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Mimicking Biocomposites with Cellulose Whiskers: A Study on Polymer Nanocomposites, Notas de estudo de Engenharia Elétrica

A research study conducted by favier, chanzy, and cavaille at the centre de recherches sur les macromolecules in grenoble, france. The researchers attempted to mimic biocomposites by blending cellulose whiskers from tunicates with synthetic polymer latices. The resulting nanocomposites had unique structural and mechanical properties, which were analyzed through various techniques including electron microscopy and electron diffraction.

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Macromolecules
1996,28,
6365-6367
6365
Polymer
Nanocomposites Reinforced
by
Cellulose
Whiskers
V.
Favier,
H.
Chanzy,*
and
J.
Y.
Cavaille*
Centre de Recherches sur les Macromolkcules Vkgktales,
CNRS and Universitk Joseph Fourier,
BP
53,
38041 Grenoble Cedex 09, France
Received April
7,
1995
Revised Manuscript Received June
20,
1995
There are numerous examples where animals or
plants synthesize extracellular high-performance skel-
etal biocomposites consisting of a matrix reinforced by
fibrous biopolymers.
lw3
Cellulose is a classical example
of these reinforcing elements which occur as whiskerlike
microfibrils that are biosynthesized and deposited in a
continuous fa~hion.~-~ In many cases, this mode of
biogenesis leads
to
crystalline microfibrils that are
almost defect-free, with the consequence of axial physi-
cal properties approaching those of perfect crystals. In
the present study, we have attempted
to
mimic biocom-
posites by blending cellulose whiskers from the mantles
of tunicates with synthetic polymer latices. The films
cast from such mixtures had a nanocomposite organiza-
tion whose structure and mechanical properties are
described in the present paper.
A batch of edible-grade tunicate
Microcosmus
fulca-
tus,
from the Mediterranean, was obtained from a local
fish shop. These sea animals had an overall diameter
between
5
and 10 cm with a
1
cm thick cellulose tunic.
After anesthetizing with chloroform, the animals were
gutted and their tunic was cut into small fragments that
were deproteinized by three successive bleaching treat-
ments, following the method of Wise
et
a1.6
The
bleached mantles (the "tunicin") were then disintegrated
in water, first with a Waring blender (at a concentration
of
5%
by weight) and then with
15
passes through a
Gaulin laboratory homogenizer operated at 400 bar (at
a concentration
of
1%
by weight). The resulting aqueous
tunicin suspension was mixed with HzSO4 to reach a
final acidwater concentration
of
55%
weight fraction.
Hydrolysis conditions were
60
"C
for 20 min under
strong stirring. A dispersion of cellulose whiskers
resulted. After sonication, the suspension was neutral-
ized and washed by dialysis. It did not sediment
or
flocculate as a consequence of surface sulfate groups
created during the sulfuric acid treatment.' When
concentrated by evaporation, the suspensions displayed
typical liquid crystal characteristics.8
The suspensions
of
cellulose whiskers were homoge-
neously mixed with polymer latices
(Tg
=
0
"C) resulting
from the copolymerization of styrene
(35%
wlw), butyl
acrylate
(65%
w/w), and a small amount
of
acrylic acid.
The suspensions were poured into poly(tetrafluor0eth-
ylene) molds and allowed to dry slowly for
1
month at
room temperature. Homogeneous and bubble-free 2
mm
thick films resulted. These films, cut into strips
35
mm
long and
6
mm wide, were analyzed with a DMTA
Metravib SA Mecanalyseur operating with a forced
oscillation pendulum. The experiments were achieved
at a fixed frequency
of
0.1 Hz and in a temperature
range
200-500
K.
Electron microscopy and electron diffraction analysis
on cellulose whiskers was achieved with a Philips
EM400T operated at 120 kV.
For
this, cellulose whisker
suspensions were deposited on carbon-coated grids and
observed under low-dose conditions, using a 20 pm
0024-9297/95/2228-6365$09.00/0
objective aperture that gave bright-field diffraction
contrast images. Microdiffraction on individual cel-
lulose whiskers was performed by the diffraction method
of Riecke and Ruska9 with
a
probe of
50
nm that
required a C2 condenser aperture of
5
pm. Observations
on the reinforced films were made on ultrathin sections
obtained by cryosectioning. These sections were ob-
served in bright-field diffraction contrast with a Philips
CM200 CRY0 operated at 200 kV and equipped with a
15 pm objective aperture. The images obtained under
low-dose conditions revealed (in black) the cellulose
crystallites within the clear polymer matrix.
An
image
of the latex particles was made under low-dose condi-
tions by depositing drops of latex suspensions on carbon-
coated grids.
A typical preparation of tunicin crystals is shown in
Figure 1A. This sample consists of parallelepiped rods
with lengths ranging from 100'nm
to
several microme-
ters for widths on the order of 10-20 nm. Upon testing
by a microelectron diffraction technique (inset), each
element gave a spot difiactogram that corresponded
to
a section of the reciprocal lattice of cellulose
I@
(here
the
a*c*
section) and persisted when the electron probe
was scanned along a given rod. As the diffractogram
indicated that the cellulose chain axis is along the long
dimension of the rods, each rod
is
therefore a whisker-
like tunicin crystal with no apparent defect. Figure
1B
is a low-dose image of the latex particles that were used
in this study. Each particle has a diameter of around
150 nm. Some
of
these particles are individual and have
kept their initial spherical shapes. Most
of
them,
however, are coalesced together due
to
the conditions
of
sample preparation, viz., room temperature which is
20
K
above the
Tg
of the latex.
Figure 2 corresponds
to
an
ultrathin cry0 cross section
of
a nanocomposite film containing
6%
(w/w) of tunicin
within the latex. In this image, recorded under low-
dose and diffraction contrast conditions, the cellulose
crystals are in black within the clear polymer matrix.
This image reveals that the cellulose whiskers are
distributed throughout the structure, without segrega-
tion or association.
When reinforced by a small percentage of tunicin
whiskers, the polymer films showed improved mechan-
ical properties which were particularly striking when
the films were heated above the glass transition
of
the
polymer. This is illustrated in Figure
3,
where part A
shows a plot of the shear modulus
G
as a function of
temperature for various whiskerflatex compositions
ranging from
0
to 14% (wlw). The curve corresponding
to the pure matrix is typical for a thermoplastic: below
Tg,
G
remained constant at around
1
GPa and dropped
rapidly to
1
MPa during the crossing of the glass-
rubber transition temperature. Above this temperature,
it
behaved as a viscous liquid, with
G
decreasing rapidly
with increasing temperature. The films that contained
cellulose whiskers had a slight increase in their
G
value
below
Tg,
but the drop in
G
value above
Tg
was
dramatically reduced: only from
1
to
0.1 GPa for a film
reinforced by
6%
(wlw) whiskers. Above
Tg,
the rein-
forced films behaved
as
rubbers as their
G
value stayed
constant over a wide temperature range. This is il-
lustrated in Figure 3B that corresponds
to
a film
reinforced by 6% (w/w) whiskers for which
G
keeps a
value of 0.1 GPa all the way
to
500
K,
a temperature at
which cellulose starts to decompose.
The variation of the shear modulus
G,
taken at 325
K
(Le.,
50
K
above
Tg)
as a function of the whisker
0
1995 American Chemical Society
pf3

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Macromolecules 1996,28, 6365-6367 6365

Polymer Nanocomposites Reinforced by

Cellulose Whiskers

V. Favier, H. Chanzy,* and J. Y. Cavaille*

Centre de Recherches sur les Macromolkcules Vkgktales, CNRS and Universitk Joseph Fourier, BP 53, 38041 Grenoble Cedex 09, France

Received April 7, 1995 Revised Manuscript Received June 20, 1995

There are numerous examples where animals or plants synthesize extracellular high-performance skel- etal biocomposites consisting of a matrix reinforced by fibrous biopolymers. lw3 Cellulose is a classical example of these reinforcing elements which occur as whiskerlike microfibrils that are biosynthesized and deposited in a continuous f a ~ h i o n. ~ - ~In many cases, this mode of

biogenesis leads t o crystalline microfibrils that are

almost defect-free, with the consequence of axial physi- cal properties approaching those of perfect crystals. In the present study, we have attempted to mimic biocom- posites by blending cellulose whiskers from the mantles of tunicates with synthetic polymer latices. The films cast from such mixtures had a nanocomposite organiza- tion whose structure and mechanical properties are described in the present paper.

A batch of edible-grade tunicate Microcosmus fulca-

tus, from the Mediterranean, was obtained from a local fish shop. These sea animals had an overall diameter between 5 and 10 cm with a 1 cm thick cellulose tunic. After anesthetizing with chloroform, the animals were gutted and their tunic was cut into small fragments that were deproteinized by three successive bleaching treat-

ments, following the method of Wise et a1.6 The

bleached mantles (the "tunicin") were then disintegrated in water, first with a Waring blender (at a concentration of 5% by weight) and then with 15 passes through a Gaulin laboratory homogenizer operated at 400 bar (at

a concentration of 1%by weight). The resulting aqueous

tunicin suspension was mixed with HzSO4 to reach a

final acidwater concentration of 55% weight fraction.

Hydrolysis conditions were 60 "C for 20 min under

strong stirring. A dispersion of cellulose whiskers resulted. After sonication, the suspension was neutral- ized and washed by dialysis. It did not sediment or flocculate as a consequence of surface sulfate groups created during the sulfuric acid treatment.' When concentrated by evaporation, the suspensions displayed typical liquid crystal characteristics.

The suspensions of cellulose whiskers were homoge-

neously mixed with polymer latices (Tg = 0 "C) resulting

from the copolymerization of styrene (35% wlw), butyl

acrylate (65% w/w), and a small amount of acrylic acid.

The suspensions were poured into poly(tetrafluor0eth- ylene) molds and allowed to dry slowly for 1 month at room temperature. Homogeneous and bubble-free 2 mm thick films resulted. These films, cut into strips 35 mm long and 6 mm wide, were analyzed with a DMTA Metravib SA Mecanalyseur operating with a forced oscillation pendulum. The experiments were achieved at a fixed frequency of 0.1 Hz and in a temperature

range 200-500 K.

Electron microscopy and electron diffraction analysis on cellulose whiskers was achieved with a Philips EM400T operated at 120 kV. For this, cellulose whisker suspensions were deposited on carbon-coated grids and observed under low-dose conditions, using a 20 pm

0024-9297/95/2228-6365$09.00/

objective aperture that gave bright-field diffraction contrast images. Microdiffraction on individual cel- lulose whiskers was performed by the diffraction method

of Riecke and Ruska9 with a probe of 50 nm that

required a C2 condenser aperture of 5 pm. Observations

on the reinforced films were made on ultrathin sections obtained by cryosectioning. These sections were ob- served in bright-field diffraction contrast with a Philips CM200 CRY0 operated at 200 kV and equipped with a 15 pm objective aperture. The images obtained under low-dose conditions revealed (in black) the cellulose crystallites within the clear polymer matrix. An image of the latex particles was made under low-dose condi- tions by depositing drops of latex suspensions on carbon- coated grids. A typical preparation of tunicin crystals is shown in Figure 1A. This sample consists of parallelepiped rods

with lengths ranging from 100'nm to several microme-

ters for widths on the order of 10-20 nm. Upon testing by a microelectron diffraction technique (inset), each element gave a spot difiactogram that corresponded to

a section of the reciprocal lattice of cellulose I@(here

the ac section) and persisted when the electron probe was scanned along a given rod. As the diffractogram indicated that the cellulose chain axis is along the long

dimension of the rods, each rod is therefore a whisker-

like tunicin crystal with no apparent defect. Figure 1B

is a low-dose image of the latex particles that were used in this study. Each particle has a diameter of around

150 nm. Some of these particles are individual and have

kept their initial spherical shapes. Most of them,

however, are coalesced together due to the conditions

of sample preparation, viz., room temperature which is

20 K above the Tg of the latex.

Figure 2 corresponds to an ultrathin cry0 cross section

of a nanocomposite film containing 6% (w/w) of tunicin

within the latex. In this image, recorded under low- dose and diffraction contrast conditions, the cellulose crystals are in black within the clear polymer matrix. This image reveals that the cellulose whiskers are distributed throughout the structure, without segrega- tion or association. When reinforced by a small percentage of tunicin whiskers, the polymer films showed improved mechan- ical properties which were particularly striking when the films were heated above the glass transition of the polymer. This is illustrated in Figure 3, where part A

shows a plot of the shear modulus G as a function of

temperature for various whiskerflatex compositions ranging from 0 to 14% (wlw). The curve corresponding to the pure matrix is typical for a thermoplastic: below

Tg,G remained constant at around 1 GPa and dropped

rapidly to 1 MPa during the crossing of the glass- rubber transition temperature. Above this temperature,

it behaved as a viscous liquid, with G decreasing rapidly

with increasing temperature. The films that contained

cellulose whiskers had a slight increase in their G value

below Tg, but the drop in G value above Tg was

dramatically reduced: only from 1 to 0.1 GPa for a film

reinforced by 6% (wlw) whiskers. Above Tg, the rein-

forced films behaved as rubbers as their G value stayed constant over a wide temperature range. This is il- lustrated in Figure 3B that corresponds to a film reinforced by 6% (w/w) whiskers for which G keeps a

value of 0.1 GPa all the way to 500 K, a temperature at

which cellulose starts to decompose.

The variation of the shear modulus G, taken at 325

K (Le., 50 K above T g ) as a function of the whisker

0 1995 American Chemical Society

8566 Communications to the Editor

u

Figure 1. (A) Electron micrograph of rcdlike cellulose mi- crystals extracted from the mantle of Microcosmus fulcatus. Scale bar: 0.5 pm. Inset: typical electron diffractogram recorded on one microcrystal. oriented with its axis vertically.

The indexation corresponds to the unit cell of cellulose I

defined by Sugiyama et QL** (B) Low-doseimage of the latices

that were used for this work. Scale bar: 0.5 pm.

Figure 2. Low-dose images of a cryosection of a nanomm- posite film consisting of 6% (w/w)tunicin whiskers in a latex as in Figure 1B. The image, recorded under difiaction con- trast bright-field conditions, revealed in black the cellulose whiskers. Scale bar: 0.5 pm.

content, is plotted in Figure 4. The observed values of

G (Figure 4) are much higher than those (dashed line

in Figure 4) predicted from a classical mean-field

mechanical model developed for short-fiber composite.

In such an approach, following Halpin and Kardos," the

modulus and the geometry of the fibers are accounted

for, but one assumes that there is no interaction

between the fibers. In particular, the mean-field model

is based on the concept that a material made of short

fibers, homogeneously dispersed in a continuous matrix,

is mechanically equivalent to a superposition of four

plies. Within each ply, the fibers are parallel to one

another and the mutual orientation of the plies is O",

+45', +go', and -45". The mechanical properties of

each ply are derived from the miemmechanic equations

of Halpin-Tsai."

Macmnwkules, Vd.28, No. 18.

10

Y'

B

6 6 A

  • 200 500 m m T.np IK)

Figure 3. Reinforcement effect as a function of temperatm

below and above the latex T (A) Log of the shear modulus

(Pa)for composites reinforced by weight fractionsof cellulose whiskers from 0 to 14%, as a function of temperature in the

range 200-350 K. (B) As in A but for temperatures up to 500

K and for a specimen reinforeed by 6% (w/w) cellulose whiskers. This specimen is compared with a control sample that does not contain any whisker.

  • 0 **o,oa a 04 0.w om *** rrN.L.nooM

Figure 4. Plot of the log of the shear modulus G (Pa)at 325

K as a function of the volume fraction of cellulose whiskers. Comparison between the experimental (black dots) and cal- culated data with two different mechanical models: a mean- field model (dashed line) and a percolation model (continuous line).

As seen in Figure 4, the mean-field approach is

obviously not able to account for the observed data. In

order to explain the unusually high G values of the

reinforced films, one needs to invoke (i) a strong

interaction between the whiskers and (ii) a percolation

effed. The influence of such an effect on the mechanical

properties of the films can be calculated following the

method of Ouali et aL'* in their adaptation of the

percolation concept to the classical parallel-series model

of Takayanagi et al.I3 The shear modulus of the

composite is then given by the equation:

(1 - 2V + VXJG'&', + (1 - X&G: (1 - X,)G, + aU,- V)G,

G =

where the subscripts s and r refer respectively to the

soft and rigid phases; X is the volume fraction of