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CHAPTER 1
INTRODUCTION
From pre-historic times, man has exploited for his own use the
properties of natural polymers such as horns, waxes and bitumens. Over the
years, it was gradually learnt that the properties of such materials could be
improved by techniques, such as purification and modification with other
substances. By the turn of the 19th
century, with the explosion of scientific
knowledge in fields such as chemistry and physics, coupled with the demands
from industry for materials with properties which could not be found in
nature, the scene was set for the development of a whole range of new
materials; among them are the early synthetic polymers.
Polymers have obviously not been discovered overnight. They came
out of long and persevering studies by a host of motivated scientists, whose
work has enriched human life. Today, polymers have become an
indispensable material for us and it is difficult to think of daily life without
them.
Just as an architect chooses bricks, stones, logs of wood etc. in
varying shapes, sizes and patterns to create various designs, a chemist
produces innumerable plastics, rubbers, foams, fibers, adhesives, composites,
etc. by judiciously combining various chemicals under desired conditions.
Thus, we can say that a polymer chemist is an “architect of molecules.”
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Depending on its ultimate form and use, a polymer can be made
available in many forms such as plastics, rubber, foam, adhesives,
composites, etc. Out of all the forms, composites are widely used in high
performance applications. High strength and light weight remain the winning
combination that propels composite materials into new arenas, but other
properties are equally important. Composite materials offer good vibrational
damping and a low coefficient of thermal expansion, characteristics that can
be engineered for specialized applications which translate into a finished
product that requires less raw material, fewer joints and fasteners, and shorter
assembly time. Composites have a proven resistance to temperature extremes,
corrosion and wear, especially in industrial settings, where these properties do
much to reduce product life-cycle costs.
Composites differ from traditional materials in that the composite
parts comprise two distinctly different components – fibres and a matrix
material (most often a polymer resin) that, when combined, remain discrete
but function interactively, to make a new material whose properties cannot be
predicted by simply summing the properties of its components. In fact, one of
the major advantages of the fibre / resin combination is its complementary
nature.
The structural properties of composite materials are derived
primarily from the fibre reinforcement. High performance composites derive
their structural properties from continuous, oriented high-strength fibre
reinforcement – most commonly carbon, glass or aramid – in a binding matrix
that promotes processability and enhances mechanical properties, such as
stiffness, and chemical and hygroscopic resistance.
The matrix material in the composite can be a polymer. In the last
forty five years there has been a flurry of activity in the synthesis and
development of high performance and high temperature polymers. This has
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been, in large part, due to the need for advanced materials required for a
diverse range of applications, including aerospace, automotive and
microelectronic industries. These applications often demand a unique
combination of properties, including high glass transition temperatures,
toughness, good adhesion, oxidative and thermal stability, and low a dielectric
constant.
In this regard, a large number of polymers have been developed,
which can be broadly categorized as either thermosets or thermoplastics.
Examples of thermosets are unsaturated polyesters, epoxies, BMI, etc., while
thermoplastics include PEEK (polyetherether ketone), polysulphones,
polyether sulphones etc.
Unsaturated polyesters are the most widely used matrix material in
composite applications, but these resins are less resistant to moisture and have
low performance properties, which limit their application in advanced
composites.
Epoxy thermosets have been widely used as matrix resins for
advanced composites due to their outstanding mechanical and thermal
properties. These properties include high modulus and tensile strength, high
glass transition temperature, high thermal stability and moisture resistance.
When cured, epoxy resins form a highly cross-linked three-dimensional
infinite network, whose microstructure provides the desirable engineering
properties. However, the highly cross linked micro structure also makes it
brittle. It also absorbs moisture that acts as a plasticizer during service, and
reduces the glass transition temperature leading to a decrease in dimensional
stability. This undesirable property restricts epoxy thermosets from
applications requiring high impact and fracture strengths.
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Another important matrix material used for advanced composites is
polyimide. Polyimides possess much better mechanical and thermal properties
than epoxies, but the drawbacks of this resin are low moisture resistance and
poor processability. Bismaleimides have better processability, but they are
excessively brittle.
Processabilty is another pivotal issue regarding the use of high
temperature thermosetting polymers for composite applications. Generally,
these systems require high temperatures for processing, and therefore, cannot
be effectively used in conjunction with low cost processing techniques like
resin transfer moulding. Therefore, attempts for developing novel high
performance thermosetting polymers with easy processing and performance
characteristics, have led to the development of cyanate ester resins. Cyanate
ester resins are a novel class of thermosetting materials, which exhibit
enhanced physical and thermal properties, when compared to traditional
polymer systems like epoxies. These cyanate esters display features including
high glass transition temperatures, low dielectric loss, low moisture
absorption, low corrosion potential, and easy processing, and thus show
promise in technical fields like aerospace and microelectronics.
With the availability of functional materials, and the feasibility of
embedding or bonding them into composite structures, new smart structural
concepts are emerging to be attractive for potentially high-performance
structural applications (Maugin 1988, Gandhi and Thompson 1992, and
Srinivasan and McFarland 2001). A smart structure is one that has surface
mounted or embedded sensors and actuators, so that it has the capability to
sense and take corrective action. Numerous conferences, workshops, and
journals dedicated to smart materials and structures, stand testimony to this
growth. The technological implications of this class of materials and
structures are immense: structures that monitor their own health, process
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monitoring, vibration isolation and control, medical applications, damage
detection, and noise and shape control.
As applications of active vibration/deflection controls in aerospace,
automobile industries and building applications, smart structures have
received considerable attention (Lowey 1997). Vibration and the shape
control of structures are essential to achieve the desirable performance in
modern structural systems. Advances made in the design and manufacturing
of smart structure systems, improve the efficiency of the structural
performance.
1.1 MATRIX MATERIAL
Although it is undoubtedly true that the high strength of composites
is largely due to the fibre reinforcement, the importance of the matrix material
cannot be underestimated as it provides support for the fibres, and assists
them in carrying the loads. It also provides stability to the composite material.
The resin matrix system acts as a binding agent in a structural component in
which the fibres are embedded. In a composite material, the matrix material
serves the following functions-
• Holds the fibres together
• Protects the fibres from the environment
• Distributes the loads evenly between fibres, so that all the
fibres are subjected to the same amount of strain
• Enhances the transverse properties of a laminate
• Improves the impact and fracture resistance of a component
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• Helps to avoid the propagation of crack growth through the
fibres, by providing an alternative failure path along the
interface between the fibres and the matrix.
• Carries interlaminar shear
The matrix plays a minor role in the tensile load-carrying capacity
of a composite structure. However, the selection of a matrix has a major
influence on the interlaminar shear, as well as on the in-plane shear properties
of the composite material. Interlaminar shear strength is an important design
consideration for structures under bending loads, whereas the in-plane shear
strength is important for torsion loads. The matrix provides lateral support
against the possibility of the fibre buckling under compression loading, thus
influencing, to some extent, the compressive strength of the composite
material. The interaction between the fibres and the matrix is also important
in designing damage tolerant structures. Finally, the processability and defects
in a composite material depend strongly on the physical and thermal
characteristics, such as viscosity, melting point, and curing temperature of the
matrix.
1.1.1 Properties of a Matrix
The needs or desired properties of the matrix which are important
for a composite structure are as follows:
• Reduced moisture absorption
• Low shrinkage
• Low coefficient of thermal expansion
• Good flow characteristics, so that it penetrates the fibre
bundles completely, and eliminates voids during the
compacting/curing process
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• Reasonable strength, modulus and elongation (elongation
should be greater than the fibre)
• Must be elastic to transfer the load to the fibres
• Strength at elevated temperature (depending on application)
• Low temperature capability (depending on application)
• Excellent chemical resistance (depending on application)
• Should be easily processable into the final composite shape
• Dimensional stability (maintains its shape)
Out of the many matrix materials known, epoxy resin is a widely
used matrix material in composite applications.
1.2 EPOXY RESIN
Epoxy resin is defined as a molecule containing more than one
epoxide groups. The epoxide group, also termed as an oxirane or ethoxyline
group, is shown in Scheme 1.1.
Scheme 1.1 Structure of Epoxide group
These resins are thermosetting polymers, and are used as adhesives,
high performance coatings, and potting and encapsulating materials. These
resins have excellent electrical properties, low shrinkage, good adhesion to
many metals, and resistance to moisture, and thermal and mechanical shock.
Viscosity, epoxide equivalent weight and molecular weight are the
important properties of epoxy resins.
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1.2.1 Types of Epoxy Resins
There are two main categories of epoxy resins, namely, glycidyl
epoxy, and non-glycidyl epoxy resins. Glycidyl epoxies are further classified
as glycidyl-ether, glycidyl-ester and glycidyl-amine. Non-glycidyl epoxies are
either aliphatic or cycloaliphatic epoxy resins. Glycidyl epoxies are prepared
via a condensation reaction of an appropriate dihydroxy compound, dibasic
acid or a diamine, and epichlorohydrin, while, non-glycidyl epoxies are
formed by the peroxidation of an olefinic double bond.
Glycidyl-ether epoxies such as, diglycidyl ether of bisphenol-A
(DGEBA) and novolac epoxy resins are the most commonly used epoxies.
1.2.2 Diglycidyl Ether of Bisphenol-A
Diglycidyl ether of bisphenol-A (DGEBA) shown in Scheme 1.2 is
a typical commercial epoxy resin and is synthesised by reacting bisphenol-A
with epichlorohydrin in the presence of a basic catalyst.
Scheme 1.2 Structure of the DGEBA
The properties of the epoxy resins depend on the value of n, which
is the number of repeating units commonly known as the degree of
polymerization. The number of repeating units depends on the stoichiometry
of the synthesis reaction. Typically, n ranges from 0 to 25 in many
commercial products.
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1.2.3 Novolac Epoxy Resins
Novolac epoxy resins shown in Scheme 1.3 are glycidyl ethers of
phenolic novolac resins. Phenols are reacted in excess, with formaldehyde in
the presence of an acidic catalyst to produce phenolic novolac resin. Novolac
epoxy resins are synthesised by reacting phenolic novolac resin with
epichlorohydrin in the presence of sodium hydroxide as a catalyst.
Scheme 1.3 Structure of novolac epoxy resin
Novolac epoxy resins generally contain multiple epoxide groups.
The number of epoxide groups per molecule depends upon the number of the
phenolic hydroxyl groups in the starting phenolic novolac resin, the extent to
which they reacted, and the degree of low molecular species being
polymerised during synthesis. Multiple epoxide groups allow these resins to
achieve high cross-link density resulting in excellent temperature, chemical
and solvent resistance. Novolac epoxy resins are widely used to formulate the
moulding compounds for microelectronics packaging, because of their
superior performance at elevated temperature, excellent mouldability and
mechanical properties, superior electrical properties, and heat and humidity
resistance.
1.2.4 Curing of Epoxy Resins
The curing process is a chemical reaction in which the epoxide
groups in the epoxy resin react with a curing agent (hardener) to form a highly
crosslinked, three-dimensional network. In order to convert epoxy resins into
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a hard, infusible, and rigid material, it is necessary to cure the resin with a
hardener. Epoxy resins cure quickly and easily at practically any temperature
from 5-150oC depending on the choice of the curing agent.
1.2.5 Curing Agents (Hardeners)
A wide variety of curing agents for epoxy resins is available,
depending on the process and properties required. The commonly used curing
agents for epoxies include amines, polyamides, phenolic resins, anhydrides,
isocyanates and polymercaptans. The cure kinetics and Tg of the cured
system, are dependent on the molecular structure of the hardener. The choice
of the resin and hardeners depends on the application, the process selected,
and the properties desired. The stoichiometry of the epoxy-hardener system
also affects the properties of the cured material. Employing different types
and amounts of hardener which, tend to control the cross-link density, vary
the structure.
The amine and phenolic resin based curing agents, described below,
are widely used for the curing of epoxy resins.
1.2.5.1 Amine based curing agents
Amines are the most commonly used curing agents for epoxy cure.
Primary and secondary amines are highly reactive with epoxy. Tertiary
amines are generally used as catalysts, commonly known as accelerators for
cure reactions. The use of an excessive amount of catalyst achieves faster
curing, but usually at the expense of working life, and thermal stability. The
catalytic activity of the catalysts affects the physical properties of the final
cured polymer.
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1.2.5.2 Phenolic based curing agents
Epoxy resins when cured with a phenolic hardener, give excellent
adhesion, strength, and chemical and flame resistance. Phenolic novolac-
cured epoxy systems are mainly used for encapsulation, because of their low
water absorption, and excellent heat and electrical resistance. The usefulness
of epoxy resins in many engineering applications is often limited by their
brittle nature and poor thermal conductivity
1.3 TOUGHENING OF EPOXY SYSTEMS
The epoxy resin is the most widely used matrix material for many
structural composites. It has many good properties like stiffness, low
shrinkage, good adhesion to glass/ carbon fibre etc. Unfortunately, the very
factor contributing to its high stiffness and heat resistance leads to its main
draw back, viz (lack of toughness), and that is its highly cross-linked
structure. Aircraft structures are often subjected to impact loads during flight,
which can cause severe damage to the structure by delamination. Toughening
can help in developing damage tolerant structural components for aircraft.
The term toughness is a measure of the material's resistance to
failure, i.e., the total amount of energy required to cause failure.A rough idea
about the fracture toughness of various materials is given in Table 1.1, which
shows that rubber toughened epoxy resins can match engineering
thermoplastics in fracture toughness values. Composites made of such matrix
systems are expected to be tougher, and hence more useful.
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Table 1.1 Fracture toughness of various materials (Bascom et al. 1989)
MaterialFracture toughness
range (kJ/m2)
Inorganic glass Very low
Epoxy/Polyester resins 10-1
Polysulphones/rubber toughened epoxy 100
Metals >10
1.3.1 Various approaches to toughening epoxy resins
The need for toughening epoxy resins was felt in the mid 1960 s.
Initially, solid rubbers like nitrile and polysulphide rubbers were
found to flexibilise epoxy resin. Such resin systems were found to be suitable
for adhesives as these rubber modified resins could sustain large
deformations, and hence, gave better peel joints than the unmodified epoxy
based adhesive. However, as they caused unacceptable levels of deterioration
of stiffness and thermal properties for composites, better tougheners were
needed.
Another method employed the introduction of inorganic as well as
organic filler materials. Of these, the organic systems, especially the one
based on elastomers, have come to the attention of material scientists. In
particular, the amine-, carboxyl- and, hydroxyl-terminatedpoly (butadiene-
co- acrylonitrile) systems (i.e., ATBN, CTBN and HTBN respectively) have
found favour, as reports of inclusion of the one of these rubbers in epoxy
matrix have indicated an increased toughness value at the expense of the
modulus and glass transition temperature (Kunz et al. 1982 and Alan Meek
1974).
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The next method is the inclusion of thermoplastics, such as
polysulphones, polyether sulphones and polyether imides into epoxy networks
(Nam Gyun Yun et al. 2004; Mimura et al. 2000; Hourtson et al. 1991; and
Akay et al. 1993). These studies show a good improvement in thermal and
mechanical properties. However, these thermoplastic polymers show poor
solubility in organic solvents, leading to difficulties in processing.
Yet another method is transverse stitching, z-spinning and 3D
weaving or braiding of reinforcement (Velmurugan et al. 2007 and Gwo-
Chung Tsai et al. 2005). It is observed that these techniques increase the
Mode I delamination toughness several times higher than that of woven fibre
reinforcement composite specimens. It is very expensive when compared to
the other toughening mechanisms.
Later toughening of epoxy was tried with interpenetrating polymer
networks (IPNs). Several studies have demonstrated that the fracture energy
of brittle matrices may be significantly improved with the formation of
interpenetrating polymer networks (Robert Vabrik et al. 1998; Harani et al.
1998 and Raymond and Bui 1998). Polyurethanes have excellent elasticity
and high impact strength; therefore, in proper ratio with epoxy resins,
materials with the desired mechanical and thermal properties can be produced
by a blending technique utilizing the interpenetrating polymer networks
(IPNs) of the two polymer components. However, these have poor mechanical
and thermal properties.
Another area which continues to attract research interest is the field
of thermoset-thermoset polymer blends, in particular, the incorporation of
inherently tough polymers into the brittle polymer systems, in order to impart
improvements in fracture toughness in the resulting blends. Hence, among the
different materials used for the modification of epoxy resins, cyanate esters
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are expected to be the best material to improve the thermomechanical
properties. As compared to epoxies, they are inherently tough, have
significantly better electrical properties and lower moisture uptake. Cyanate
esters also offer ease of handling and processing similar to that of epoxy resin
systems. In addition the dicyanate monomers are expensive to prepare, and
hence, blending a small amount of dicyanate with epoxy resin to get a
polymer resin with superior properties seems to be the best way. Thus,
blending of epoxy with cyanate ester resin continues to attract research
interest in order to impart improvements in fracture toughness, without
compromising other mechanical and thermal properties.
1.4 CYANATE ESTER RESIN
The term “cyanate ester resin” is used to describe prepolymers and
cured resins, the former containing the reactive ring forming cyanate (-OCN)
functional group. Attempts begun in 1857 to react unsubstituted phenoxide
with cyanogen halides produced only mixtures of imidocarbonates and
cyanurates. O-alkylated aryl cyanates were prepared by this method in 1960.
Synthesis via the thermolysis of 1,2,3,4 thio-triazoles was also successful, but
too expensive for commercial interests. Most alkylcyanates were found to
readily undergo exothermic isomerization to the more stable isocyanate form.
Exceptions to this are cyanates of bicyclic alcohols having the OH group in
the bridgehead position, and acidic alcohols containing electronegative
substituents such as halogens.
Based on the cyanogen halide chemistry, the first simple route to the
synthesis of cyanate esters by reacting phenol with cyanogen halide, was
discovered by Grigat and Pütter in 1963.
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ArOH + ClCN ArOCN
Base.HCl
Base+
-
Scheme 1.4 Synthesis of cyanate esters
Among the various reported routes for the Scheme 1.4 synthesis of
cyanate esters, the first reported methods were not quite as simple and
resulted in relatively low yields.
Aryl dicyanates were found to undergo nearly quantitative
conversion to cross-linked cyanate homopolymers by cyclotrimerization to S-
triazines. Tractable prepolymers of up to 50% conversion, produced
commercially by thermally quenching the cyclotrimerization reaction, were
found to be superior for pressure lamination than the low viscosity molten
monomers.
It was discovered that blends of cyanate esters and epoxides
coreacted to form cost-effective hybrids. The complex reaction pathway,
involving cyanate trimerization, epoxide insertion and ring cleavage with
additional epoxide to form substituted oxazolidinones, was not investigated
until much later. Nevertheless, blends of bis-phenol A dicyanate prepolymer
with 45-55% epoxy resin were the predominant cyanate ester, of the 1980s.
With the advancement of integrated circuit technology, interest was
generated in the 1970s, for resins with low dielectric constants to achieve
faster signal propagation via reduced resistance to the passage of
electromagnetic fields. Increased glass transition temperature, Tg, for
matching molten solder temperatures (~250°C) was also of interest for
improving the dimensional stability and reliability of multilayer circuit
boards. Bayer AG developed a prepolymer of bis-phenol A dicyanate and
commercialized this laminating solution as Triazine A resin in 1976. Two
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years later, Bayer exited this business, citing a premature market. A private
communication suggested that carbamate impurities resulting from the use of
an aqueous base during monomer synthesis and zinc co-ordination metal
catalysts, may have contributed to the severe blistering of some laminates
during the solder application. Bayer AG licensed their CE technology to
Mitsubishi Gas chemical in 1978 and to Celanese in 1984.
Mitsubishi Gas Chemical commercially introduced BT resins,
blends of bisphenol. A dicyanate and or its prepolymers with bismaleimides
BMI in 1978. The basic patent describes gel times for CE blends with several
BMIs, including a Michael addition product of methylene dianiline and
excess BMI monomer derived from the same aromatic amine. Although
isoureas produced from the reaction with cyanates and secondary aromatic
amine are known cyclotrimerization catalysts, no supporting evidence was
offered for the proposed heterocyclic rings reported in subsequent
publications, from the cycloaddition reactions between cyanates and
maleimide C=C unsaturation. Mitsubishi Gas Chemical Co. supplied BT
resins in addition to the formulated prepreg and clad laminate to circuit board
manufacturers.
Celanese Corp. (now Ciba-Geigy) initiated research in 1981 that
utilized chemically tailored bisphenols and polyphenols to expand CE
capabilities in the directions to lower dielectric loss properties, increased
hydrolytic and thermal stabilities, lower cure temperatures and liquid
monomer forms. These efforts combined with those of Dow Chemical Co.
and Allied Signal have expanded the family of commercially available CE
monomer, to the current seven structurally distinct monomers and numerous
other speciality monomers and prepolymers.
Beginning in 1979, considerable research was directed at
toughening CE resins by alloying them with initially soluble engineering
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thermoplastics that phase separated into continuous morphologies during
cure. These efforts have produced composites for aircraft primary structures
with melt processability similar to that of thermosetting epoxies, but which
pass the wet condition tests for supersonic aircraft rated at 177°C skin
temperatures. The same concept has been extended to ketone laminating
solutions for toughened circuit board laminates with improved drilling
characteristics and thin (50-100 m) double sided circuits with robust
handling properties for multichip module construction (Treliant Fang and
David A. Shimp 1995).
Today, CEs are established thermosetting resins for insulating high
speed, high density electronic circuitry, as matrix resins for aircraft
composites, geostationary broadcast satellites, radomes and antennae, and
have potential as versatile adhesives as well as passive wave guides or active
electrooptic components for processing light signals in fibre optic
communication.
1.4.1 Curing of Dicyanate
Cyanate ester resins are bisphenolic or polyphenolic derivatives
containing the ring forming cyanate (-OCN) functional groups. Chemically,
this family of thermosetting monomers and their pre-polymers are esters of
bisphenol (or polyphenol) and cyanic acid. The esters cyclotrimerize to form
substituted triazine rings on heating. Cross linking of cyanate esters occurs
via cyclotrimerization to form 3-dimensional networks of oxygen linked
triazine rings. The curing reaction is classified as an addition polymerization
and occurs without the emission of volatile by-products.
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NCO Ar OCN N
N
N
OAr
OArArO
--
--
--[
n
Three Dimensional Polycyanurate N
Catalyst
Heat/
Scheme 1.5 Formation of three dimensional networks by cyclotrimerization
Pure cyanate ester monomers will cure relatively slowly. However,
the addition of a catalyst exponentially increases the cure rate. Effective
catalysts recommended by Rhone-Poulenc for cyclotrimerization were a
combination of transition metal complexes and active hydrogen, non-volatile,
liquid phenolic compounds, eg. nonyl phenol, that serves as a co-catalyst.
The latter also promoted enhanced solubility of the metal catalyst in the
cyanate resin. In general, organic soluble compounds of most coordination
metals serve as potent trimerization accelerators. Zinc, copper, manganese
and cobalt compounds were preferred over the more reactive transition metals
like iron, tin, titanium, lead and antimony. This solution is consistent with the
observation that the latter group promotes the undesirable hydrolysis of an
otherwise stable cyanate ester linkage. Specifically, chelated metals of
acetylacetonates are less active hydrolysis catalysts (relative to the metal
carboxylates, octoates and naphthenates) and also have the added advantage
of increased latency (less trimerization activity at room temperature per unit
of elevated temperature activity) due to the lower activity of the chelate.
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1.4.2 Copolymerization with Epoxides
Early reports on the epoxide–cyanate co-reaction noted the
formation of oxazole (5-membered ring) structures without elaboration on the
mechanism or the complete reaction scheme. Publications in the period 1987
–90 noted that the trimerization of the cyanate group preceded reactions
involving epoxide, and demonstrated that cured hybrid properties were
independent of the CE prepolymerization, and thus proposed additional
epoxide consumption via polyetherification catalyzed by the triazine ring.
Monofunctional epoxy and CE model compounds were first
employed in 1988 to separate and identify reaction products by GPC and IR.
Publications by Bauer and later by Shimp, elucidated and supported a
complex reaction pathway partially described in Scheme 1.6. The sequence
of CE trimerization followed by epoxide insertion, isomerization of glycidyl
cyanurates to isocyanurates and isocyanurate ring cleavage / rearrangement
with additional epoxide to form substituted oxazolidinones, can be observed
by heating the trimer of a mono cyanate with monoepoxide. The complicated
insertion – rearrangement – cleavage sequence is expected to occur only at
higher temperature, due to both the lack of homoconjugation in the alkyl
cyanurates and the high activation barrier to breaking the isocyanurate ring.
(1) Trimerization
Trimerization
3 Ar' OCNN
N
N
OAr
OArArO
Aryl cyanurate
Aryl cyanate
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(2) Epoxide Insertion
N
N
N
OAr'
Ar'O OAr'
Aryl Cyanurate
+ 3 Ar" CH2 CH CH2O
O
N
N
N
OAlk
AlkO OAlk
Alkyl Cyanurate
Alk = CH2 CH CH2 O Ar"
OAr'
Epoxide
(3) Rearrangement
N
N
N
OAlk
AlkO OAlk
Alkyl Cyanurate
N
N
N
O
O O
Alk
Alk Alk
Alkyl Cyanurate
(4) Ring cleavage and reformation
3 Ar" CH2 CH CH2O
O
+N
N
N
O
O O
Alk
Alk Alk
Alkyl Cyanurate
3 Ar" CH2O
N
CH2
O
CH
O
Alk
Epoxide
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(5) Direct Ring Formation
Ar' OCN
Aryl cyanate
+ Ar" CH2 CH CH2O
O
Epoxide
Ar" CH2O
N
CH2
O
CH
O
Alk
Scheme 1.6 Proposed cyanate – epoxy reaction pathway
Reactions (1) and (5) are the major oxazolidinone reactions
occurring at lower temperatures (T < 150°C) (Martin et al. 1999).
1.5 SMART STRUCTURES
A smart structure involves distributed actuators and sensors, and one
or more microprocessors that analyze the response from the sensors, and use
the distributed parameter control theory to command the actuator to apply
localized strains. A smart structure has the capability to respond to a changing
external environment (such as loads and shape changes) as well as to a
changing internal environment (such as damage or failure). Many types of
actuators and sensors are being considered, such as piezoelectric materials,
shape memory alloys, electrostrictive materials, magnetostrictive materials,
electrorheological fluids and fiber optics. These can be integrated with the,
main load carrying structure by surface bonding or embedding without
causing any significant changes in the structural stiffness of the system.
Among these materials, the piezoelectric are the most popular. They undergo
surface elongation (strain) when an electric field is supplied across them, and
produce a voltage when surface strain is applied, and hence can be used both
as actuators and sensors. In an applied field these materials, however,
generate a very low strain but cover a wide range of actuation frequency. The
most widely used piezoceramics (such as Lead Zirconate Titanate) are in the
form of thin sheets, which can be readily embedded or attached to a
composite structure.
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1.5.1 Piezoelectric Materials
Piezoelectric materials have become very popular in the dynamic
sensing, actuation and control of active structural and mechanical systems.
They can act both as actuators and sensors. In the development of intelligent
structural systems, piezoelectric are widely used as sensors and actuators for
the dynamic monitoring and control of structural and mechanical systems. In
general, piezoelectric materials respond to force/pressure and generate a
charge/voltage; this is referred to as the direct piezoelectric effect; on the
other hand, the material exhibits stress/strain changes when a strong external
voltage/charge is applied, and this is called the converse piezoelectric effect.
In addition, the material would also respond to a temperature
fluctuation and generate a charge/voltage, and this is referred to as the
piezoelectric effect. It has been over 120 years since the first discovery of
piezoelectric materials. However, it is only relatively recently that engineers
and scientists have again recognized the potential of piezoelectric materials in
distributed actuators and sensors, high precision systems,
microelectromechanical systems, and adaptive structural systems.
Consequently significant efforts have been devoted to the research and
development of piezoelectric technologies in recent years. Besides mechanical
and electrical coupling and interaction, temperature can also influence the
performance of piezoelectric devices. For example, temperature variation can
introduce voltage/charge generation in piezoelectric sensors. In addition,
control voltage can cause a temperature rise in piezoelectric actuators.
1.6 SCOPE AND OBJECTIVES
In recent years, a new damping material has been developed on the
basis of a new damping mechanism. For some specialized composites,
mechanical vibrating energy is first transmitted to piezoelectric ceramic
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powders and converted into an alternating potential energy by the
piezoelectric effect. Such an energy transferring effect is referred to as the
piezo-damping effect (Sheng et al, 2008). Lead Zirconate Titanate (PZT) is
usually used as piezoelectric ceramic fillers to construct the piezo-electric
units in the polymer matrix. It is well known that reinforcement can improve
the mechanical property of the composite greatly. The damping property of
the composite may also be improved, if the reinforcement is chosen properly
and combined with the matrix in a special way, to make varied damping
mechanisms playing roles together in the composite. Thus the work throws
light on the mechanical and damping properties of the quarternary composite
with varying cyanate and PZT loading, and on analyzing the effect of cyanate
and PZT loading and on the properties.
In view of the challenges associated with the manufacturing of the
high performance composites discussed above, the present research proposal
is focused on the,
Development of new matrix material
Determination of the mechanical properties of the prepared
composites
Application of newly developed composites
The objectives of the present work are given below.
1. Development of the matrix material.
Arocy b10 (bis phenol dicyanate) is chosen to prepare
blends in different loading levels of 0%, 20%, 40% and
60% with commercial epoxy resin system (LY556) using
DDM(HT972) as curing agent.
24
A ceramic material, namely, lead zirconate titanate is
loaded in different loading levels of 10%, 20% and 30%
with the best cyanate loaded epoxy resin system.
2. Fabrication of composite plates
The fabrication of the Piezothermoelastic polymer matrix
E-glass fibre composites using various blends with the
combination of the following matrix materials:
a. Epoxy Resin
b. Cyanate Ester
c. Lead Zirconate Titanate
3. Testing and determination of the Mechanical properties
Determination of the following mechanical properties:
a. Tensile Strength
b. Tensile Modulus
c. Flexural Strength
d. Flexural Modulus
e. Fracture Toughness
4. Vibration analysis of the fabricated composites with and
without the piezoelectric material.(Experimental and Finite
Element Analysis)
Study of the natural frequency, damping factor, stiffness,
storage modulus and loss modulus
5. Performance and emission characteristics of the lead zirconate
titanate loaded cyanate modified epoxy coated combustion
chamber in a diesel engine
25
Study of the brake fuel consumption, brake thermal
efficiency, pressure, heat release rate, hydrocarbon
emission, oxides of nitrogen, carbon monoxide emission
and exhaust gas temperature.
The following are the contributions of this thesis:
I Scientific contribution
i) Development of a Piezothermoelastic cyanate based epoxy
composite material.
II Technical contribution
i) Application of an analytical expression to determine the
damping factor and modulus of the developed composite
material.
ii) a. Fabrication of the Piezothermoelastic epoxy-cyanate
ester matrix glass fibre composite.
b. Determination of the tensile properties, flexural
properties and fracture toughness of the fabricated
composite.
c. Determination of the vibration characteristics of the
fabricated composites.
III Contribution towards practical application
i) Use of the developed composite for high temperature
application in an engine, which can be extended to
aircraft also.
26
1.7 LITERATURE SURVEY
1.7.1 Epoxy Toughening
Kinloch et al (1983) studied the microstructure and fracture
behaviour of an unmodified and a rubber-modified epoxy. Values of the stress
intensity factor, KIc, at the onset of crack growth, the type of crack growth,
and the detailed nature of the associated fracture surfaces have been
ascertained. Both materials exhibit essentially the same types of crack growth,
but the values of KIc for the rubber-modified material were usually
significantly higher than those for the unmodified epoxy. The mechanisms for
this increased toughness have been considered, and one that accounts for all
the observed characteristics, has been proposed.
Smiley and Pipes (1987) have investigated the rate effect on Mode I
interlaminar fracture toughness in graphite/PEEK and graphite/epoxy
composites. The tests were performed over a range of crosshead speeds from
4.2 x 10-6
to 6.7 x 10-1
m/s. The results indicate that the toughness of both
material systems is rate sensitive. The Mode I interlaminar fracture toughness
of the graphite/PEEK material decreases from 1.5 to 0.35 kJ/m2 over five
decades of the opening rate. The fracture toughness of the graphite/epoxy
material decreases from 0.18 to 0.04 kJ/m2 over four decades of the loading
rate.
Chu (1989) has made a study of the non-linear effect on Mode-I
interlaminar fracture toughness. Large deflections occur on testing thinner
specimens or thicker specimens with larger delamination lengths using a
linear analysis; theIC
G value increases with increasing delamination growth,
and a significant difference is indicated between the first and the last test
point. However, a non-linear analysis shows much better results than a linear
analysis.
27
Madhu S.Madhukar and Drazal (1990) have studied the fiber-matrix
adhesion and its effect on composite mechanical properties for Mode-I and
Mode-II fracture toughness of graphite/epoxy composite. This method
demonstrated that there is a strong dependency of the composites
interlamination fracture toughness and failure modes on fiber-matrix
adhesion. The full potential of a composites inter laminar fracture toughness
can be realized only when the fiber matrix interface is strengthened to its
maximum level.
Verchere et al (1990) studied the effect of a bisphenol-A
diglycidylether based epoxy cured with a cycloaliphatic diamine (4,4 -
diamino-3,3 -dimethyldicyclohexylmethane, 3DCM), in the presence of an
epoxy terminated butadiene-acrylonitrile random copolymer (ETBN). Results
showed that the vitrification is slightly delayed with the rubber addition. The
maximum Tg of the rubber-modified matrix does not depend on the cure
temperature, but decreases with the initial rubber concentration. This implies
that a significant amount of rubber remains in the solution in the continuous
phase. This explains the delay in vitrification.
Bazhenov (1991) has made a study on strong bending in the DCB
interlaminar test of thin, E-glass woven –fabric-reinforced laminates. In this
case only the critical crack extension force needs to be measured to determine
the fracture toughness. The interlaminar fracture toughness of fabric-
reinforced laminates is significantly higher than that of non-woven
unidirectional composites. The crack propagation between the fabric layers is
unstable, whereas it is stable if the crack intersects some fabric layer.
Verchere et al (1991) studied the mechanical properties of a system
consisting of a bisphenol A diglycidylether epoxy, cured with a cycloaliphatic
diamine (4,4 -diamino-3,3 dimethyldicyclohexyl-methane, 3DCM), in the
presence of an epoxy-terminated butadiene-acrylonitrile random copolymer
(ETBN), as a function of the cure schedule and the initial rubber
28
concentration. Fracture toughness (KIc) and fracture energy (GIc) were
increased, while Young's modulus and yield strength decreased slightly with
increasing volume fraction of the dispersed phase. There is no significant
influence of the precure schedule and of the various observed particle
diameters on the mechanical properties for a constant rubber volume
fraction.The main deformation process in the rubber-modified epoxy
networks is shear yielding, while cavitation is negligible.
Hourston and Lane (1992) prepared a series of blends by adding a
polyetherimide, in varying proportions, to a trifunctional epoxy resin,
triglycidylparaaminophenol, cured with 4,4 -diaminodiphenylsulphone. All
the materials showed a two-phase morphology when characterized by a
dynamic mechanical thermal analysis and scanning electron microscopy.
Addition of the thermoplastic resulted in improved fracture properties (K1C
and G1C), as measured by three-point bending experiments, although no
obvious correlation with blend morphology was observed.
Roxana et al (1993) used castor oil (CO) to replace polydisperse
commercial rubbers (carboxy- or epoxy-terminated butadiene-acrylonitrile
random copolymers, CTBN or ETBN) in model systems, developed to
analyse the origin of the phase separation process in rubber-modified
thermosets. Mixtures of CO with an epoxy resin based on the diglycidyl ether
of bisphenol A showed a higher miscibility than a typical CTBN (18%
acrylonitrile)-DGEBA system. Percentage conversions at the cloud point
during the DGEBA-EDA polymerization were experimentally determined,
and compared with theoretical predictions using the pseudo-binary approach
in the framework of the Flory-Huggins lattice model. Reasonable agreement
was found, giving direct evidence of the fact that phase separation results
from the decrease in the entropic contribution to the free energy of mixing
during polymerization.
29
Dong Chen et al (1993) introduced butadiene-acrylonitrile random
copolymers with various molecular weights and end-groups into a system
consisting of the diglycidyl ether of bisphenol A and 3,3 -dimethyl-4,4 -
diamino dicyclohexyl methane (3DCM) cured at 50°C. They studied the
influence of a low level of soluble additive on the polymerization rate,
evolution of viscosity, gelation and vitrification times, and the final network
in the case of different additive molecular weights and end groups of the
additive. It was found that the additive influences the final network only by
dissolving in the matrix, and that the dilution effect plays a minor role, but the
catalytic effect of an additive can play a significant role on polymerization
depending on the additive end groups. However, in all the rubber-modified
systems, phase separation has no direct influence on the polymerization rate
and the change of viscosity.
Min et al (1993) used near infra-red spectroscopy techniques to
study the cure reactions of various epoxy resin formulations based on the
diglycidyl ether of bisphenol A resins cured with 4,4 -diaminodiphenyl
sulfone (DDS) hardener. Stoichiometric and non-stoichiometric
DGEBA/DDS resin formulations, using neat as well as thermoplastic
toughened systems containing two phenolic hydroxyl terminated polysulfones
with different molecular weights were involved in this study. This series of
quantitative analysis of the major chemical groups in several resin systems,
led to a clear understanding of not only the reaction mechanism in each
system but also the cure kinetics.
Cho et al (1993) used tetraglycidyl-4,4 -diaminodiphenyl methane
based resin with 30 phr diaminodiphenyl sulfone as the curing agent and was
toughened with poly(ether imide) (PEI). The effects of morphology on the
fracture toughness of modified epoxy resins were investigated. Morphology
was controlled by changing the curing conditions. The co-continuous
30
structure and morphology of the PEI spherical domain dispersed in the epoxy
matrix were obtained. Phase-inversed morphology with PEI matrix was also
obtained with 30 phr PEI content. The cured resin with phase-inversed
morphology showed the highest fracture toughness. The modified epoxy
resins with enhanced fracture toughness exhibited other improved mechanical
properties such as flexural strength, flexural modulus and strain at break.
Tzong-Hann Ho and Chun-Szhan Wang (1994) used dispersed
acrylate rubbers to improve the toughness of cresol-formaldehyde Novolac
epoxy resin cured with phenolic novolac resin for electronic encapsulation
application. The effect of the alkyl group of acrylate monomer on the phase
separation of the resultant elastomers from epoxy resin was investigated. The
dispersed acrylate rubbers effectively improve the toughness of cured epoxy
resins by reducing the coefficient of thermal expansion (CTE) and flexural
modulus, while the glass transition temperature (Tg) was hardly depressed.
Electronic devices encapsulated with the dispersed acrylate rubber-modified
epoxy molding compounds have exhibited excellent resistance to the thermal
shock cycling test and resulted in an extended device use life.
ZhiQiang Cao et al (1994) studied several rubbers (acrylonitrile–
butadiene copolymer) or thermoplastic (polyethersulfone) additives bearing
different chain ends introduced into pure aromatic dicyanates. The influence
of these initially miscible modifiers on the polymerization kinetics, as a
function of their chemical structure and concentration, were also studied. It
appears that apart from those bearing a labile hydrogen atom, the additives
play almost no role on the polycyclotrimerization rate; neither does phase
separation. However, the additives influence the structure of the final
networks insofar as they partially dissolve in the matrix, and thus modify both
the final Tg and the onset of vitrification, compared with the pure monomer.
31
Tzong-Hann Ho and Chun-Shan Wang (1994) investigated the use
of dispersed silicone rubbers to reduce the stress of cresol–formaldehyde
novolac epoxy resin cured with phenolic novolac resin for electronic
encapsulation application. The effects of structure, molecular weight, and
contents of the vinylsiloxane oligomer on reducing the stress of the
encapsulant were studied. Morphology and the dynamic mechanical behavior
of the rubber-modified epoxy resins were also studied. The dispersed silicone
rubbers effectively reduce the stress of the cured epoxy resins by reducing
flexural modulus and the coefficient of thermal expansion (CTE), whereas the
glass transition temperature (Tg) was hardly depressed. Electronic devices
encapsulated with the dispersed silicone rubber modified epoxy molding
compounds have exhibited excellent resistance to the thermal shock cycling
test and have resulted in an extended device use life.
Philippe Bussi and Hatsuo Ishida (1994) studied the dynamic
mechanical properties of blends of diglycidyl ether of bisphenol-A-based
epoxy resin and internally epoxidized polybutadiene rubber. It is shown that
the influence of the composition of the continuous phase and of the dispersed
phase can be studied not only from the variations of the glass transition
temperature but also from the changes in the apparent enthalpy of activation
associated with this transition. As the initial rubber content increases, the
composition of the dispersed phase remains practically constant while more
rubber is able to dissolve in the continuous phase.
Youjiang Wang and Dongming Zhao (1995) have studied the
characterization of the interlaminar fracture behavior of woven fabric
reinforced polymeric composites. A large displacement, small strain non-
linear beam model was used to calculate the interlaminar fracture toughness.
The fabrics used included fiberglass and Kevlar woven structures with
different weave patterns. This study shows that the improvement in the
32
interlaminar fracture behavior of laminated polymeric composites has
generally focused on the matrix material, the reinforcement and the fiber-
matrix interface.
Tsung-Han Ho et al (1996) used polyol or polysiloxane
thermoplastic polyurethanes (TPU) to reduce micro-cracking in cresol–
formaldehyde novolac epoxy resin cured with phenolic Novolac resin for
electronic encapsulation application. A stable dispersion of TPU particles in
an epoxy resin matrix was achieved via the epoxy ring opening with
isocyanate groups of urethane prepolymer to form an oxazolidone. The effects
of the structure and molecular weight of TPU in reducing the stress of the
electronic encapsultant were investigated. The mechanical and dynamic
viscoelastic properties and morphologies of TPU modified epoxy networks
were also studied.
Reza Bagheri and Raymond (1996) elucidated the role of particle
cavitation in toughening through a comparative examination of epoxies
modified by conventional rubber modifiers and hollow plastic particles. The
results of this study illustrate that rubber particles with different cavitation
resistance and pre-existing microvoids toughen the present epoxy matrix in
the same manner. Therefore, they concluded that the cavitation resistance of
the rubbery phase does not directly contribute to toughness, but instead
simply allows the matrix to deform by shear. An additional mechanism of
microcracking was observed when 40- m hollow plastic particles were
employed. Despite the similar behaviour in fracture toughness testing, rubber
particles and microvoids differ considerably in how they affect the
compressive yield strength of the blend. The results of this study suggest the
possible importance of inter-particle distance in the toughening of epoxies.
This concept will be examined in part 2 of this study.
33
King-Fu Lin and Yeow-Der Shieh (1998) employed a two-stage,
multistep soapless emulsion polymerization to prepare various sizes of
reactive core–shell particles (CSPs) with butyl acrylate (BA) as the core and
methyl methacrylate (MMA) copolymerizing with various concentrations of
glycidyl methacrylate (GMA) as the shell. Ethylene glycol dimethacrylate
(EGDMA) was used to crosslink either the core or shell. The number of
epoxy groups in a particle of the prepared CSP measured by chemical titration
was close to the calculated value, based on the assumption that the added
GMA participated in the entire polymerization unless it was higher than
29 mol %. Similar results were also found for their solid-state13C
-NMR
spectroscopy.
Tsung-Han Ho and Chun-Shan Wang (1999) synthesized a series of
phenol-based and naphthol-based aralkyl epoxy resins by the condensation of
p-xylylene glycol with phenol, o-cresol, p-cresol, or 2-naphthol, respectively,
followed by the epoxidation of the resulting aralkyl novolacs with
epichlorohydrin. The incorporation of stable dispersed polysiloxane
thermoplastic polyurethane particles in the synthesized epoxy resin's matrix
was achieved via epoxy ring-opening with the isocyanate groups of urethane
prepolymer to form an oxazolidone. The mechanical and dynamic viscoelastic
properties of cured aralkyl novolac epoxy resins were investigated. A sea-
island structure was observed in all cured rubber-modified epoxy networks
via SEM. The results indicate that a naphthalene containing aralkyl epoxy
resin has a low coefficient of thermal expansion, heat resistance, and low
moisture absorption, whereas phenol aralkyl type epoxy resins are capable of
imparting low elastic modulus, resulting in a low stress matrix for
encapsulation applications.
Shun-Fa Hwang and Bon-Cherng Shen (1999) have studied the
opening-mode interlaminar fracture toughness of interply hybrid composite
materials. This method demonstrated that crack growth in the three types of
34
specimens is dominated by the opening mode and the Mode-I interlaminar
fracture toughness can be approximated. For hybrid composite specimens, the
effect of geometrical non-linearity should be included. This study clearly
shows that the effect of geometric non-linearity increases with an increase of
the crack length.
Hua and Hu (2000) have investigated a new kind of simultaneous
interpenetrating polymer networks (SINs) composed of epoxy resin (epoxy)
and urethane acrylate resin (UAR) having various amounts of hard segment
and prepared with poly(oxypropylene) polyol (PPO) having different
molecular weights, and the relationship between the morphologies and
mechanical properties of these SINs were investigated in detail. It was found
that the different morphologies of these SINs were related to various
structures of the UAR network. The morphology of such SINs not only
depends on the compatibility between the poly(methyl methyacrylate)
segments existing in the UAR network and epoxy network, but is related to
the microphase separation of the UAR network as well.
Kessler and White (2001) have studied the self-activated healing of
delamination damage in woven E-glass/epoxy composites. With the ultimate
goal of self-healing in mind, two types of healing processes are studied.
Healing efficiencies relative to the virgin fracture toughness of up to 67% are
obtained when the catalyzed monomer is injected and about 19% for the self-
activated materials.
Hsieh et al (2001) have investigated polyurethanes (PU) based on
poly(butylene adipate) [PU(PBA)] and poly(oxypropylene) [PU(PPG)]
polyols as a graft agent to prepare interpenetrating polymer networks of
urethane-modified bismaleimide (UBMI) and the diglycidyl ether of
bisphenol A (Ep) (UBMI/Ep graft-IPNs). The UBMI was introduced and
partially grafted to the epoxy by PU graft agents, and then the simultaneous
35
bulk polymerization technique was used to prepare the graft-IPNs.All the PU
graft agents were characterized by infrared (IR). The tensile strength of both
the UBMI/Ep graft-IPNs with PU (PBA) and PU (PPG) graft agent systems
increased to a maximum value with increasing UBMI content in the system,
and then decreased with further increasing the UBMI content. For both kinds
of PU with various molecular weights in the UBMI/Ep graft-IPNs, the Izod
impact strength increased with the UBMI contents increasing. The better
compatibility of PU (PBA)-based UBMI/Ep graft-IPNs led to higher impact
strength.
Fellahi et al (2001) used kaolin as a modifier at different contents to
improve the toughness of diglycidyl ether of bisphenol A epoxy resin with
polyamino-imidazoline as a curing agent. The chemical reactions suspected of
taking place during the modification of the epoxy resin were monitored and
evaluated with the Fourier transform infrared spectroscopy. The glass-
transition temperature (Tg) was measured with differential scanning
calorimetry. The mechanical behavior of the modified epoxy resin was
evaluated in terms of the Izod impact strength (IS), the critical stress intensity
factor (KIC), and the tensile properties at different modifier contents. Scanning
electron microscopy (SEM) was used to elucidate the mechanisms of
deformation and toughening in addition to other morphological features.
Finally, the adhesive properties of the modified epoxy resin were measured in
terms of the tensile shear strength (TSS).
Dispenza et al (2001) chose a high molecular weight acrylonitrile
/butadiene /methacrylic acid (Nipol 1472) rubber to control the processability
and mechanical properties of a TGDDM (tetra glycidyl diphenyl methane)
based epoxy resin formulation for aerospace composite applications. The
physical blend of rubber and epoxy resin, achieved by the dissolution of all
the components in a common solvent, forms a heterogeneous system after
36
solvent removal and presents coarse phase separation during cure, which
impairs any practical relevance of this material. A marked improvement of
rubberepoxy miscibility is achieved by the reactive blending (‘pre-reaction’)
of the epoxy oligomer with the functional groups present in the rubber.
Shangjin He et al (2001) synthesized two kinds of reactive
toughening accelerators for epoxy resin, amine-terminated chain-extended
urea (ATU) and imidazole-terminated chain-extended urea (ITU) from
polyurethane prepolymer. Compared with the unmodified system, the curing
activity, dynamic mechanical behavior, impact property and fracture surface
morphology of the modified systems were systematically investigated.
Results show that the curing activity of the modified epoxy resin E-
51/dicyandiamide (dicy) systems is so greatly enhanced that the apparent
activation energy of the curing reaction decreases from 130.2 kJ/mol for the
unmodified system to 75–85 kJ/mol for the modified systems. The curing
reaction mechanism of the E-51/dicy system accelerated by ITU is different
from that of the system accelerated by ATU, and a little different from that of
the system accelerated by imidazole. Furthermore, the impact strength of the
cured systems modified with ITU is 2–3 times higher than that of the
unmodified system, while the glass transition temperatures are a little altered,
and the fracture surfaces of all modified systems display tough fracture
feature.
Fábio et al (2002) employed hydroxy-terminated polybutadiene
functionalized with isocyanate groups and in preparation of a block
copolymer of polybutadiene and bisphenol A diglycidyl ether (DGEBA)-
based epoxy resin. The block copolymer was characterized by the Fourier
transform infrared (FTIR) spectroscopy and size-exclusion chromatography
(SEC). Cured blends of epoxy resin and hydroxy-terminated polybutadiene
(HTPB) or a corresponding block copolymer were characterized by
37
differential scanning calorimetry (DSC), dynamic mechanical analysis
(DMTA), and scanning electron microscopy (SEM). All modified epoxy resin
networks presented an improved impact resistance with the addition of the
rubber component at a proportion of up to 10 wt % when compared to the
neat cured resin.
Raffaele Mezzenga et al (2002) studied the effect of the structural
buildup during the reticulation of thermoset systems containing reactive
modifiers to strongly influence the final properties of such blends. This was
studied by considering the rheological behavior during the cure of an
epoxy/amine thermoset system blended with reactive dendritic hyperbranched
polymers (HBPs). Depending on the chemical structure of the HBP used in
the blend, a phase separation could be observed. The onset and offset of the
phase separation process could be detected by observing the evolution of the
viscoelastic properties. The phase separation onsets obtained by rheological
measurements were compared with the values obtained by traditional cloud
point observations. A good agreement between the two techniques was
observed.
Kim et al (2002) synthesized amine-terminated poly(arylene ether
sulfone)–carboxylic-terminated butadiene-acrylonitrile–poly(arylene ether
sulfone) (PES-CTBN-PES) triblock copolymers with controlled molecular
weights of 15,000 (15K) or 20,000 (20K) g/mol from amine-terminated PES
oligomer and commercial CTBN rubber (CTBN 1300x13). The copolymers
were utilized to modify a diglycidyl ether of bisphenol A epoxy resin by
varying the loading from 5 to 40 wt %. The epoxy resins were cured with
4,4 -diaminodiphenylsulfone and subjected to tests for thermal properties,
plane strain fracture toughness (KIC), flexural properties, and solvent
resistance measurements. The fracture surfaces were analyzed with SEM to
elucidate the toughening mechanism. The properties of the copolymer-
38
toughened epoxy resins were compared with those of the samples modified by
the PES/CTBN blends, PES oligomer, or CTBN. The PES-CTBN-PES
copolymer (20K) showed a KIC of 2.33 MPa m0.5
at 40 wt % loading while
maintaining good flexural properties and chemical resistance.
Giannotti et al (2004) modified epoxy–aromatic diamine
formulations simultaneously with two immiscible thermoplastics (TPs),
poly(ether imide) (PEI) and polysulfone (PSF). The epoxy monomer is based
on the diglycidyl ether of bisphenol A and the aromatic diamines (ADs) are
either 4,4 -diaminodiphenylsulfone or 4,4 -methylenebis(3-chloro 2,6-
diethylaniline). The influence of the TPs on the epoxy–amine kinetics is
investigated. It is found that PSF can act as a catalyst. The presence of the TP
provokes an increase of the gel times.
Valéria et al (2005) prepared composites using epoxy resin (ER),
carboxyl-terminated butadiene acrylonitrile copolymer (CTBN) and hydroxyl-
terminated polybutadiene (HTPB), in different proportions. A chemical link
between the HTPB and the epoxy resin was promoted employing tolylene
diisocyanate (TDI). The reactions between elastomers and epoxy resin were
followed by FTIR. The mechanical properties of the composites were evaluated
and the microstructure was investigated through scanning electronic microscopy
(SEM). The results showed that the impact resistance of the CTBN-modified ER
was superior to that of the pure epoxy resin. For the composites with HTPB, the
impact resistance increased with elastomer concentration of up to three parts per
hundred parts of resin (phr). Higher concentrations of HTPB resulted in larger
particles and gave lower impact values.
Maity et al (2007) modified the diglycidyl ether of bisphenol-A
(DGEBA) resin with amine functional aniline acetaldehyde condensate
(AFAAC), and cured with an ambient temperature curing agent triethylene
tetramine. The resulting networks displayed significantly improved fracture
39
toughness. The AFAAC was synthesized by the condensation reaction of
aniline and acetaldehyde in the acid medium (pH 4) and characterized by
FTIR and NMR spectroscopy, elemental analysis, viscosity measurements,
and mole of primary and secondary amine analysis. The DGEBA and
AFAAC were molecularly miscible, but developed a two-phase
microstructure upon network formation. Epoxy/AFAAC compositions were
systematically varied to study the effect of AFAAC concentration on the
impact, adhesive, tensile, and flexural properties of modified networks. The
dynamic mechanical analysis and scanning electron microscopy studies
showed two phase morphology in the cured networks, where AFAAC
particles were dispersed. The AFAAC modified epoxy network was thermally
stable up to around 280°C.
1.7.2 Epoxy and Cyanate Ester Blends and Composites
Ian Hamerton et al (1998) presented a review article on recent
technological developments in the field of cyanate ester resin. In this article,
recent developments in the processing, toughening properties and applications
of the cyanate ester resin are reviewed.
Hwang et al (1999) studied the effect of the composition of
polysulphone (PSF) on the cyanate ester system. From the study it is found
that homogeneous bisphenol A dicyanate (BADCy) / PSF blends with a low
content of PSF (less than 10 wt%) are cured isothermally, and blends are
phase separated by nucleation and growth mechanism to form the PSF
particle structure. But with more than 20 wt% of PSF content the BADCy /
PSF blends are phase separated by spinodal decomposition to form the
BADCy particle structure, and when the PSF content was 15 wt% the blends
are phase separated by nucleation and growth, and spinodal decomposition
resulting in the formation of a combined structure having both PSF and
BADCy particle structure.
40
Roman et al (2000) investigated the effects of temperature and
moisture on the thermal and mechanical properties of thermoplastic and
elastomer toughened high-temperature cyanate ester composite material. The
thermoplastic modified cyanate ester showed increased thermal stability. The
elastomer modified cyanate ester showed the highest mode I fracture
toughness values, primarily because the toughener did not phase separate.
Kimo Chung et al (2001) evaluated the thermomechanical property
changes of carbon fibre/cyanate ester composites by DMA through time-
temperature equivalence. From the study a modelling methodology was
developed which quantitatively provided an understanding of the ageing
process of fibre reinforced composites in isothermal environments.
Ian Hamerton et al (2002) prepared carbon fibre impregnated tape
from a range of prepolymers comprising several different blends of akenyl
functionalized cyanate ester monomers with commercial cyanate ester and
BMI monomers and blends. Incorporation of akenyl-functionalised cyanate
ester monomers into commercial cyanate ester/ BMI blends raised the Tg
value while maintaining GIC and other mechanical properties. This
enhancement in neat resin fracture toughness was translated into the
corresponding composites.
Jerome Dupuy et al (2002) investigated the thermophysical
properties (heat capacity, thermal conductivity) and modelled neat resin and
glass fibre composites. The models are used to stimulate the thermal transfers
in an instrumented heated mould. The calculated local temperatures and
surface heat fluxes appear to be in very good agreement with measurements
for both the neat resin and the composite. The moisture absorption studies of
cyanate ester modified epoxy resin matrices under constant hydrothermal
conditions are an attempt to understand the so-called “reverse thermal effect.”
From the swelling study it is argued that in the initial stage of the absorption
41
process the water diffuses into the regions of volume equal to or greater than
the volume of water molecules, which does not result in swelling. In the later
stage, the water molecules penetrate the regions with a volume less than that
of the volume of water molecules, with molecular reorganization of the resin
network, resulting in swelling (Sunil K. Karad et al 2002).
Shinn-Gwo Hong et al (2003) studied the effect of copper oxide on
the thermal degradation of bis-maleimide triazine (BT) prepreg with IR, ATR
and TGA. The results indicate that the thermal degradation in the bulk BT is
mainly from the epoxy constituent while that in the copper oxide contacted
BT happens not only from the epoxy but also from the more stable cyanate
ester constituent.
Baochun Gwo et al (2003) investigated the chemical nature of the
changes in a cyanate ester-novolac epoxy resin blend caused by hygrothermal
ageing, and the effects of the residual reaction in the blends on the
hygrothermal ageing resistance. The results of the study indicate that the
long-term hygrothermal ageing may cause substantial changes in the chemical
nature of the blends when the cure extent is not sufficiently high.
Tim J. Wooster et al (2003) studied the effect of filler incorporation
on the thermal, mechanical and conductivity properties of cyanate ester
composites. From the study it is concluded that silica filler increased the
thermal conductivity, Young’s modulus and dielectric constant (slightly) and
decreased thermal expansion. It is also found that the addition of silica
resulted in a marginal decrease in strength.
Sabyasachi Ganguli et al (2003) prepared nanocomposites of
cyanate ester by dispersing organically modified layered silicate into the
resin. The inclusion of only 2.5 % by weight of organically modified layered
silicates showed a 30% increase in both the modulus and toughness.
42
1.7.3 PZT Modified Polymer Composites
Edward et al (1987) presented analytical and experimental studies
on piezoelectric actuators as elements of intelligent structures with highly
distributed actuators, sensors and processing networks. Static and dynamic
analytical models are derived for segmented piezoelectric actuators that are
either bonded to an elastic substructure or embedded in a laminated
composite.
Lee (1991) developed a piezoelectric laminate theory that uses the
piezoelectric phenomenon to effect distributed control and sensing of
bending, torsion, shearing, shrinking and stretching of a flexible plate. The
reciprocal relationship of the piezoelectric sensor and actuators is unveiled.
Dimitriadis et al (1991) analytically investigated the behavior of two
dimensional patches of piezoelectric material bonded to the surface of elastic
distributed structures, and used as vibration actuators to the supported elastic
structure. The theory is then applied to develop an approximate dynamic
model of the vibration response of a simply supported elastic rectangular plate
excited by a piezoelectric patch of variable rectangle geometry.
Woo-Seok Hwang et al (1993) presented a finite element
formulation for the vibration control of a laminated plate with piezoelectric
sensors/actuators. The classical lamination theory with the induced strain
actuation and Hamilton’s principle are used to formulate the equations of
motion. The total charge developed on the sensor layer is calculated from the
direct piezoelectric equation of motion.
Ghosh and Batra (1995) showed the deflection of the centerline of a
simply supported plate and the tip deflection of a cantilever plate, both
43
deformed quasistatically, that can be controlled by applying suitable voltage
to the PZTs. The first order shear deformation theory is used to study the
infinitesimal elastic deformations. The adhesive between the PZT and the
plate is assumed to be of negligible thickness, and the displacement and
surface tractions across the interfaces between the PZTs and the plate were
taken to be continous.
Paul Heyliger and Saravanos (1995) developed exact solutions for
predicting the coupled electro mechanical vibration characteristic of simply
supported laminated piezoelectric plates composed of orthorhombic layers.
The three dimensional equations of motion and the charge equations are
solved using the assumptions of the linear theory of piezoelectricity.
Dimitris A Saravanaos et al (1997) presented the structural
mechanics for the analysis of laminated composite plate structures with
piezoelectric actuators and sensors. The theories implement the layer wise
representation of displacements and electric potentials, and can model both
the global and local electromechanical response of smart composite
laminates.Finite element formulations are developed for the quasi-static and
dynamic analyzing of smart composite structures containing piezoelectric
layers.
Vardarajan et al (1998) discussed the shape control of a laminated
composite plate with integrated piezoelectric actuator. The effectiveness of
the piezoelectric actuators and position sensors is investigated for shape
control under the influence of quasi statically varying unknown loads.
Hernandes et al (2000) investigated the free vibration behavior of
thin composite plates with surface bonded piezoelectric patches, including
stress stiffening effects. A finite element formulation is presented, based on
the Reissener mindlin theory and including non-linear strain displacement
relations to formulate a free vibration Eigen value problem in the presence of
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a geometric stiffness matrix. The case of the symmetric laminate and ideal
linear behavior is assumed for the piezoelectric actuation.
Hori et al (2001) developed new types of piezoelectric damping
materials, piezoelectric ceramic (PZT) powder/carbon black (CB)
powder/epoxy (EP) resin composites, and studied their mechanical and
damping properties. Here, the mechanical energy of vibrations and noises
were transformed into electric energy (current) by PZT, and the electric
current was conducted to an external circuit through CB powders and then
dissipated as thermal energy through a resistor. When CB was added to
PZT/EP (70/30 in wt%), the mechanical loss factor (h), a measure of the
mechanical and damping intensity, showed a maximum value of 0.08 at the
CB content of 0.51 wt%, at which the CB particles electrically just contact
each other. In this work, it was found that the PZT/CB/EP composite of
90.0/0.5/9.5 shows a large h value of 0.15.
Hajime Kishi et al (2004) characterized the damping properties of
carbon fiber-reinforced interleaved epoxy composites. Several types of
thermoplastic-elastomer films, such as polyurethane elastomers, polyethylene-
based ionomers and polyamide elastomers were used as the interleaving
materials. The damping properties of the composite laminates with/without
the interleaf films were evaluated by the mechanical impedance method. Also,
the effects of the lay-up arrangements of the carbon-fiber prepregs on the
damping properties of the interleaved laminates were examined. The
viscoelastic properties of the interleaved polymer films were reflected in the
damping properties of the corresponding interleaved laminates. The loss
tangent of the interleaf films at the test temperature played an important role
in the loss factor of the interleaved laminates. Also, the stiffness of the films
at the resonant frequency of the laminates was another important parameter
that controlled the loss factor of the interleaved laminates.
45
Botelho et al (2005) determined the viscoelastic properties, such as
the storage modulus (E’) and loss modulus (E’’), for a glass fiber/epoxy
composite, aluminum 2024-T3 alloy and for a glass fiber/epoxy/aluminum
laminate (Glare). It was found that the glass fiber/epoxy (G/E) composites
decrease the E’ modulus during hygrothermal conditioning up to the
saturation point (6 weeks). However, for Glare laminates the E’’ modulus
remains unchanged (49 GPa) during the cycle of hygrothermal conditioning.
The outer aluminum sheets in the Glare laminate shield the G/E composite
laminae from moisture absorption, which in turn prevent, to a certain extent,
the material from hygrothermal degradation effects.
Botelho et al (2006) investigated the viscoelastic properties, such as
elastic (E’), and the viscous (E’’) responses were obtained for the aluminum
2024 alloy, carbon fiber/epoxy, glass fiber/epoxy and their hybrids aluminum
2024 alloy/carbon fiber/epoxy and aluminum 2024 alloy/glass fiber/epoxy
composites. The experimental results were compared with the calculated E
modulus values by using the composite micromechanics approach. For all the
specimens studied, the experimental values showed good agreement with the
theoretical values. The damping behavior, i.e., the storage modulus and the
loss factor, from the aluminum 2024 alloy and fiber epoxy composites can be
used to estimate the viscoelastic response of the hybrid FML
Tsantzalis et al (2007) investigated the fracture toughness of carbon
fiber reinforced polymer (CFRP) laminates doped with carbon nanofibers
(CNF) and/or piezoelectric (PZT) particles. An increase of 100% in fracture
energy was observed after the addition of 1% CNF in the matrix of the
laminates. The investigation of the fracture surfaces showed extensive fiber
bridging because of the presence of CNFs, which verifies the enhanced
fracture properties. On the other hand, the introduction of PZT particles led to
46
a reduction in the fracture toughness, mainly due to the brittle character of the
particle inclusions.
Jian Gu et al 2007 prepared and characterized the high damping
properties of the promising low density epoxy/fly ash composites, a series of
epoxy composites filled with fly ash of a different volume fraction. Damping
tests of cured epoxy composites are performed in the temperature range of
40 to 150 C and in the frequency range of 10 to 800 Hz, by using a tension-
compression mode. The results show that the values of tangent delta (tan )
reach their peak values at the glass transition temperatures for the composites
with 30–50 vol.% fly ash, and the tan values attenuate slowly with the
increase in frequency, which indicates that the damping properties of such
composites are better than those of other composites. Scanning electron
microscopy was used to observe the fractured surfaces of the composites, and
to clarify the dispersion and distribution of fly ash particulates in the matrix.
In addition, the thermogravimetric curves were also employed to characterize
the heat-resistant performance of the composites.
Tsantzalis et al (2007) studied vapor growth carbon nanofibers
(CNF), lead zirconate titanate piezoelectric (PZT) particles, as well as a
combination of these two added in an epoxy resin (EP), and their influence on
the mechanical quasi-static properties. Moreover, the prepared samples were
characterized by a dynamic thermal mechanical analysis, and optical and
scanning electron microscopy. An enhancement of the mechanical properties
was observed by the addition of the CNF. The uncured mixtures were also
used as matrix material for manufacturing unidirectional carbon fiber
reinforced laminates.
In this paper, the author, Toshio Tanimoto, summarizes the previous
works on the passive damping of carbon-fiber reinforced plastic (CFRP)
cantilever beams using: (1) interleaving of viscoelastic thermoplastic films,
47
(2) surface-bonded piezoelectric ceramics, and (3) dispersed PZT particle
interlayers. Introducing polyethylene-based film interlayers between
composite plies resulted in a significant increase in the vibration loss factor. It
is also shown that the vibration damping of CFRP laminates can be improved
passively by means of resistively shunted, surface-bonded piezoelectric
ceramic, PbZrO3–PbTiO3 (PZT) sheets.
Kostopoulos et al (2007) investigated the influence of carbon
nanofibers (CNF) and/or piezoelectric (PZT) particles on the fracture
behaviour of carbon fiber reinforced polymer laminates. For this purpose the
fillers were added as dopants in the epoxy matrix of the laminates. An
increase of 100% in the fracture energy was observed after the addition of 1%
CNF in the matrix of the laminates, while the introduction of the PZT
particles led a to reduction in the fracture energy, mainly due to the brittle
character of the particle inclusions. In addition, the acoustic emission
technique was used for monitoring the fracture process of the laminates.
Rodríguez et al (2008) investigated the catalytic performance of
3 wt.% copper supported on carbon nanofibers (CNFs) in liquid phase
oxidation, using a batch stirred tank microreactor in order to determine the
decolorization and total organic carbon (TOC) removal efficiency in washing
textile wastewater (WTW). A preliminary study was carried out in a
temperature range of 120–160 °C and two oxygen partial pressures of 6.3 and
8.7 bar. TOC removal and toxicity reduction were as high as 74.1% and 43%,
respectively at 140 °C and 8.7 bar, after 180 min reaction. The main
intermediates detected in raw wastewater were decanoic acid, methyl ester
and 1,2-benzenedicarboxylic acid, and they have been degraded by means of a
Cu/CNF catalyst. The application of CWAO to the treatment of a textile
effluent at 160 °C and 8.7 bar of oxygen partial pressure showed that the use
of a Cu/CNF catalyst significantly improves the TOC and color removal
48
efficiencies, and it can be considered as an option for a pretreatment step in
the treatment of these industrial effluents.
Sheng Tian et al (2008) prepared a new type of rigid piezo-damping
epoxy-matrix composites, containing multi-walled carbon nanotubes(CNT)
and piezoelectric lead zirconate titanate (PZT), and investigated their
electrical and damping properties. The dynamic mechanical thermal analysis
revealed that the loss factors of the composites were improved by the
incorporation of PZT and CNT under the concentration above a critical
electrical percolation. Based on this piezo-damping material, the PZT
contributes to the transformation of mechanical noise and vibration energies
into electric energy, while the CNT serves in the shorting of the generated
electric current to the external circuit. An optimum formulation for the piezo-
damping epoxy based materials can be designed on the basis of the results of
this study.
1.7.4 Engine Coating
Dennis N. Assanis (1988) deals with the transient analysis of piston-
liner heat transfer in low-heat-rejection diesel engines.A two-dimensional
finite element program has been developed to analyze the transient heat flow
paths in low-heat-rejection engine combustion chambers. This analysis tool
has been used to study the transient heat transfer performance of a ceramic-
coated piston-liner assembly and compare it with the performance of baseline
cast-iron components. The direction of the gas-to-liner and piston-to-liner
heat flux, changes several times during the cycle, and these changes occur at
different instants, as the distance from the cylinder fire-deck varies. In the
conventional metal engine, heat flows from the relatively hotter piston to the
liner, via the rings for most part of the cycle. In contrast, for the LHR
configuration, the net heat transfer is from the liner to the rings, and thus to
the piston.
49
Miyairi (1988) deals with the computer simulation of a low heat
rejection direct injection diesel engine using a two zone combustion model
and Anand’s heat transfer model. Spray penetration, deflection, growth, and
rate of entrainment were considered under the steady state condition. The
combustion and heat transfer characteristics were studied in this literature by
taking into account the high temperature swing in the low heat rejection
engines. The heat transfer through the combustion chamber components was
studied, by solving the unsteady conduction heat transfer equations. This
literature is used in this work as a basic support for the formulation of various
models for the combustion and heat transfer calculations.
Randolph A Churchill et al (1988) studied a low heat rejection
engine. Reducing heat losses from the engine cylinder makes minimal
changes to the efficiencies of the existing engines. It reduces the need for
cooling systems and their cost, reducing weight and reducing the complexity.
Partially stabilized zirconia has been developed, that decreases the magnitude
of the phase changes and is now considered a good candidate for engine use.
Recovering the available exhaust heat will also aid in controlling pollution. It
may be possible to build an unlubricated engine with 55% thermal efficiency.
Jorge J.G.Martins (2004) deals with the thermodynamic analysis of
an over expanded engine. The equation of an over-expanded engine is
developed with the equation for the otto cycle, diesel cycle and dual cycle at
part load condition. It is clear that the most efficient cycle under light and part
load condition is the miller cycle with a fixed trapped compression ratio,
particularly at very low loads (0.3 to 0.4), where it can achieve theoretical
efficiencies approaching 73%. In the diesel cycle, the amount of intake air is
the same as there is no restriction on the intake. So, the change in the cycle
configuration to a lower load will be the reduction of heat supplied during the
isobaric heating.