Nghiên cứu ảnh hưởng của sự biến đổi bề mặt một số khoáng chất đến tương tác pha và tính chất cơ lý của vật liệu tổ hợp trên cơ sở nhựa nền polypropylen tt tieng anh

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PREFACE
1. Urgency of the thesis
Reinforcement of thermoplastic by using particle has studied in few decades ago. Until now, it
plays an important role in as well [1]. The flexibility of thermoplastic composite materials expands the
scope of application in the life and research field. When the materials are reinforced by fillers, their
properties are changed. Typically, the filler impacts in hardness, thermal conductivity, thermal expansion.
However, they improve strength and elasticity as well because of the filler properties and the changing of
morphology matrix. The inorganic filler are used wide in thermoplastic such as CaCO3, talc, SiO2, mice
and Mg(OH)2.
Most of the researches carried paying attention on the factors such as (i) component; (ii) shape and
size; (iii) composition; (iv) compatibility of matrix and filler. Some of them showed a polymer layer
locating aninteraction phase between filler surface and matrix which have special property. However, the
role, influenceand a parameters relationship ofthe phase interaction betweenthe filler and the matrix on
the mechanical properties (i.e. tensile strength, impact resistance) is not determined clearly.
Thus, supervisor and PhD student carried on a thesis:” Effect of surface fillers modification on
phase interaction and mechanical properties of thermoplastic materials”
2. The aim of thesis
To study relation of molecular structural changing between polypropylene microcomposite system
and the particle fillers with varies phase interactions by using solid-state NMR(ssNMR) spectra.Therein,emphasizing the molecular flexibility on mechanical properties of materials.
3. Main contents of thesis
a. Preparing polypropylene composites materials by using the filler was modified/unmodified
surface at varies contents.
b. Research phase interaction morphology, determine the mechanical properties of materials
including tensile strength and impact resistance (integral J).
c. Application of solid-state nuclear magnetic resonance (ss-NMR) method to determine molecular
mobility in polymer composite materials, study the relation of mechanical properties of material.
Outline of the thesis: The thesis has 24 pages including introduction, 4 chapters of content, contributions
and a list of publication.
The main results of the thesis are published in:
- 01 article in an international journal in the ISI list (IF = 3.7)

- 04 articles in national journal
- 05 reports in the International Science Conference (1 international conference to publish
ISBN)


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Chapter 1: INTRODUCTION
1.1. Thermoplastic polypropylene
Polypropylene (PP) was invented by research groups in the United States and Europe in the early
1950s. The commercial production of PP began in 1957 in the US and in 1958 in Europe. On the other
hand, PP ranks first in the largest volumes group of thermoplastic products used such as: polyethylene
(PE), polyvinylchloride (PVC) and polystyrene (PS). Average consumption of PP increases about 10%
per year and the trend will keep increasing in future.
The flexibility is important property of PP. The structure and characteristics (including processing)
of PP can be adjusted according to usage requirements. Polypropylene has many advantagedproperties
such as low density, chemical resistance, easy processing and recyclability. In addition, its mechanical
properties are well suited to engineering plastics. Besides, PP also has some disadvantages such as
deteriorationin properties at low temperatures and low impact resistance. Thus, PP copolymers and their
blendsare studied to develop in commercial fields.
1.2. Polymer composite materials base on fillers reinforced PP
Fillers reinforced PP composite materials have been used in large quantities in many different
fields such as automotive, furniture, electrical equipment, etc. Because of the relation between cost and
achieved properties, filler reinforced PP composites are used widely and gradually replaced ABS inthe
traditional fields. Other materials like. Many efforts have been made to expand its scope of application in
engineering thermoplastic materials
There are many types of reinforced fillers using in PP, however, CaCO3, talcand fiber glass play the
most important role and will keep it in the near future including. In thermoplastic market, CaCO3
consumptionmakes up a majority of the filler field. However,talc mineral ranks first inthe PP market,
CaCO3 only ranks second and glass fiber follow. Hence, glass fiber reinforced PP is studied to improve its
capabilities and expand its scope of application. In despite of many efforts,they are still potential and

expectant researches. In reality, application and the growth rate of fiber glass for PP are lower than that of
particle fillers.
Nowadays, not only the technical and aesthetic requirements but also the costs of processing and
raw materialsare increasing. To meet these requirements, the researchers need understanding the relevant
properties of fillers as well as their influence on the structure and properties of composite materials touse
all the advantages of fillers or just use them as diluents forreducing costs.
1.3 . Solid state magnetic resonance spectroscopy and its application for molecular mobility in
polypropylene composites
Today, the high-resolution 13 C NMR spectrum is a common tool for studying the structure of
polymers. 1 H-NMR isa standard technique in structural analysis of liquid-state substances, but in solidstate substances. Isotactic polypropylene isa polymorphic material due to a modifying arrangement of
polymer chains. Hence, ss-NMR spectroscopy technique showed complicatedanalysis for
polypropylene.It is more complicated particularlyif the composition of these components that plays a
decisive role changing the properties of polymer is significantly lower than composition of the matrix.
This difference prevents the use calibration curve analysis. Therefore, special method must be used to


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describe the small differences between the amorphous and crystals disordering in the phase interaction
region.
However, the less attention has been paid to the multi-molecular analysis of the ss-NMR spectrum
for amorphous or disordered solids, which can be considered an extreme limit due to the frequency range
being too much for signals for which only one signal is available are defined. Therefore, the thesis also
demonstrates that 13 C MAS ss-NMR spectrocopy is a fast, reliable tool for describing extremely
complex crystal forms in PP material for clarifying the relationship between spectral data at the
molecular level and the macroscopic properties of materials such as mechanical properties.
1.4 . These studies were carriedon in Vietnam
The basic researches in Vietnam on thermoplastic composite materials in general and
polypropylene in particular were studied by Hoang Thai and et al at the Institute of Tropical Technology
and Dieu Tran Vinh and et al at Hanoi University of Technology.
Hoang Thai et al treated titan dioxide or nano BaSO4 surface by silane coupling agent for studying

mechanical properties and morphological structure of titan dioxide or nano BaSO4 filled polypropylene
composites. This surface modification process improved significantly the mechanical properties of
composite materials. Tensile strength and elastic modulus of PP composite materials with 2% of surfacemodified nanoparticles are 42 Mpa and 979 Mpa, respectively. Based on results of the cumulative module
(G ') and phase interaction from X-ray diffraction analysis and FE-SEM, they showed that the properties
and phase interaction of the material containing modified nanoparticle are better than these of the material
containing unmodified nanoparticle. .
Besides, the research team of Prof. Hoang Thai mixed melting polypropylene and vinysilane
modified fly ash particles. The effect of fly ash content on viscosity, mechanical properties and material
morphology was determined. The results indicated that the viscosity of the mixture decreased with
increasing fly ash content. Tensile strength and elongation at break of the material with different loading
of untreated fly ash are lower than the original PP. After modifying by vinyl silane,PP / fly ash composite
material showed higher tensile strength and elongation at break while viscosity of the mixture was lower.
The research team of Prof. Dieu Tran Vinh had many studies on composite materials based organic
fibers reinforced polypropylene . They was considered that the adhesion between the plastic substrate and
polar organic fiber affects incredibly the properties of the composite. Thus, maleic anhydride–
grafted polypropylene (MA-g-PP) compatibilizer or acetic anhydride and acrylonitrile was used.
Comparing the mechanical properties of polypropylene composite materials containing jute fibers and
glass fibers, although tensile strength and elastic modulus of jute were lower than that of fiberglass, the
specific module of jute was higher than glass fiber, and the module cost of jute is much higher than that of
fiberglass. The effect of jute and MAPP on PP tensile and flexural strength were determined. When 50%
weight of jute is loaded, the flexural strength of PP increases from 31.33 Mpa to 49.97 Mpa and increases
sharply to 87.66 Mpa when adding 3% of MAPP weight. Tensile strength does not increase much without
MAPP. However, when MAPP has tensile strength, composites increase about 2 times (from 28.92 MPa
to 59.12 MPa).
Similarly, composite is reinforced with NaOH solution treated short bamboo fiber adding 0.6% of
MAPP compatibilizer, its tensile strength, flexural strength and impact strength are respectively increased
by 24%; 23% and 40% compared with its of raw PP. The team also carried on the acetylation of bamboo


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fibers and determined the effect of this process on the reinforcement of polypropylene based composite
material. Acetylation reduces the hygroscopic of bamboo fibers, increases the adhesion between bamboo
fibers and PP resin. 50% of short bamboo fibers reinforced PP composites has the highest tensile strength
(36.45 MPa), increase of 2% compared with its raw PP.
Chapter 2. EXPERIMENTAL
2.1. Materials
2.1.1. Polymer
Isotactic polypropylene homopolymer Mosten 52.412 (Chemopetrol, Czech Republic) was used
as a matrix in this study.
2.1.2. Fillers
Glass beads, average size ~ 20 µm supplied by SOVITEC, France.
Calcium carbonate, average particle size ~ 1.7 µm (1VA) and ~ 12 µm (15VA), supplied by
Omycarb, Switzerland.
Talc mineral originated from Thanh Son district, Phu Tho province, Vietnam. The main
components of this mineral are SiO2 (60,82 %) and MgO (32,16 %). Average particle size ~ 6,58 µm.
2.1.3. Surface modification agents
Vinyltriethoxysilane
supplied
by
Momentive
(Switzerland)
and
methacryloxy
propyltrimethoxysilane supplied by DowCorning (USA). Oleic and stearic acids (technical grade products
supplied by Sigma-Aldrich) were used for calcium carbonate surface modification.
2.1.4. Other materials
Dicumyl peroxite (technical grade ) supplied by Sigma-Aldrich.
2.2. Methods
2.2.1. Surface modification
The surface modification of filler particles is carried out in 96% ethanol solution containing 2%

of the surface modification agent.
2.2.2. Composite preparation
Polypropylene and fillers were been compounded in the twin-screw compounder (extruder)
Brabender DSE and subsequently injection-molded into form of specimens (dog-bone) by ENGEL Spex
victory 50 machine.
2.3. Properties assessment
2.3.1. Morphology
The morphology was assessed by scanning electron microscope (SEM) taken on impact fracture
cross-section of composites.
2.3.2. Tensile properties
Tensile mechanical tests were carried out on Instron 5800 material tester at room temperature and
cross-head speeds alternating of 1 mm/min and 50 mm/min.


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2.3.3. Impact properties
An instrumented Charpy impact tester Ceast Resil Impactor with 7,5J work capacity was used for
the J-integral evaluation.
2.3.4. ss-NMR
The ss-NMR experiments were performed using a Bruker Avance 500 WB/US NMR (Karlsruhe,
Germany, 2003; B0 ¼ 11.7 T) with 4 mm ZrO2 rotors at a MAS frequency of 6 kHz. The 13C
crosspolarization (CP) MAS NMR spectra were measured with a B1(13C) field nutation frequency of 62.5
kHz, a contact time of 1.75 ms and a recycle delay of 2 s. To record the T1-filtered, domain-selective
spectra of the highly mobile components, the single-pulse 13C MAS NMR spectrawere measured with a
repetition delay of 2 s. The VT experiments were performed in the temperature range from 295 to 355 K.
The frictional heating of the sample was compensated, and the sample temperature was calibrated using
the 207Pb chemical shift in Pb(NO3)2.
2.3.5. Factor analysis (FA)
FA is a method that uses the Singular Value Decomposition (SVD) algorithm to extract specific
information from experimental data. This technique allows visualization and distinguishing subtle

differences between the prepared PP/CaCO3 microcomposites in 2D or 3D maps.
Chapter 3: RESULS AND DISCUSION
3.1. Composite based on polypropylene and glass beads
3.1.1. Morphology observation
The introduction of inorganic filler into a polymer matrix results in a heterogeneous system.
Adhesion among different materials is created by physical or chemical bonds between the adhesive and
the substrate, and this depends on the selection of coupling agent. Figure 3.1 presents structure
morphology taken of the impact fracture cross section of PP/glass beadcomposites with 20% of filler
content.

a)

b)

c)

Fig. 3.1. Degree of interfacial adhesion between glass bead and PP matrix.
As revealed by SEM in the cases of non-treated and NO adhesion, there was a poor interfacial
with the strong debonding of particles. While in case of GOOD adhesion, a strong bonding achieved
between glass bead particles and PP matrix, coated spheres adhere to the matrix.
3.1.2. Tensile properties
The effects of glass bead with different surface properties on the mechanical properties of
composites are showed in Fig. 3.2. It can be sheen that the tensile moduli in all cases of composites


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increase with increasing filler loading. Generally, the addition of rigid particulate fillers increases
stiffness, which is measured through Young's modulus. This is due to the fact that fillers often exhibit
higher stiffness compared matrix polymer. Besides, Young's modulus is measured at the very beginning
of a tensile test, where deformation is insufficient to cause particle-matrix debonding. However, obtained

results indicated slightly change in value among cases of no-treated, NO adhesion and GOOD adhesion.
This comes from the difference in adhesion between particles and polymer matrix with zero adhesion in
case of NO adhesion and a strong adhesion in case of GOOD adhesion. The increasing in Young's
modulus of glass bead-filled composites indicates an increase in the rigidity of PP related to the
restriction of the mobility in PP matrix due to the presence of fillers. This mechanical restraint resulted
from the enhanced surface interaction between two phases in composites. The similar trend also found in
other studies that enhancement of the interfacial adhesion between the matrix and glass beads is helpful in
improving the stiffness of filled PP composites.

Fig. 3.2. Tensile properties of PP/Glass beads composites
For particulate filled thermoplastic composites, it is generally believed that the interfacial
adhesion between the filler particles and matrix is an important factor affecting strength and toughness of
composites. On the other hand, yield stress gives information on filler-matrix interactions and
consequently it is one of the preferred methods of composite testing. In thecase of a poor interaction (nontreated and NO adhesion) between the matrixand the filler, the interfacial layer cannot transferstresswas
reflected by the lower yield stress value in comparison with a strong interaction in case of GOOD
adhesion (Fig. 3.2). Therefore, one can assume that the strengthof a particulate-filled composite is
determined by theeffective available area of load borne by the matrix asa result of the absence of the
filler.
The higher yield stress values in case of GOOD adhesion in comparison with cases of non-treated
and NO adhesion at the corresponding concentration reflect the interaction between glass bead particles
and polypropylene matrix. On the other hand, it can be seen that in all cases, yield stress decreases with
increasing filler loading.This is due to the fact that theconcentration of the inclusions is the main
factoraffecting the yield strength of a filled polymer besidesthe interfacial adhesion between the fillers
and matrix. The presence of glass beads has a weakening effect on the composite due to debonding. Poor
adhesion and debonding reduce the volume fraction which can carry the applied load.Tensile strain at
break is a parameter characterizing the extensibility of materialsand it is usually inversely proportional to
tensile strength which means that increasing the tensile strength of filled material usually contributes to a
decrease in the strain at break. The strain at break value for composite of GOOD adhesion had a lowest
strain at break value which corresponds with highest tensile strength value.

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3.1.3. Impact properties
The J-integral was used to characterize the energy absorption of polymer materials at the initial
stage of crack and the resistance for crack initiation. Figure 3.3 showed Jld values of polypropylene and
glass bead composites.

Fig. 3.3. Impact strength of PP/glass beads composites
The fracture behavior of polymers is strongly affected by the addition of rigid particles. The
incorporation of them into the polypropylene matrix leads to differences in the overall process of crack
propagation and fracture. The process starts with the plastic deformation of the matrix ahead of the initial
crack. The adsorption of polymer molecules on the filler surface through chemical bonds leads to the
rigidity in structure of polymer chains. This leads to earlier crack initiation and propagation with
dramatically decreasing of J-integral value in case of GOOD adhesion (Figure 3.3). Plastic deformation of
the matrix polymer is the main energy absorbing process in impact and this increases when the interaction
between particles and polymer matrix is lowered in case of non-treated and NO adhesion.
3.1.4. ss-NMR
In general, narrowing of 1H lineshapes indicates the increase in global segmental dynamics as 1H1
H dipolar couplings are motionally averaged out. As demonstrated in Figure 3.4 in our particular case,
the most mobile polymers segments were found in parent PP. Slightly hindered segmental dynamics in
the composites Non-treated and NO-adhesion is reflected by the broadening of the corresponding signals.
The most rigid polymer segments were found in the composite GOOD-adhesion that is reflected by the
broadest 1H MAS NMR line


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GOOD-adhesion

Non-treated and

NO adhesion

PP

Fig. 3.4. 1H MAS NMR spectra of the parent PP and composites recorded at 350 K and MAS 6 kHz.
Similar trends were found in the 1H MAS NMR spectra measured with Hahn-echo (Figure 3.5)
that allowed separation of relatively flexible fractions of polymer chains of amorphous phase.

GOOD-adhesion

Non-treated

PP and
NO adhesion

Hình 3.5. 1H MAS Hahn-echo NMR spectra of the parent PP and composites recorded at 350 K and
MAS 6 kHz
In contrast to solid-state 1H NMR spectra it is generally accepted that narrowing of 13C CP/MAS
NMR signals indicates the increase in conformational ordering, and in extreme cases of perfectly evolved
crystal phases very narrow signals are expected. In polypropylene systems presence of polymorphic form
alpha is reflected by the doublet of CH signal at ca. 44 ppm. The doublet is schematically indicated by
dashed lines in Figure 3.6, and evolution of the narrow symmetric doublet requires long term annealing. If
considerable amount of amorphous phase is presented than the expected symmetrical doublet disappears.


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Rather an asymmetric broad line is expected. Such a signal was detected for the parent PP (Figure 3.6).
In contrast, the prepared composites exhibit symmetrization of the doublet and increase in spectral
resolution. This finding can be explained by the conformational ordering occurred particularly in the
composite NO-adhesion (additional crystallization, reorganization of the amorphous phase, formation of

protocrystalline phases etc….).

GOOD-adhesion
Non-treated
NO-adhesion
PP
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Fig. 3.6. C CP/ MAS NMR spectra of the parent PP and composites recorded at 300 K and MAS 6
kHz.
3.3. Composite based on polypropylene and calcium carbonate
3.3.1. Morphology observation
The introduction of inorganic filler into a polymer matrix results in a heterogeneous system.
Adhesion between different materials is created by physical or chemical bonds between the adhesive and
the substrate, and this depends on the selection of coupling agent.
The morphology of the compounds up to concentration of 40 wt% treated and untreated CaCO3
are shown in Figure 3.7 and Figure 3.8. The CaCO3 particles are generally supplied as agglomerates,
however, it can be seen that aggregates are broken up to the primary particles during the extrusion
process. In the case of CaCO3 with average particle size ~ 1.7 µm, the interaction between untreated filler
particles with the polymer matrix is stronger compared with treated filler particles (Figure 1a). The strong
debonding of particles can be observed in cases of treated particles (Figure 3.7-b and 3.7-c).
a

b

c

Figure 3.7. SEM images of morphology of PP filled with a) untreated CaCO3, b) oleic acid
treated CaCO3 and c) stearic acid treated CaCO3, average particle size ~ 1.7 µm, filler content 40 wt%

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Similar trend was found in case of CaCO3 with higher size (12 µm, Figure 2) of filler particles,
filler-matrix interaction in case of treated filler is lower compared with untreated filler.
a

b

c
)

Figure 3.8. SEM images of morphology of PP filled with a) untreated CaCO3, b) oleic acid
treated CaCO3 and c) stearic acid treated CaCO3, average particle size ~12 µm, filler content 40% wt.
3.3.2. Tensile properties
Tensile mechanical properties of composites of PP matrix with calcium carbonate particles were
investigated (Figure 3.9). Generally, the addition of rigid particulate fillers increases stiffness, which is
measured through Young modulus. As can be seen in the figure, all the samples investigated in the
present study show monotonic increasing of Young modulus values. This is due to the fact that fillers
often exhibit higher stiffness compared with polymer matrix. Furthermore, Young modulus is measured at
the very beginning of a tensile test, where deformation is insufficient to cause particle-matrix debonding.
Experimental results also indicated that, Young modulus of composites have none effect by particle size
and surface modification.
Strength and toughness are very important for polymer composites used as structural materials. For
particulate filled thermoplastic composites, it is generally believed that the interfacial adhesion between
the filler particles and matrix is an important factor affecting strength and toughness of composites. As
revealed by SEM, the lower adhesion in case of treated filler led to a decrease in yield stress of
composites compared with untreated filler for both particle size, especially at filler content of 40 wt%. In
addition to the decreasing yield stress value as the filler content increases, the smaller of the particle size
leading to the higher of value of tensile yield stress. On the other hand, surface treatment reduced particleparticle interaction, therefore, reduced the aggregation of filler particles, resulting a better dispersion of
particle filler in polymer matrix, increasing interface leading to increasing yield stress.

The extent of plastic deformation characterized by strain at break is then very sensitive to
composition and morphology of the composites. As shown in Figure 3.9, various types of calcium
carbonate fillers have distinctly different effects in strain at break values.


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Figure 3.9. Effects of particle size, surface modification and filler loading on the tensile mechanical
behaviour of injection-moulded specimens.
3.3.3. Độ bền va đập
J-integral was originally defined by Rice as a contour integral independent on the path, which
express the energy per unit area necessary to create new fracture surfaces in a loaded body containing a
crack. Figure 4 show J-integral values of PP/CaCO3 composites with different types of particle size, filler
loading and surface properties.


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Figure 3.10. Fracture behaviour of PP/CaCO3 composites.
The addition of calcium carbonate led to a change in the fracture mode from brittle fracture for
virgin PP to ductile fracture for the filled composites, which was attributed to the changes of stress fields
in the PP matrix around the filler particles. For the unfilled PP, when the notched composite specimen
receives an impact load, the crazes will be rapidly developed cracks, and then will propagate toward the
whole cross section. The incorporation of rigid particles into the polypropylene matrix leads to
differences in the overall process of crack propagation and fracture. The process starts with the plastic
deformation of the matrix ahead of the initial crack. Assuming a poor bonding between filler and matrix
in cases of treated calcium carbonate, the filler particles detach easily from the matrix by creating voids as
observed by SEM. These voids be formed will absorb impact deformation energy. Otherwise, the particle
will block the propagation of the crack developed from the crazes to increase the fracture resistance.
Jilken et al. [8] also observed that the high impact strength, at high filler content, could be obtained for

low aspect ratio filler, such as dolomite and calcium carbonate. And this only obtains for sufficiently fine
fraction and if the filler particles are good dispersion. That is why J-integral values for composites of
small particle size higher than those of large particle size. The results in Figure 3.10 also showed that
fracture resistance was increased up to 20 wt% of calcium carbonate.
3.2.4. ss-NMR
Two types of VT ss-NMR experiments were performed in a temperature range from 295 to 355
K. The C CP/MAS NMR spectra preferentially detect rigid molecular segments. When the 13C CP/MAS
NMR spectra were acquired at 295 K, three signals corresponding to the CH2 (44 ppm), CH (26 ppm) and
CH3 (21.3 ppm) groups were easily distinguished.
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Figure 3.11. 13C CP/MAS NMR spectra at 295 Figure 3.12. 13C MAS NMR spectra at 295 K
K and 355 K of the pure PP and modified PP.
and 355 K of pure PP and modified PP.
At elevated temperatures (far above Tg), the segmental motion in the amorphous phase increased,
as indicated by the separate signals corresponding to the free r.c.amorphous phase that appeared in the
high-frequency region (Fig. 3.11). The recorded spectra clearly identified the disordered α2 polymorphic
form of isotactic polypropylene.
However, the corresponding 13C MAS NMR spectra measured with a short repetition delay (1-2
s) reflected a preference for the highly mobile fractions. Consequently, the signals of the CH and CH2
groups were suppressed, and at high temperatures, the signals for the polymer segments in the amorphous
r.c. conformation were relatively enhanced (Figure 3.12). Unfortunately, although the prepared PP/CaCO3
systems considerably differed in their mechanical properties, a visual inspection of the recorded 13C
CP/MAS NMR and 13C MAS NMR spectra did not reveal any systematic spectral changes or features that
reflected the plastic deformation.
In a subsequent step, we determined the amount of the highly mobile r.c. amorphous fraction in
the prepared composite materials using the 13C MAS NMR spectra measured at 355 K. As shown in Fig.

3.13, the amount of the highly mobile amorphous r.c. fraction systematically decreased as the critical
value of the J-integral increased, which represents a measure of the composite. The neat, unfilled PP
surprisingly had a dependence in the middle of the other dependences, and regardless of the amount of
filler particles the composite systems that were modified by larger particles (12 mm) nearly exclusively
exhibited a lower J-integral critical value in comparison with the systems that were modified by smaller
particles (1.7 mm).


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: Jid [N/m] is calibrated to [%]
: Highly-mobile fraction of CH %

Figure 3.13. Graph of the toughness expressed as the J-integral (JId) critical value and the contents of the
highly mobile amorphous fractions in the PP systems calculated from the integral intensities of the CH
signal in the 13C MAS NMR spectra. The maximum integral intensity value was calibrated to the
maximum content (100%) of the highly mobile fraction. The maximum J-integral value was normalized
to 100%.
To find other consistent trends and characteristic spectral features related to the changes in the
mechanical properties of the samples, we used FA to extract the key information from the relatively large
experimental data sets that were obtained. The recorded 13C CP/MAS NMR and/or 13C MAS NMR
spectra were separately analyzed in sets representing each temperature.
Subsequently, the FA generated subspectra, Sj, and the corresponding singular values, wj, for
each set of NMR spectra. Because only the singular values w1 - w4 were significantly high (Fig. 3.14, left
panel), the spectral variation in the analyzed dataset was completely described by the corresponding
subspectra, S1eS4
Sau đó, FA tạo ra các phổ thế, Sj và các giá trị bất thường tương ứng, wj cho mỗi phổ NMR. Do
chỉ các giá trị đơn w1 – w4 ở mức cao đáng kể (hình 3.26), biến thể phổ trong tập dữ liệu được phân tích
đã được mô tả hoàn toàn bởi phổ thế tương ứng, S1 – S4.

Fig. 3.14. Singular value calculated from the set of 13C MAS NMR spectra at 355 K (on the left) and the
relevant subspectra S1, S2 and S4 used for the FA (on the right). The subspectra reflecting the changes in
the amorphous (am.) phase and crystalline (cryst.) phase in the CH3 region
The first-rank subspectrum, S1, corresponds to the average 13C MAS NMR spectrum for the
superposition of the experimental data recorded for all the prepared samples at a given temperature, and
the second-order subspectrum, S2, shows the most significant spectral differences found in the analyzed


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data set. In the subspectrum S2, all the components are equally highlighted, including the highly mobile
amorphous and crystalline fractions. Specifically, for the CH3 signal, the amorphous phase was
characterized by a positive signal at approximately 22 ppm, and the crystalline phasewas characterized by
a negative signal at approximately 21 ppm. In addition, we determined from the analysis of the calculated
subspectra that the most significant differences between the samples were in the CH3 regions of the
subspectra S1, S2, and S4 (Fig. 3.26). The observed differences were subsequently quantified using the
corresponding normalized coefficients, Vi1, Vi2 and Vi4. These parameters and their correlation plots were
used to find the relationship between the spectroscopically specific features and the changes in the
physicochemical and mechanical properties of the analyzed composites.
Consequently, by applying this strategy, especially for the 13C MAS NMR spectra obtained at 355
K with increased segmental motion, we saw clear clustering of the Vij parameters into two groups that
were separated by a vertical line, which is visualized in the 3D correlation plot of the relevant parameters,
Vi1, Vi2 and Vi4 (Fig. 15 and Fig. 3.16). These groups correspond to composite systems that differ in their:
(i) highly mobile amorphous fraction content; (ii) filler particle size; (iii) toughening effects; and (iv)
PP/filler aspect ratio. The correlation plot in Fig. 5 shows the two groups of prepared microcomposites
that differ in the J-integral critical value. The group on the left represents systems with an average JId
value of 3.5 N mm-1 (3.2-3.8 N mm-1), and the cluster on the right represents systems with an average JId
value of 4.8 N mm-1. The correlation plots for the other characteristics are shown in Fig. 3.17.

Fig. 3.15. 3D correlation plots for the Vi1, Vi2 Fig. 3.16. 3D correlation plots for the Vi1, Vi2
and Vi4 coefficients evaluated from the 13C and Vi4 coefficients evaluated from the 13C

MAS NMR data using FA for the full spectra
MAS NMR data using FA for the single CH3
signals at 355 K.


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Fig. 3.17. 3D correlation plots of the Vi1, Vi2 and Vi4 coefficients evaluated from the 13C MAS
NMR data at 355 K using FA.
The FA results also give information on the addition of fatty acids into the PP/CaCO3
microcomposites. In this case, at high temperatures (330-355 K), clustering of the systems based on the
surface treatment of the CaCO3 particles was not observed. However, at lower temperatures (325 K),
clustering based on the surface treatment, i.e., with OA or SA and without an acid treatment, was
observed (Fig. 3.18). This clustering was likely revealed by the lower temperatures because the
amorphous phase segmental motion in the systems is not completely free, and the full differences in the
chain mobility and the trans-crystalline layer are not yet well resolved. Therefore, the samples are
clustered based on the subtle differences in the system homogeneity, which is influenced by the nontreated or treated regimes of the two fatty acids.


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Fig. 3.18. 3D correlation plot of the Vi1, Vi2 and Vi4 coefficients evaluated from the 13C MAS NMR data
at 325 K using FA. The plot shows the PP samples based on the fatty acid treatment and the
corresponding 13C MAS NMR spectra of the grouped systems and the pure PP sample.
When searching for the molecular origin of the toughness differences in the prepared PP/CaCO3
microcomposites, we determined that the systems with a higher toughness (higher JId) mostly contained
filler particles with a smaller diameter (1.7 mm), smaller amounts of these particles (80/20), and smaller
amounts of the highly mobile r.c. amorphous fraction based on the 13C MAS NMR spectra at 355 K. The
key role of the amorphous phase in understanding the toughness of the PP/CaCO3 composites was further
evidenced by the FA, which highlighted the prominent spectral differences between the prepared
composite systems. In particular, the subspectrum S4 unambiguously identified the signal at 22 ppm as

corresponding to the methyl groups of the amorphous, free polymer chains in the r.c. conformation. The
crystallinity of the prepared systems was determined by wide angle X-ray scattering experiments to be
approximately 50%, and the crystallinity did not show a systematic trend with respect to the observed
changes in the composite toughness. Therefore, the observed decrease in the free r.c. amorphous fraction
amount must be compensated by an increase in the amount of amorphous PP chains with a helical
conformation in the confined domains. The PP chains that adopt a helical conformation can be attributed
to the transcrystalline phase described in the literature. In general, the formation of this trans-crystalline
phase is induced: i) by the adsorption of polymer chains onto the active sites of the filler particles; ii) by a
suitable orientation of the backbone bonds in the polymer toward the solid surface; and iii) by the
hindered chain mobility, which affects the crystallization kinetics and induces the formation of imperfect
crystallites. These imperfect crystallites are thought to undergo a larger plastic deformation in the system
than the perfect crystallites, and this deformation increases the composite toughness. Our experimental
findings indicate that the key mechanism that is responsible for the enhanced toughness in the PP/CaCO3
composites is related to the PP chain mobility. The mobility is induced by the presence of filler particles,
and these particles do not allow perfect crystallites to form and promote the formation of partially ordered
amorphous and trans-crystalline domains near the filler surfaces to dissipate the deformation energy.
Smaller filler particles with larger specific surface areas offer more active sites for polymer adhesion onto
the solid surface, which consequently results in a larger decrease in the polymer chain motion, the
creation of imperfect crystallites and increased toughness. However, systematic trends in the 13C NMR
parameters were observed only at high temperatures. Although we measured the spectra for the whole
temperature range from 295 to 355 K at 5 K increments, the trends in the signal intensities and the sample
clustering in the principle components plots first appeared at 325 K. At this temperature, the thermal
energy introduced into the systemswas sufficient to overcome the energy barriers and free the highamplitude segmental motions of the polymer chains in the amorphous domains with an r.c. conformation.
As the temperature increased, the higher energy barriers were overcome, and the highamplitude
cooperative motions of the PP chains occurred above the critical temperature (approximately 350 K) as
expected. Near and above the critical fusion temperature, the differences among the prepared composites
were observable using ss-NMR spectroscopy. Below this temperature, these differences were hidden by
the overlapping and unresolved signals.
3.3. Composite based on polypropylene and talc
3.3.1. Morphology observation

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Fracture surface morphology of polypropylene composites containing 40% talc mineral powder
non-modified surface is shown in Figure 3.19.

Fig. 3.19. SEM images of morphology of PP filled with 40% untreated talc
SEM images of the fracture surface of the material samples show that talc minerals are not
denatured, the surface is unevenly dispersed in the polypropylene substrate with the appearance of
agglomerated particles in the substrate. In addition, the interaction between the phases is poor when gaps
appear between the filler particles and the polymer substrate.

Fig. 3.20. SEM images of morphology of PP filled with 40% silane treated talc.
In the case of modified talc mineral powders (Figure 3.20), the dispersion and phase
interoperability were improved. Thus, it is clear that the surface modification process has been shown to
be effective when increasing the adhesion between the surface of the talc and the polypropylene substrate.
3.3.2. Tensile properties
a. Young’s modulus
Effects of talc content and surface modification on mechanical behaviour of polypropylene based
composites were investigated. Figure 3.21 showed Young’s modulus of composites. The results showed
that Young’s modulus values of composites increased as a function of filler content. Generally, the
addition of rigid particulate fillers increases stiffness, which is measured through Young modulus. This is
due to the fact that fillers often exhibit higher stiffness compared matrix polymer. On the other hand,
Young’s modulus is measured at the very beginning of a tensile test, where deformation is insufficient to
cause particle-matrix debonding


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Fig. 3.21. The effects of content and filler surface on the Young’s modulus of PP based composites

Surprisingly, there was a difference in Young modulus at high filler content (40 wt%) in
comparing between treated and untreated filler. This can be explained that the better dispersion of filler
particles in the case of PP/talc/T2Mt leads to the increased stress concentration.
b. Yield stress
As well known that only when filler particles become very small does the yield stress value
increase as the concentration increases. However, yield stress behavior not only depends on particle size
but also on the interaction with the matrix, yield stress gives additional information on filler-matrix
interactions and consequently it is one of the preferred methods of composite testing. It can be seen that
yield stress values of composites strongly increased with the incorporation of talc filler into
polypropylene matrix at small concentration (Figure 3.22). At higher concentration, the increasing is not
strongly. This occurred for both cases treated and untreated talc.

Fig. 3.22. Effects of talc content and filler surface on the yield stress values of PP based composites
The result also indicated that a stronger interaction between the filler and the matrix in case of
PP/talc/T2Mt has a higher yield stress value compared with PP/talc at the corresponding concentration.
c. Strain at break
The strain at break is usually inversely proportional to tensile strength which means that
increasing the tensile strength usually contributes to a decrease in the strain at break. It can be seen that
the addition of talc filler leaded to a marked decrease in the value of strain at break (Fig. 3.23). And this
trend continued at higher concentration for both PP/talc and PP/talc/T2Mt composites.


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Fig. 3.23. Effects of talc content and filler surface on the strain at break values of PP based composites
3.3.3. Fracture behaviour
Introduction of fillers into a polypropylene matrix results in a heterogeneous system. Under the
effect of an external load these heterogeneities induce stress concentrations, the magnitude of which
depends on the geometry of the particles (mean diameter and average size distribution), on the relative
properties of the components and on interfacial adhesion. Heterogeneous stress distribution and local

stress maximums developing in the composite influence its deformation and fracture behaviour as well as
its overall performance. Also, any influence on the crystalline structure produced by the filler addition
will have an influence on the fracture behaviour and deformation mechanisms of the composite.
Some authors reported a maximum of the notched impact strength at a talc content in range of 10 –
20 %. Results in figure 3.24 had a similar trend. Maximum of the notched Charpy impact strength at talc
content of 10%. After this concentration, notched impact toughness decreased with increasing talc
content.
On the other hand, the adsorption of polymer molecules on the filler surface through stronger bonds
leading to the rigidity in structure of polymer chains. This leads to earlier crack initiation and propagation
with decreasing of impact strength values in case of PP/talc/T2Mt composites compared with PP/talc
composites at corresponding concentration (figure 4). Plastic deformation of the polymer matrix is the
main energy absorbing process in impact and this increases when the interaction between particles and
polymer is lowered in case of PP/talc composites.

Fig. 3.24. Effects of talc content and filler surface on the values of notched Charpy impact strength of PP
based composites


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Chapter 4: CONCLUSIONS AND RECOMMENDATIONS
A. Conclusion
The thesis investigated the effect of phase interaction, molecular mobility on the mechanical
properties of polypropylene basedcomposite materials reinforcing with three typical fillers such as glass
beads, calcium carbonate and talc mineral powder. Glass beads are surface treated with silicone oil and
vinyl silane, calcium carbonate are surface treated withstearic acid and oleic acid and talc are surface
treated withmetacryloxypropyltrimetoxy silane.
Strong phase interaction increases the modulus of elasticity and tensile strengbut reduces the
elongation at break. , the value of impact energy absorptionis higher with weak phase interaction. Of
Among of 3 fillers, talc is the best reinforced filler for polypropylene, the tensile and impact strength
composite increase with loadingof 10% talc.

By using the solid-state magnetic resonance spectroscopy for PP / glass beads composite, the least
flexible polymer segments with strong phase interactionare identified. Meanwhile, if glass beads surface
is modified/unmodified by silicon oil,the more flexible segments are found. The raw PP molecule has the
highest flexibility segment. Application of factor analysis (FA) fromss-NMR spectroscopy, PP / CaCO3
composites system has been able to distinguish the difference in: (i) content of highly flexible amorphous
segments; (ii) size of particles fillers; (iii) influence of chemical sustainability; and (iv) the ratioof PP and
CaCO3 in composite material. These spectral differences explain a systematic changeof the impact
strength of material samples.
Thus, the changes of the molecular mobilityin different phases interaction is determinedby solid
state magnetic resonance spectroscopyin both PP / glass beads and PP / CaCO3 materials. They cause the
change in mechanical properties, especially the destructive mechanical properties of the material.
B. Recommendations
The thesis pays attention on analyzing the solid-state magnetic resonance spectrum of composite
material samples, so loading of glass beads and CaCO3 are up to 20 % and 40 % respectively to fabricate
material . In future, the others content of filler will carry on .
In the case of PP / talc materials, talc minerals play more complex role, PhD student will keep
studying on applying solid-state magnetic resonance spectroscopy on this material system.
NEW CONTRIBUTIONS OF THE THESIS
- By the method of solid-state resonance spectroscopy, molecular mobility has been determined in
PP/glass beads and PP/CaCO3 composite materials. The molecular mobility in different phase interaction
changes systematically with the change in mechanical properties of the material. These information
contribute significantly for building up microstructure polypropylene materials. New materials posses
designed properties and they will be applied in polymer materials and chemical engineering.
- Study on the effects of talc mineral, is the separated products of the Institute of Materials
Science, Vietnam Academy of Science and Technology, on the mechanical properties of polypropylene
composite materials. The research results show that polypropylene materials was reinforced with 10% of
talc mineral powder achieves the highest tensile strength and impact. Talc, is considered as mineral good
quality, can be used as reinforcing fillers for composite polymer materials.

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LIST OF PAPERS PUBLISHED
A. List of papers
1. Olivia Kukackova, Nguyen Viet Dung, Sabina Abbrent, Martina Urbanova, Jiri Kotek, Jiri Brus. “A
novel insight into the origin of toughness in polypropyleneecalcium carbonate microcomposites:
Multivariate analysis of ss-NMR spectra”. Polymer 132 (IF = 3,7), 106-113, 2017.
2. Nguyen Viet Dung, Ngo Ke The and Jiri Kotek. “Effect of particle size and fatty surface treatment of
calcium carbonate on the deformation and fracture behaviour of polypropylene-based composites”,
Vietnam Journal of Chemistry, Vol. 53 (2e1), 26-30, 2015.
3. Nguyen Viet Dung and Ngo Ke The. “Effects of talc content and interfacial adhesion on mechanical
behaviour of polypropylene-based composites”, Vietnam Journal of Chemistry, Vol. 53 (4A), 2015.
4. Nguyen Viet Dung, Ngo Ke The and Jiri Kotek. “A solid-state NMR study of molecular mobility and
resulting deformation and fracture behaviour of glass beads filled polypropylene composites”,
Vietnam Journal of Chemistry, Vol. 53(6e4), 240-244, 12/2015.
5. Nguyen Viet Dung, Ngo Ke The and Jiri Kotek. “Effect of interfacial adhesion on deformation and
fracture behaviour of composites based on polypropylene and galss beads”, Journal of Science and
Technology, Vol. 54(1A), 300-307, 2016.
B. List of papers in Conference
1. Nguyen Viet Dung, Libor Kobera and Jiri Kotek. “Effects of filler surface on molecular mobility and
resulting deformation and fracture behaviour of thermoplastic polymer composites”. Carreer in
Polymer VI, Prague, Czech Republic, ISBN 978-80-85009-79-8, 18-19 July 2014.
2. Nguyen Viet Dung, Ngo Ke The and Jiri Kotek. "Effects of filler surface on crack initiation and
propagation of particulate filled polymer composites". 7th International Workshop on Advanced
Materials Science and Nanotechnology, Ha Long city, Vietnam, 2-6 November 2014.
3. Nguyen Viet Dung, Ngo Ke The and Jiri Kotek. "Effect of particle size and fatty acid coatings of
calcium carbonate on the deformation and fracture behaviour of polypropylene-based composites".
Vietnam Malaysia International Congress 2014, Ha Noi, Viet Nam, 7-9 November 2014.
4. Nguyen Viet Dung, Ngo Ke The. “Deformation and fracture behaviour of isotactic polypropylene
reinforced particle fillers”, The 5th Asian Materials Data Symposium, Hanoi, Vietnam, Oct 30th –
Nov 02nd 2016.

5. Nguyen Viet Dung, Ngo Ke The. “A solid-state NMR Study of molecular Mobility and Resulting
Deformation and Fracture Behaviour of Polypropylene Filled Glass Beads Composites”. The 8th
Regional Conference on Chemical Engineering, 29 November – 01 December 2015.