations of 8% at maximum. Taking into consideration the importance of
polymeric materials in daily life, a very broad spectrum of possible applications for
intelligent polymers opens up, covering an area from minimally invasive surgery
to high performance textiles, and to self-repairing plastic components in all kinds
of technical devices.
Stimuli-sensitive implant materials have a high potential for applications
in minimally invasive surgery. Degradable implants could be inserted into the
human body in a compressed (temporary) shape through a small incision where
they obtain their shape relevant for the specific application after warming up to
body temperature. After a defined time period the implant is degraded. In this
case subsequent surgery to remove the implant is not necessary. For applica-
tions in biomedicine, it is necessary to have tailor-made shape-memory polymers
whose thermal, mechanical, or degradation properties can be varied over a wide
range. A substantially new development in this context is polymer systems. These
are families of polymers in which macroscopic properties can be controlled by a
125
Encyclopedia of Polymer Science and Technology. Copyright John Wiley & Sons, Inc. All rights reserved.
126 SHAPE-MEMORY POLYMERS
Vol. 4
specific variation of molecular parameters. In this way shape-memory polymers
having a specific combination of properties required for specific applications
can be obtained by slight variation of the molecular structure and chemical
composition.
Definitions of Shape-Memory Polymer and Related Technical Terms
Shape-memory polymers are stimuli-responsive materials. Upon application of an
external stimulus they have the ability to change their shape. A change in shape
initiated by a change in temperature is called
thermally induced shape-memory
effect
. The shape-memory effect results from the polymer’s structure, that is, its
morphology in combination with a certain processing and programming technol-
ogy. Therefore, shape-memory behavior can be observed for several polymers that
may differ significantly in their chemical composition.
The process of programming and recovering the shape of a polymer is shown
schematically in Figure 1. The polymer is processed into its permanent shape
by conventional methods. Afterwards, it is deformed and the desired temporary
shape is fixed. The latter process is called programming. The programming pro-
cess consists of heating the sample, deforming and cooling the sample, or drawing
the sample at a low temperature (“cold drawing”). The permanent shape is now
stored while the sample is in the temporary shape. Heating the programmed
polymer above a temperature higher than the transition temperature
T
trans
re-
sults in activating the shape-memory effect. As a consequence, the recovery of the
memorized, permanent shape can be observed. Cooling of the polymer below the
transition temperature leads to solidification of the material. However, the poly-
mer sample does not return to its temporary shape. The described effect is called
a
“one-way” shape-memory effect
. The programming process including a mechan-
ical deformation can be repeated. The new temporary shape is not necessarily
Fig. 1.
Schematic demonstration of the thermally induced one-way shape-memory effect.
By the programming process the permanent shape is transferred to the temporary shape.
Heating up of the sample to a temperature above the switching transition
T
trans
initiates
the recovery of the permanent shape. From Ref. 2.
Vol. 4
SHAPE-MEMORY POLYMERS 127
Fig. 2.
The series of photos demonstrates (top–down) the transition from the temporary
shape (spiral) to the permanent shape (rod) for a shape-memory network that has been
synthesized of poly(
ε
-caprolactone)dimethacrylate and butylacrylate (comonomer content:
50 wt%). The switching temperature of this polymer is 46
◦
C. The recovery process takes
35 s when heated up to 70
◦
C.
supposed to match the temporary shape resulting from the former programming
process.
In Figure 2, a photo sequence demonstrates impressively the perfor-
mance of shape-memory polymers. The permanent shape of the polymer
sample is that of a rod. This rod has been deformed to a spiral (tempo-
rary shape) during the programming process. Under the influence of hot air
having a temperature of 70
◦
C the permanent shape is recovered as soon as
128 SHAPE-MEMORY POLYMERS
Vol. 4
the switching temperature
T
trans
is reached. With optimized programming con-
ditions the permanent shape can be recovered with an accuracy of more than
99% (1).
Molecular Mechanism of the Shape-Memory Effect
All shape-memory polymers discussed henceforth are
elastomers
. On the molecu-
lar level they represent polymer networks consisting of segment chains that are
connected by netpoints. The netpoints can be formed by entanglements of the
polymer chains or intermolecular interaction of certain polymer blocks. These
cross-links are called
physical netpoints
. Cross-links in the form of covalent bonds
form
chemical netpoints
. An elastomer exhibits a shape-memory functionality if
the material can be stabilized in the deformed state in a temperature range that is
relevant for the particular application. This can be achieved by using the network
chains as a kind of molecular switch. For this purpose, it should be possible to
limit the flexibility of the segments as a function of the temperature. This process
is supposed to be reversible. The ability to incorporate a control function into the
material provides a thermal transition
T
trans
of the network chains in the tem-
perature range of interest for the particular application. At temperatures above
T
trans
the chain segments are flexible, whereas the flexibility of the chains below
this thermal transition is at least partly limited. In the case of a transition from
the rubber-elastic, ie viscous, to the glassy state the flexibility of the entire seg-
ment is limited. The molecular mechanism of programming the temporary and
recovering the permanent shape is demonstrated schematically in Figure 3 for
a linear multiblock copolymer as an example of a thermoplastic shape-memory
polymer with a crystalline hard segment.
Fig. 3.
Schematic demonstration of the molecular mechanism of the thermally induced
shape-memory effect for a multiblock copolymer,
T
trans
=
T
m
. If the rise in temperature
is higher than
T
trans
of the switching segments, these segments are flexible (marked red,
here) and the polymer can be deformed elastically. The temporary shape is fixed by cooling
down below
T
trans
(marked blue, here). If the polymer is heated up again the permanent
shape is recovered.
Vol. 4
SHAPE-MEMORY POLYMERS 129
Table 1. Possible Combinations of Hard-Segment- and
Switching-Segment-Determining Blocks in Linear, Thermoplastic Block
Copolymers with Thermally Induced Shape-Memory Effect
a
Hard-segment-
Switching-segment-
Phase-separated
determining
determining
block copolymers
Thermal transition
block (Block A )
block (Block B)
Possible
determining the
Highest
Second
Highest
Second
switching
permanent shape
thermal
thermal
thermal
thermal
transitions
at
T
perm
transition transition transition transition
T
perm
T
trans
Melting point
T
m
,
A
T
g
,
A
T
m
,
B
T
g
,
B
T
m
,
A
T
m
,
B
,
T
g
,
A
,
T
g
,
B
T
perm
=
T
m
,
A
T
m
,
A
T
g
,
A
T
m
,
B
T
g
,
B
T
m
,
A
T
m
,
B
,
T
g
,
mix
T
m
,
A
T
g
,
A
T
g
,
B
T
m
,
A
T
g
,
A
,
T
g
,
B
T
m
,
A
T
g
,
A
T
g
,
B
T
m
,
A
T
g
,
mix
Glass transition
T
g
,
A
T
m
,
B
T
g
,
B
T
g
,
A
T
m
,
B
,
T
g
,
B
(
T
perm
=
T
g
,
A
)
T
g
,
A
T
m
,
B
T
g
,
B
T
g
,
A
T
m
,
B
,
T
g
,
mix
T
g
,
A
T
g
,
B
T
g
,
A
T
g
,
B
a
Ref. 2.
T
perm
, and on the
other hand the fixation determining the permanent shape. The materials are di-
vided into two categories according to the thermal transition of the particular
switching segment the shape-memory effect is based on. Either the transition
temperature
T
trans
is a melting temperature
T
m
or a glass-transition temperature
T
g
. In case of a melting temperature one observes a relatively sharp transition
in most cases, whereas glass transitions always extend over a broad tempera-
ture interval. In case there is no sufficient phase separation between the “hard-
segment-determining” block (Block A) and the “switching-segment-determining”
block (Block B), mixed glass-transition temperatures
T
g
,
mix
between the glass
transiton of the “hard-segment- and the switching-segment-determining” blocks
may occur. Mixed glass-transition temperatures are also qualified to act as
switching transitions for the thermally induced shape-memory effect. Table 1
gives an overview about possible combinations of “hard-segment- and switching-
segment-determining” blocks in linear, thermoplastic shape-memory polymers
(2).
<
In chemically cross-linked shape-memory networks the permanent shape
is stabilized by the covalent netpoints. In analogy to linear block copolymers
with shape-memory, the temporary shape of covalently cross-linked shape-
memory networks can be fixed either by crystallizable segment chains or by
a glass transition of the segment chains that is in the temperature range of
interest.
The mechanism of the thermally induced shape-memory effect of linear block
copolymers is based on the formation of a phase-separated morphology with one
phase acting as molecular switch. The phase showing the highest thermal tran-
sition
T
perm
is by the formation of physical netpoints, on the one hand provid-
ing the mechanical strength of the material, especially at
T
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